Powered by Deep Web Technologies
Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


1

Data:D4d0defa-3abe-4a7f-9538-3e1cdf1b906a | Open Energy Information  

Open Energy Info (EERE)

d0defa-3abe-4a7f-9538-3e1cdf1b906a d0defa-3abe-4a7f-9538-3e1cdf1b906a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Butler Rural Electric Coop Inc Effective date: 2012/10/01 End date if known: Rate name: General Service-Seasonal Service(Single Phase) Sector: Commercial Description: Consumers during intermittent single-phase service and transformer capacity not to exceed 25KVa,located in non permanent structured such as campers or mobile homes not permanently in place,or areas zoned as planned recreational vehicle parks,for uses subject to established rules and regulations of the cooperative may be served under this schedule on an annual basis.

2

Data:C6cdf6fb-f3cb-4851-abee-ad65362075a2 | Open Energy Information  

Open Energy Info (EERE)

fb-f3cb-4851-abee-ad65362075a2 fb-f3cb-4851-abee-ad65362075a2 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Marshfield, Wisconsin (Utility Company) Effective date: 2012/02/01 End date if known: Rate name: Gs-1 General Service Single Phase less than 50kW Demand with Parallel Generation(20kW or less) Sector: Commercial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0515 per kilowatt-hour.

3

CDF photos  

NLE Websites -- All DOE Office Websites (Extended Search)

- Identifying Particles - D0 Detector - CDF Detector - Links Project Contact: Thomas Jordan - jordant@fnal.gov Web Maintainer: qnet-webmaster@fnal.gov Last Update: April 13, 2001...

4

Data:89596325-a877-4943-96b0-556b68909034 | Open Energy Information  

Open Energy Info (EERE)

6325-a877-4943-96b0-556b68909034 6325-a877-4943-96b0-556b68909034 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Lincoln Electric System Effective date: End date if known: Rate name: Large Power Contract Off-Peak Dual Primary Sector: Description: Excess kVA Source or reference: http://www.les.com/your_business/rate_schedules_lpc.aspx Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >>

5

CDF Top Physics  

DOE R&D Accomplishments (OSTI)

The authors present the latest results about top physics obtained by the CDF experiment at the Fermilab Tevatron collider. The data sample used for these analysis (about 110 pb{sup{minus}1}) represents almost the entire statistics collected by CDF during four years (1992--95) of data taking. This large data size has allowed detailed studies of top production and decay properties. The results discussed here include the determination of the top quark mass, the measurement of the production cross section, the study of the kinematics of the top events and a look at top decays.

Tartarelli, G. F.; CDF Collaboration

1996-05-00T23:59:59.000Z

6

Diffraction Results from CDF  

Science Conference Proceedings (OSTI)

We present final results by the CDF II collaboration on diffractive W and Z production, report on the status of ongoing analyses on diffractive dijet production and on rapidity gaps between jets, and briefly summarize results obtained on exclusive production pointing to their relevance to calibrating theoretical models used to predict exclusive Higgs-boson production at the LHC.

Goulianos, Konstantin

2012-04-01T23:59:59.000Z

7

QCD results at CDF  

SciTech Connect

Recent QCD measurements from the CDF collaboration at the Tevatron are presented, together with future prospects as the luminosity increases. The measured inclusive jet cross section is compared to pQCD NLO predictions. Precise measurements on jet shapes and hadronic energy flows are compared to different phenomenological models that describe gluon emissions and the underlying event in hadron-hadron interactions.

Norniella, Olga; /Barcelona, IFAE

2005-01-01T23:59:59.000Z

8

NetCDF at NERSC  

NLE Websites -- All DOE Office Websites (Extended Search)

NetCDF NetCDF NetCDF Description and Overview NetCDF (Network Common Data Form) is a set of software libraries and machine-independent data formats that support the creation, access, and sharing of array-oriented scientific data. This includes the libnetcdf.a library as well as the NetCDF Operators (NCO), Climate Data Operators (CDO), NCCMP, and NCVIEW packages. Files written with previous versions can be read or written with the current version. Using NetCDF on Cray System There are separate NetCDF installations provided by Cray and by NERSC. On Hopper and Edison, Cray installations are recommended because they are simpler to use. To see the available Cray installations and versions use the following command: module avail cray-netcdf To see the NERSC installations and versions use the following command:

9

Data:Ce7bcd1a-3552-4059-96b7-c45de0244033 | Open Energy Information  

Open Energy Info (EERE)

bcd1a-3552-4059-96b7-c45de0244033 bcd1a-3552-4059-96b7-c45de0244033 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Nebraska Public Power District Effective date: 2013/01/01 End date if known: Rate name: 100 W High Pressure Sodium- Post Top Nonwood Sector: Lighting Description: To all night street lighting service (dusk to daylight) from the overhead systems conforming to the District's standard specifications. Nonwood; Post Top Electricity is provided through the Village, which obtains electric power from Nebraska Public Power District (NPPD) Source or reference: http://www.nppd.com/assets/municipalstreetlightingservice.pdf

10

Data:6b720975-87b5-4806-a93d-96b520026853 | Open Energy Information  

Open Energy Info (EERE)

20975-87b5-4806-a93d-96b520026853 20975-87b5-4806-a93d-96b520026853 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: UNS Electric, Inc Effective date: 2011/01/01 End date if known: Rate name: Rider - 5 General Service - SGS-10 Sector: Commercial Description: Pricing Plan Rider-5 is for individually metered customers who wish to participate in the Bright Arizona Community Solar Program. Under Rider-5, customers will be able to purchase blocks of electricity from solar generation sources. Participation in Rider-5 is limited in the Company's sole discretion to the amount of solar generation available and subscription will be made on a first come, first served basis.

11

Data:Cc506003-6304-4767-96b9-822276df7d4d | Open Energy Information  

Open Energy Info (EERE)

03-6304-4767-96b9-822276df7d4d 03-6304-4767-96b9-822276df7d4d No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: PUD No 1 of Klickitat County Effective date: End date if known: Rate name: Irrigation Service TOU Single Phase Sector: Description: Source or reference: http://www.klickitatpud.com/ratesAndPolicies/electricRates/rateSchedule51.aspx Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous

12

Data:7ad16ffd-9864-433c-96b7-8978781281e6 | Open Energy Information  

Open Energy Info (EERE)

ffd-9864-433c-96b7-8978781281e6 ffd-9864-433c-96b7-8978781281e6 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: East Central Oklahoma Elec Coop Inc Effective date: 1996/05/02 End date if known: Rate name: Residential Time-Of-Use, Schedule TOU-R Sector: Residential Description: Farm and residential customers Source or reference: Rates Binder B #4 Source Parent: Comments Subject to Power Cost Adjustment and Tax Adjustment Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

13

CDF results on B decays  

SciTech Connect

The authors present recent CDF results on B lifetimes, B meson mass measurements, ratios of branching ratios, and rare decays. In addition, they present the first measurement of time-dependent B{sub d} mixing at CDF. Several results have been updated and a few new ones included since the workshop.

Skarha, J.E. [Johns Hopkins Univ., Baltimore, MD (United States)

1995-05-01T23:59:59.000Z

14

Top Physics at CDF  

Science Conference Proceedings (OSTI)

We present the recent results of top-quark physics using up to 6 fb{sup -1} of p{bar p} collisions at a center of mass energy of {radical}s = 1.96 TeV analyzed by the CDF collaboration. Thanks to this large data sample, precision top quark measurements are now a reality at the Tevatron. Further, several new physics signals could appear in this large dataset. We will present the latest measurements of top quark intrinsic properties as well as direct searches for new physics in the top sector.

Moon, Chang-Seong

2011-06-01T23:59:59.000Z

15

CDF Hot Topics  

SciTech Connect

We present recent CDF results based on approximately 1 fb{sup -1} of p{bar p} collisions at {radical}s = 1.96 TeV delivered at Fermilab Tevatron. Results shown include the observation of the B{sub s} oscillation frequency, the first observation of bottom baryon {Sigma}{sub b}{sup (*){+-}} states, updates on B hadrons lifetimes, and searches for rare decays in the b {yields} s{mu}{sup +}{mu}{sup -} transition and in charmless two-body B decays.

Casal, B.; /Cantabria Inst. of Phys.

2007-06-01T23:59:59.000Z

16

SM Higgs Searches at CDF  

SciTech Connect

We present the latest CDF searches for the Standard Model Higgs boson with 1.96 TeV center-of-mass energy collisions produced at the Fermilab Tevatron. The data was collected with the CDF II detector at the Tevatron collider and correspond to an integrated luminosity from 2 to 4.8 1/fb. To achieve maximal sensitivity, many channels are analyzed including final states from gluon fusion, vector boson fusion, and associated production with W and Z bosons.

Alvarez Gonzalez, Barbara; /Oviedo U.

2010-06-01T23:59:59.000Z

17

The CDF Silicon Vertex Detector  

Science Conference Proceedings (OSTI)

A silicon strip vertex detector was designed, constructed and commissioned at the CDF experiment at the Tevatron collider at Fermilab. The mechanical design of the detector, its cooling and monitoring are presented. The front end electronics employing a custom VLSI chip, the readout electronics and various components of the SVX system are described. The system performance and the experience with the operation of the detector in the radiation environment are discussed. The device has been taking colliding beams data since May of 1992, performing at its best design specifications and enhancing the physics program of CDF.

Tkaczyk, S.; Carter, H.; Flaugher, B. [and others

1993-09-01T23:59:59.000Z

18

Higgs bosons searches at CDF  

SciTech Connect

Advanced analysis techniques together with increasing data samples are bringing the sensitivity of CDF to the Higgs boson very close to the SM predictions. These improvements translate into more stringent exclusions of parameter space in BSM Higgs sectors and of the SM mass range. The CDF Collaboration has a very active program on Higgs searches that comprises most accessible production mechanisms and decay channels in {bar p}p collisions at {radical}s = 1.96 TeV. This contribution will also review the combination of the different channels, data samples and analysis techinques that currently produces one of the most exciting experimental results in our field.

Cuenca Almenar, Cristobal; /UC, Irvine

2010-01-01T23:59:59.000Z

19

Rare B decays at CDF  

SciTech Connect

The confidence level limits of the CDF search for the B{sub s}{sup 0} and B{sub d}{sup 0} {yields} {mu}{sup +}{mu}{sup -} rare decays and the branching ratio measurement of B{sub s}{sup 0} {yields} D{sub s}{sup +} D{sub s}{sup -} are presented.

Farrington, Sinead M.; /Liverpool U.

2006-10-01T23:59:59.000Z

20

Top physics results at CDF  

SciTech Connect

The most recent results on top quark physics at CDF are reported. Measurements of cross-section and mass are presented, and the status of single top quark production searches are discussed. The results obtained from probing various top quark properties are also presented.

Vickey, Trevor; /Illinois U., Urbana

2005-05-01T23:59:59.000Z

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


21

Commissioning the CDF offline software  

SciTech Connect

CDF II is one of the two large collider experiments at Fermilab's Tevatron. Over the past two years we have commissioned the offline computing system. A task that has involved bringing up hundreds of computers and millions of lines of C++ software. This paper reports on this experience, concentrating on the software aspects of the project. We will highlight some of the successes as well as describe some of the work still to do.

Elizabeth Sexton-Kennedy and Pasha Murat

2004-03-17T23:59:59.000Z

22

New phenomena searches at CDF  

SciTech Connect

The authors report on recent results from the Collider Detector at Fermilab (CDF) experiment, which is accumulating data from proton-antiproton collisions with {radical}s = 1.96 TeV at Run II of the Fermilab Tevatron. The new phenomena being explored include Higgs, Supersymmetry, and large extra dimensions. They also present the latest results of searches for heavy objects, which would indicate physics beyond the Standard Model.

Soha, Aron; /UC, Davis

2006-04-01T23:59:59.000Z

23

Characterization of ultra-fine grained aluminum produced by accumulative back extrusion (ABE)  

SciTech Connect

In the present work, the microstructural evolutions and microhardness of AA1050 subjected to one, two and three passes of accumulative back extrusion (ABE) were investigated. The microstructural evolutions were characterized using transmission electron microscopy. The results revealed that applying three passes of accumulative back extrusion led to significant grain refinement. The initial grain size of 47 {mu}m was refined to the grains of 500 nm after three passes of ABE. Increasing the number of passes resulted in more decrease in grain size, better microstructure homogeneity and increase in the microhardness. The cross-section of ABEed specimen consisted of two different zones: (i) shear deformation zone, and (ii) normal deformation zone. The microhardness measurements indicated that the hardness increased from the initial value of 31 Hv to 67 Hv, verifying the significant microstructural refinement via accumulative back extrusion. - Highlights: Black-Right-Pointing-Pointer A significant grain refinement can be achieved in AA1050, Al alloy by applying ABE. Black-Right-Pointing-Pointer Microstructural homogeneity of ABEed samples increased by increasing the number of ABE cycles. Black-Right-Pointing-Pointer A substantial increase in the hardness, from 31 Hv to 67 Hv, was recorded.

Alihosseini, H., E-mail: hamid.alihossieni@gmail.com [Mechanical Engineering Department, University of Tehran, Tehran (Iran, Islamic Republic of); Materials Science and Engineering Department, Engineering School, Amirkabir University, Tehran (Iran, Islamic Republic of); Faraji, G.; Dizaji, A.F. [Mechanical Engineering Department, University of Tehran, Tehran (Iran, Islamic Republic of); Dehghani, K. [Materials Science and Engineering Department, Engineering School, Amirkabir University, Tehran (Iran, Islamic Republic of)

2012-06-15T23:59:59.000Z

24

Collider Detector at Fermilab (CDF): Data from Supersymmetry, New Phenomena Research of the CDF Exotics Group  

DOE Data Explorer (OSTI)

The Collider Detector at Fermilab (CDF) is a Tevatron experiment at Fermilab. The Tevatron, a powerful particle accelerator, accelerates protons and antiprotons close to the speed of light, and then makes them collide head-on inside the CDF detector. The CDF detector is used to study the products of such collisions. The CDF Physics Group at Fermilab is organized into six working groups, each with a specific focus. The Exotics group searches for Supersymmetry and other New Phenomena. Their public web page makes data and numerous figures available from both CDF Runs I and II.

25

CDF Status and B Physics Prospects  

Science Conference Proceedings (OSTI)

With extensive upgrades to the detector and electronics, CDF has started collecting data with Run II of the Tevatron. The enhanced silicon coverage and the use of silicon based tracks in the trigger, make CDF well suited for a broad program of B hadron measurements. We present the current status of the experiment and prospects for measurements in Run II.

J. Stephen Miller

2002-10-07T23:59:59.000Z

26

Top quark physics at CDF  

SciTech Connect

We present the recent results of top-quark physics using up to 6 fb{sup -1} of p{bar p} collisions analyzed by the CDF collaboration. The large number of top quark events analyzed, of the order of several thousands, allows stringent checks of the standard model predictions. Also, the top quark is widely believed to be a window to new physics. We present the latest measurements of top quark intrinsic properties as well as direct searches for new physics in the top sector.

Potamianos, Karolos

2011-12-01T23:59:59.000Z

27

Search for Higgs at CDF  

E-Print Network (OSTI)

We present the results on the searches for the SM and the non-SM Higgs boson production in ppbar collisions at sqrt(s)=1.96 TeV with the CDF detector at the Fermilab Tevatron. Using data corresponding to 300--700pb-1, we search for the Higgs boson in various production and decay channels. No signal is observed, therefore, we set upper limits on the production cross-section times branching fraction as a function of the Higgs boson mass.

Shin-Shan Yu

2006-10-18T23:59:59.000Z

28

Higgs Boson Searches at CDF  

SciTech Connect

Results are presented on searches for standard model and non-standard model production of a Higgs boson in pbar-p collisions at {radical}s = 1.96 TeV with the CDF II detector at the Fermilab Tevatron. Using data corresponding to 2-3.6 1/fb of integrated luminosity, searches are performed in a number of different production and decay modes. No excess in data above that expected from backgrounds is observed; therefore, we set upper limits on the production cross section times branching fraction as a function of the Higgs boson mass.

Group, Robert Craig; /Fermilab

2009-05-01T23:59:59.000Z

29

Search for Higgs at CDF  

SciTech Connect

We present the results on the searches for the SM and the non-SM Higgs boson production in p{bar p} collisions at {radical}s = 1.96 TeV with the CDF detector at the Fermilab Tevatron. Using data corresponding to 300-700 pb{sup -1}, we search for the Higgs boson in various production and decay channels. No signal is observed, therefore, we set upper limits on the production cross-section times branching fraction as a function of the Higgs boson mass.

Yu, Shin-Shan; /Fermilab

2006-10-01T23:59:59.000Z

30

Data:8ac9ddbc-cd04-4f5b-9557-f4822a96b8db | Open Energy Information  

Open Energy Info (EERE)

ac9ddbc-cd04-4f5b-9557-f4822a96b8db ac9ddbc-cd04-4f5b-9557-f4822a96b8db No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Russell, Massachusetts (Utility Company) Effective date: 2009/01/01 End date if known: Rate name: RESIDENTIAL SERVICE SCHEDULE R1- FARM DISCOUNT Sector: Residential Description: Additional Info: Availability: To residential customers for all domestic uses in individual residences or apartments. It includes 10% farm discount. Minimum Bill: $4.50. Flat rate buy = Distribution + Transmission + Generation. Flat rate Adjustment = TAC + ECS + PPA. Source or reference: http://www.townofrussell.us/ElectricRates.html

31

Data:Bae9114f-4066-401d-96b3-a71a837c4ead | Open Energy Information  

Open Energy Info (EERE)

Bae9114f-4066-401d-96b3-a71a837c4ead Bae9114f-4066-401d-96b3-a71a837c4ead No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Shawano Municipal Utilities Effective date: 2007/08/20 End date if known: Rate name: Residential Single Phase Sector: Residential Description: Source or reference: http://www.shawano.tv/id75.html Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous

32

Data:5ecfcad3-df00-4719-80bc-8c0f96b94ce6 | Open Energy Information  

Open Energy Info (EERE)

ecfcad3-df00-4719-80bc-8c0f96b94ce6 ecfcad3-df00-4719-80bc-8c0f96b94ce6 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Northeast Nebraska P P D Effective date: 2013/01/01 End date if known: Rate name: Schedule L - Special Annual Lighting Sector: Lighting Description: Availability All customers are eligible to lease private lighting owned and maintained by NeNPPD. This leased lighting is unmetered and NeNPPD provides all of the energy required. See other side for private lighting service agreement Source or reference: www.nnppd.com/billing/rates/ Source Parent: Comments Applicability Demand (kW)

33

Data:D19c53df-3351-4b2d-a96b-cbe3ce02af56 | Open Energy Information  

Open Energy Info (EERE)

df-3351-4b2d-a96b-cbe3ce02af56 df-3351-4b2d-a96b-cbe3ce02af56 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: New Hampshire Elec Coop Inc Effective date: 2013/05/01 End date if known: Rate name: Ski Area Contract (1000 KVA)SKI Sector: Commercial Description: The Coop Power rate will be NHEC's cost for procuring energy service and other NEPOOL Products applicable for the member's hourly load, adjusted to retail for losses and for NHEC administrative costs. Source or reference: http://www.nhec.com/filerepository/rate_change_sheets_for_2013_may01_final.pdf Source Parent:

34

Data:3727be14-96b6-46b7-9501-b97fc69a2366 | Open Energy Information  

Open Energy Info (EERE)

4-96b6-46b7-9501-b97fc69a2366 4-96b6-46b7-9501-b97fc69a2366 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Ninnescah Rural E C A Inc Effective date: 2012/03/01 End date if known: Rate name: Three Phase Service Sector: Commercial Description: Available for three-phase general usage service of 60 kW and under and single character supplied at one point of delivery, subject to the cooperative's established rules and regulations. Source or reference: Rate Binder #7 (Illinois State University) Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh)

35

Data:E1cd96c4-8117-4576-96b0-3e10685fc5e0 | Open Energy Information  

Open Energy Info (EERE)

cd96c4-8117-4576-96b0-3e10685fc5e0 cd96c4-8117-4576-96b0-3e10685fc5e0 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Washington Elec Member Corp Effective date: End date if known: Rate name: Rate-07 (GSD) Sector: Commercial Description: To all electric service consumers, other than for residential use, whose transformer capacity requirements are fifty (50) kVA or greater. Electric service of one standard voltage is delivered at one point and metered at or compensated to that voltage. Source or reference: http://facts.psc.state.ga.us/Public/GetDocument.aspx?ID=129296 Source Parent: Comments

36

Data:C21f9094-9531-4a3a-a975-46557d1bc96b | Open Energy Information  

Open Energy Info (EERE)

94-9531-4a3a-a975-46557d1bc96b 94-9531-4a3a-a975-46557d1bc96b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Long Island Power Authority Effective date: 2013/06/01 End date if known: Rate name: 284 - Primary Sector: Commercial Description: Source or reference: www.lipower.org/pdfs/account/rates_comm.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous

37

Data:D12a4ee9-489c-4929-96b2-6324a0b8e925 | Open Energy Information  

Open Energy Info (EERE)

ee9-489c-4929-96b2-6324a0b8e925 ee9-489c-4929-96b2-6324a0b8e925 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Raton Public Service Company Effective date: End date if known: Rate name: Security Lights 3- Prompt Payment Discount Sector: Lighting Description: Security lights are available to all (except as noted) residential, commercial and industrial customers served by the Raton Public Service Company for outside lighting purposes at the voltage and phase of the company's distribution system. RPS owns fixture and pole, power is furnished by customer. RPS furnishes parts & service.

38

Data:E4c54ab2-96b0-434b-8fc1-fd0428454d6e | Open Energy Information  

Open Energy Info (EERE)

ab2-96b0-434b-8fc1-fd0428454d6e ab2-96b0-434b-8fc1-fd0428454d6e No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tillamook Peoples Utility Dist Effective date: 2010/11/01 End date if known: Rate name: AREA LIGHTING SPECIAL RATE FOR LIGHTS - Wide Angle Flood Lights 400w Sector: Lighting Description: "SPECIAL RATE FOR LIGHTS CONNECTED BEHIND CUSTOMER'S METER" Available to all customers for dusk to dawn outdoor area lighting not served under street lighting contract. Service under this schedule is also available for television amplifiers for cable systems, and other flat rate services.

39

Data:Cc836610-fe61-4a96-b75b-dde63bda480c | Open Energy Information  

Open Energy Info (EERE)

Cc836610-fe61-4a96-b75b-dde63bda480c Cc836610-fe61-4a96-b75b-dde63bda480c No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: C & L Electric Coop Corp Effective date: 2012/09/24 End date if known: Rate name: Outdoor Lighting Service - 250 Watt HPS/MH Sector: Lighting Description: Source or reference: ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous

40

Data:Fd2b9529-a0f7-4099-bd77-88d96b2aadba | Open Energy Information  

Open Energy Info (EERE)

9-a0f7-4099-bd77-88d96b2aadba 9-a0f7-4099-bd77-88d96b2aadba No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Danville, Virginia (Utility Company) Effective date: 2012/08/28 End date if known: Rate name: Outdoor Rental Lighting Service- Standard Security Lights- (250W HPS Flood) Sector: Lighting Description: Available for outdoor lighting of yards, walkways and other areas. Lights to be served hereunder shall be at locations that are easily and economically accessible to Utility equipment and personnel for construction and maintenance. Source or reference: http://www.danville-va.gov/DocumentCenter/View/8181

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


41

Data:Ab43dcc9-7038-4e96-b8ff-1f5fff80ef49 | Open Energy Information  

Open Energy Info (EERE)

Ab43dcc9-7038-4e96-b8ff-1f5fff80ef49 Ab43dcc9-7038-4e96-b8ff-1f5fff80ef49 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Perennial Public Power Dist Effective date: 2013/01/01 End date if known: Rate name: URBAN RESIDENTIAL (Rate Code 23) Sector: Residential Description: AVAILABILITY: To residential customers within the corporate limits of the municipalities served by the District. The entire residential service, including any electric space heating and/or water heating service, must be taken through a single meter. TYPE OF SERVICE: A.C., 60 cycles, single-phase or three-phase at any of the District's standard voltages.

42

Data:2f7dc82b-736b-46c0-b96b-ab7a7b948f04 | Open Energy Information  

Open Energy Info (EERE)

b-736b-46c0-b96b-ab7a7b948f04 b-736b-46c0-b96b-ab7a7b948f04 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Clay Electric Cooperative, Inc Effective date: 2011/01/01 End date if known: Rate name: Rate Schedule - L (B) Sector: Lighting Description: Large light, 20,000 Lumens fixture mounted on a Cooperative pole. Source or reference: https://www.clayelectric.com/rates.aspx Source Parent: Comments 87 kWh/month estimate. $10.25 fixed monthly is per customer which is added to a $3.50/customer/month for the cooperatives pole (if necessary). Plus current month's Power Cost Adjustment and applicable taxes.

43

Data:3d5212b3-3731-4f47-96b7-1adf226bd28c | Open Energy Information  

Open Energy Info (EERE)

b3-3731-4f47-96b7-1adf226bd28c b3-3731-4f47-96b7-1adf226bd28c No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Nashville Electric Service Effective date: 2012/12/01 End date if known: Rate name: RS Sector: Residential Description: This rate shall apply only to electric service to a single-family dwelling (including its appurtenances if served through the same meter), where the major use of electricity is for domestic purposes such as lighting, household appliances, and the personal comfort and convenience of those residing therein. Hydro Allocation Credit:1.60$ per month Source or reference: http://www.nespower.com/documents/RSDec12.pdf

44

Data:260485c0-7af8-433d-b85b-96b51dc2d41b | Open Energy Information  

Open Energy Info (EERE)

-7af8-433d-b85b-96b51dc2d41b -7af8-433d-b85b-96b51dc2d41b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Tacoma, Washington (Utility Company) Effective date: 2013/04/01 End date if known: Rate name: Schedule CP - Contract Industrial Sector: Industrial Description: See source for more information Source or reference: www.nytpu.org/file_viewer.aspx?id=6168 Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category:

45

Top Physics Results from CDF  

E-Print Network (OSTI)

The top quark is by far the most massive fundamental particle observed so far, and the study of its properties is interesting for several reasons ranging from its possible special role in electroweak symmetry breaking to its sensitivity to physics beyond the Standard Model. We present recent top physics results from CDF based on 160-320 inverse pb of ppbar collision data at a center-of-mass energy of 1.96 TeV. The ttbar cross section and the top mass have been measured in different decay channels and using different methods. We have searched for evidence of single top production, setting upper limits on its production rate. Other results shown in this conference include studies of the polarization of W bosons from top decays, a search for charged Higgs decaying from top, and a search for additional heavy t' quarks.

Gervasio Gomez

2005-05-30T23:59:59.000Z

46

Search for New Physics at CDF  

E-Print Network (OSTI)

We present the current status of the search for new physics at CDF, using integrated luminosity up to 3.2 fb-1. We cover searches for supersymmetry, extra dimensions, new heavy bosons, and generic dilepton resonances.

John Strologas

2009-06-22T23:59:59.000Z

47

Data:85c17ee4-15f9-4a96-b427-19a7302fb359 | Open Energy Information  

Open Energy Info (EERE)

ee4-15f9-4a96-b427-19a7302fb359 ee4-15f9-4a96-b427-19a7302fb359 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Entergy Gulf States Louisiana LLC Effective date: 2005/09/28 End date if known: Rate name: 2 GS - TOD general service time of use (secondary voltage) Sector: Commercial Description: This rate is applicable on a voluntary basis under the regular terms and conditions of the company to customers having the appropriate metering and who contract for not less than 5 kW or not more than 4000 kW of electric service to be used for general lighting and power. Source or reference: http://www.entergy-louisiana.com/content/price/tariffs/egsi/egsila_gs-tod.pdf

48

Data:1b784821-a30c-4d64-96b0-df4947aea12b | Open Energy Information  

Open Energy Info (EERE)

b784821-a30c-4d64-96b0-df4947aea12b b784821-a30c-4d64-96b0-df4947aea12b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Village of Pardeeville, Wisconsin (Utility Company) Effective date: 2007/10/10 End date if known: Rate name: Rg-1 Residential Service Three Phase with Parallel Generation(20kW or less) Sector: Residential Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0680 per kilowatt-hour.

49

Data:29dcf4eb-9ae8-4070-96b1-d655fb106e84 | Open Energy Information  

Open Energy Info (EERE)

dcf4eb-9ae8-4070-96b1-d655fb106e84 dcf4eb-9ae8-4070-96b1-d655fb106e84 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Duke Energy Indiana Inc Effective date: 2009/09/14 End date if known: Rate name: AL - 100 watt HPS - Post Top - Classic Sector: Lighting Description: Availability This rate schedule is no longer available after September 1, 2004. Potential lighting customers wanting a lighting system installed and maintained by Company can do so via the Outdoor Lighting Equipment agreement (OLE). Potential customers should contact a Company account representative for further information concerning OLE options. This rate schedule terminates May 1, 2014. Customers currently being provided service under this rate schedule can continue being provided service under this rate schedule until their contract expires or this rate schedule terminates, whichever occurs first.

50

Data:6939cbfe-f9d8-4a96-b8ef-6056ccec0dfa | Open Energy Information  

Open Energy Info (EERE)

cbfe-f9d8-4a96-b8ef-6056ccec0dfa cbfe-f9d8-4a96-b8ef-6056ccec0dfa No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Northern States Power Co - Wisconsin Effective date: 2012/01/01 End date if known: Rate name: CUSTOMER OWNED STREET LIGHTING SV 50 W Sector: Lighting Description: Availability: Available for year-round illumination of public streets, parkways, and highways by electric lamps mounted on standards where the customer owns and maintains an Ornamental Street Lighting system complete with standards, luminaires with refractors, lamps and other appurtenances, together with all necessary cables extending between standards and to points of connection to Company's facilities as designated by Company. Mercury Vapor street lighting service under this schedule is limited to the luminaires being served as of December 31, 1987.

51

Data:E9c0221a-8a04-4f3a-96b8-f4b3279ff5db | Open Energy Information  

Open Energy Info (EERE)

a-8a04-4f3a-96b8-f4b3279ff5db a-8a04-4f3a-96b8-f4b3279ff5db No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Grayson Rural Electric Coop Corp Effective date: 2011/06/01 End date if known: Rate name: Schedule 3- Off Peak Marketing Rate Sector: Residential Description: Available to members of the Cooperative eligible for service under Tariff Schedule I-- Domestic-Farm & Home Service, or Tariff Schedule 2--Commercial and Small Power Less than 50 KVA, who have installed Cooperative approved load management devices for the use of power during off-peak hours. This rate shall only apply to programs which have been expressly approved by the Public Service Commission to be offered under the Marketing Rate of East Kentucky Power Cooperative's Wholesale Rate Schedule A.

52

Data:8bbeed18-d96b-4b7c-ba9e-fc73b479ef77 | Open Energy Information  

Open Energy Info (EERE)

bbeed18-d96b-4b7c-ba9e-fc73b479ef77 bbeed18-d96b-4b7c-ba9e-fc73b479ef77 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Algoma Utility Comm Effective date: 2008/05/28 End date if known: Rate name: General Service - Optional Time-of-Day Single Phase less than 100kW 8am-8pm Sector: Industrial Description: Application: This rate schedule is optional to all Gs-1, General Service customers. Customers that wish to be served on this rate schedule must apply to the utility for service. Once an optional customer begins service on this rate schedule, the customer shall remain on the rate for a minimum of one year. Any customer choosing to be served on this rate schedule waives all rights to billing adjustments arising from a claim that the bill for service would be less on another rate schedule than under this rate schedule. Gs-2 General Service Optional TOD $2.25 per customer per month

53

Data:11398f25-15eb-4c96-b0b0-c047f26167d9 | Open Energy Information  

Open Energy Info (EERE)

f25-15eb-4c96-b0b0-c047f26167d9 f25-15eb-4c96-b0b0-c047f26167d9 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Edgecombe-Martin County E M C Effective date: 2006/08/01 End date if known: Rate name: GENERAL SERVICE Three Phase( with Small Renewable Generation Rider) Sector: Commercial Description: AVAILABILITY: Electric service is available under this Schedule in the territory served by the Cooperative for nonresidential use with less than 100 kVA of transformer capacity. Resale and standby services are not permitted. Rates are subject to wholesale power cost adjustments, power factor adjustments,a North Carolina Sales Tax and Rider EE (Energy Efficiency Rider).

54

Data:Eca116ba-8be4-4cf8-b96b-98de1f09a3e1 | Open Energy Information  

Open Energy Info (EERE)

Eca116ba-8be4-4cf8-b96b-98de1f09a3e1 Eca116ba-8be4-4cf8-b96b-98de1f09a3e1 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Village of Enosburg Falls, Vermont (Utility Company) Effective date: 2010/10/01 End date if known: Rate name: Station Service - Rate 6 - 250 kW up to 500 kW Sector: Commercial Description: This rate is available for single and three phase electric service at secondary voltage within the service territory of the village of Enosburg. Source or reference: ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh)

55

Data:489fddc8-0713-4c7f-96b5-5c73cd8f85e8 | Open Energy Information  

Open Energy Info (EERE)

fddc8-0713-4c7f-96b5-5c73cd8f85e8 fddc8-0713-4c7f-96b5-5c73cd8f85e8 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: South Central Ark El Coop, Inc Effective date: 2013/10/24 End date if known: Rate name: Optional Agricultural Water Pumping Service Sector: Commercial Description: To electric service for agricultural water pumping for the irrigation of crops, fish farming and other agricultural purposes which require large quantities of water. The Demand Charge will apply to the usage of June through September. Source or reference: https://cas.sharepoint.illinoisstate.edu/grants/Sunshot/Lists/DATA%20ENTRY%20Rates%20Collected/Attachments/282/South%20Central%20Arkansas%20Electric%20Coop,%20INC%20Rates.PDF

56

Data:485cf6ea-9484-4a00-96b9-06b900098d35 | Open Energy Information  

Open Energy Info (EERE)

cf6ea-9484-4a00-96b9-06b900098d35 cf6ea-9484-4a00-96b9-06b900098d35 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Salt River Electric Coop Corp Effective date: 2011/06/01 End date if known: Rate name: 250 Watt HPS 104 kWh Outdoor Lighting Sector: Lighting Description: Source or reference: http://psc.ky.gov/tariffs/Electric/Salt%20River%20Electric%20Coop.%20Corp/Tariff.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category:

57

Data:C01b5717-123d-4c96-b4a4-3eee5f91b328 | Open Energy Information  

Open Energy Info (EERE)

b5717-123d-4c96-b4a4-3eee5f91b328 b5717-123d-4c96-b4a4-3eee5f91b328 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Columbia River Peoples Ut Dist Effective date: 2011/10/01 End date if known: Rate name: General Service - Greater Than 400 Amp Service Sector: Commercial Description: To commercial and general service Customers not subject to other specific rate schedules whose service entrance requirements are either, single-phase service and exceed 400 amps, or three-phase service and exceed 200 amps, and with a peak monthly load of less than 1,875 kW. BPA Power Cost Adjustment All applicable BPA Power Cost Adjustment charges per Rate Schedule 94 shall apply to all kWh's billed to Customers under this Rate Schedule.. Average Power Factor Charge

58

Data:Be4c0539-d2cf-4f67-809e-b96b9f472c15 | Open Energy Information  

Open Energy Info (EERE)

39-d2cf-4f67-809e-b96b9f472c15 39-d2cf-4f67-809e-b96b9f472c15 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Lake Mills Light & Water Effective date: 2009/06/01 End date if known: Rate name: Cp-1 TOD Small Power Optional Time-of-Day Service between 50kW and 200kW Demand 7am-9pm with Parallel Generation(20kW or less) Sector: Industrial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0767 per kilowatt-hour.

59

Data:9234fbe7-0569-4d2b-96b1-0c4b962deb01 | Open Energy Information  

Open Energy Info (EERE)

fbe7-0569-4d2b-96b1-0c4b962deb01 fbe7-0569-4d2b-96b1-0c4b962deb01 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Georgetown, Texas (Utility Company) Effective date: 2011/01/01 End date if known: Rate name: Large Industrial Service Sector: Industrial Description: * 2000 kW minimum, not less than $10,600.00 The Power Cost Adjustment is shown in the Flat rate adjustment field. Source or reference: http://billing.georgetown.org/rates/ Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage

60

Data:40ecc6e7-d175-45b9-96b9-c350ef4c7113 | Open Energy Information  

Open Energy Info (EERE)

ecc6e7-d175-45b9-96b9-c350ef4c7113 ecc6e7-d175-45b9-96b9-c350ef4c7113 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: A & N Electric Coop Effective date: 2008/01/02 End date if known: Rate name: Former Delmarva Power Territory: Public Lighting Service-Outdoor Lighting-High Pressure Sodium-Existing Pole-400 W Sector: Lighting Description: Estimated Monthly Average Usage: 164kWh Additional Monthly Charges: Ornamental or Decorative Luminaires, $2.12 Poles Wood 25ft - 40 ft, $4.23 Fiberglass or Aluminum, Embedded, less than 25 ft, $4.23 Fiberglass or Aluminum, Embedded,25 ft- 35 ft, $8.47 Fiberglass or Aluminum, Bolt Base, without foundation, 25 ft- 35 ft, $9.42

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


61

ARM - Reading netCDF, HDF, and GRIB Files  

NLE Websites -- All DOE Office Websites (Extended Search)

DocumentationReading netCDF, HDF, and GRIB Files DocumentationReading netCDF, HDF, and GRIB Files Policies, Plans, Descriptions Data Documentation Home Data Sharing and Distribution Policy Data Management and Documentation Plan Data Product Registration and Submission Reading netCDF and HDF Data Files Time in ARM netCDF Data Files Data Archive Documentation ARM Archive's Catalog of Data Streams (Updated monthly) Access to Historical ARM Data More on Understanding and Finding ARM Data Data Quality Problem Reporting Reading netCDF, HDF, and GRIB Files netCDF Files Most ARM data are stored in netCDF format. This format allows for the definition of data fields and storage of operational information in the header of the file. All ARM netCDF files are in UTC time and represent time as "seconds since January 1, 1970,'' which is called the "epoch time.'' For

62

Data:De0febb6-38bd-416e-a96b-6d2f0e4126c8 | Open Energy Information  

Open Energy Info (EERE)

De0febb6-38bd-416e-a96b-6d2f0e4126c8 De0febb6-38bd-416e-a96b-6d2f0e4126c8 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Kiel, Wisconsin (Utility Company) Effective date: 2011/05/06 End date if known: Rate name: Pgs-2 Customer-Owned Generation Systems (Greater than 20kW) Sector: Description: Pgs-2 Customer-Owned Generation Systems (Greater than 20kW) - Available for single-phase and three-phase where part or all of the electrical requirements of the customer are supplied by the customer's generating facilities, where such requirements of the customer are supplied by the customer's generating facilities have a total generating capacity of greater than 20kW and less than or equal to 100kW, where such facilities are connected in parallel with the utility. Customers not desiring to sell energy under this rate have the right to negotiate a buy-back rate. Customers with generating facilities greater than 100kW can negotiate a buy-back rate and shall be billed by the utility for metering and associating billing expenses specified in the latest rates of the wholesale supplier unless the latest rates of the wholesale supplier do not properly reflect avoided costs. See Kiel Electric Utility Rate Tariff, Schedule Pgs-2 for more details.

63

Collider Detector at Fermilab (CDF): Data from B Hadrons Research  

DOE Data Explorer (OSTI)

The Collider Detector at Fermilab (CDF) is a Tevatron experiment at Fermilab. The Tevatron, a powerful particle accelerator, accelerates protons and antiprotons close to the speed of light, and then makes them collide head-on inside the CDF detector. The CDF detector is used to study the products of such collisions. The CDF Physics Group is organized into six working groups, each with a specific focus. The Bottom group studies the production and decay of B hadrons. Their public web page makes data and numerous figures available from both CDF Runs I and II.

64

Inclusive and dijet b productions at CDF  

Science Conference Proceedings (OSTI)

This contribution reports recent CDF measurements of the inclusive b?jet and bb? dijet production cross sections obtained at the Tevatron Run II in pp? collisions at s ?=?1.96? TeV . Preliminary results are in reasonable agreement with QCD predictions.

Rgis Lefvre; CDF and Collaboration

2005-01-01T23:59:59.000Z

65

New results on jet fragmentation at CDF  

SciTech Connect

Presented are the latest results of jet fragmentation studies at the Tevatron using the CDF Run II detector. Studies include the distribution of transverse momenta (Kt) of particles jets, two-particle momentum correlations, and indirectly global event shapes in p{bar p} collisions. Results are discussed within the context of recent Next-to-Leading Log calculations as well as earlier experimental results from the Tevatron and e{sup +}e{sup -} colliders.

Jindariani, Sergo; /Florida U.

2006-12-01T23:59:59.000Z

66

Searches for New Physics at CDF  

Science Conference Proceedings (OSTI)

The search for physics beyond the Standard Model is one of the primary motivations of the Run II at the Tevatron. The CDF collaboration has been very active in this field by searching in a variety of final states for signals of new physics processes. The observation of no significant deviation from the Standard Model has led to limits on the cross?sections of the considered processes

Mario Paolo Giordani

2005-01-01T23:59:59.000Z

67

Tools for top physics at CDF  

SciTech Connect

The authors describe here the different tools used for top physics analysis in the CDF Collaboration. In particular, they discuss how the jet energy scale, lepton identification, b tagging algorithms and the neural networks help to improve the signal to background ratio of the top sample in some cases and to reduce the dominant uncertainties in other. Results using each one of these tools are also presented.

Palencia, E.; /Fermilab

2008-07-01T23:59:59.000Z

68

ARM - Reading netCDF, HDF, and GRIB Files  

NLE Websites -- All DOE Office Websites (Extended Search)

govDataReading netCDF, HDF, and GRIB Files govDataReading netCDF, HDF, and GRIB Files Reading netCDF, HDF, and GRIB Files netCDF Files Most ARM data are stored in netCDF format. This format allows for the definition of data fields and storage of operational information in the header of the file. All ARM netCDF files are in UTC time and represent time as "seconds since January 1, 1970,'' which is called the "epoch time.'' For example, an epoch time of 1 means "Thu Jan 1 00:00:01 1970''; an epoch time of 992794875 is "Sun Jun 17 16:21:15 2001.'' To learn more about how to convert epoch time, see Time in ARM netCDF Data Files. More information on the netCDF format and tools is available from UCAR at http://www.unidata.ucar.edu/packages/netcdf/index.html. HDF Files Some data files also contain one or more measurements distributed over a

69

Suppressed $B_s$ decays at CDF  

SciTech Connect

We review three recent results of the CDF collaboration on B{sub s}{sup 0} suppressed decays: the first search for CP-violation in the B{sub s}{sup 0} {yields} {phi}{phi} decay, where two CP-violating asymmetries expected to be zero in the Standard Model are measured, and the observation and the branching ratio measurements of B{sub s}{sup 0} {yields} J/{Psi} f{sub 0}(980) and B{sub s}{sup 0} {yields} J/{Psi} K{sup (*)} decays.

Dorigo, Mirco

2011-05-01T23:59:59.000Z

70

Online b-jets tagging at CDF  

Science Conference Proceedings (OSTI)

We propose a method to identify b-quark jets at trigger level which exploits recently increased CDF trigger system capabilities. b-quark jets identification is of central interest for the CDF high-P{sub T} physics program, and the possibility to select online b-jets enriched samples can extend the physics reaches especially for light Higgs boson searches where the H {yields} b{bar b} decay mode is dominant. Exploiting new trigger primitives provided by two recent trigger upgrades, the Level2 XFT stereo tracking and the improved Level2 cluster-finder, in conjunction with the existing Silicon Vertex Tracker (SVT), we design an online trigger algorithm aimed at selecting good purity b-jets samples useful for many physics measurements, the most important being inclusive H {yields} b{bar b} searches. We discuss the performances of the proposed b-tagging algorithm which must guarantee reasonable trigger rates at luminosity greater than 2 x 10{sup 32} cm{sup -2}s{sup -1} and provide high efficiency on H {yields} b{bar b} events.

Casarsa, M.; /Fermilab; Ristori, L.; /INFN, Pisa; Amerio, S.; Lucchesi, D.; Pagan Griso, S.; /INFN, Padua; Torre, S.T.; /Frascati; Cortiana, G.; /Padua U., Astron. Dept.

2007-04-01T23:59:59.000Z

71

Multi-muon events at CDF  

E-Print Network (OSTI)

We report a study of multi-muon events produced at the Fermilab Tevatron collider and recorded by the CDF II detector. In a data set acquired with a dedicated dimuon trigger and corresponding to an integrated luminosity of 2100 pb$^{-1}$, we isolate a significant sample of events in which at least one of the identified muons has large impact parameter and is produced outside the beam pipe of radius 1.5 cm. We are unable to fully account for the number and properties of the events through standard model processes in conjunction with our current understanding of the CDF II detector, trigger and event reconstruction. Several topological and kinematic properties of these events are also presented. In contrast, the production cross section and kinematics of events in which both muon candidates are produced inside the beam pipe are successfully modeled by known QCD processes which include heavy flavor production. The presence of these anomalous multi-muon events offers a plausible resolution to long-standing inconsistencies related to $b\\bar{b}$ production and decay.

F. Ptochos

2009-07-01T23:59:59.000Z

72

Multi-muon events at CDF  

SciTech Connect

We report a study of multi-muon events produced at the Fermilab Tevatron collider and recorded by the CDF II detector. In a data set acquired with a dedicated dimuon trigger and corresponding to an integrated luminosity of 2100 pb{sup -1}, we isolate a significant sample of events in which at least one of the identified muons has large impact parameter and is produced outside the beam pipe of radius 1.5 cm. We are unable to fully account for the number and properties of the events through standard model processes in conjunction with our current understanding of the CDF II detector, trigger and event reconstruction. Several topological and kinematic properties of these events are also presented. In contrast, the production cross section and kinematics of events in which both muon candidates are produced inside the beam pipe are successfully modeled by known QCD processes which include heavy flavor production. The presence of these anomalous multi-muon events offers a plausible resolution to long-standing inconsistencies related to b{bar b} production and decay.

Ptochos, F.; /Cyprus U.

2009-07-01T23:59:59.000Z

73

Data:25b7f6d5-f073-4c84-96b2-723f754aa8a9 | Open Energy Information  

Open Energy Info (EERE)

f6d5-f073-4c84-96b2-723f754aa8a9 f6d5-f073-4c84-96b2-723f754aa8a9 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Mille Lacs Energy Cooperative Effective date: End date if known: Rate name: Off-Peak Energy Rate Sector: Residential Description: Available to members taking service concurrently under another rate schedule. This rate is for interruptible service to electric water and space heating loads. Service under this schedule will be available for approximately eight hours per day, during off peak hours. Systems must be sized for sufficient heat during the on peak period Source or reference: Rate Binder A

74

Underlying event studies at ATLAS and CDF  

SciTech Connect

Improving our understanding and modeling of the underlying event in high energy collider environment is important for more precise measurements at the LHC. CDF Run II data for the underlying event associated with Drell-Yan lepton pair production and early ATLAS data measuring underlying event activity with respect to the leading transverse momentum track are presented. The data are compared with several QCD Monte Carlo models. It is seen that no current standard Monte Carlo tune adequately describes all the early ATLAS data and CDF data simultaneously. The underlying event observables presented here are particularly important for constraining the energy evolution of multiple parton interaction models. One of the goals of these analyses is to provide data that can be used to test and improve MC models for current and future physics studies at the LHC. The underlying event observables presented here are particularly important for constraining the energy evolution of multiple partonic interaction models, since the plateau heights of the underlying event profiles are highly correlated to multiple parton interaction activity. The data at 7 TeV are crucial for MC tuning, since measurements are needed with at least two energies to constrain the energy evolution of MPI activity. PYTHIA tune A and tune AW do a good job in describing the CDF data on the underlying-event observables for leading jet and Drell-Yan events, respectively, although the agreement between predictions and data is not perfect. The leading-jet data show slightly more activity in the underlying event than PYTHIA Tune A, although they are very similar - which may indicate the universality of underlying event modeling. However, all pre-LHC MC models predict less activity in the transverse region (i.e in the underlying event) than is actually observed in ATLAS leading track data, for both center-of-mass energies. There is therefore no current standard MC tune which adequately describes all the early ATLAS data. However, using diffraction-limited minimum bias distributions and the plateau of the underlying event distributions presented here, ATLAS has developed a new PYTHIA tune AMBT1 (ATLAS Minimum Bias Tune 1) and a new HERWIG+ JIMMY tune AUET1 (ATLAS Underlying Event Tune 1) which model the p{sub T} and charged multiplicity spectra significantly better than the pre-LHC tunes of those generators. It is critical to have sensible underlying event models containing our best physical knowledge and intuition, tuned to all relevant available data.

Kar, D.; /Dresden, Tech. U.

2011-01-01T23:59:59.000Z

75

Data:Adfd0729-d47a-4cf6-922a-bee6ff34522f | Open Energy Information  

Open Energy Info (EERE)

Adfd0729-d47a-4cf6-922a-bee6ff34522f No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading......

76

Charm and beauty results from CDF and D0  

SciTech Connect

I report, for the CDF and D0 collaborations, results from the 92-93 Tevatron Collider run concerning charm and beauty quark production and beauty meson decay properties.

Derwent, P. [Michigan Univ., Ann Arbor, MI (United States); CDF and D0 Collaborations

1995-05-01T23:59:59.000Z

77

Inclusive jet cross-section measurement at CDF  

SciTech Connect

The CDF Collaboration has measured the inclusive jet cross section using 1992-93 collider data at 1.8 TeV. The CDF measurement is in very good agreement with NLO QCD predictions for transverse energies (E{sub T}) below 200 GeV. However, it is systematically higher than NLO QCD predictions for E{sub T} above 200 GeV.

Norniella, Olga; /Barcelona, IFAE

2007-05-01T23:59:59.000Z

78

Data:09bc8904-6dbc-4746-be4b-22975abe80b1 | Open Energy Information  

Open Energy Info (EERE)

04-6dbc-4746-be4b-22975abe80b1 04-6dbc-4746-be4b-22975abe80b1 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Lee County Electric Coop, Inc Effective date: 2008/07/01 End date if known: Rate name: Private Area Lighting- Shoebox Fixture (1000W MH Galleria) Sector: Lighting Description: Applicable to customers, other than Street Light Districts, for automatically controlled dusk-to-dawn outdoor lighting where existing overhead secondary circuits are located. Source or reference: https://www.lcec.net/pdf/EntireRateTariff.pdf#page=18 Source Parent: Comments Applicability Demand (kW) Minimum (kW):

79

Data:Fc83962f-30b8-4420-8464-abe452386d8d | Open Energy Information  

Open Energy Info (EERE)

3962f-30b8-4420-8464-abe452386d8d 3962f-30b8-4420-8464-abe452386d8d No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Jackson Electric Member Corp Effective date: End date if known: Rate name: Outdoor Lighting Decashield MV 400 W Non Wood Pole Sector: Lighting Description: Fixtures No Longer Offered Effective June 1, 2005 Source or reference: http://www.jacksonemc.com/business-manage-my-account-commercial-rates-options/schedules/outdoor-lighting-service Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months):

80

Data:6dccfbbc-6ab8-404a-bee3-46bd26766cfc | Open Energy Information  

Open Energy Info (EERE)

dccfbbc-6ab8-404a-bee3-46bd26766cfc dccfbbc-6ab8-404a-bee3-46bd26766cfc No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Groton, South Dakota (Utility Company) Effective date: End date if known: Rate name: Schedule I-Load Management Nonparticipating Single phase general services rates Sector: Commercial Description: 150% of their Participating Rate Class Schedule Source or reference: http://city.grotonsd.gov/electric.html Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V):

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


81

Data:0422665c-8abe-459e-a932-95424edd01b9 | Open Energy Information  

Open Energy Info (EERE)

8abe-459e-a932-95424edd01b9 8abe-459e-a932-95424edd01b9 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Lebanon, Indiana (Utility Company) Effective date: 2013/04/01 End date if known: Rate name: SL - Public Street Lighting 400 watt sodium vapor Sector: Lighting Description: Availability Available for any standard overhead Public Street Lighting Service. Character of Service Public Street Lighting Service using lamps available under this schedule. Source or reference: http://www.lebanon-utilities.com/e_rates.html Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):

82

Collider Detector at Fermilab (CDF): Data from W, Z bosons and Drell Yan lepton pairs research of the CDF Electroweak Group  

DOE Data Explorer (OSTI)

The Collider Detector at Fermilab (CDF) is a Tevatron experiment at Fermilab. The Tevatron, a powerful particle accelerator, accelerates protons and antiprotons close to the speed of light, and then makes them collide head-on inside the CDF detector. The CDF detector is used to study the products of such collisions. The CDF Physics Group at Fermilab is organized into six working groups, each with a specific focus. The Electroweak group studies production and properties of W, Z bosons and Drell Yan lepton pairs. Their public web page makes data and numerous figures available from both CDF Runs I and II.

83

CDF's Higgs sensitivity status  

SciTech Connect

The combined sensitivity of CDF's current Standard Model Higgs boson searches is presented. The expected 95% CL limits on the production cross section times the relevant Higgs boson branching ratios are computed for the W{sup {+-}}H {yields} {ell}{sup {+-}}{nu}b{bar b}, ZH {yields} {nu}{bar {nu}}b{bar b}, gg {yields} H {yields} W{sup +}W{sup -} W{sup {+-}}H {yields} W{sup {+-}}W{sup +}W{sup -} channels as they stand as of the October 2005, using results which were prepared for Summer 2005 conferences and a newer result form the gg {yields} H {yields} W{sup +}W{sup -} channel. Correlated and uncorrelated systematic uncertainties are taken into account, and the luminosity requirements for 95% CL exclusion, 3{sigma} evidence, and 5{sigma} discovery are computed for median experimental outcomes. A list of improvements required to achieve the sensitivity to a SM Higgs boson as quantified in the Higgs Sensitivity Working Group's report is provided.

Junk, Tom; /Illinois U., Urbana

2005-10-01T23:59:59.000Z

84

Data:Fc5d3d19-6ac8-4cdc-96b0-954b69f2b786 | Open Energy Information  

Open Energy Info (EERE)

d19-6ac8-4cdc-96b0-954b69f2b786 d19-6ac8-4cdc-96b0-954b69f2b786 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Pontotoc Electric Power Assn Effective date: 2013/07/01 End date if known: Rate name: General Power Service GSA (Under 50 kW) Single-Phase Sector: Commercial Description: Source or reference: http://www.sitemason.com/files/fjDo1q/May%202012.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring:

85

Data:B514f4d5-96b7-4f4a-ae11-2b7a1ef1057d | Open Energy Information  

Open Energy Info (EERE)

d5-96b7-4f4a-ae11-2b7a1ef1057d d5-96b7-4f4a-ae11-2b7a1ef1057d No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Tecumseh, Nebraska (Utility Company) Effective date: 2013/05/01 End date if known: 2013/09/30 Rate name: General Service- Single Phase Sector: Commercial Description: Applicable to any customer for lighting, heating and power purposes where all service is taken through a single meter and where the customer's monthly peak demand does not exceed 60 kW for 2 consecutive months. Source or reference: ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW):

86

Data:3b2a84a9-6b00-43b8-8e50-a9cb8a930831 | Open Energy Information  

Open Energy Info (EERE)

a84a9-6b00-43b8-8e50-a9cb8a930831 a84a9-6b00-43b8-8e50-a9cb8a930831 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Athens Utility Board Effective date: 2011/04/01 End date if known: Rate name: Outdoor Lighting: Metal Halide 400W Box Sector: Lighting Description: Installations charge per light: $50.00 Pole charge per month: $2.00(included in the fixed monthly charge) Source or reference: http://www.aub.org/rate_power_ol.php Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V):

87

Data:2a9d9626-d25d-4db0-8d50-96b5c5e06e68 | Open Energy Information  

Open Energy Info (EERE)

26-d25d-4db0-8d50-96b5c5e06e68 26-d25d-4db0-8d50-96b5c5e06e68 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc Effective date: 2012/08/01 End date if known: Rate name: 250 Watt MVL 110 kWh Street Light Sector: Lighting Description: Source or reference: http://navopache.coopwebbuilder.com/sites/navopache.coopwebbuilder.com/files/security_lights_2012.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category:

88

Data:D7f3a2ad-a2cc-4417-b20f-96b3fd8d7b55 | Open Energy Information  

Open Energy Info (EERE)

a2cc-4417-b20f-96b3fd8d7b55 a2cc-4417-b20f-96b3fd8d7b55 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Public Service Co of Colorado Effective date: 2012/10/11 End date if known: Rate name: ENERGY ONLY STREET LIGHTING SERVICE - SCHEDULE ESL - 108.1-111.0 kWh per light Sector: Lighting Description: Source or reference: www.xcelenergy.com/staticfiles/xe/Regulatory/Regulatory PDFs/psco_elec_entire_tariff.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V):

89

ARM - Time in ARM NetCDF Files  

NLE Websites -- All DOE Office Websites (Extended Search)

govDataTime in ARM NetCDF Files govDataTime in ARM NetCDF Files Page Contents Introduction Time Zones Epoch Time Time Variables Conversion Examples and Hints Perl Example C Example Fortran Example IDL Example Notes on Generating Epoch Times Contact Information Time in ARM NetCDF Files Introduction This document explains most of the issues related to the use of time in ARM netCDF data files. Time Zones All ARM netCDF files are in UTC. Note that this has some implications for solar-based data; we tend to split our files at midnight, but the sun is still up at 0000 UTC at SGP in the late spring and summer, and all the time at TWP. This means a given solar arc may be broken across two different files. That's just the way it is; using local time in ARM files would have been a bigger mess. Note that splitting files at 0000 UTC is not an ARM standard, and many

90

Prospects for measuring B{sub s} mixing at CDF  

SciTech Connect

The original design of the Collider Detector at Fermilab (CDF) was optimized for high p{sub T} physics measurements associated with W and Z boson, top quark, and QCD jet production. This choice resulted in an emphasis on the central pseudorapidity region ({vert_bar}{eta}{vert_bar} < 1.0) for detector coverage. Thus, CDF has excellent tracking, good calorimetry, and a suitable muon system in the central region. Even with this limited coverage, the large {bar p}p {yields} bX cross section of nearly 100 {mu}barns for {vert_bar}{eta}{vert_bar} < 1.0 has allowed the CDF experiment to make many B physics measurements. In addition, with the successful operation of the CDF silicon vertex detector (SVX), the capability for making time-dependent B{sub s} mixing measurements becomes a reality. Upgrade plans, which include extending the tracking and lepton identification into the forward region and the implementation of a high-rate DAQ system, make a time-dependent B{sub s} mixing measurement an attractive goal during the anticipated high-luminosity Main Injector collider runs. We discuss here the feasibility and potential of making a B{sub s} mixing measurement based on extrapolations of the current CDF detector performance using colliding beam data and the expected upgrade plans.

Skarha, J.E. [Johns Hopkins Univ., Baltimore, MD (United States). Dept. of Physics and Astronomy; Wicklund, A.B. [Argonne National Lab., IL (United States)

1993-10-01T23:59:59.000Z

91

CDF Note 9999 Combined Upper Limit on Standard Model Higgs Boson Production  

E-Print Network (OSTI)

CDF Note 9999 Combined Upper Limit on Standard Model Higgs Boson Production The CDF Collaboration for the Standard Model Higgs boson at CDF. The six major analyses combined are the WH b¯b channels, the WH + ZH E Model decay branching fractions of the Higgs boson and that the ratios of the rates for the WH, ZH, gg

Fermilab

92

Analysis of Bs flavor oscillations at CDF  

SciTech Connect

The search for and study of flavor oscillations in the neutral B{sub s}B{sub s} meson system is an experimentally challenging task. It constitutes a flagship analysis of the Tevatron physics program. In this dissertation, they develop an analysis of the time-dependent B{sub s} flavor oscillations using data collected with the CDF detector. The data samples are formed of both fully and partially reconstructed B meson decays: B{sub s} {yields} D{sub s}{pi}({pi}{pi}) and B{sub s} {yields} D{sub s}lv. A likelihood fitting framework is implemented and appropriate models and techniques developed for describing the mass, proper decay time, and flavor tagging characteristics of the data samples. The analysis is extended to samples of B{sup +} and B{sup 0} mesons, which are further used for algorithm calibration and method validation. The B mesons lifetimes are extracted. The measurement of the B{sup 0} oscillation frequency yields {Delta}m{sub d} = 0.522 {+-} 0.017 ps{sup -1}. The search for B{sub s} oscillations is performed using an amplitude method based on a frequency scanning procedure. Applying a combination of lepton and jet charge flavor tagging algorithms, with a total tagging power {epsilon}'D{sup 2} of 1.6%, to a data sample of 355 pb{sup -1}, a sensitivity of 13.0 ps{sup -1} is achieved. They develop a preliminary same side kaon tagging algorithm, which is found to provide a superior tagging power of about 4.0% for the B{sub s} meson species. A study of the dilution systematic uncertainties is not reported. From its application as is to the B{sub s} samples the sensitivity is significantly increased to about 18 ps{sup -1} and a hint of a signal is seen at about 175. ps{sup -1}. They demonstrate that the extension of the analysis to the increasing data samples with the inclusion of the same side tagging algorithm is capable of providing an observation of B{sub s} mixing beyond the standard model expectation. They show also that the improved knowledge of {Delta}m{sub s} has a considerable impact on constraining the CKM matrix elements.

Leonardo, Nuno T.; /MIT

2006-09-01T23:59:59.000Z

93

Collider Detector at Fermilab (CDF): Data from the Top Group's Top Quark Research  

DOE Data Explorer (OSTI)

The Collider Detector at Fermilab (CDF) is a Tevatron experiment at Fermilab. The Tevatron, a powerful particle accelerator, accelerates protons and antiprotons close to the speed of light, and then makes them collide head-on inside the CDF detector. The CDF detector is used to study the products of such collisions. The CDF Physics Group at Fermilab is organized into six working groups, each with a specific focus. The Top group studies the properties of the top quark, the heaviest known fundamental particle. Their public web page makes data and numerous figures available from both CDF Runs I and II.

94

The CDF computing and analysis system: First experience  

SciTech Connect

The Collider Detector at Fermilab (CDF) collaboration records and analyses proton anti-proton interactions with a center-of-mass energy of 2 TeV at the Tevatron. A new collider run, Run II, of the Tevatron started in April. During its more than two year duration the CDF experiment expects to record about 1 PetaByte of data. With its multi-purpose detector and center-of-mass energy at the frontier, the experimental program is large and versatile. The over 500 scientists of CDF will engage in searches for new particles, like the Higgs boson or supersymmetric particles, precision measurement of electroweak parameters, like the mass of the W boson, measurement of top quark parameters, and a large spectrum of B physics. The experiment has taken data and analyzed them in previous runs. For Run II, however, the computing model was changed to incorporate new methodologies, the file format switched, and both data handling and analysis system redesigned to cope with the increased demands. This paper (4-036 at Chep 2001) gives an overview of the CDF Run II compute system with emphasis on areas where the current system does not match initial estimates and projections. For the data handling and analysis system a more detailed description is given.

R. Colombo et al.

2001-11-02T23:59:59.000Z

95

CDF Note 10796 Search for Standard Model Higgs Boson Production  

E-Print Network (OSTI)

CDF Note 10796 Search for Standard Model Higgs Boson Production in Association with a W± Boson present a search for the standard model Higgs boson produced in association with a W± boson. This search that at least one jet be identified to originate from a bottom quark. Discrimination between the Higgs boson

Fermilab

96

B-Tagging at CDF and DO, Lessons for LHC  

E-Print Network (OSTI)

The identification of jets resulting from the fragmentation and hadronization of b quarks is an important part of high-pT collider physics. The methods used by the CDF and DO collaborations to perform this identification are described, including the calibration of the efficiencies and fake rates. Some thoughts on the application of these methods in the LHC environment are also presented.

T. Wright; for the CDF; D Collaborations

2007-07-11T23:59:59.000Z

97

Data:Abe99966-bea2-4562-a56c-db27792bebeb | Open Energy Information  

Open Energy Info (EERE)

Abe99966-bea2-4562-a56c-db27792bebeb Abe99966-bea2-4562-a56c-db27792bebeb No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Medford, Wisconsin (Utility Company) Effective date: 1997/06/27 End date if known: Rate name: Ms-1 Street Lighting Service 250 W MV Sector: Lighting Description: The schedule will be applied to municipal street lighting. The utility will furnish, install and maintain street lighting units. Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0351 per kilowatt-hour.

98

Data:84fabcc8-aa6d-4556-9abe-b586bef88efe | Open Energy Information  

Open Energy Info (EERE)

fabcc8-aa6d-4556-9abe-b586bef88efe fabcc8-aa6d-4556-9abe-b586bef88efe No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of New Richmond, Wisconsin (Utility Company) Effective date: 2010/02/01 End date if known: Rate name: Cp-1 Small Power Service with Parallel Generation(20kW or less) Sector: Industrial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0710 per kilowatt-hour.

99

Vista at CDF: Results of a model-independent search for new physics in 927 pb**-1 at CDF  

SciTech Connect

A global, model-independent search for high-pT exotic phenomena is presented using 927 pb{sup -1} of CDF II data. The search algorithms employed in this analysis are Vista and Sleuth. These proceedings focus on Vista, including a description of the method and a summary of results.

Choudalakis, Georgios; /MIT, LNS

2007-10-01T23:59:59.000Z

100

in2p3-00112874,version1-10Nov2006 November 10, 2006 11:4 WSPC/INSTRUCTION FILE abe-KDf  

E-Print Network (OSTI)

for the saddle. Then, results by realistic calculations are given for the cold fusion. Ambiguities of the model) For the synthesis of superheavy elements, it is indispensable to divide the fusion process into two steps Yasuhisa ABE et al. fusion hindrance, we first employ an analytic model with an inverted parabola

Paris-Sud XI, Université de

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


101

Minimum bias and underlying event studies at CDF  

SciTech Connect

Soft, non-perturbative, interactions are poorly understood from the theoretical point of view even though they form a large part of the hadronic cross section at the energies now available. We review the CDF studies on minimum-bias ad underlying event in p{bar p} collisions at 2 TeV. After proposing an operative definition of 'underlying event', we present part of a systematic set of measurements carried out by the CDF Collaboration with the goal to provide data to test and improve the QCD models of hadron collisions. Different analysis strategies of the underlying event and possible event topologies are discussed. Part of the CDF minimum-bias results are also presented: in this sample, that represent the full inelastic cross-section, we can test simultaneously our knowledge of all the components that concur to form hadronic interactions. Comparisons with MonteCarlo simulations are always shown along with the data. These measurements will also contribute to more precise estimates of the soft QCD background of high-p{sub T} observables.

Moggi, Niccolo; /INFN, Bologna

2010-01-01T23:59:59.000Z

102

Data:Ccb5294a-00d2-4093-917a-be563dd3e3eb | Open Energy Information  

Open Energy Info (EERE)

Ccb5294a-00d2-4093-917a-be563dd3e3eb Ccb5294a-00d2-4093-917a-be563dd3e3eb No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Canoochee Electric Member Corp Effective date: 2006/07/01 End date if known: Rate name: Load Mangament Service- LM-3 Sector: Commercial Description: Applicable, at the consumer's request, to commercial, industrial, governmental and other consumers for all uses, provided that the consumer's metered electrical load is at least 750 kilowatts or the consumer's connected electrical load is 900 kilowatts or more. Source or reference: ISU Documentation Source Parent: Comments Applicability

103

Data:3e9819c9-390a-4476-9ce2-1cf2c2abed59 | Open Energy Information  

Open Energy Info (EERE)

819c9-390a-4476-9ce2-1cf2c2abed59 819c9-390a-4476-9ce2-1cf2c2abed59 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Hickman, Kentucky (Utility Company) Effective date: End date if known: Rate name: General Power - Commercial / Industrial, Class 40 Sector: Commercial Description: Source or reference: ISU documents Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous

104

Data:75dfaf36-ae84-4bdb-a820-c7ba5abe8686 | Open Energy Information  

Open Energy Info (EERE)

dfaf36-ae84-4bdb-a820-c7ba5abe8686 dfaf36-ae84-4bdb-a820-c7ba5abe8686 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: MidAmerican Energy Co Effective date: 2006/03/06 End date if known: Rate name: Private Lighting - North - 175W MV MP Sector: Lighting Description: Source or reference: www.midamericanenergy.com/include/pdf/ Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous

105

Data:0c27a871-113f-4f9a-bee9-a34de8bb56db | Open Energy Information  

Open Energy Info (EERE)

1-113f-4f9a-bee9-a34de8bb56db 1-113f-4f9a-bee9-a34de8bb56db No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: South Central Public Pwr Dist Effective date: 2012/05/01 End date if known: Rate name: Area&Directional Lighting Service Rate N733 - Fringe Sector: Lighting Description: Source or reference: Illinois State University Rate Binder #10 Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous

106

Data:C154144e-a859-4438-aad8-147d1a3abee7 | Open Energy Information  

Open Energy Info (EERE)

a859-4438-aad8-147d1a3abee7 a859-4438-aad8-147d1a3abee7 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Consumers Power, Inc Effective date: 2011/10/01 End date if known: Rate name: 250 W HPS Street Lighting, Customer-Owned Sector: Lighting Description: * Applicable to service furnished from the dusk to dawn for area lighting,lighting of public streets,highways,alleys and parks. Source or reference: Rate binder # 4(Illinios State University) Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months):

107

Data:E13b1ccd-4c31-4890-bafd-06aa82abed50 | Open Energy Information  

Open Energy Info (EERE)

ccd-4c31-4890-bafd-06aa82abed50 ccd-4c31-4890-bafd-06aa82abed50 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Detroit Edison Co Effective date: 2011/12/21 End date if known: Rate name: Alternative Electric Metal Melting < 4.8 kV secondary - 0 - 11,500 kWh Sector: Industrial Description: Source or reference: www.dteenergy.com/pdfs/detroitEdisonTariff.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring:

108

Data:6abe6dcf-4386-4be2-a9bd-0b94736d7240 | Open Energy Information  

Open Energy Info (EERE)

abe6dcf-4386-4be2-a9bd-0b94736d7240 abe6dcf-4386-4be2-a9bd-0b94736d7240 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of New Smyrna Beach, Florida (Utility Company) Effective date: 2011/02/01 End date if known: Rate name: MH-Providence 250 watts Sector: Lighting Description: Fixed Monthly Charge= Energy Rate + Maintenance Source or reference: http://ucnsb.org/pdf/Rates%20Charges%20and%20Fees.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

109

Data:5827d02c-6f00-4a4a-be27-34d2089b6d21 | Open Energy Information  

Open Energy Info (EERE)

6f00-4a4a-be27-34d2089b6d21 6f00-4a4a-be27-34d2089b6d21 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: PUD No 1 of Kittitas County Effective date: 2013/02/01 End date if known: Rate name: Aggregated Residential Net Metering Service Sector: Residential Description: This schedule is limited to farms and single family residences for customers with a solar, wind turbine or micro-hydro electrical generating facility, or a hybrid system of one or more types, with a total rated capacity of not more than 25 kW. Source or reference: http://www.kittitaspud.com/rate_schedule.php Source Parent:

110

Data:51910892-d368-49b7-8d44-94abe4ca0f05 | Open Energy Information  

Open Energy Info (EERE)

910892-d368-49b7-8d44-94abe4ca0f05 910892-d368-49b7-8d44-94abe4ca0f05 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Southwest Rural Elec Assn Inc Effective date: 2010/11/01 End date if known: Rate name: Irrigation Option C Sector: Commercial Description: * Applicable to water pumping over 5HP.The facilities and demand charges are billed June- September. Minimum:Higher of facilities charge plus kW/Demand charge of $96 per year. All bills are adjusted by applicable taxes. Summer rates cover May- October and Winter cover November- April . Source or reference: Rate binder # 4(Illinios State University)

111

Data:Db4abe55-b47a-4ec5-abb7-e61b3930b67a | Open Energy Information  

Open Energy Info (EERE)

abe55-b47a-4ec5-abb7-e61b3930b67a abe55-b47a-4ec5-abb7-e61b3930b67a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Ark Valley Elec Coop Assn, Inc Effective date: End date if known: Rate name: Irrigation Service Sector: Industrial Description: * Annual Horsepower Charge $5.50 per HP Source or reference: http://www.arkvalley.com/content/electric-rate-schedules Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring:

112

Data:5d3b0cda-7b7e-4272-b1ab-e48373d258bc | Open Energy Information  

Open Energy Info (EERE)

b0cda-7b7e-4272-b1ab-e48373d258bc b0cda-7b7e-4272-b1ab-e48373d258bc No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Ohio Edison Co Effective date: 2009/01/23 End date if known: Rate name: RS (Residential Service) Sector: Residential Description: Available for residential service to installations served through one meter for each family unit in a residence or apartment. Source or reference: https://www.firstenergycorp.com/content/dam/customer/Customer%20Choice/Files/Ohio/tariffs/OE-2012-Electric-Service.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months):

113

Data:C7a3f01a-1997-401b-8688-d8abe4ef1153 | Open Energy Information  

Open Energy Info (EERE)

a3f01a-1997-401b-8688-d8abe4ef1153 a3f01a-1997-401b-8688-d8abe4ef1153 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Butler Rural Electric Coop Inc Effective date: 2012/10/01 End date if known: Rate name: Residential Time-Of-Day Sector: Residential Description: On peak KWh= On peak KWh distribution charges+ on peak Kwh generation and transmission Charges. The non-variable and variable charges are determined pursuant to the schedule generation and transmission clause(GTC). Source or reference: Rate Binder#8 (Illinois State University) Source Parent: Comments Applicability Demand (kW) Minimum (kW):

114

Data:37b26203-282c-4abe-95bc-c7f8e634648f | Open Energy Information  

Open Energy Info (EERE)

82c-4abe-95bc-c7f8e634648f 82c-4abe-95bc-c7f8e634648f No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Danville, Virginia (Utility Company) Effective date: 2012/08/28 End date if known: Rate name: Street Lighting Service- 100W HPS Underground Existing Pole- Wood Sector: Lighting Description: Available for lighting streets and roadways, whether public or private, which are thoroughfares for normal flow of vehicular traffic. This rate is generally available to governmental agencies. Source or reference: http://www.danville-va.gov/DocumentCenter/View/8181 Source Parent: Comments

115

Data:73c3b699-1abe-4fbd-b9bf-8d65b0578683 | Open Energy Information  

Open Energy Info (EERE)

99-1abe-4fbd-b9bf-8d65b0578683 99-1abe-4fbd-b9bf-8d65b0578683 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Eastern Illinois Elec Coop Effective date: 2013/04/15 End date if known: Rate name: OUTDOOR LIGHTING SERVICE(400-watt Sodium Vapor Directional Unit)(DL Sector: Lighting Description: This rate schedule is available to all member/owners for dusk-to-dawn outdoor lighting in close proximity to existing overhead secondary circuits. Source or reference: http://eiec.org/wp-content/uploads/2013/04/EIEC_Rate_OL.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):

116

Data:F8e4daa4-abe4-4f69-aee6-9ec4e61a3dce | Open Energy Information  

Open Energy Info (EERE)

daa4-abe4-4f69-aee6-9ec4e61a3dce daa4-abe4-4f69-aee6-9ec4e61a3dce No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of West Point, Mississippi (Utility Company) Effective date: 2012/11/01 End date if known: Rate name: Seasonal Demand and Energy Manufacturing- SMSB Sector: Industrial Description: Source or reference: ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2

117

Data:B721e2af-e511-4bf7-bf2d-9e83abe831c2 | Open Energy Information  

Open Energy Info (EERE)

e2af-e511-4bf7-bf2d-9e83abe831c2 e2af-e511-4bf7-bf2d-9e83abe831c2 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Cleveland, Tennessee (Utility Company) Effective date: 2011/04/01 End date if known: Rate name: Seasonal Demand, Manufacturing Service Rate-- Schedule SMSC Sector: Commercial Description: Source or reference: http://www.clevelandutilities.com/PDF/2011JulyElectricRates.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

118

Data:90d50353-93d6-4eed-b520-8b450e69abe4 | Open Energy Information  

Open Energy Info (EERE)

53-93d6-4eed-b520-8b450e69abe4 53-93d6-4eed-b520-8b450e69abe4 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Rolling Hills Electric Coop Effective date: 2010/07/01 End date if known: Rate name: Private Street and Area Lighting (PSL-10) Unmetered MV 175W(1) Sector: Lighting Description: There are two rates with the same name, but different charges. The schedule doesn't differentiate between them. http://rollinghills.coopwebbuilder.com/sites/rollinghills.coopwebbuilder.com/files/rate_tariffs.pdf Source or reference: http://rollinghills.coopwebbuilder.com/sites/rollinghills.coopwebbuilder.com/files/rate_tariffs.pdf

119

Data:7c4e8032-2fdd-4f5a-be8f-42ae498b9f60 | Open Energy Information  

Open Energy Info (EERE)

032-2fdd-4f5a-be8f-42ae498b9f60 032-2fdd-4f5a-be8f-42ae498b9f60 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Jackson Electric Member Corp Effective date: End date if known: Rate name: Outdoor Lighting Directional Flood HPS 250 W Non Wood Pole Sector: Lighting Description: Source or reference: http://www.jacksonemc.com/business-manage-my-account-commercial-rates-options/schedules/outdoor-lighting-service Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V):

120

Data:1d928226-d715-44c7-86f7-abe9d5f00c02 | Open Energy Information  

Open Energy Info (EERE)

8226-d715-44c7-86f7-abe9d5f00c02 8226-d715-44c7-86f7-abe9d5f00c02 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Sullivan, Illinois (Utility Company) Effective date: 2012/11/13 End date if known: Rate name: Commercial All Electric (Including Heat) - Year Round Rate: Single Phase - 250-500 kva installation Sector: Commercial Description: For customers with usage of less than twenty-five thousand (25,000) KWH per month and certain seasonal customers such as grain elevators and fertilizer plants. Source or reference: http://www.sullivanil.us/government.html Source Parent: Comments

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


121

Data:Abe00d44-2e45-45ff-a690-7ab7534bdefc | Open Energy Information  

Open Energy Info (EERE)

Abe00d44-2e45-45ff-a690-7ab7534bdefc Abe00d44-2e45-45ff-a690-7ab7534bdefc No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Blue Earth, Minnesota (Utility Company) Effective date: End date if known: Rate name: Industrial Electric - Demand Credit Sector: Industrial Description: Source or reference: http://www.belw.org/Rate Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >>

122

Data:Bec72faf-e2a7-40d1-abe3-acb0f1b657c1 | Open Energy Information  

Open Energy Info (EERE)

Bec72faf-e2a7-40d1-abe3-acb0f1b657c1 Bec72faf-e2a7-40d1-abe3-acb0f1b657c1 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of New Bern, North Carolina (Utility Company) Effective date: 2009/02/01 End date if known: Rate name: Standard Residential- Three Phase Sector: Residential Description: Service under this Schedule is available for separately metered and billed supply of alternating electric current to single family residences, including a residential farm where the farm uses are not taken through a separate meter. Source or reference: http://www.ci.new-bern.nc.us/Elec/documents/residentialservicerates0107-2009.pdf

123

Data:7e3d0fed-2037-43f0-a4f8-da456abe7e5a | Open Energy Information  

Open Energy Info (EERE)

fed-2037-43f0-a4f8-da456abe7e5a fed-2037-43f0-a4f8-da456abe7e5a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Escanaba, Michigan (Utility Company) Effective date: 2012/07/01 End date if known: Rate name: Electric Heat City Residential Sector: Residential Description: To all customers for such service when separately metered upon application and approval of permanently installed equipment; subject to such rules and regulations as are established by the utility. When air conditioning is installed in an electrically heated area, it may be connected to the same meter for space conditioning purposes.

124

Data:076f7cb8-e72f-4e38-90ee-abe9b81aef37 | Open Energy Information  

Open Energy Info (EERE)

e72f-4e38-90ee-abe9b81aef37 e72f-4e38-90ee-abe9b81aef37 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Emerson, Nebraska (Utility Company) Effective date: 2013/01/01 End date if known: Rate name: General Service- Three Phase Sector: Commercial Description: Service under this schedule is for non-seasonal, non-residential and non-farm service, including but not limited to commercial establishments, separate garages and out-buildings only and other loads which are not classified for service under other rate schedules. Service is subject to the District's established rules and regulations and limited to 150 kva of transformer capacity.

125

Data:D254aed8-8415-4899-be7c-2abe183b7d89 | Open Energy Information  

Open Energy Info (EERE)

aed8-8415-4899-be7c-2abe183b7d89 aed8-8415-4899-be7c-2abe183b7d89 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Nolin Rural Electric Coop Corp Effective date: 2011/06/01 End date if known: Rate name: Schedule 9 - Industrial Sector: Commercial Description: Applicable to contracts with contract demands of 1000-4999 kW with a monthly energy usage equal to or greater than 425 hours per kW of contract demand. Source or reference: www.nolinrecc.com Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months):

126

Data:6b5bbfff-bd77-42e9-be19-3abe3591ed47 | Open Energy Information  

Open Energy Info (EERE)

bbfff-bd77-42e9-be19-3abe3591ed47 bbfff-bd77-42e9-be19-3abe3591ed47 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Baltimore Gas & Electric Co Effective date: 2013/02/23 End date if known: Rate name: 20000 lumen 454 watt MV Sector: Lighting Description: Source or reference: http://www.bge.com/myaccount/billsrates/ratestariffs/electricservice/pages/electric-services-rates-and-tariffs.aspx Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

127

Data:Aa7fa4ab-abe1-4750-a787-0edbf7c0b912 | Open Energy Information  

Open Energy Info (EERE)

ab-abe1-4750-a787-0edbf7c0b912 ab-abe1-4750-a787-0edbf7c0b912 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Abbeville, South Carolina (Utility Company) Effective date: 2011/01/06 End date if known: Rate name: Commercial service rate - Schedule H Sector: Commercial Description: For Abbeville Hospital only Source or reference: http://www.abbevilleutilities.com/electric/Commercial Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

128

Data:810d9662-a725-43b5-aa20-932abe5a2d81 | Open Energy Information  

Open Energy Info (EERE)

d9662-a725-43b5-aa20-932abe5a2d81 d9662-a725-43b5-aa20-932abe5a2d81 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Village of Davenport, Nebraska (Utility Company) Effective date: 2012/11/11 End date if known: Rate name: Directional Lighting HPS 250 W Sector: Lighting Description: Area/directional lighting of farmyards, backyards, patios, parking lots, storage yards, trailer courts, industrial sites, schools churches, apartments, businesses and many other applications where lighting is needed for identification, merchandising, environment, aesthetics, safety, security, protection or convenience.

129

Data:16d1c617-0312-43e6-841a-be1f18a18ade | Open Energy Information  

Open Energy Info (EERE)

7-0312-43e6-841a-be1f18a18ade 7-0312-43e6-841a-be1f18a18ade No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Fayetteville, Tennessee (Utility Company) Effective date: 2012/08/01 End date if known: Rate name: Security Lights: 1000W Sector: Lighting Description: Source or reference: http://www.fpunet.com/node/15 Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous

130

Data:5c930136-8abe-4301-a2f5-d3afc71e4705 | Open Energy Information  

Open Energy Info (EERE)

6-8abe-4301-a2f5-d3afc71e4705 6-8abe-4301-a2f5-d3afc71e4705 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Duke Energy Carolinas, LLC (South Carolina) Effective date: 2012/10/01 End date if known: Rate name: LGS (Large General Service) Sector: Commercial Description: Available to the individual customer with a kilowatt demand of more than 75 kW. If the customer's measured demand is 75 kW or less for twelve consecutive months, the customer will be served under Schedule SGS. Source or reference: http://www.duke-energy.com/pdfs/SCScheduleLGS.pdf Source Parent: Comments Applicable to 75kW-Infinity

131

Data:E543dfd9-f0d4-4b0a-be41-4428970b11a8 | Open Energy Information  

Open Energy Info (EERE)

f0d4-4b0a-be41-4428970b11a8 f0d4-4b0a-be41-4428970b11a8 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Polk County Rural Pub Pwr Dist Effective date: 2012/01/01 End date if known: Rate name: Irrigation CYC 1 - Time of Use - Single Phase Sector: Industrial Description: Source or reference: Illinois State University Binder #10. Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >>

132

PoS(ACAT)027 Online Monitoring for the CDF Run II Experiment  

E-Print Network (OSTI)

- gency situation handling were defined, e.g. remote shifter replacement with a local (Fnal) one in casePoS(ACAT)027 Online Monitoring for the CDF Run II Experiment and the Remote Operation Facilities T the CDF Run II online event monitoring system and operation, with enphasis on the remote monitoring shift

133

CDF/PUB/EXOTIC/PUBLIC/10737 Search for a Standard Model Higgs Boson Decaying Into Photons  

E-Print Network (OSTI)

CDF/PUB/EXOTIC/PUBLIC/10737 Search for a Standard Model Higgs Boson Decaying Into Photons at CDF) A search for the SM Higgs boson in the diphoton decay channel is reported using data corre- sponding are set on the production cross section times the H branching fraction for hypothetical Higgs boson

Fermilab

134

CDF Note 10625 Search for the Standard Model Higgs boson in +  

E-Print Network (OSTI)

CDF Note 10625 Search for the Standard Model Higgs boson in + - + jets final state with 8.3fb-1 a search for the Standard Model Higgs boson in + - + jets final state, using CDF Run II data with an integrated luminosity of 8.3 fb-1 . The Signal considered in this search is four Higgs boson production

Fermilab

135

Combination of searches for the Higgs boson using the full CDF data set T. Aaltonen,21  

E-Print Network (OSTI)

Combination of searches for the Higgs boson using the full CDF data set T. Aaltonen,21 S. Amerio,40 Higgs boson using the full CDF Run II data set, which corresponds to an integrated luminosity of 9 or Z boson or a t¯t pair. Depending on the production mode, Higgs boson decays to W+ W- , ZZ, b

Fermilab

136

Computing Models of CDF and D0 in Run II  

SciTech Connect

The next collider run of the Fermilab Tevatron, Run II, is scheduled for autumn of 1999. Both experiments, the Collider Detector at Fermilab (CDF) and the D0 experiment are being modified to cope with the higher luminosity and shorter bunch spacing of the Tevatron. New detector components, higher event complexity, and an increased data volume require changes from the data acquisition systems up to the analysis systems. In this paper we present a summary of the computing models of the two experiments for Run II.

Lammel, S.

1997-05-01T23:59:59.000Z

137

Using Feedback to Control Deadtime in the CDF Trigger System  

Science Conference Proceedings (OSTI)

The CDF experiment uses a three-level trigger system to select events produced during p{bar p} collisions. As the luminosity of the Tevatron accelerator falls by a factor of four over a 24 hour period, trigger selections are adjusted automatically in order to make full use of the data processing bandwidth. The selections are made to maximize high purity triggers and keep the deadtime as low as possible at any given luminosity throughout the entire course of a run. We describe the algorithms used to obtain these goals and how the changing conditions are accounted for in the analysis of the data.

Torretta, D.; /Fermilab

2007-04-01T23:59:59.000Z

138

Personal extrapolation of CDF test beam use to the SSC  

SciTech Connect

The author's personal experience in test beam usage at CDF is used to predict SSC needs at the point of turn-on. It is concluded that the test beam demand will reflect the scale of effort involved in SSC detectors rather than the total number of them. Provision for later expansion is recommended. It is also recommended that the test beam facilities, as well as detector electronics, should reflect the available dynamic range; particularly, a single high energy beam derived from the SSC could be shared by several groups. (LEW)

Nodulman, L.

1986-06-23T23:59:59.000Z

139

Collider Detector at Fermilab (CDF): Data from the QCD Group's Research into Properties of the Strong Interaction  

DOE Data Explorer (OSTI)

The Collider Detector at Fermilab (CDF) is a Tevatron experiment at Fermilab. The Tevatron, a powerful particle accelerator, accelerates protons and antiprotons close to the speed of light, and then makes them collide head-on inside the CDF detector. The CDF detector is used to study the products of such collisions. The CDF Physics Group at Fermilab is organized into six working groups, each with a specific focus. The QCD group studies the properties of the strong interaction. Their public web page makes data and numerous figures available from both CDF Runs I and II.

,

140

Collider Detector at Fermilab (CDF): Data from Standard Model and Supersymmetric Higgs Bosons Research of the Higgs Group  

DOE Data Explorer (OSTI)

The Collider Detector at Fermilab (CDF) is a Tevatron experiment at Fermilab. The Tevatron, a powerful particle accelerator, accelerates protons and antiprotons close to the speed of light, and then makes them collide head-on inside the CDF detector. The CDF detector is used to study the products of such collisions. The CDF Physics Group at Fermilab is organized into six working groups, each with a specific focus. The Higgs group searches for Standard Model and Supersymmetric Higgs bosons. Their public web page makes data and numerous figures available from both CDF Runs I and II.

The Higgs Group (CDF Physics) Fermilab; The CDF Collaboration

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


141

Updated measurements of hadronic B decays at CDF  

SciTech Connect

The CDF experiment at the Tevatron p{bar p} collider established that extensive and detailed exploration of the b-quark dynamics is possible in hadron collisions, with results competitive and supplementary to those from e{sup +}e{sup -} colliders. This provides a rich, and highly rewarding program that has currently reached full maturity. In the following I report some recent results on hadronic decays: the evidence for the charmless annihilation decay mode B{sub s}{sup 0} {yields} {pi}{sup +}{pi}{sup -}, and the first reconstruction in hadron collisions of the suppressed decays B{sup -} {yields} D({yields} K{sup +}{pi}{sup 0})K{sup -} and B{sup -} {yields} D({yields} K{sup +} {pi}{sup -}){pi}{sup -}.

Morello, Michael J.

2012-01-01T23:59:59.000Z

142

Combination of Standard Model Higgs searches at CDF  

Science Conference Proceedings (OSTI)

We present the latest combination of searches for a standard model (SM) Higgs boson in p{bar p} collisions at {radical}s = 1.96 TeV recorded by the CDF II detector at the Fermilab Tevatron. Using data corresponding to 2.3-5.9 fb{sup -1} of integrated luminosity, we perform searches in a number of different production and decay modes and then combine them to improve sensitivity. No excess in data above that expected from backgrounds is observed; therefore, we set upper limits on the production cross section times branching fraction as a function of the SM Higgs boson mass (m{sub H}). The combined observed (expected) limit is 1.9 (1.8) times the SM prediction at m{sub H} =115 GeV/c{sup 2} and 1.0 (1.1) times the SM prediction at m{sub H} = 165 GeV/c{sup 2}.

Potamianos, Karolos; /Purdue U. /Fermilab

2010-12-01T23:59:59.000Z

143

Standard model high mass Higgs search at CDF  

SciTech Connect

The CDF collaboration has analyzed almost 6 f b{sup -1} of data collected at the Tevatron Collider at {radical}{ovr s} = 1.96 TeV to search for Standard Model Higgs boson through the decay into W{sup +}W{sup -}*. Starting from events with two leptons, advanced analysis techniques are applied to better discriminate signal from background. The Higgs sensitivity is maximized combining together analysis that exploit different event topologies. No significant excess over the expected background is observed and data is used to set a limit in units of Standard Model expectations. The limit plays a fundamental role in the Higgs search excluding the existence of this particle with mass between 158 and 175 GeV/c{sup 2} when combined with D0, the other Tevatron experiment.

Lucchesi, Donatella; /INFN, Padua

2010-01-01T23:59:59.000Z

144

CDF DZERO Reports | U.S. DOE Office of Science (SC)  

Office of Science (SC) Website

DZERO Reports Print Text Size: A A A RSS Feeds FeedbackShare Page DOE Review Committee Report on the Baseline Review of the RUN IIb CDF and D-Zero Detector Projects .pdf file...

145

Selection of tau leptons with the CDF Run 2 trigger system  

SciTech Connect

We have implemented triggers for hadronically decaying tau leptons within a framework of the CDF Run 2 trigger system. We describe the triggers, along with their physics motivations, and report on their initial performance.

A. Anastassov; S. Baroiant; M. Chertok

2003-07-01T23:59:59.000Z

146

Measurement of b-quark Jet Shapes at CDF  

SciTech Connect

The main topic of this thesis is the measurement of b-quark jet shapes at CDF. CDF is an experiment located at Fermilab, in the United States, which studies proton-antiproton collisions at a center of mass energy of 1.96TeV. To reach this energy, the particles are accelerated using the Tevatron accelerator which is currently the highest energy collider in operation. The data used for this analysis were taken between February 2002 and September 2004 and represent an integrated luminosity of about 300 pb{sup -1}. This is the first time that b-quark jet shapes have been measured at hadron colliders. The basis of this measurement lies in the possibility of enhancing the b-quark jet content of jet samples by requiring the jets to be identified as having a displaced vertex inside the jet cone. Such jets are called tagged. This enhances the b-quark jet fraction from about 5% before tagging to 20-40% after tagging, depending on the transverse momentum of the jets. I verified that it is possible to apply this secondary vertex tagging algorithm to different cone jet algorithms (MidPoint and JetClu) and different cone sizes (0.4 and 0.7). I found that the performance of the algorithm does not change significantly, as long as the sub-cone inside which tracks are considered for the tagging is kept at the default value of 0.4. Because the b-quark purity of the jets is still relatively low, it is necessary to extract the shapes of b-quark jets in a statistical manner from the jet shapes both before and after tagging. The other parameters that enter into the unfolding equation used to extract the b-quark jet shapes are the b-jet purities, the biases due to the tagging requirement both for b- and nonbjets and the hadron level corrections. The last of these terms corrects the measured b-jet shapes back to the shapes expected at hadron level which makes comparisons with theoretical models and other experimental results possible. This measurement shows that, despite relatively large systematic uncertainties, the measured b-quark jet shapes are significantly different from those expected from the so-called Pythia Tune A Monte Carlo simulation, the most widely used Leading Order Monte Carlo model at CDF. This difference can be mostly attributed to the fact that the fraction of b-quark jets that originate from flavour creation (where a single b-quark is expected inside the same jet cone) over those that originate from gluon splitting (where two b-quarks are expected to be inside the same jet cone) is slightly different in the Pythia Tune A Monte Carlo predictions than in data. This measurement can help in the tuning of the fraction of gluon splitting to flavour creation b-quark jets in the Monte Carlo simulation. This tuning is particularly important for the extrapolation up to LHC energies where many searches will involve b-quark jets. During the first year of my thesis work, I worked on the implementation of a prototype detector control system for the electromagnetic calorimeter which is being built for the CMS experiment at CERN. The prototype which I implemented was used to monitor and control the high voltage, low voltage, cooling and precision temperature monitoring systems during the summer 2003 test-beam. This was one of the first, almost complete, systems implemented and used by an LHC experiment for test-beam monitoring.

Lister, Alison; /Zurich, ETH

2006-03-01T23:59:59.000Z

147

Data:78abe03e-7fa4-411e-9443-7ae34c3bc240 | Open Energy Information  

Open Energy Info (EERE)

abe03e-7fa4-411e-9443-7ae34c3bc240 abe03e-7fa4-411e-9443-7ae34c3bc240 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Independence, Missouri (Utility Company) Effective date: 2013/07/01 End date if known: Rate name: Large Power Service - Over 1800 kW Sector: Industrial Description: For first 1800 kW of energy charges, see rate Large Power Service - 1800 kW and under Source or reference: www.ci.independence.mo.us/userdocs/pl/Rates/IPL Rates - T (7-1-12) - LP-2.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh):

148

Data:7352fd77-7327-4f74-848f-a6abe6538a8f | Open Energy Information  

Open Energy Info (EERE)

7-7327-4f74-848f-a6abe6538a8f 7-7327-4f74-848f-a6abe6538a8f No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Blue Grass Energy Coop Corp Effective date: 2013/01/01 End date if known: Rate name: Interruptible Service - Credit Sector: Industrial Description: Interruptible Service : Annual Hours of Interruption 200 300 400 10 notice minutes - $4.20 $4.90 $5.60 60 notice minutes - $3.50 $4.20 $4.90 Source or reference: Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V):

149

Data:0c6a9591-def4-4abe-b362-964082e712fe | Open Energy Information  

Open Energy Info (EERE)

a9591-def4-4abe-b362-964082e712fe a9591-def4-4abe-b362-964082e712fe No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Carteret-Craven El Member Corp Effective date: 2013/01/01 End date if known: Rate name: Medium General Service Time-Of-Use Sector: Commercial Description: * Fixed monthly charge includes $2.08 REPS (Rider REPS-1) rate-Renewable Energy & Energy Efficiency Portfolio Standard. This schedule is available as an optional rate for electric service normally provided under the Cooperative's Medium General Service - Schedule MGS.Service under this schedule is closed and not available for any building, structure, or premise not receiving service under this schedule prior to January 1, 2007. Buildings, structures, or premises receiving service under this schedule prior to January 1, 2007 may continue receiving service until the name of the customer responsible for the service is changed.

150

Data:440158cd-1abe-4fbe-b412-878bb0d61a6a | Open Energy Information  

Open Energy Info (EERE)

abe-4fbe-b412-878bb0d61a6a abe-4fbe-b412-878bb0d61a6a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Connecticut Light & Power Co Effective date: 2013/07/01 End date if known: Rate name: Rate 27- SMALL TIME-OF-DAY GENERAL ELECTRIC SERVICE (Bundled Service) Sector: Commercial Description: AVAILABLE for the entire electrical requirements at a single service location measured through one metering installation where the customer's maximum demand is less than 350 kW. Notwithstanding the applicability provisions of other rates, this rate is also available to full requirements customers that (i) prior to March 1, 1992, had a maximum monthly 30-minute demand in excess of 350 kW; (ii) had a maximum monthly 30-minute demand in the twelve billing periods prior to March 1, 1992, that equaled or exceeded twice the average of the customer's maximum monthly 30-minute demands during the same billing periods; (iii) as of March 1, 1992, had established, and had a reasonable expectation of continuing, a seasonal pattern of electrical usage approximating that established during the twelve billing periods prior to March 1, 1992; and (iv) had not discontinued taking service under this rate or Rate 30 after March 1, 1992.

151

Data:Cd4372b7-e847-4c82-abee-7dc7a3168f43 | Open Energy Information  

Open Energy Info (EERE)

72b7-e847-4c82-abee-7dc7a3168f43 72b7-e847-4c82-abee-7dc7a3168f43 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Caddo Electric Coop, Inc Effective date: 2007/05/01 End date if known: Rate name: Domestic-All Electric Load Control-Rate 4,Single Phase Sector: Residential Description: 1. Available to homes,schools,churches and community halls for all uses including mobile homes,who also agree to allow control of air-conditioning systems and water heaters by means of automated load Control Relays and subject to the established rules and regulations of the cooperative. 2. The capacity of individual motors served under this schedule shall not exceed 10 horsepower.

152

Data:05aa389c-abf1-499e-abe4-89ef2dab169b | Open Energy Information  

Open Energy Info (EERE)

89c-abf1-499e-abe4-89ef2dab169b 89c-abf1-499e-abe4-89ef2dab169b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Manitowoc Public Utilities Effective date: 2009/06/01 End date if known: Rate name: Cp-3 Large Power Time-of-Day Service(<6000 volts) Transformer Ownership Discount with Parallel Generation(20kW or less) Sector: Industrial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0361 per kilowatt-hour.

153

Data:787abe10-21ff-4dae-9ac1-d6b6ad3f4673 | Open Energy Information  

Open Energy Info (EERE)

abe10-21ff-4dae-9ac1-d6b6ad3f4673 abe10-21ff-4dae-9ac1-d6b6ad3f4673 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Monroe County Elec Coop, Inc Effective date: 2013/07/01 End date if known: Rate name: Schedule City of Red Bud Residential- Rate 0033 Sector: Residential Description: This rate is available to those members who are receiving service from the cooperative and whose residence and/or business has been annexed into the city limits of Red Bud. Source or reference: http://www.mcec.org/Documents/2013%20Rates.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):

154

Data:C9a47dde-6d96-4513-abe0-08ff1314d6ab | Open Energy Information  

Open Energy Info (EERE)

a47dde-6d96-4513-abe0-08ff1314d6ab a47dde-6d96-4513-abe0-08ff1314d6ab No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Decatur County Rural E M C Effective date: 2010/04/01 End date if known: Rate name: SMALL COMMERCIAL ELECTRIC SERVICE Sector: Commercial Description: Three phase, 60 hertz, at standard voltages; where service is supplied three phase, transformation will be approximately 240 or 480 volts three wire delta, 240/480 volts or 120/240 volts four wire delta, or 208Y/120 or 480Y/277 volts four wire wye. Should Customer require a non-standard voltage, Customer shall, at his own expense, furnish and maintain all transformers and protective equipment therefore necessary in order to obtain such non-standard voltage.

155

Data:Abe526c1-9c10-4b5c-a982-dbd652ca6b20 | Open Energy Information  

Open Energy Info (EERE)

Abe526c1-9c10-4b5c-a982-dbd652ca6b20 Abe526c1-9c10-4b5c-a982-dbd652ca6b20 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Halifax Electric Member Corp Effective date: 2012/10/01 End date if known: Rate name: RESIDENTIAL SERVICE Sector: Residential Description: AVAILABILITY: This Schedule is available in all territory served by the Cooperative, subject to its established Service Rules and Regulations. APPLICABILITY: This Schedule is applicable when electric service is used for domestic purposes in and about a residential dwelling unit. Service under this Schedule is not applicable for farm operations such as crop dryers or tobacco barns, or for other commercial purposes. However, where this type of service is in combination with residential service and the total demand of the nonresidential usage is not greater than the total demand of the residential service requirements, the consumer may be served under this Schedule. If the predominant demand is nonresidential in nature, the Member must be served under a General Service schedule or the residential and nonresidential loads will be metered separately and billed under the appropriate schedule for each service. Service shall be provided at one location through one meter.

156

Data:559a7827-73cf-4e5a-be1b-93726239c9fa | Open Energy Information  

Open Energy Info (EERE)

827-73cf-4e5a-be1b-93726239c9fa 827-73cf-4e5a-be1b-93726239c9fa No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Burke-Divide Electric Coop Inc Effective date: 2012/01/01 End date if known: Rate name: A1 Single Phase Commercial Sector: Commercial Description: AVAILABILITY Available for all uses, subject to the established rules and regulations of the Seller, for:Commercial TYPE OF SERVICE Single-phase, 60 cycles, at available secondary voltage. The capacity of individual motors served under this schedule shall not exceed 10 H.P. except by special permission. This permission may be granted when voltage drop studies indicate a minimal voltage drop to other consumers.

157

Data:Abe398ae-d3b6-4e6e-9181-24ab0cc00478 | Open Energy Information  

Open Energy Info (EERE)

Abe398ae-d3b6-4e6e-9181-24ab0cc00478 Abe398ae-d3b6-4e6e-9181-24ab0cc00478 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of St Marys, Ohio (Utility Company) Effective date: 2001/06/10 End date if known: Rate name: Commercial Space Heating and Water Heating Rate Sector: Commercial Description: *This rate is available to all stores, offices, hotels, apartment buildings and other places of business for separately metered service for space-heating and/or water heating purposes. character of service:120/240, 120/208 Volt Alternating Current, 60 Hertz, Single Phase. distribution and ancillary charges added to energy and transmission charge.

158

Data:675aef35-8052-49ba-abe9-464e1b6f0b6b | Open Energy Information  

Open Energy Info (EERE)

aef35-8052-49ba-abe9-464e1b6f0b6b aef35-8052-49ba-abe9-464e1b6f0b6b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Cedarburg Light & Water Comm Effective date: 2011/01/01 End date if known: Rate name: Small Power Optional Time-of-Day Rate - between 50kW and 200kW Demand Primary Metering Discount Sector: Industrial Description: "On-Peak" period: 8 a.m. to 8 p.m., Monday through Friday, excluding holidays. The optional time-of-day rate who are metered on the primary side receive a discount. A discount is also available for customers who own and maintain their own transformer.

159

Data:0f6aef47-90d5-4abe-bcc1-41da2e81331b | Open Energy Information  

Open Energy Info (EERE)

7-90d5-4abe-bcc1-41da2e81331b 7-90d5-4abe-bcc1-41da2e81331b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Wapakoneta, Ohio (Utility Company) Effective date: End date if known: Rate name: General Service- Three-Phase Sector: Commercial Description: Demand Charges: First 5 kW: No Charge Over 5 kW: $6.00/kW Source or reference: http://www.amlegal.com/nxt/gateway.dll/Ohio/wapakone/partten-streetsutilitiesandpublicservice/titlefour-utilities/chapter1046electricity?f=templates$fn=default.htm$3.0$vid=amlegal:wapakoneta_oh$anc=JD_1046.07 Source Parent: Comments Applicability Demand (kW)

160

Data:3c4f38a9-a290-47ff-9e09-32abe7803a47 | Open Energy Information  

Open Energy Info (EERE)

8a9-a290-47ff-9e09-32abe7803a47 8a9-a290-47ff-9e09-32abe7803a47 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Bartholomew County Rural E M C Effective date: 2011/10/01 End date if known: Rate name: Public Street Lighting Service, Metal Halide Lamps, 36,000 Lumens, 458W (New Wood Pole) Sector: Lighting Description: The above rates for Standard Public Street Lighting Service are based on the costs of standard overhead service and standard wood poles. The Customer will be required to pay a one-time contribution-in-aide-of construction (CIAC) to cover the additional costs of any non-standard lighting service requested by the Customer. Non-standard public street lighting service consists of installations requiring more than one wood pole and special poles, transformers, line extensions, non-standard fixtures and lamps, or underground service. The CIAC shall be based on the difference between the cost to provide standard service and the actual cost of the non-standard service as per current standard cost .

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


161

Data:B0db37c8-abe3-43e2-9f5f-dfeb7ccde908 | Open Energy Information  

Open Energy Info (EERE)

7c8-abe3-43e2-9f5f-dfeb7ccde908 7c8-abe3-43e2-9f5f-dfeb7ccde908 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Public Service Co of Colorado Effective date: 2012/10/11 End date if known: Rate name: ENERGY ONLY STREET LIGHTING SERVICE - SCHEDULE ESL - 72.1-75.0 kWh per light Sector: Lighting Description: Source or reference: www.xcelenergy.com/staticfiles/xe/Regulatory/Regulatory PDFs/psco_elec_entire_tariff.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V):

162

Data:225863a7-2abe-47a9-82a2-c154ea60f869 | Open Energy Information  

Open Energy Info (EERE)

a7-2abe-47a9-82a2-c154ea60f869 a7-2abe-47a9-82a2-c154ea60f869 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Rockwood, Tennessee (Utility Company) Effective date: 2012/12/01 End date if known: Rate name: Outdoor Lighting Metal Halide Flood Light 1000w Sector: Lighting Description: ROCKWOOD ELECRIC UTILITY can install a private security light on your residential or commercial property under most conditions. All new requests for outdoor lighting require the applicant to sign a minimum two year contract for security lighting service. If you have security concerns and would like to discuss outdoor lighting options, please contact our Engineering Department to look at the situation with you.

163

Data:03eca578-3abe-47d6-9a5b-df9668be1afc | Open Energy Information  

Open Energy Info (EERE)

eca578-3abe-47d6-9a5b-df9668be1afc eca578-3abe-47d6-9a5b-df9668be1afc No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of New Bern, North Carolina (Utility Company) Effective date: 2008/07/01 End date if known: Rate name: Area Lighting Schedule - Retrofit Sodium Vapor 12,000 Lumen 150w Sector: Lighting Description: Source or reference: www.newbern-nc.org/Elec/ElectricRates.php Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category:

164

Data:Abee1802-a08c-4fb9-a50f-f9b4204f86c8 | Open Energy Information  

Open Energy Info (EERE)

Abee1802-a08c-4fb9-a50f-f9b4204f86c8 Abee1802-a08c-4fb9-a50f-f9b4204f86c8 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Columbus, Wisconsin (Utility Company) Effective date: 2006/02/01 End date if known: Rate name: Cp-1 Small Power Service Primary Metering and Transformer Ownership Discount with Parallel Generation(20kW or less) Sector: Industrial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kWh of sales) is greater or lesser than the base cost of power purchased (per kWh of sales). The base cost of power is $0.0549 per kWh. See schedule PCAC.

165

Precision Top-Quark Mass Measurements at CDF  

Science Conference Proceedings (OSTI)

We present a precision measurement of the top-quark mass using the full sample of Tevatron {radical}s = 1.96 TeV proton-antiproton collisions collected by the CDF II detector, corresponding to an integrated luminosity of 8.7 fb{sup -1}. Using a sample of t{bar t} candidate events decaying into the lepton+jets channel, we obtain distributions of the top-quark masses and the invariant mass of two jets from the W boson decays from data. We then compare these distributions to templates derived from signal and background samples to extract the top-quark mass and the energy scale of the calorimeter jets with in situ calibration. The likelihood fit of the templates from signal and background events to the data yields the single most-precise measurement of the top-quark mass, mtop = 172.85 {+-} 0.71 (stat) {+-} 0.85 (syst) GeV/c{sup 2}.

Aaltonen, T.; /Helsinki Inst. of Phys.; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U. /Fermilab; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Arisawa, T.; /Waseda U.; Artikov, A.; /Dubna, JINR /Texas A-M

2012-07-01T23:59:59.000Z

166

Design and first tests of the CDF Run 2 farms  

SciTech Connect

The high energy physics experiment CDF, located in the anti-proton-proton collider at Fermilab, will write data in Run 2 at a rate of 20 MByte/s, twenty times the rate of Run 1. The offline production system must be able to handle this rate. Components of that system include a large PC farm, I/O systems to read/write data to and from mass storage, and a system to split the reconstructed data into physics streams which are required for analysis. All of the components must work together seamlessly to ensure the necessary throughput. A description will be given of the overall hardware and software design for the system. A small prototype farm has been used for about one year to study performance, to test software designs and for the first Mock Data Challenge. Results from the tests and experience from the first Mock Data Challenge will be discussed. The hardware for the first production farm is in place and will be used for the second Mock Data Challenge. Finally, the possible scaling of the system to handle larger rates foreseen later in Run 2 will be described.

Jaroslav Antos et al.

2000-05-30T23:59:59.000Z

167

Improving Higgs Sensitivity at CDF by Introducing New Muon Triggers  

Science Conference Proceedings (OSTI)

A search for Standard Model Higgs boson production in the H {yields} WW {yields} {ell}{nu}jj channel using 5.7 fb{sup -1} of CDF II data is presented. The search is performed using a matrix element technique in which event probability densities for the signal and background hypotheses are calculated and used to create a powerful disciminator (called the event probability discriminant, EPD). The EPD distributions for signal and background are fit to the data using a binned likelihood approach to search for the Higgs boson signal. To improve the limits on the H production cross section, a new muon category, CMP, is added. No evidence for a Higgs boson signal is observed, and 95% confidence level upper limits on the H cross section times the branching ratio of the Higgs boson to decay to two W of {sigma}(p{bar p} {yields} H) x BR(H {yields} WW)/SM Higgs boson masses of between m{sub H} = 150 GeV/c{sup 2} and m{sub H} = 200 GeV/c{sup 2} are found. The expected (median) limit estimated in pseudo-experiments is {sigma}(p{bar p} {yields} H) x BR(H {yields} WW)/SM < 12.5 to 41.0 at 95% C.L. The inclusion of the phi gap trigger lead to improvements in the sensitivity of up to 7.3%; on average, the improvement in the sensitivity was 3.3%.

Buchmann, Marco-Andrea; /Zurich, ETH

2010-07-01T23:59:59.000Z

168

CDF GlideinWMS usage in grid computing of high energy physics  

SciTech Connect

Many members of large science collaborations already have specialized grids available to advance their research in the need of getting more computing resources for data analysis. This has forced the Collider Detector at Fermilab (CDF) collaboration to move beyond the usage of dedicated resources and start exploiting Grid resources. Nowadays, CDF experiment is increasingly relying on glidein-based computing pools for data reconstruction. Especially, Monte Carlo production and user data analysis, serving over 400 users by central analysis farm middleware (CAF) on the top of Condor batch system and CDF Grid infrastructure. Condor is designed as distributed architecture and its glidein mechanism of pilot jobs is ideal for abstracting the Grid computing by making a virtual private computing pool. We would like to present the first production use of the generic pilot-based Workload Management System (glideinWMS), which is an implementation of the pilot mechanism based on the Condor distributed infrastructure. CDF Grid computing uses glideinWMS for its data reconstruction on the FNAL campus Grid, user analysis and Monte Carlo production across Open Science Grid (OSG). We review this computing model and setup used including CDF specific configuration within the glideinWMS system which provides powerful scalability and makes Grid computing working like in a local batch environment with ability to handle more than 10000 running jobs at a time.

Zvada, Marian; /Fermilab /Kosice, IEF; Benjamin, Doug; /Duke U.; Sfiligoi, Igor; /Fermilab

2010-01-01T23:59:59.000Z

169

Improving Higgs Sensitivity at CDF by Introducing New Muon Triggers  

SciTech Connect

A search for Standard Model Higgs boson production in the H {yields} WW {yields} {ell}{nu}jj channel using 5.7 fb{sup -1} of CDF II data is presented. The search is performed using a matrix element technique in which event probability densities for the signal and background hypotheses are calculated and used to create a powerful disciminator (called the event probability discriminant, EPD). The EPD distributions for signal and background are fit to the data using a binned likelihood approach to search for the Higgs boson signal. To improve the limits on the H production cross section, a new muon category, CMP, is added. No evidence for a Higgs boson signal is observed, and 95% confidence level upper limits on the H cross section times the branching ratio of the Higgs boson to decay to two W of {sigma}(p{bar p} {yields} H) x BR(H {yields} WW)/SM < 7.7 to 62.1 for Higgs boson masses of between m{sub H} = 150 GeV/c{sup 2} and m{sub H} = 200 GeV/c{sup 2} are found. The expected (median) limit estimated in pseudo-experiments is {sigma}(p{bar p} {yields} H) x BR(H {yields} WW)/SM < 12.5 to 41.0 at 95% C.L. The inclusion of the phi gap trigger lead to improvements in the sensitivity of up to 7.3%; on average, the improvement in the sensitivity was 3.3%.

Buchmann, Marco-Andrea; /Zurich, ETH

2010-07-01T23:59:59.000Z

170

Final measurement of $B^0_s$ mixing phase in the full CDF Run II data set  

E-Print Network (OSTI)

We report the final CDF measurement of the $B^0_s$ mixing phase, mean lifetime, and decay-width difference through the fit of the time evolution of flavor-tagged $B^0_s \\rightarrow J/\\psi \\phi$ decays. The measurement is based on the full data set of 1.96 TeV $p\\bar{p}$ collisions collected between February 2002 and September 2011 by the CDF experiment. The results are consistent with the standard model and other experimental determinations and are amongst the most precise to date.

Sabato Leo

2012-07-28T23:59:59.000Z

171

Measurement of low $p_{T}$ $D^{0}$ meson production cross section at CDF II.  

Science Conference Proceedings (OSTI)

In this thesis we present a study of the production of D{sup 0} meson in the low transverse momentum region. In particular the inclusive differential production cross section of the D{sup 0} meson (in the two-body decay channel D{sup 0} {yields} K{sup -}{pi}{sup +}) is obtained extending the published CDF II measurement to p{sub T} as low as 1.5 GeV/c. This study is performed at the Tevatron Collider at Fermilab with the CDF II detector.

Mussini, Manuel; /Bologna U.

2011-05-01T23:59:59.000Z

172

Recent beauty results from CDF and the Run-II upgrades  

SciTech Connect

This paper reports on the most recent results from the Collider Detector Facility (CDF) from 110 pb{sup -1} of data taken at the Fermilab Tevatron from 1992 to 1995. Improved measurements of B meson spectroscopy, lifetimes, and searches for new particle states are presented. Evidence for the effectiveness of same side tagging techniques in the context of mixing measurements is shown with applicability for CP violation studies in Run-II explained. The planned upgrades of importance to {ital b} physics for Run-II are briefly detailed with an emphasis on the expected physics reach in Run-II by CDF.

Huffman, B.T. [Pittsburgh Univ., PA (United States); CDF Collaboration

1996-09-01T23:59:59.000Z

173

Data:0b5b6f54-7715-4e36-a8ab-e475ad6736d7 | Open Energy Information  

Open Energy Info (EERE)

Data Data Edit with form History Facebook icon Twitter icon » Data:0b5b6f54-7715-4e36-a8ab-e475ad6736d7 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: New York Power Authority Effective date: 2013/07/01 End date if known: Rate name: SC 68 Conventional Sector: Industrial Description: New York City Customers Source or reference: http://www.nypa.gov/about/documents.htm Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

174

Data:F319e702-4ef4-4a4e-9bc5-abed3a4e456e | Open Energy Information  

Open Energy Info (EERE)

Data Data Edit with form History Facebook icon Twitter icon » Data:F319e702-4ef4-4a4e-9bc5-abed3a4e456e No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Sand Mountain Electric Coop Effective date: 2013/05/01 End date if known: Rate name: Schedule GSA - General Power Service - Part 1 Sector: Commercial Description: Source or reference: Illinois State University Archives Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

175

Data:9fb4ba6f-444e-4d67-a06a-be8f9b787c80 | Open Energy Information  

Open Energy Info (EERE)

fb4ba6f-444e-4d67-a06a-be8f9b787c80 fb4ba6f-444e-4d67-a06a-be8f9b787c80 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Hendricks County Rural E M C Effective date: End date if known: Rate name: NET METERING- Residential consumers with an RGS on their premises with a nameplate rating of 10 KW or less. Sector: Residential Description: Available to any member of the organization located on its lines for residential buildings. This rate schedule will serve single-phase member. As of April 1, 2012, the Wholesale Power Tracker is $0.001061 per kwh. This charge describes the fees that Hendricks Power incurs each month in purchasing wholesale power on your behalf. The charge fluctuates each quarter as fuel prices change. Power plants in the Midwest burn primarily coal as the fuel to generate electricity. When the market price changes for the coal they purchase, they pass that charge along to us. We then use the fuel charge to reflect your portion of the fuel expense we incur. By structuring the charge in this manner, we avoid having to incorporate these fluctuating expenses in the base electric rate. When fuel prices decline, this component of the bill can appear as a credit on your bill.

176

Data:35276a3c-abed-4b10-88aa-13ce3d186247 | Open Energy Information  

Open Energy Info (EERE)

a3c-abed-4b10-88aa-13ce3d186247 a3c-abed-4b10-88aa-13ce3d186247 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Nodak Electric Coop Inc Effective date: End date if known: Rate name: Industrial- Distribution Delivery - Three Phase Sector: Industrial Description: Applies to all customers who historically meet the following criteria: 1. average greater than 50 KW monthly demand per year, or 2. have a monthly demand greater than 100 KW two or more times per year, or 3. require service to an irrigation site. Load Management Options - Two options are available to C/I customers who wish to lower their coincidental demand charges by participating in the Load Management Program. 1. Full load management - Under full load management, the customer is expected to curtail load during all hours of load management. Under this option, the customer can avoid all seasonal coincidental demand charges. 2. Incremental pricing - Customers also have the option of purchasing energy during certain control periods. Nodak will provide a signal at the load management receiver indicating whether or not incremental energy is available. The customer is responsible to monitor the load management system status. If the customer chooses to operate through periods when incremental energy is available, coincidental demand charges will not accrue; however, an incremental adder will be charged for each kilowatt-hour consumed during those hours. These charges are as follows: Irrigation incremental adder up to *$0.12/Kwh All other C/I accounts incremental adder up to *$0.095/Kwh

177

Data:0d717abe-f0bc-4ec0-bb14-07d8a2ffda7b | Open Energy Information  

Open Energy Info (EERE)

7abe-f0bc-4ec0-bb14-07d8a2ffda7b 7abe-f0bc-4ec0-bb14-07d8a2ffda7b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Town of High Point, North Carolina (Utility Company) Effective date: 2012/07/06 End date if known: Rate name: General Service- Time of Use Sector: Commercial Description: (a) Available on a voluntary and limited basis to individual establishments. (b) Service under this Schedule shall be used only by the contracting customer in a single enterprise, located entirely on a single, contiguous premise. (c) This Schedule is not available to the individual customer who qualifies for a Residential Schedule nor for auxiliary or breakdown service and power hereunder shall not be used for resale or exchange or in parallel with other electric power, or as a substitute for power contracted for or which may be contracted for, under any other schedule of the City, except at the option of the City, under special terms and conditions expressed in writing in the contract with the customer. (d) The obligations of the City in regard to supplying power are dependent upon its securing and retaining all necessary rights-of-way, privileges, satisfactory point of delivery and permits, for the delivery of such power, and the City shall not be liable to any customer or applicant for power in the event it is delayed in, or is prevented from, furnishing the power by its failure to secure and retain such rights, privileges, satisfactory point of delivery and permits.

178

Data:4edc3d50-7a19-4fb4-aa9e-64abe5464fed | Open Energy Information  

Open Energy Info (EERE)

edc3d50-7a19-4fb4-aa9e-64abe5464fed edc3d50-7a19-4fb4-aa9e-64abe5464fed No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: PUD No 1 of Chelan County Effective date: 2012/01/01 End date if known: Rate name: RESIDENTIAL THREE PHASE Sector: Residential Description: This schedule is available throughout Chelan County served by the District with the exception of the Stehekin area, and is applicable to service for private residence, apartment, summer home, farm and incidental farm power purposes. RATE DISCOUNT: 1. A rate discount not to exceed $9.25 per month is available to qualifying low income seniors 62 years and older and low income disabled as provided for in State of Washington R.C.W. 74.38.070. The rate discount will not exceed the amount of the monthly bill up to $9.25 per month and will be applied to one account only. 2. To qualify for the rate discount applicants must provide satisfactory proof of the following: FOR LOW INCOME SENIORS: 1. Age 62 years or older prior to or during the month in which the discount is to apply. 2. Total household income including his or her spouse or co-tenant does not exceed the amount specified in R.C.W. 84.36.381 (5)(b). 3. Ownership or occupancy as head of household residing therein at certain property being served electricity within the District's service area.

179

Control and data acquisition electronics for the CDF Silicon Vertex Detector  

SciTech Connect

A control and data acquisition system has been designed for the CDF Silicon Vertex Detector (SVX) at Fermilab. The system controls the operation of the SVX Rev D integrated circuit (SVX IC) that is used to instrument a 46,000 microstrip silicon detector. The system consists of a Fastbus Sequencer, a Crate Controller and Digitizer modules. 11 refs., 6 figs., 3 tabs.

Turner, K.J.; Nelson, C.A.; Shaw, T.M.; Wesson, T.R.

1991-11-01T23:59:59.000Z

180

Search for a Higgs Boson Decaying to Two W Bosons at CDF  

E-Print Network (OSTI)

We present a search for a Higgs boson decaying to two W bosons in pp? collisions at ?s=1.96??TeV center-of-mass energy. The data sample corresponds to an integrated luminosity of 3.0??fb-1 collected with the CDF II detector. ...

Makhoul, K.

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


181

Novel inclusive search for the Higgs boson in the four-lepton final state at CDF  

E-Print Network (OSTI)

An inclusive search for the standard model Higgs boson using the four-lepton final state in proton-antiproton collisions produced by the Tevatron at ?s=1.96??TeV is conducted. The data are recorded by the CDF II detector ...

Gomez-Ceballos, Guillelmo

182

CDF Note 10709 A Search For Dark Matter in the Monojet + Missing Transverse Energy  

E-Print Network (OSTI)

CDF Note 10709 A Search For Dark Matter in the Monojet + Missing Transverse Energy Signature in 6: November 23, 2011) We present the results of a search for dark matter production in the monojet + missing transverse energy signature. We analyze a sample of Tevatron pp collisions at s=1.96 TeV, recorded

Quigg, Chris

183

Data:Cdf30079-caa9-4dfd-8cdd-186045328942 | Open Energy Information  

Open Energy Info (EERE)

Cdf30079-caa9-4dfd-8cdd-186045328942 Cdf30079-caa9-4dfd-8cdd-186045328942 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Elkhorn Rural Public Pwr Dist Effective date: 2013/01/01 End date if known: Rate name: RATE 37- Irrigation Pumping--10-Hour Daily Control Sector: Commercial Description: AVAILABLE: In the general area served by the District. APPLICABLE: To year-round irrigation service to customers who will contract for a ten hour period of each day for twenty (20) horsepower or more and who have entered into an agreement to facilitate the necessary control for a ten hour period of controlled pumping.

184

Past, present and future highlights in top and higgs physics from the CDF experiment  

SciTech Connect

The 1992-1995 running of the Fermilab Tevatron (the so-called Run 1) ended with many important physics goals accomplished, including the discovery of the top quark, and the anticipation of many further questions be to answered in the future. In March 2002, after many detector upgrades by both the CDF and D0 experiments, and significant upgrades of the accelerator itself, the Tevatron Run 2 began (after a detector commissioning run) with the ultimate goal of discovering the Higgs boson. Here, we will highlight some important Run 1 results from CDF in the areas of top quark and Higgs boson physics, show some preliminary studies from Run 2, and give some expectations of what Run 2 will ultimately provide to our understanding of matter.

M. C. Kruse

2003-12-15T23:59:59.000Z

185

Searches for the standard model Higgs boson at the CDF experiment  

SciTech Connect

The understanding of the dynamics behind the breaking of the electroweak symmetry is one of the most important goals in the field of high energy physics. In the Standard Model (SM) Higgs mechanism plays a key role in the symmetry breaking, one manifestation of which is spin-0 Higgs boson. Thus the search for the Higgs boson is one of the flag-ship analyses at the Tevatron. Over the past few years the CDF experiment has made significant improvements in its sensitivity on the search for the SM Higgs boson. In this paper we summarize CDF's most recent results on the searches for the SM Higgs boson production at the Tevatron using data samples of integrated luminosities up to 3 fb{sup -1}. We also present the Tevatron's latest combined results on the SM Higgs boson search, and discuss the possibility that it could be found at the Tevatron in the near future.

Wang, Song-ming; /Taiwan, Inst. Phys.

2009-01-01T23:59:59.000Z

186

Measuring the CKM matrix element V{sub tb} at D-zero and CDF  

SciTech Connect

I present measurements by the CDF collaboration of the Standard Model three generation CKM matrix element V{sub tb} and of a special case extension with additional assumptions, using current Tevatron t{anti t} data. I then show how we can significantly improve the precision on V{sub tb} and at the same time extend the measurement so it is not constrained by Standard Model assumptions, using single top production at the upgraded Tevatron.

Heinson, A.P.

1997-07-01T23:59:59.000Z

187

Combined upper limit on Standard Model Higgs boson production at CDF  

E-Print Network (OSTI)

The Higgs boson is the only elementary particle predicted by the Standard Model (SM) that has neither been confirmed nor refuted. The CDF collaboration has performed SM Higgs searches in many channels using $p\\pbar$ collisions at a centre-of-mass energy $\\sqrt{s}=1.96\\tev$. We present the latest combined Higgs boson search at CDF. Since the previous year's combination, the sensitivity is increased through the addition of new channels, the improvement of existing channels and the addition of new data samples. We also use the latest parton distribution functions and $gg \\rightarrow H$ theoretical cross sections when modelling the signal event yields. Using integrated luminosities of up to 8.2 $\\invfb$, we observe a good agreement between data and the background prediction. Since we do not see a Higgs boson excess, we set 95% CL upper limits on the Higgs boson cross section in the range between 100 and 200 $\\gevcc$, with 5 $\\gevcc$ increments. The observed (expected) limits for a 115 and a 165 $\\gevcc$ Higgs boson are 1.55 (1.49) and 0.75 (0.79) $\\times$ SM, respectively. Since last year, the Higgs boson excluded range by CDF is extended to 156.5 - 173.7 and 100 - 104.5 $\\gevcc$.

Buzatu Adrian

2012-02-09T23:59:59.000Z

188

Combined upper limit on Standard Model Higgs boson production at CDF  

Science Conference Proceedings (OSTI)

The Higgs boson is the only elementary particle predicted by the Standard Model (SM) that has neither been confirmed nor refuted. The CDF collaboration has performed SM Higgs searches in many channels using p{bar p} collisions at a centre-of-mass energy {radical}s = 1.96 TeV. We present the latest combined Higgs boson search at CDF. Since the previous year's combination, the sensitivity is increased through the addition of new channels, the improvement of existing channels and the addition of new data samples. We also use the latest parton distribution functions and gg {yields} H theoretical cross sections when modelling the signal event yields. Using integrated luminosities of up to 8.2 fb{sup -1}, we observe a good agreement between data and the background prediction. Since we do not see a Higgs boson excess, we set 95% CL upper limits on the Higgs boson cross section in the range between 100 and 200 GeV/c{sup 2}, with 5 GeV/c{sup 2} increments. The observed (expected) limits for a 115 and a 165 GeV/c{sup 2} Higgs boson are 1.55 (1.49) and 0.75 (0.79) x SM, respectively. Since last year, the Higgs boson excluded range by CDF is extended to 156.5 - 173.7 and 100 - 104.5 GeV/c{sup 2}.

Adrian, Buzatu; /McGill U.

2012-02-01T23:59:59.000Z

189

Search for Anomalous Production of Events with Two Photons and Additional Energetic Objects at CDF  

SciTech Connect

The authors present results of a search for anomalous production of two photons together with an electron, muon, {tau} lepton, missing transverse energy, or jets using p{bar p} collision data from 1.1-2.0 fb{sup -1} of integrated luminosity collected by the Collider Detector at Fermilab (CDF). The event yields and kinematic distributions are examined for signs for new physics without favoring a specific model of new physics. The results are consistent with the standard model expectations. The search employs several new analysis techniques that significantly reduce instrumental backgrounds in channels with an electron and missing transverse energy.

Aaltonen, T.; /Helsinki Inst. of Phys.; Adelman, J.; /Chicago U., EFI; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Amerio, S.; /Padua U. /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U.; Annovi, A.; /Frascati; Antos, J.; /Comenius U. /Kosice, IEF; Apollinari, G.; /Fermilab; Apresyan, A.; /Purdue U.; Arisawa, T.; /Waseda U. /Dubna, JINR

2009-10-01T23:59:59.000Z

190

Combination of CDF and D0 Results on the W-Boson Width  

SciTech Connect

The results on the direct measurements of the W-boson width, based on the data collected by the Tevatron experiments CDF and D0 at Fermilab during Run-I from 1992 to 1996 and Run-II since 2001 are summarized. The combination of the published Run-I and preliminary Run-II results, taking correlated uncertainties properly into account, is presented. The resulting preliminary Tevatron average for the total decay width of the W boson is: {Lambda}{sub W} = 2078 {+-} 87 MeV, where the total error consists of a statistical part of 62 MeV and a systematic part of 60 MeV.

Not Available

2005-12-01T23:59:59.000Z

191

Search for Supersymmetry in the Dilepton Final State with Taus at CDF Run II  

SciTech Connect

This thesis presents the results a search for chargino and neutralino supersymmetric particles yielding same signed dilepton final states including one hadronically decaying tau lepton using 6.0 fb{sup -1} of data collected by the the CDF II detector. This signature is important in SUSY models where, at high tan {beta}, the branching ratio of charginos and neutralinos to tau leptons becomes dominant. We study event acceptance, lepton identification cuts, and efficiencies. We set limits on the production cross section as a function of SUSY particle mass for certain generic models.

Forrest, Robert David; /California U., Davis

2011-09-01T23:59:59.000Z

192

Search for non-standard model signatures in the WZ/ZZ final state at CDF run II  

SciTech Connect

This thesis discusses a search for non-Standard Model physics in heavy diboson production in the dilepton-dijet final state, using 1.9 fb{sup -1} of data from the CDF Run II detector. New limits are set on the anomalous coupling parameters for ZZ and WZ production based on limiting the production cross-section at high {cflx s}. Additionally limits are set on the direct decay of new physics to ZZ andWZ diboson pairs. The nature and parameters of the CDF Run II detector are discussed, as are the influences that it has on the methods of our analysis.

Norman, Matthew; /UC, San Diego

2009-01-01T23:59:59.000Z

193

Study of the top quark electric charge at the CDF experiment  

Science Conference Proceedings (OSTI)

We report on the measurement of the top quark electric charge using the jet charge tagging method on events containing a single lepton collected by the CDF II detector at Fermilab between February 2002 and February 2010 at the center-of-mass energy {radical}s = 1.96 TeV. There are three main components to this measurement: determining the charge of the W (using the charge of the lepton), pairing the W with the b-jet to ensure that they are from the same top decay branch and finally determining the charge of the b-jet using the Jet Charge algorithm. We found, on a sample of 5.6 fb{sup -1} of data, that the p-value under the standard model hypothesis is equal to 13.4%, while the p-value under the exotic model hypothesis is equal to 0.014%. Using the a priori criteria generally accepted by the CDF collaboration, we can say that the result is consistent with the standard model, while we exclude an exotic quark hypothesis with 95% confidence. Using the Bayesian approach, we obtain for the Bayes factor (2ln(BF)) a value of 19.6, that favors very strongly the SM hypothesis over the XM one. The presented method has the highest sensitivity to the top quark electric charge among the presented so far top quark charge analysis.

Bartos, Pavol; /Comenius U.

2011-09-01T23:59:59.000Z

194

Search for rare SM processes in the MET+b-jets signature at CDF  

Science Conference Proceedings (OSTI)

The missing transverse energy (E{sub T}) plus b-jets signature is very promising for searches for the Higgs boson or new physics. Indeed, E{sub T} naturally arises from unidentified particles such as neutrinos, neutralinos, gravitons, etc., and b-quarks are the main decay products of a low mass Higgs boson as well as of several exotic particles. The main challenge is to identify and reject the numerous standard model (SM) backgrounds that mimic this signature. This is especially so for QCD multi-jet production, a large background due to mis-measurement (rather than undetectable particles). We present state-of-the-art data-driven and multivariate techniques to characterize and reject this instrumental background. These techniques make analyses in this signature as sensitive as those using lepton identification and allow probing for rare SM processes. We describe searches for electroweak single top production, a part of the observation of single top by CDF, and for a low mass SM Higgs boson, one of the most sensitive among low mass Higgs searches at CDF. We also present a measurement of the top pair cross-section in this signature, and discuss other analyses and future prospects.

Potamianos, Karolos

2011-05-01T23:59:59.000Z

195

Top decay physics at CDF and measurement of the CKM element V{sub tb}  

SciTech Connect

Now that the top quark`s existence has been firmly established by the CDF and D0 experiments{sup 1,2)}, we begin to measure its properties. Branching fractions are of particular interest in the case of the t quark, since they probe the couplings of the top quark to gauge bosons and other quarks, and because ``the top quark is the only quark with reasonable mass``{sup 3)}. Because the top quark is the only quark with mass comparable to the electroweak scale, its decays, particularly non-standard decays, might shed some light on what makes the top quark different from lighter quarks, and the role it plays in electroweak symmetry breaking. This paper describes some recent measurements on the decay of the top quark using the CDF detector, a general purpose detector designed to study p{bar p} collisions at {radical}s=1.8 TeV; it has been described in detail elsewhere{sup 4,1)}. The analyses presented use 100-110 pb{minus}{sup 1} of data collected between 1992 and 1995 at the Fermilab TeVatron.

LeCompte, T.J.

1995-12-31T23:59:59.000Z

196

Data:9fbd634e-80c2-4a3a-be2a-e5a62d2dbe5a | Open Energy Information  

Open Energy Info (EERE)

fbd634e-80c2-4a3a-be2a-e5a62d2dbe5a fbd634e-80c2-4a3a-be2a-e5a62d2dbe5a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Duke Energy Ohio Inc Effective date: 2013/05/06 End date if known: Rate name: Rate NSP - Private Outdoor Lighting for Non-Standard Units - 7,000 Lumen Mercury Mounted on 30-foot Fiberglass Pole - 175 Watt Sector: Lighting Description: Applicable to service for outdoor lighting on private property with Company owned overhead lighting fixtures in the Company's entire territory where secondary distribution lines are adjacent to the premise to be served. Not applicable to service for lighting of dedicated or undedicated public thoroughfares.

197

Data:5df79e82-7d10-48b9-b5ab-e69db05a4c49 | Open Energy Information  

Open Energy Info (EERE)

df79e82-7d10-48b9-b5ab-e69db05a4c49 df79e82-7d10-48b9-b5ab-e69db05a4c49 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Bonneville Power Admin Effective date: 2011/10/01 End date if known: 2013/09/30 Rate name: PF - 12 Public - Average Tier 1 + Tier 2 rate Sector: Residential Description: Source or reference: http://www.bpa.gov/Power/PSP/rates/current.shtml Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring:

198

2012 Update of the Combination of CDF and D0 Results for the Mass of the W Boson  

SciTech Connect

We summarize and combine the results on the direct measurements of the mass of the W boson in data collected by the Tevatron experiments CDF and D0 at Fermilab. Earlier results from CDF Run-0 (1988-1989), D0 and CDF Run-I (1992-1995) and D0 results from 1 fb{sup -1} (2002-2006) of Run-II data are now combined with two new, high statistics Run-II measurements: a CDF measurement in both electron and muon channels using 2.2 fb{sup -1} of integrated luminosity collected between 2002 and 2007, and a D0 measurement in the electron channel using 4.3 fb{sup -1} collected between 2006 and 2009. As in previous combinations, the results are corrected for inconsistencies in parton distribution functions and assumptions about electroweak parameters used in the different analyses. The resulting Tevatron average for the mass of the W boson is M{sub W} = 80,387 {+-} 16 MeV and a new world average including data from LEP II is M{sub W} = 80,385 {+-} 15 MeV.

Tevatron Electroweak Working Group,

2012-04-01T23:59:59.000Z

199

Inclusive Search for Standard Model Higgs Boson Production in the WW Decay Channel Using the CDF II Detector  

E-Print Network (OSTI)

We present a search for standard model (SM) Higgs boson production using pp? collision data at ?s=1.96??TeV, collected with the CDF II detector and corresponding to an integrated luminosity of 4.8??fb[superscript -1]. We ...

Xie, Si

200

Combined Search for the Standard Model Higgs Boson Decaying to a bb? Pair Using the Full CDF Data Set  

E-Print Network (OSTI)

We combine the results of searches for the standard model (SM) Higgs boson based on the full CDF Run II data set obtained from ?s=1.96??TeV pp? collisions at the Fermilab Tevatron corresponding to an integrated luminosity ...

Gomez-Ceballos, Guillelmo

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


201

CDF note 10798 Seach for the SM Higgs boson in the ET +b-jets signature with relaxed  

E-Print Network (OSTI)

CDF note 10798 Seach for the SM Higgs boson in the ET +b-jets signature with relaxed kinematic cuts) We present a search for the Higgs boson produced in association with a Z or W boson in the ET +b the Higgs boson signal from the remaining background. We check the goodness of our background modeling

Fermilab

202

CDF note 10582 Search for SM Higgs boson production in association with tt using no lepton final state  

E-Print Network (OSTI)

CDF note 10582 Search for SM Higgs boson production in association with t¯t using no lepton final is that t¯t decay all hadronic mode (all t decay into bqq ). In both cases we consider that the Higgs boson discriminant variable from different neural network to discriminate the Higgs boson signal from remained

Fermilab

203

Search for anomalous production of multiple leptons in association with $W$ and $Z$ bosons at CDF  

Science Conference Proceedings (OSTI)

This paper presents a search for anomalous production of multiple low-energy leptons in association with a W or Z boson using events collected at the CDF experiment corresponding to 5.1 fb{sup -1} of integrated luminosity. This search is sensitive to a wide range of topologies with low-momentum leptons, including those with the leptons near one another. The observed rates of production of additional electrons and muons are compared with the standard model predictions. No indications of phenomena beyond the standard model are found. A 95% confidence level limit is presented on the production cross section for a benchmark model of supersymmetric hidden-valley Higgs production. Particle identification efficiencies are also provided to enable the calculation of limits on additional models.

Aaltonen, T.; /Helsinki Inst. of Phys.; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U. /Fermilab; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Arisawa, T.; /Waseda U.; Artikov, A.; /Dubna, JINR /Texas A-M

2012-02-01T23:59:59.000Z

204

Evidence for a bottom baryon resonance Lambda_b* in CDF data  

E-Print Network (OSTI)

Using data from proton-antiproton collisions at Ecms=1.96 TeV recorded by the CDF II detector at the Fermilab Tevatron, evidence for the excited resonance state Lambda_b* is presented in its Lambda_b0 pi+ pi- decay, followed by the Lambda_b0 -->Lambda_c+ (-->proton K- pi+) pi- decays. The analysis is based on a data sample corresponding to an integrated luminosity of 9.6/fb collected by an online event selection based on charged-particle tracks displaced from the proton-antiproton interaction point. The significance of the observed signal is 3.5 Gaussian sigmas. The mass of the observed state is found to be 5919.22 +- 0.76 MeV in agreement with similar findings in proton-proton collision experiments.

CDF Collaboration; T. Aaltonen; S. Amerio; D. Amidei; A. Anastassov; A. Annovi; J. Antos; G. Apollinari; J. A. Appel; T. Arisawa; A. Artikov; J. Asaadi; W. Ashmanskas; B. Auerbach; A. Aurisano; F. Azfar; W. Badgett; T. Bae; A. Barbaro-Galtieri; V. E. Barnes; B. A. Barnett; P. Barria; P. Bartos; M. Bauce; F. Bedeschi; S. Behari; G. Bellettini; J. Bellinger; D. Benjamin; A. Beretvas; A. Bhatti; K. R. Bland; B. Blumenfeld; A. Bocci; A. Bodek; D. Bortoletto; J. Boudreau; A. Boveia; L. Brigliadori; C. Bromberg; E. Brucken; J. Budagov; H. S. Budd; K. Burkett; G. Busetto; P. Bussey; P. Butti; A. Buzatu; A. Calamba; S. Camarda; M. Campanelli; F. Canelli; B. Carls; D. Carlsmith; R. Carosi; S. Carrillo; B. Casal; M. Casarsa; A. Castro; P. Catastini; D. Cauz; V. Cavaliere; M. Cavalli-Sforza; A. Cerri; L. Cerrito; Y. C. Chen; M. Chertok; G. Chiarelli; G. Chlachidze; K. Cho; D. Chokheli; A. Clark; C. Clarke; M. E. Convery; J. Conway; M. Corbo; M. Cordelli; C. A. Cox; D. J. Cox; M. Cremonesi; D. Cruz; J. Cuevas; R. Culbertson; N. d'Ascenzo; M. Datta; P. de Barbaro; L. Demortier; L. Marchese; M. Deninno; F. Devoto; M. D'Errico; A. Di Canto; B. Di Ruzza; J. R. Dittmann; M. D'Onofrio; S. Donati; M. Dorigo; A. Driutti; K. Ebina; R. Edgar; A. Elagin; R. Erbacher; S. Errede; B. Esham; S. Farrington; J. P. Fernndez Ramos; R. Field; G. Flanagan; R. Forrest; M. Franklin; J. C. Freeman; H. Frisch; Y. Funakoshi; C. Galloni; A. F. Garfinkel; P. Garosi; H. Gerberich; E. Gerchtein; S. Giagu; V. Giakoumopoulou; K. Gibson; C. M. Ginsburg; N. Giokaris; P. Giromini; G. Giurgiu; V. Glagolev; D. Glenzinski; M. Gold; D. Goldin; A. Golossanov; G. Gomez; G. Gomez-Ceballos; M. Goncharov; O. Gonzlez Lpez; I. Gorelov; A. T. Goshaw; K. Goulianos; E. Gramellini; S. Grinstein; C. Grosso-Pilcher; R. C. Group; J. Guimaraes da Costa; S. R. Hahn; J. Y. Han; F. Happacher; K. Hara; M. Hare; R. F. Harr; T. Harrington-Taber; K. Hatakeyama; C. Hays; J. Heinrich; M. Herndon; A. Hocker; Z. Hong; W. Hopkins; S. Hou; R. E. Hughes; U. Husemann; M. Hussein; J. Huston; G. Introzzi; M. Iori; A. Ivanov; E. James; D. Jang; B. Jayatilaka; E. J. Jeon; S. Jindariani; M. Jones; K. K. Joo; S. Y. Jun; T. R. Junk; M. Kambeitz; T. Kamon; P. E. Karchin; A. Kasmi; Y. Kato; W. Ketchum; J. Keung; B. Kilminster; D. H. Kim; H. S. Kim; J. E. Kim; M. J. Kim; S. B. Kim; S. H. Kim; Y. K. Kim; Y. J. Kim; N. Kimura; M. Kirby; K. Knoepfel; K. Kondo; D. J. Kong; J. Konigsberg; A. V. Kotwal; M. Kreps; J. Kroll; M. Kruse; T. Kuhr; M. Kurata; A. T. Laasanen; S. Lammel; M. Lancaster; K. Lannon; G. Latino; H. S. Lee; J. S. Lee; S. Leo; S. Leone; J. D. Lewis; A. Limosani; E. Lipeles; A. Lister; H. Liu; Q. Liu; T. Liu; S. Lockwitz; A. Loginov; A. Luc; D. Lucchesi; J. Lueck; P. Lujan; P. Lukens; G. Lungu; J. Lys; R. Lysak; R. Madrak; P. Maestro; S. Malik; G. Manca; A. Manousakis-Katsikakis; F. Margaroli; P. Marino; M. Martnez; K. Matera; M. E. Mattson; A. Mazzacane; P. Mazzanti; R. McNulty; A. Mehta; P. Mehtala; C. Mesropian; T. Miao; D. Mietlicki; A. Mitra; H. Miyake; S. Moed; N. Moggi; C. S. Moon; R. Moore; M. J. Morello; A. Mukherjee; Th. Muller; P. Murat; M. Mussini; J. Nachtman; Y. Nagai; J. Naganoma; I. Nakano; A. Napier; J. Nett; C. Neu; T. Nigmanov; L. Nodulman; S. Y. Noh; O. Norniella; L. Oakes; S. H. Oh; Y. D. Oh; I. Oksuzian; T. Okusawa; R. Orava; L. Ortolan; C. Pagliarone; E. Palencia; P. Palni; V. Papadimitriou; W. Parker; G. Pauletta; M. Paulini; C. Paus; T. J. Phillips; G. Piacentino; E. Pianori; J. Pilot; K. Pitts; C. Plager; L. Pondrom; S. Poprocki; K. Potamianos; F. Prokoshin; A. Pranko; F. Ptohos; G. Punzi; N. Ranjan; I. Redondo Fernndez; P. Renton; M. Rescigno; F. Rimondi; L. Ristori; A. Robson; T. Rodriguez; S. Rolli; M. Ronzani; R. Roser; J. L. Rosner; F. Ruffini; A. Ruiz; J. Russ; V. Rusu; W. K. Sakumoto; Y. Sakurai; L. Santi; K. Sato; V. Saveliev; A. Savoy-Navarro; P. Schlabach; E. E. Schmidt; T. Schwarz; L. Scodellaro; F. Scuri; S. Seidel; Y. Seiya; A. Semenov; F. Sforza; S. Z. Shalhout; T. Shears; P. F. Shepard; M. Shimojima; M. Shochet; I. Shreyber-Tecker; A. Simonenko; K. Sliwa; J. R. Smith; F. D. Snider; V. Sorin; H. Song; M. Stancari; R. St. Denis; D. Stentz; J. Strologas; Y. Sudo; A. Sukhanov; I. Suslov; K. Takemasa; Y. Takeuchi; J. Tang; M. Tecchio; P. K. Teng; J. Thom; E. Thomson; V. Thukral; D. Toback; S. Tokar; K. Tollefson; T. Tomura; D. Tonelli; S. Torre; D. Torretta; P. Totaro; M. Trovato; F. Ukegawa; S. Uozumi; F. Vzquez; G. Velev; C. Vellidis; C. Vernieri; M. Vidal; R. Vilar; J. Vizn; M. Vogel; G. Volpi; P. Wagner; R. Wallny; S. M. Wang; D. Waters; W. C. Wester III; D. Whiteson; A. B. Wicklund; S. Wilbur; H. H. Williams; J. S. Wilson; P. Wilson; B. L. Winer; P. Wittich; S. Wolbers; H. Wolfe; T. Wright; X. Wu; Z. Wu; K. Yamamoto; D. Yamato; T. Yang; U. K. Yang; Y. C. Yang; W. -M. Yao; G. P. Yeh; K. Yi; J. Yoh; K. Yorita; T. Yoshida; G. B. Yu

2013-08-08T23:59:59.000Z

205

Search for Standard Model Higgs Boson in H to WW Channel at CDF  

E-Print Network (OSTI)

We present a search for standard model Higgs boson to WW(*) production in dilepton plus missing transverse energy final states in data collected by the CDF II detector corresponding to 4.8/fb of integrated luminosity. To maximize sensitivity, the multivariate discriminants used to separate signal from background in the opposite-sign dilepton event sample are independently optimized for final states with zero, one, or two or more identified jets. All significant Higgs boson production modes (gluon fusion, associated production with either a W or Z boson, and vector boson fusion) are considered in determining potential signal contributions. We also incorporate a separate analysis of the same-sign dilepton event sample which potentially contains additional signal events originating from associated Higgs boson production mechanisms. Cross section limits relative to the combined SM predictions are presented for a range of Higgs boson mass hypotheses between 110 and 200 GeV/c^2.

J. Pursley; for the CDF Collaboration

2009-10-08T23:59:59.000Z

206

Search for a Higgs Boson Decaying to Two W Bosons at CDF  

SciTech Connect

We present a search for a Higgs boson decaying to two W bosons in p{bar p} collisions at {radical}s = 1.96 TeV center-of-mass energy. The data sample corresponds to an integrated luminosity of 3.0 fb{sup -1} collected with the CDF II detector. We find no evidence for production of a Higgs boson with mass between 110 and 200 GeV/c{sup 2}, and determine upper limits on the production cross section. For the mass of 160 GeV/c{sup 2}, where the analysis is most sensitive, the observed (expected) limit is 0.7 pb (0.9 pb) at 95% Bayesian credibility level which is 1.7 (2.2) times the standard model cross section.

Aaltonen, T.; /Helsinki Inst. of Phys.; Adelman, J.; /Chicago U., EFI; Akimoto, T.; /Tsukuba U.; Albrow, Michael G.; /Fermilab; Alvarez Gonzalez, B.; /CSIC, Catalunya; Amerio, S.; /INFN, Padua; Amidei, Dante E.; /Michigan U.; Anastassov, A.; /Northwestern U.; Annovi, Alberto; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab /Purdue U.

2008-09-01T23:59:59.000Z

207

Search for Standard Model Higgs Boson in H ---> WW Channel at CDF  

SciTech Connect

We present a search for standard model (SM) Higgs boson to WW{sup (*)} production in dilepton plus missing transverse energy final states in data collected by the CDF II detector corresponding to 4.8 fb{sup -1} of integrated luminosity. To maximize sensitivity, the multivariate discriminants used to separate signal from background in the opposite-sign dilepton event sample are independently optimized for final states with zero, one, or two or more identified jets. All significant Higgs boson production modes (gluon fusion, associated production with either a W or Z boson, and vector boson fusion) are considered in determining potential signal contributions. We also incorporate a separate analysis of the same-sign dilepton event sample which potentially contains additional signal events originating from associated Higgs boson production mechanisms. Cross section limits relative to the combined SM predictions are presented for a range of Higgs boson mass hypotheses between 110 and 200 GeV/c{sup 2}.

Pursley, J.; /Wisconsin U., Madison

2009-10-01T23:59:59.000Z

208

Search for the neutral MSSM Higgs bosons in the ditau decay channels at CDF Run II  

SciTech Connect

This thesis presents the results on a search for the neutral MSSM Higgs bosons decaying to tau pairs, with least one of these taus decays leptonically. The search was performed with a sample of 1.8 fb{sup -1} of proton-antiproton collisions at {radical}s = 1.96 TeV provided by the Tevatron and collected by CDF Run II. No significant excess over the Standard Model prediction was found and a 95% confidence level exclusion limit have been set on the cross section times branching ratio as a function of the Higgs boson mass. This limit has been translated into the MSSM Higgs sector parameter plane, tan{beta} vs. M{sub A}, for the four different benchmark scenarios.

Cuenca Almenar, Cristobal; /Valencia U., IFIC

2008-04-01T23:59:59.000Z

209

The Development of an Academically-Based Entertainment-Education (ABEE) Model: Co-opting Behavioral Change Efficacy of Entertainment-Education for Academic Learning Targeting the Societal Landscape of U.S. Geographic Illiteracy  

E-Print Network (OSTI)

Educators and scholars continue to lament United States citizens' geographic illiteracy and are calling on Congress to address the crisis. However, despite recent public attention, a lack of national commitment to teaching geography in all public school grade levels persists. Therefore, non-formal educational avenues need to be pursued to address this crisis. One such avenue may be Entertainment-Education (E-E). E-E interventions have been used outside of the U.S. to impact social problems and detrimental behaviors by presenting positive role models in entertainment products designed to stimulate changes in viewers' behavior. For example, soap operas promote condoms use as a HIV prevention strategy (Tanzania), model culturally-sensitive actions to stop domestic violence (South Africa), and promote infant oral-rehydration therapy (Egypt). This study posits academic learning can be facilitated in a similar fashion as behavior change through an E-E methodology. Beginning with an examination of the E-E field by indexing E-E literature found in scholarly publication databases, this study demonstrates the 30-year health message focus of the field and presents a catalogue of E-E interventions cross-referenced by name and target country. The combination of these two products illuminates how U.S. audiences and non-behaviorally based outcomes have not been targeted, leaving academic subject learning as an area into which E-E can expand. The expansion of E-E methodology into geography education (or any other subject) requires understanding of how academic concepts interact with the structure of fictional narratives. Using a grounded theory approach, this study analyzes the U.S. television series NUMB3RS, which uses math to drive the story (as opposed to simply serving as context), to develop an Academically-Based Entertainment-Education (ABEE) model. ABEE is then applied to Google Earth, exploring how to leverage non-linear and visually dependent narratives as well as develop user-driven learning experiences. The implications of research presented here and through future refinement of the ABEE model may potentially (1) develop educative entertainment products supporting formal education and (2) bring geographic knowledge into the realm of popular culture through mass media, thereby impacting geographic literacy at a societal level in the U.S. The electronic version of this dissertation is accessible from http://hdl.handle.net/1969.1/ETD-TAMU-2011-05-9128.

Simms, Michelle

2011-05-01T23:59:59.000Z

210

Measurement of the polarization amplitudes of the Bs -> PhiPhi decay at CDF II  

Science Conference Proceedings (OSTI)

In this thesis we present the first measurement of the polarization amplitudes for the charmless B{sub s} {yields} {phi}{phi} {yields} [K{sup +}K{sup -}][K{sup +}K{sup -}] decay of the B{sub s} meson. The result is achieved using an unbinned Maximum Likelihood fit to the data collected by the Collider Detector at Fermilab (CDF) in Run II (CDFII), in a period starting from March 2001 till April 2008, which corresponds to an integrated luminosity of 2.9 fb{sup -1}. The resulting yield consists of 300 signal events selected by the Two Track Trigger (TTT). Furthermore, our work puts in evidence an original topic, that was never observed until now: an unexpected dependence of the signal acceptance on the proper decay time (t) of the B{sub s} mesons. This specific issue, which is most likely a general feature induced by any signal selection based on the lifetime information, is supposed to be related to the on-line TTT and off-line selections based on the impact parameter. The involved fit, indeed, reproduces the biases observed in large statistics Monte Carlo (MC) samples. The thesis presents the same analysis performed for the B{sub s}{sup 0} {yields} J{psi}{phi} decay as well, which is used as a control sample. The polarizations amplitudes we find are consistent with the published ones; this result contributes to enforce the reliability of the analysis. This work is considered ready to begin the procedure for official approval by the CDF collaboration pending the finalization of the systematic uncertainty which has not yet been fully completed.

Dorigo, Mirco; /Trieste U. /INFN, Trieste

2009-10-01T23:59:59.000Z

211

Influence of luminosity leveling on the CDF-II B-Physics program  

Science Conference Proceedings (OSTI)

The effective bandwidth of the CDF-II level 1 trigger is approximately 25 kHz. Some of this bandwidth is used to record events that form the data sets used by the high p{sub T} physics analyses. The remaining bandwidth is used by triggers that are sensitive to hadronic B decays and provide one of the most important samples used for the study of B{sub s}{sup 0} mixing. At high luminosities, the hadronic B triggers have rates that greatly exceed the available bandwidth. Rather than incur large dead-times associated with these excessive rates, these B triggers are prescaled to limit the total trigger rate to the effective level 1 trigger bandwidth. The prescales are dynamically adjusted as the store progresses so that all of the bandwidth that is not used for the high p{sub T} physics program is used to record hadronic B triggers. In principle, the luminosity could be held at a more constant level throughout the store in such a way that the integrated luminosity would be the same as that obtained from a normal store. It has been suggested that this would allow B triggers to be recorded with lower prescales and consequently with higher B{sub s}{sup 0} signal efficiencies. This note describes a parametric model of the high p{sub T} and hadronic B triggers used by CDF and compares the yields of reconstructed B{sub s}{sup 0} decays that would result with and without luminosity leveling.

Jones, Matthew; /Purdue U.; Lewis, Jonathan; /Fermilab

2005-05-01T23:59:59.000Z

212

A Search for the Higgs Boson in the $ZH$ Dilepton Decay Channel at CDF II  

SciTech Connect

This dissertation describes a search for the Standard Model Higgs boson produced in association with the Z boson via Higgs-strahlung at the CDF II detector at the Tevatron. At a Higgs boson mass between 100 GeV/c{sup 2} and 135 GeV/c{sup 2}, the primary Higgs decay mode is to a pair of b quarks. The associated Z boson can decay to a pair of electrons or muons, allowing detection of a final event signature of two visible leptons and two b quarks. This final state allows reduction of large QCD backgrounds compared to a hadronic Z boson decay, leading to a more sensitive search. To increase sensitivity, standard model matrix element probabilities for ZH signal and the dominant backgrounds are used as components to a likelihood fit in signal fraction. In 2.7 fb{sup -1} of CDF II data, we see no evidence of production of a Higgs boson with a mass between 100 GeV c{sup 2} and 150 GeV/c{sup 2}. Using the Feldman-Cousins technique to set a limit, at 95% coverage and a Higgs boson mass of 115 GeV/c{sup 2}, the median expected limit was 12.1 x {sigma}{sub SM} and a limit of 8.2 x {sigma}{sub SM} was observed, where {sigma}{sub SM} is the NNLO theoretical cross section of p{bar p} {yields}ZH {yields} l +l -b{bar b} at {radical}s=1.96 TeV . Cross section limits are computed at a range of Higgs boson mass values between 100 GeV/c {sup 2} and 150 GeV/c{sup 2}.

Shekhar, Ravi; /Duke U.

2009-07-01T23:59:59.000Z

213

Level-3 Calorimetric Resolution available for the Level-1 and Level-2 CDF Triggers  

E-Print Network (OSTI)

As the Tevatron luminosity increases sophisticated selections are required to be efficient in selecting rare events among a very huge background. To cope with this problem, CDF has pushed the offline calorimeter algorithm reconstruction resolution up to Level 2 and, when possible, even up to Level 1, increasing efficiency and, at the same time, keeping under control the rates. The CDF Run II Level 2 calorimeter trigger is implemented in hardware and is based on a simple algorithm that was used in Run I. This system has worked well for Run II at low luminosity. As the Tevatron instantaneous luminosity increases, the limitation due to this simple algorithm starts to become clear: some of the most important jet and MET (Missing ET) related triggers have large growth terms in cross section at higher luminosity. In this paper, we present an upgrade of the Level 2 Calorimeter system which makes the calorimeter trigger tower information available directly to a CPU allowing more sophisticated algorithms to be implemented in software. Both Level 2 jets and MET can be made nearly equivalent to offline quality, thus significantly improving the performance and flexibility of the jet and MET related triggers. However in order to fully take advantage of the new L2 triggering capabilities having at Level 1 the same L2 MET resolution is necessary. The new Level-1 MET resolution is calculated by dedicated hardware. This paper describes the design, the hardware and software implementation and the performance of the upgraded calorimeter trigger system both at Level 2 and Level 1.

A. Canepa; M. Casarsa; T. Liu; G. Cortiana; G. Flanagan; H. Frisch; D. Krop; C. Pilcher; V. Rusu; V. Cavaliere; V. Greco; P. Giannetti; M. Piendibene; L. Sartori; M. Vidal

2008-10-21T23:59:59.000Z

214

Updated search for the standard model Higgs boson in events with jets and missing transverse energy using the full CDF data set  

E-Print Network (OSTI)

We present an updated search for the Higgs boson produced in association with a vector boson in the final state with missing transverse energy and two jets. We use the full CDF data set corresponding to an integrated ...

Gomez-Ceballos, Guillelmo

215

Search for the Standard Model Higgs Boson Decaying to a bb? Pair in Events with Two Oppositely Charged Leptons Using the Full CDF Data Set  

E-Print Network (OSTI)

We present a search for the standard model Higgs boson produced in association with a Z boson in data collected with the CDF II detector at the Tevatron, corresponding to an integrated luminosity of 9.45??fb[superscript ...

Gomez-Ceballos, Guillelmo

216

Data:Dc4f43be-be61-4b71-9d3c-a255e2e1abee | Open Energy Information  

Open Energy Info (EERE)

f43be-be61-4b71-9d3c-a255e2e1abee f43be-be61-4b71-9d3c-a255e2e1abee No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of College Station, Texas (Utility Company) Effective date: 2012/02/23 End date if known: Rate name: Schedule SRE - (Small Renewable Energy Customers Conencting Single Phase Distributed Generation from Renewable Sources less than or equal to twenty (20) kW) Sector: Description: Applicable to any retail customer receiving single phase electric service under a City of College Station electric rate schedule who owns and operates an on-site generating system powered by a renewable energy technology capable of producing not more than twenty (20) kW of power and who interconnects with the City of College Station's electric distribution system. Renewable energy technology is any technology that exclusively relies on an energy source that is naturally regenerated over a short time and derived directly from the sun, indirectly from the sun, or from moving water or other natural movements and mechanisms of the environment. Renewable energy technologies include those that rely on energy derived directly from the sun, wind, geothermal source, hydroelectric source, wave or tidal energy; or on biomass or biomass based waste products including landfill gas. A renewable energy technology does not rely on energy resources derived from fossil fuels, waste products from fossil fuels, or waste products from inorganic sources. This section applies to a retail customer owned generation system that primarily offsets part or all of the customer's electric service provided by the City of College Station.

217

Data:15fe5cdf-0d41-4745-adb6-d160abba40bf | Open Energy Information  

Open Energy Info (EERE)

fe5cdf-0d41-4745-adb6-d160abba40bf fe5cdf-0d41-4745-adb6-d160abba40bf No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: PUD No 2 of Grant County Effective date: 2003/04/01 End date if known: Rate name: RATE SCHEDULE NO. 6 -- 2003 STREET LIGHTING SERVICE Decorative Unit 2 Sector: Lighting Description: DECORATIVE STREET LIGHTING: AVAILABLE: To municipalities only for enhancement of central shopping and contiguous business areas. Source or reference: http://grantpud.org/customer-service/payments-billing/rates-and-fees Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months):

218

Data:Ea71c04b-94f5-4459-8cdf-0862879806eb | Open Energy Information  

Open Energy Info (EERE)

1c04b-94f5-4459-8cdf-0862879806eb 1c04b-94f5-4459-8cdf-0862879806eb No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Rural Elec Coop Inc Effective date: 2011/02/01 End date if known: Rate name: Seasonal Turtles 2C Sector: Commercial Description: * Seasonal Turtles 2 Cost of service Source or reference: Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous

219

Data:A364fb58-2cdf-4759-84a6-b65024454dce | Open Energy Information  

Open Energy Info (EERE)

4fb58-2cdf-4759-84a6-b65024454dce 4fb58-2cdf-4759-84a6-b65024454dce No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Modesto Irrigation District Effective date: 2013/04/01 End date if known: Rate name: Schedule SL - Lamp and Fixture on Existing Pole - 100 Watt SV Sector: Lighting Description: This section of this Schedule is applicable to all night lighting on the public streets, alleys, highways and parks for cities, lighting districts or other public bodies. Public outdoor area lighting for other than all night lighting is supplied under Rate Schedule GS. Source or reference: www.mid.org/tariffs/rates/SL_STREET_LIGHTING.pdf

220

Recent results from the CDF (Collider Detector at Fermilab) experiment at the Tevatron proton-antiproton collider  

SciTech Connect

Recent results from the CDF experiment are described. The Standard Model gives a good description of jet production, and W/Z production and decay. There is no evidence yet for the top quark, for fourth generation quarks, or for deviations from the Standard Model ascribable to quark substructure, supersymmetric particles, or heavy additional W-like or Z-like bosons. Limits are given where applicable. A search for a light Higgs Boson is also described. 11 refs., 24 figs.

Geer, S. (Harvard Univ., Cambridge, MA (USA). High Energy Physics Lab.)

1989-09-01T23:59:59.000Z

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


221

Search for Technicolor Particles Produced in Association with a W Boson at CDF  

Science Conference Proceedings (OSTI)

We present a search for the technicolor particles {rho}{sub T} and {pi}{sub T} in the process p{bar p} {yields} {rho}{sub T} {yields} W{pi}{sub T} at a center of mass energy of {radical}s = 1.96 TeV. The search uses a data sample corresponding to approximately 1.9 fb{sup -1} of integrated luminosity accumulated by the CDF II detector at the Fermilab Tevatron. The event signature we consider is W {yields} {ell}{nu} and {pi}{sub T} {yields} b{bar b}, b{bar c} or b{bar u} depending on the {pi}{sub T} charge. We select events with a single high-p{sub T} electron or muon, large missing transverse energy, and two jets. Jets corresponding to bottom quarks are identified with multiple b-tagging algorithms. The observed number of events and the invariant mass distributions are consistent with the standard model background expectations, and we exclude a region at 95% confidence level in the {rho}{sub T}-{pi}{sub T} mass plane. As a result, a large fraction of the region m({rho}{sub T}) = 180-250 GeV/c{sup 2} and m({pi}{sub T}) = 95-145 GeV/c{sup 2} is excluded.

Aaltonen, T.; /Helsinki Inst. of Phys.; Adelman, J.; /Chicago U., EFI; Alvarez Gonzalez, B.; /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U.; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Apresyan, A.; /Purdue U.; Arisawa, T.; /Waseda U. /Dubna, JINR

2009-12-01T23:59:59.000Z

222

CP violation in the D0 -> pi+ pi- decay at CDF  

SciTech Connect

We report a measurement of the CP violating asymmetry in D{sup 0} {yields} {pi}{sup +}{pi}{sup -} decays using approximately 215,000 decays reconstructed in about 5.94 fb{sup -1} of CDF data. We use the strong D*{sup +} {yields} D{sup 0}{pi}{sup +} decay ('D* tag') to identify the flavor of the charmed meson at production time and exploit CP-conserving strong c{bar c} pair-production in p{bar p} collisions. Higher statistic samples of Cabibbo-favored D{sup 0} {yields} K{sup -}{pi}{sup +} decays with and without D* tag are used to highly suppress systematic uncertainties due to detector effects. The result, A{sub CP}(D{sup 0} {yields} {pi}{sup +}{pi}{sup -}) = [0.22 {+-} 0.24 (stat.) {+-} 0.11 (syst.)]%, is the world's most precise measurement to date and it is fully consistent with no CP violation.

Morello, Michael Joseph

2010-12-01T23:59:59.000Z

223

Combination of CDF and D0 measurements of the $W$ boson helicity in top quark decays  

Science Conference Proceedings (OSTI)

We report the combination of recent measurements of the helicity of the W boson from top quark decay by the CDF and D0 collaborations, based on data samples corresponding to integrated luminosities of 2.7-5.4 fb{sup -1} of p{bar p} collisions collected during Run II of the Fermilab Tevatron Collider. Combining measurements that simultaneously determine the fractions of W bosons with longitudinal (f{sub 0}) and right-handed (f{sub +}) helicities, we find f{sub 0} = 0.722 {+-} 0.081 [{+-} 0.062 (stat.) {+-} 0.052 (syst.)] and f{sub +} = -0.033 {+-} 0.046 [{+-} 0.034 (stat.) {+-} 0.031 (syst.)]. Combining measurements where one of the helicity fractions is fixed to the value expected in the standard model, we find f{sub 0} = 0.682 {+-} 0.057 [{+-} 0.035 (stat.) {+-} 0.046 (syst.)] and f{sub +} = ?0.015 {+-} 0.035 [{+-} 0.018 (stat.) {+-} 0.030 (syst.)]. The results are consistent with standard model expectations.

Aaltonen, T.; /Helsinki Inst. of Phys.; Abazov, V.M.; /Dubna, JINR; Abbott, B.; /Oklahoma U.; Acharya, B.S.; /Tata Inst.; Adams, M.; /Illinois U., Chicago; Adams, T.; /Florida State U.; Alexeev, G.D.; /Dubna, JINR; Alkhazov, G.; /St. Petersburg, INP; Alton, A.; /Augustana Coll., Sioux Falls /Michigan U.; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Alverson, G.; /Northeastern U. /INFN, Padua

2012-02-01T23:59:59.000Z

224

Observation of D0-D0bar Mixing using the CDF II Detector  

E-Print Network (OSTI)

We measure the time dependence of the ratio of decay rates for D0 -> K+ pi- to the Cabibbo-favored decay D0 -> K- pi+. The charge conjugate decays are included. A signal of 3.3 x 10^4 D*+ -> pi+ D0, D0 -> K+ pi- decays is obtained with D0 proper decay times between 0.75 and 10 mean D0 lifetimes. The data were recorded with the CDF II detector at the Fermilab Tevatron and correspond to an integrated luminosity of 9.6 fb-1 for p-pbar collisions at sqrt(s) = 1.96 TeV. Assuming CP conservation, we search for D0-D0bar mixing and measure the mixing parameters to be R_D = (3.51 +/- 0.35) x 10^{-3}, y' = (4.3 +/- 4.3) x 10^{-3}, and x'^2 = (0.08 +/- 0.18) x 10^{-3}. We report Bayesian probability intervals in the x'^2 - y' plane and find that the significance of excluding the no-mixing hypothesis is equivalent to 6.1 Gaussian standard deviations, providing the second observation of D0-D0bar mixing from a single experiment.

Aaltonen, T; Amidei, D; Anastassov, A; Annovi, A; Antos, J; Apollinari, G; Appel, J A; Arisawa, T; Artikov, A; Asaadi, J; Ashmanskas, W; Auerbach, B; Aurisano, A; Azfar, F; Badgett, W; Bae, T; Barbaro-Galtieri, A; Barnes, V E; Barnett, B A; Barria, P; Bartos, P; Bauce, M; Bedeschi, F; Behari, S; Bellettini, G; Bellinger, J; Benjamin, D; Beretvas, A; Bhatti, A; Bland, K R; Blumenfeld, B; Bocci, A; Bodek, A; Bortoletto, D; Boudreau, J; Boveia, A; Brigliadori, L; Bromberg, C; Brucken, E; Budagov, J; Budd, H S; Burkett, K; Busetto, G; Bussey, P; Butti, P; Buzatu, A; Calamba, A; Camarda, S; Campanelli, M; Canelli, F; Carls, B; Carlsmith, D; Carosi, R; Carrillo, S; Casal, B; Casarsa, M; Castro, A; Catastini, P; Cauz, D; Cavaliere, V; Cavalli-Sforza, M; Cerri, A; Cerrito, L; Chen, Y C; Chertok, M; Chiarelli, G; Chlachidze, G; Cho, K; Chokheli, D; Clark, A; Clarke, C; Convery, M E; Conway, J; Corbo, M; Cordelli, M; Cox, C A; Cox, D J; Cremonesi, M; Cruz, D; Cuevas, J; Culbertson, R; d'Ascenzo, N; Datta, M; de Barbaro, P; Demortier, L; Marchese, L; Deninno, M; Devoto, F; D'Errico, M; Di Canto, A; Di Ruzza, B; Dittmann, J R; D'Onofrio, M; Donati, S; Dorigo, M; Driutti, A; Ebina, K; Edgar, R; Elagin, A; Erbacher, R; Errede, S; Esham, B; Farrington, S; Ramos, J P Fernndez; Field, R; Flanagan, G; Forrest, R; Franklin, M; Freeman, J C; Frisch, H; Funakoshi, Y; Galloni, C; Garfinkel, A F; Garosi, P; Gerberich, H; Gerchtein, E; Giagu, S; Giakoumopoulou, V; Gibson, K; Ginsburg, C M; Giokaris, N; Giromini, P; Giurgiu, G; Glagolev, V; Glenzinski, D; Gold, M; Goldin, D; Golossanov, A; Gomez, G; Gomez-Ceballos, G; Goncharov, M; Lpez, O Gonzlez; Gorelov, I; Goshaw, A T; Goulianos, K; Gramellini, E; Grinstein, S; Grosso-Pilcher, C; da Costa, J Guimaraes; Hahn, S R; Han, J Y; Happacher, F; Hara, K; Hare, M; Harr, R F; Harrington-Taber, T; Hatakeyama, K; Hays, C; Heinrich, J; Herndon, M; Hocker, A; Hong, Z; Hopkins, W; Hou, S; Hughes, R E; Husemann, U; Hussein, M; Huston, J; Introzzi, G; Iori, M; Ivanov, A; James, E; Jang, D; Jayatilaka, B; Jeon, E J; Jindariani, S; Jones, M; Joo, K K; Jun, S Y; Junk, T R; Kambeitz, M; Kamon, T; Karchin, P E; Kasmi, A; Kato, Y; Ketchum, W; Keung, J; Kilminster, B; Kim, D H; Kim, H S; Kim, J E; Kim, M J; Kim, S B; Kim, S H; Kim, Y K; Kim, Y J; Kimura, N; Kirby, M; Knoepfel, K; Kondo, K; Kong, D J; Konigsberg, J; Kotwal, A V; Kreps, M; Kroll, J; Kruse, M; Kulkarni, N; Kuhr, T; Kurata, M; Laasanen, A T; Lammel, S; Lancaster, M; Lannon, K; Latino, G; Lee, H S; Lee, J S; Leo, S; Leone, S; Lewis, J D; Limosani, A; Lipeles, E; Lister, A; Liu, H; Liu, Q; Liu, T; Lockwitz, S; Loginov, A; Luc, A; Lucchesi, D; Lueck, J; Lujan, P; Lukens, P; Lungu, G; Lys, J; Lysak, R; Madrak, R; Maestro, P; Malik, S; Manca, G; Manousakis-Katsikakis, A; Margaroli, F; Marino, P; Martnez, M; Matera, K; Mattson, M E; Mazzacane, A; Mazzanti, P; McNulty, R; Mehta, A; Mehtala, P; Mesropian, C; Miao, T; Mietlicki, D; Mitra, A; Miyake, H; Moed, S; Moggi, N; Moon, C S; Moore, R; Morello, M J; Mukherjee, A; Muller, Th; Murat, P; Mussini, M; Nachtman, J; Nagai, Y; Naganoma, J; Nakano, I; Napier, A; Nett, J; Neu, C; Nigmanov, T; Nodulman, L; Noh, S Y; Norniella, O; Oakes, L; Oh, S H; Oh, Y D; Oksuzian, I; Okusawa, T; Orava, R; Ortolan, L; Pagliarone, C; Palencia, E; Palni, P; Papadimitriou, V; Parker, W; Pauletta, G; Paulini, M; Paus, C; Phillips, T J; Piacentino, G; Pianori, E; Pilot, J; Pitts, K; Plager, C; Pondrom, L; Poprocki, S; Potamianos, K; Prokoshin, F; Pranko, A; Ptohos, F; Punzi, G; Ranjan, N; Fernndez, I Redondo; Renton, P; Rescigno, M; Rimondi, F; Ristori, L; Robson, A; Rodriguez, T; Rolli, S; Ronzani, M; Roser, R; Rosner, J L; Ruffini, F; Ruiz, A; Russ, J; Rusu, V; Sakumoto, W K; Sakurai, Y; Santi, L; Sato, K; Saveliev, V; Savoy-Navarro, A; Schlabach, P; Schmidt, E E; Schwarz, T; Scodellaro, L; Scuri, F; Seidel, S; Seiya, Y; Semenov, A; Sforza, F; Shalhout, S Z; Shears, T; Shepard, P F; Shimojima, M; Shochet, M; Shreyber-Tecker, I; Simonenko, A; Sliwa, K; Smith, J R; Snider, F D; Sorin, V; Song, H; Stancari, M; Denis, R St; Stentz, D; Strologas, J; Sudo, Y; Sukhanov, A; Suslov, I; Takemasa, K; Takeuchi, Y; Tang, J; Tecchio, M; Teng, P K; Thom, J; Thomson, E; Thukral, V; Toback, D; Tokar, S; Tollefson, K; Tomura, T; Tonelli, D; Torre, S; Torretta, D; Totaro, P; Trovato, M; Ukegawa, F; Uozumi, S; Vzquez, F; Velev, G; Vellidis, C; Vernieri, C; Vidal, M; Vilar, R; Vizn, J; Vogel, M; Volpi, G; Wagner, P; Wallny, R; Wang, S M; Waters, D; Wester, W C; Whiteson, D; Wicklund, A B; Wilbur, S; Williams, H H; Wilson, J S; Wilson, P; Winer, B L; Wittich, P; Wolbers, S; Wolfe, H; Wright, T; Wu, X; Wu, Z; Yamamoto, K; Yamato, D; Yang, T; Yang, U K; Yang, Y C; Yao, W -M; Yeh, G P; Yi, K; Yoh, J; Yorita, K; Yoshida, T; Yu, G B; Yu, I; Zanetti, A M; Zeng, Y; Zhou, C; Zucchelli, S

2013-01-01T23:59:59.000Z

225

Observation of D0-D0bar Mixing using the CDF II Detector  

E-Print Network (OSTI)

We measure the time dependence of the ratio of decay rates for D0 -> K+ pi- to the Cabibbo-favored decay D0 -> K- pi+. The charge conjugate decays are included. A signal of 3.3 x 10^4 D*+ -> pi+ D0, D0 -> K+ pi- decays is obtained with D0 proper decay times between 0.75 and 10 mean D0 lifetimes. The data were recorded with the CDF II detector at the Fermilab Tevatron and correspond to an integrated luminosity of 9.6 fb-1 for p-pbar collisions at sqrt(s) = 1.96 TeV. Assuming CP conservation, we search for D0-D0bar mixing and measure the mixing parameters to be R_D = (3.51 +/- 0.35) x 10^{-3}, y' = (4.3 +/- 4.3) x 10^{-3}, and x'^2 = (0.08 +/- 0.18) x 10^{-3}. We report Bayesian probability intervals in the x'^2 - y' plane and find that the significance of excluding the no-mixing hypothesis is equivalent to 6.1 Gaussian standard deviations, providing the second observation of D0-D0bar mixing from a single experiment.

CDF Collaboration; T. Aaltonen; S. Amerio; D. Amidei; A. Anastassov; A. Annovi; J. Antos; G. Apollinari; J. A. Appel; T. Arisawa; A. Artikov; J. Asaadi; W. Ashmanskas; B. Auerbach; A. Aurisano; F. Azfar; W. Badgett; T. Bae; A. Barbaro-Galtieri; V. E. Barnes; B. A. Barnett; P. Barria; P. Bartos; M. Bauce; F. Bedeschi; S. Behari; G. Bellettini; J. Bellinger; D. Benjamin; A. Beretvas; A. Bhatti; K. R. Bland; B. Blumenfeld; A. Bocci; A. Bodek; D. Bortoletto; J. Boudreau; A. Boveia; L. Brigliadori; C. Bromberg; E. Brucken; J. Budagov; H. S. Budd; K. Burkett; G. Busetto; P. Bussey; P. Butti; A. Buzatu; A. Calamba; S. Camarda; M. Campanelli; F. Canelli; B. Carls; D. Carlsmith; R. Carosi; S. Carrillo; B. Casal; M. Casarsa; A. Castro; P. Catastini; D. Cauz; V. Cavaliere; M. Cavalli-Sforza; A. Cerri; L. Cerrito; Y. C. Chen; M. Chertok; G. Chiarelli; G. Chlachidze; K. Cho; D. Chokheli; A. Clark; C. Clarke; M. E. Convery; J. Conway; M. Corbo; M. Cordelli; C. A. Cox; D. J. Cox; M. Cremonesi; D. Cruz; J. Cuevas; R. Culbertson; N. d'Ascenzo; M. Datta; P. de Barbaro; L. Demortier; L. Marchese; M. Deninno; F. Devoto; M. D'Errico; A. Di Canto; B. Di Ruzza; J. R. Dittmann; M. D'Onofrio; S. Donati; M. Dorigo; A. Driutti; K. Ebina; R. Edgar; A. Elagin; R. Erbacher; S. Errede; B. Esham; S. Farrington; J. P. Fernndez Ramos; R. Field; G. Flanagan; R. Forrest; M. Franklin; J. C. Freeman; H. Frisch; Y. Funakoshi; C. Galloni; A. F. Garfinkel; P. Garosi; H. Gerberich; E. Gerchtein; S. Giagu; V. Giakoumopoulou; K. Gibson; C. M. Ginsburg; N. Giokaris; P. Giromini; G. Giurgiu; V. Glagolev; D. Glenzinski; M. Gold; D. Goldin; A. Golossanov; G. Gomez; G. Gomez-Ceballos; M. Goncharov; O. Gonzlez Lpez; I. Gorelov; A. T. Goshaw; K. Goulianos; E. Gramellini; S. Grinstein; C. Grosso-Pilcher; R. C. Group; J. Guimaraes da Costa; S. R. Hahn; J. Y. Han; F. Happacher; K. Hara; M. Hare; R. F. Harr; T. Harrington-Taber; K. Hatakeyama; C. Hays; J. Heinrich; M. Herndon; A. Hocker; Z. Hong; W. Hopkins; S. Hou; R. E. Hughes; U. Husemann; M. Hussein; J. Huston; G. Introzzi; M. Iori; A. Ivanov; E. James; D. Jang; B. Jayatilaka; E. J. Jeon; S. Jindariani; M. Jones; K. K. Joo; S. Y. Jun; T. R. Junk; M. Kambeitz; T. Kamon; P. E. Karchin; A. Kasmi; Y. Kato; W. Ketchum; J. Keung; B. Kilminster; D. H. Kim; H. S. Kim; J. E. Kim; M. J. Kim; S. B. Kim; S. H. Kim; Y. K. Kim; Y. J. Kim; N. Kimura; M. Kirby; K. Knoepfel; K. Kondo; D. J. Kong; J. Konigsberg; A. V. Kotwal; M. Kreps; J. Kroll; M. Kruse; N. Kulkarni; T. Kuhr; M. Kurata; A. T. Laasanen; S. Lammel; M. Lancaster; K. Lannon; G. Latino; H. S. Lee; J. S. Lee; S. Leo; S. Leone; J. D. Lewis; A. Limosani; E. Lipeles; A. Lister; H. Liu; Q. Liu; T. Liu; S. Lockwitz; A. Loginov; A. Luc; D. Lucchesi; J. Lueck; P. Lujan; P. Lukens; G. Lungu; J. Lys; R. Lysak; R. Madrak; P. Maestro; S. Malik; G. Manca; A. Manousakis-Katsikakis; F. Margaroli; P. Marino; M. Martnez; K. Matera; M. E. Mattson; A. Mazzacane; P. Mazzanti; R. McNulty; A. Mehta; P. Mehtala; C. Mesropian; T. Miao; D. Mietlicki; A. Mitra; H. Miyake; S. Moed; N. Moggi; C. S. Moon; R. Moore; M. J. Morello; A. Mukherjee; Th. Muller; P. Murat; M. Mussini; J. Nachtman; Y. Nagai; J. Naganoma; I. Nakano; A. Napier; J. Nett; C. Neu; T. Nigmanov; L. Nodulman; S. Y. Noh; O. Norniella; L. Oakes; S. H. Oh; Y. D. Oh; I. Oksuzian; T. Okusawa; R. Orava; L. Ortolan; C. Pagliarone; E. Palencia; P. Palni; V. Papadimitriou; W. Parker; G. Pauletta; M. Paulini; C. Paus; T. J. Phillips; G. Piacentino; E. Pianori; J. Pilot; K. Pitts; C. Plager; L. Pondrom; S. Poprocki; K. Potamianos; F. Prokoshin; A. Pranko; F. Ptohos; G. Punzi; N. Ranjan; I. Redondo Fernndez; P. Renton; M. Rescigno; F. Rimondi; L. Ristori; A. Robson; T. Rodriguez; S. Rolli; M. Ronzani; R. Roser; J. L. Rosner; F. Ruffini; A. Ruiz; J. Russ; V. Rusu; W. K. Sakumoto; Y. Sakurai; L. Santi; K. Sato; V. Saveliev; A. Savoy-Navarro; P. Schlabach; E. E. Schmidt; T. Schwarz; L. Scodellaro; F. Scuri; S. Seidel; Y. Seiya; A. Semenov; F. Sforza; S. Z. Shalhout; T. Shears; P. F. Shepard; M. Shimojima; M. Shochet; I. Shreyber-Tecker; A. Simonenko; K. Sliwa; J. R. Smith; F. D. Snider; V. Sorin; H. Song; M. Stancari; R. St. Denis; D. Stentz; J. Strologas; Y. Sudo; A. Sukhanov; I. Suslov; K. Takemasa; Y. Takeuchi; J. Tang; M. Tecchio; P. K. Teng; J. Thom; E. Thomson; V. Thukral; D. Toback; S. Tokar; K. Tollefson; T. Tomura; D. Tonelli; S. Torre; D. Torretta; P. Totaro; M. Trovato; F. Ukegawa; S. Uozumi; F. Vzquez; G. Velev; C. Vellidis; C. Vernieri; M. Vidal; R. Vilar; J. Vizn; M. Vogel; G. Volpi; P. Wagner; R. Wallny; S. M. Wang; D. Waters; W. C. Wester III; D. Whiteson; A. B. Wicklund; S. Wilbur; H. H. Williams; J. S. Wilson; P. Wilson; B. L. Winer; P. Wittich; S. Wolbers; H. Wolfe; T. Wright; X. Wu; Z. Wu; K. Yamamoto; D. Yamato; T. Yang; U. K. Yang; Y. C. Yang; W. -M. Yao; G. P. Yeh; K. Yi; J. Yoh; K. Yorita; T. Yoshida

2013-09-16T23:59:59.000Z

226

Measurement of the W-boson helicity fractions in top-quark decays at CDF  

SciTech Connect

We present a measurement of the fractions F{sub 0} and F{sub +} of longitudinally polarized and right-handed W bosons in top-quark decays using data collected with the CDF II detector. The data set used in the analysis corresponds to an integrated luminosity of approximately 955 pb{sup -1}. We select t{bar t} candidate events with one lepton, at least four jets, and missing transverse energy. Our helicity measurement uses the decay angle {theta}*, which is defined as the angle between the momentum of the charged lepton in the W boson rest-frame and the W momentum in the top-quark rest-frame. The cos{theta}* distribution in the data is determined by full kinematic reconstruction of the t{bar t} candidates. We find F{sub 0}= 0.59 {+-} 0.12(stat){sup +0.07}{sub -0.06}(syst) and F{sub +}=-0.03 {+-} 0.06(stat){sup +0.04}{sub -0.03}(syst), which is consistent with the standard model prediction. We set an upper limit on the fraction of right-handed W bosons of F{sub +} {le} 0.10 at the 95% confidence level.

Chwalek, Thorsten; /Karlsruhe U., EKP

2007-05-01T23:59:59.000Z

227

Search for Standard Model Higgs Boson Production in Association with a W Boson at CDF  

SciTech Connect

We present a search for standard model Higgs boson production in association with a W boson in proton-antiproton collisions (p{bar p} {yields} W{sup {+-}}H {yields} {ell}{nu}b{bar b}) at a center of mass energy of 1.96 TeV. The search employs data collected with the CDF II detector which correspond to an integrated luminosity of approximately 1 fb{sup -1}. We select events consistent with a signature of a single lepton (e{sup {+-}}/{mu}{sup {+-}}), missing transverse energy, and two jets. Jets corresponding to bottom quarks are identified with a secondary vertex tagging method and a neural network filter technique. The observed number of events and the dijet mass distributions are consistent with the standard model background expectations, and we set 95% confidence level upper limits on the production cross section times branching ratio ranging from 3.9 to 1.3 pb for Higgs boson masses from 110 to 150 GeV/c{sup 2}, respectively.

Aaltonen, T.; /Helsinki Inst. of Phys.; Adelman, J.; /Chicago U., EFI; Akimoto, T.; /Tsukuba U.; Albrow, M.G.; /Fermilab; Alvarez Gonzalez, B.; /Cantabria U., Santander; Amerio, S.; /Padua U.; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U.; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab

2008-03-01T23:59:59.000Z

228

Observation of Electroweak Single Top-Quark Production with the CDF II Experiment  

SciTech Connect

The standard model of elementary particle physics (SM) predicts, besides the top-quark pair production via the strong interaction, also the electroweak production of single top-quarks [19]. Up to now, the Fermilab Tevatron proton-antiproton-collider is the only place to produce and study top quarks emerging from hadron-hadron-collisions. Top quarks were directly observed in 1995 during the Tevatron Run I at a center-of-mass energy of {radical}s = 1.8 TeV simultaneously by the CDF and D0 Collaborations via the strong production of top-quark pairs. Run II of the Tevatron data taking period started 2001 at {radical}s = 1.96 TeV after a five year upgrade of the Tevatron accelerator complex and of both experiments. One main component of its physics program is the determination of the properties of the top quark including its electroweak production. Even though Run II is still ongoing, the study of the top quark is already a successful endeavor, confirmed by dozens of publications from both Tevatron experiments. A comprehensive review of top-quark physics can be found in reference. The reasons for searching for single top-quark production are compelling. As the electroweak top-quark production proceeds via a Wtb vertex, it provides the unique opportunity of the direct measurement of the CKM matrix element |V{sub tb}|, which is expected to be |V{sub tb}| {approx} 1 in the SM. Significant deviations from unity could be an indication of a fourth quark generation, a production mode via flavor-changing neutral currents, and other new phenomena, respectively. There are two dominating electroweak top-quark production modes at the Fermilab Tevatron: the t-channel exchange of a virtual W boson striking a b quark and the s-channel production of a timelike W boson via the fusion of two quarks. In proton-antiproton-collisions the third electroweak production mode, the associated Wt production of an on-shell W boson in conjunction with a top quark has a comparatively negligible small predicted cross section. Therefore, the vast majority of the CDF and D0 single top-quark analyses search for the combined s- and t-channel signal, with the production ratio to be given by the SM. In Tevatron Run I, several limits on the single top-quark production cross section were set by CDF and D0, whereas in Run II, even stronger limits followed by both collaborations. Furthermore, limits on the non-SM production of single top-quarks via flavor-changing neutral currents could be obtained. The electroweak production of single top-quarks has not yet been observed up to the time of this thesis, although the D0 and shortly thereafter the CDF Collaborations found first evidence. The experimental challenge of the search for single top-quark production is the tiny expected signal beneath a large and imprecisely known amount of background processes. The relative fraction of background events is at the order of about ten times higher compared to the top-quark pair production. Consequently, the expected signal amounts to about 5% of the full candidate event sample whose background contribution is only known to a level at the order of 20%. Furthermore, the signal events themselves are expected to be not as distinct from the background as the top-quark pair production since there is only one heavy object present in the event. Thus, experimental methods like simple counting experiments are not sufficiently sensitive and the development of more sophisticated analysis techniques is required to distinguish such small signals from alike and inaccurately known background processes. Neural networks comply with those requirements. They can be used to distinguish between signal and background processes by combining the information contained in several variables into a powerful discriminant, while each variable has a rather low separation capability. The application of those neural network discriminants to collision data provide a method for the extraction of the signal fraction and its significance. This thesis presents a neural network search for combined as well as separate

Lueck, Jan; /KARLSRUHE U., EKP

2009-07-01T23:59:59.000Z

229

Observation of Electroweak Single Top-Quark Production with the CDF II Experiment  

Science Conference Proceedings (OSTI)

The standard model of elementary particle physics (SM) predicts, besides the top-quark pair production via the strong interaction, also the electroweak production of single top-quarks [19]. Up to now, the Fermilab Tevatron proton-antiproton-collider is the only place to produce and study top quarks emerging from hadron-hadron-collisions. Top quarks were directly observed in 1995 during the Tevatron Run I at a center-of-mass energy of {radical}s = 1.8 TeV simultaneously by the CDF and D0 Collaborations via the strong production of top-quark pairs. Run II of the Tevatron data taking period started 2001 at {radical}s = 1.96 TeV after a five year upgrade of the Tevatron accelerator complex and of both experiments. One main component of its physics program is the determination of the properties of the top quark including its electroweak production. Even though Run II is still ongoing, the study of the top quark is already a successful endeavor, confirmed by dozens of publications from both Tevatron experiments. A comprehensive review of top-quark physics can be found in reference. The reasons for searching for single top-quark production are compelling. As the electroweak top-quark production proceeds via a Wtb vertex, it provides the unique opportunity of the direct measurement of the CKM matrix element |V{sub tb}|, which is expected to be |V{sub tb}| {approx} 1 in the SM. Significant deviations from unity could be an indication of a fourth quark generation, a production mode via flavor-changing neutral currents, and other new phenomena, respectively. There are two dominating electroweak top-quark production modes at the Fermilab Tevatron: the t-channel exchange of a virtual W boson striking a b quark and the s-channel production of a timelike W boson via the fusion of two quarks. In proton-antiproton-collisions the third electroweak production mode, the associated Wt production of an on-shell W boson in conjunction with a top quark has a comparatively negligible small predicted cross section. Therefore, the vast majority of the CDF and D0 single top-quark analyses search for the combined s- and t-channel signal, with the production ratio to be given by the SM. In Tevatron Run I, several limits on the single top-quark production cross section were set by CDF and D0, whereas in Run II, even stronger limits followed by both collaborations. Furthermore, limits on the non-SM production of single top-quarks via flavor-changing neutral currents could be obtained. The electroweak production of single top-quarks has not yet been observed up to the time of this thesis, although the D0 and shortly thereafter the CDF Collaborations found first evidence. The experimental challenge of the search for single top-quark production is the tiny expected signal beneath a large and imprecisely known amount of background processes. The relative fraction of background events is at the order of about ten times higher compared to the top-quark pair production. Consequently, the expected signal amounts to about 5% of the full candidate event sample whose background contribution is only known to a level at the order of 20%. Furthermore, the signal events themselves are expected to be not as distinct from the background as the top-quark pair production since there is only one heavy object present in the event. Thus, experimental methods like simple counting experiments are not sufficiently sensitive and the development of more sophisticated analysis techniques is required to distinguish such small signals from alike and inaccurately known background processes. Neural networks comply with those requirements. They can be used to distinguish between signal and background processes by combining the information contained in several variables into a powerful discriminant, while each variable has a rather low separation capability. The application of those neural network discriminants to collision data provide a method for the extraction of the signal fraction and its significance. This thesis presents a neural network search for combined as well as separate

Lueck, Jan; /KARLSRUHE U., EKP

2009-07-01T23:59:59.000Z

230

Combination of CDF and D0 measurements of the W boson helicity in top quark decays  

E-Print Network (OSTI)

We report the combination of recent measurements of the helicity of the W boson from top quark decay by the CDF and D0 collaborations, based on data samples corresponding to integrated luminosities of 2.7 - 5.4 fb^-1 of ppbar collisions collected during Run II of the Fermilab Tevatron Collider. Combining measurements that simultaneously determine the fractions of W bosons with longitudinal (f0) and right-handed (f+) helicities, we find f0 = 0.722 \\pm 0.081 [\\pm 0.062 (stat.) \\pm 0.052 (syst.)] and f+ = -0.033 \\pm 0.046 [\\pm 0.034 (stat.) \\pm 0.031 (syst.)]. Combining measurements where one of the helicity fractions is fixed to the value expected in the standard model, we find f0 = 0.682 \\pm 0.057 [\\pm 0.035 (stat.) \\pm 0.046 (syst.)] and f+ = -0.015\\pm0.035 [\\pm 0.018 (stat.) \\pm 0.030 (syst.)]. The results are consistent with standard model expectations.

Aaltonen, T; Abbott, B; Acharya, B S; Adams, M; Adams, T; Alexeev, G D; Alkhazov, G; Alton, A; Gonzlez, B lvarez; Alverson, G; Amerio, S; Amidei, D; Anastassov, A; Annovi, A; Antos, J; Aoki, M; Apollinari, G; Appel, J A; Arisawa, T; Artikov, A; Asaadi, J; Ashmanskas, W; Askew, A; sman, B; Atkins, S; Atramentov, O; Auerbach, B; Augsten, K; Aurisano, A; Avila, C; Azfar, F; Badaud, F; Badgett, W; Bae, T; Bagby, L; Baldin, B; Bandurin, D V; Banerjee, S; Barbaro-Galtieri, A; Barberis, E; Baringer, P; Barnes, V E; Barnett, B A; Barreto, J; Barria, P; Bartlett, J F; Bartos, P; Bassler, U; Bauce, M; Bazterra, V; Bean, A; Bedeschi, F; Begalli, M; Behari, S; Belanger-Champagne, C; Bellantoni, L; Bellettini, G; Bellinger, J; Benjamin, D; Beretvas, A; Beri, S B; Bernardi, G; Bernhard, R; Bertram, I; Besanon, M; Beuselinck, R; Bezzubov, V A; Bhatia, S; Bhatnagar, V; Bhatti, A; Bhat, P C; Bisello, D; Bizjak, I; Bland, K R; Blazey, G; Blessing, S; Bloom, K; Blumenfeld, B; Bocci, A; Bodek, A; Boehnlein, A; Boline, D; Boos, E E; Borissov, G; Bortoletto, D; Bose, T; Boudreau, J; Boveia, A; Brandt, A; Brandt, O; Brigliadori, L; Brock, R; Bromberg, C; Brooijmans, G; Bross, A; Brown, D; Brown, J; Brucken, E; Bu, X B; Budagov, J; Budd, H S; Buehler, M; Buescher, V; Bunichev, V; Burdin, S; Burkett, K; Bussey, P; Buszello, C P; Buzatu, A; Calamba, A; Calancha, C; Camacho-Prez, E; Camarda, S; Campanelli, M; Campbell, M; Canelli, F; Carls, B; Carlsmith, D; Carosi, R; Carrillo, S; Carron, S; Casal, B; Casarsa, M; Casey, B C K; Castilla-Valdez, H; Castro, A; Catastini, P; Caughron, S; Cauz, D; Cavaliere, V; Cavalli-Sforza, M; Cerri, A; Cerrito, L; Chakrabarti, S; Chakraborty, D; Chan, K M; Chandra, A; Chapon, E; Chen, Y C; Chen, G; Chertok, M; Chevalier-Thry, S; Chiarelli, G; Chlachidze, G; Chlebana, F; Choi, S; Chokheli, D; Choudhary, B; Cho, D K; Cho, K; Cho, S W; Chung, W H; Chung, Y S; Cihangir, S; Ciocci, M A; Claes, D; Clarke, C; Clark, A; Clutter, J; Compostella, G; Convery, M E; Conway, J; Cooke, M; Cooper, W E; Corbo, M; Corcoran, M; Cordelli, M; Couderc, F; Cousinou, M -C; Cox, C A; Cox, D J; Crescioli, F; Croc, A; Cuevas, J; Culbertson, R; Cutts, D; d'Ascenzo, N; d'Errico, M; D'Onofrio, M; Dagenhart, D; Das, A; Datta, M; Davies, G; Dliot, F; Dell'Orso, M; Demina, R; Demortier, L; Deninno, M; Denisov, D; Denisov, S P; Desai, S; Deterre, C; DeVaughan, K; Devoto, F; de Barbaro, P; de Jong, S J; De La Cruz-Burelo, E; Diehl, H T; Diesburg, M; Ding, P F; Dittmann, J R; Di Canto, A; Di Ruzza, B; Dominguez, A; Donati, S; Dong, P; Dorigo, M; Dorigo, T; Dorland, T; Dubey, A; Dudko, L V; Duggan, D; Duperrin, A; Dutt, S; Dyshkant, A; Eads, M; Ebina, K; Edmunds, D; Elagin, A; Ellison, J; Elvira, V D; Enari, Y; Eppig, A; Erbacher, R; Errede, S; Ershaidat, N; Eusebi, R; Evans, H; Evdokimov, A; Evdokimov, V N; Facini, G; Farrington, S; Feindt, M; Ferbel, T; Feng, L; Fernandez, J P; Fiedler, F; Field, R; Filthaut, F; Fisher, W; Fisk, H E; Flanagan, G; Forrest, R; Fortner, M; Fox, H; Franklin, M; Frank, M J; Freeman, J C; Fuess, S; Funakoshi, Y; Furic, I; Gallinaro, M; Garcia, J E; Garcia-Bellido, A; Garca-Guerra, G A; Garfinkel, A F; Garosi, P; Gavrilov, V; Gay, P; Geng, W; Gerbaudo, D; Gerber, C E; Gerberich, H; Gerchtein, E; Gershtein, Y; Giagu, S; Giakoumopoulou, V; Giannetti, P; Gibson, K; Ginsburg, C M; Ginther, G; Giokaris, N; Giromini, P; Giurgiu, G; Glagolev, V; Glenzinski, D; Goldin, D; Gold, M; Goldschmidt, N; Golossanov, A; Golovanov, G; Gomez-Ceballos, G; Gomez, G; Goncharov, M; Gonzlez, O; Gorelov, I; Goshaw, A T; Goulianos, K; Goussiou, A; Grannis, P D; Greder, S; Greenlee, H; Grenier, G; Grinstein, S; Gris, Ph; Grivaz, J -F; Grohsjean, A; Grosso-Pilcher, C; Grnendahl, S; Grnewald, M W; Guillemin, T; da Costa, J Guimaraes; Guo, F; Gutierrez, G; Gutierrez, P; Haas, A; Hagopian, S; Hahn, S R; Haley, J; Halkiadakis, E; Hamaguchi, A; Han, J Y; Han, L; Happacher, F; Hara, K; Harder, K; Hare, D; Hare, M; Harel, A; Harr, R F; Hatakeyama, K; Hauptman, J M; Hays, C; Hays, J; Head, T; Hebbeker, T; Heck, M; Hedin, D; Hegab, H; Heinrich, J; Heinson, A P; Heintz, U; Hensel, C; La Cruz, I Heredia-De; Herndon, M; Herner, K; Hesketh, G; Hewamanage, S; Hildreth, M D; Hirosky, R; Hoang, T; Hobbs, J D; Hocker, A; Hoeneisen, B; Hohlfeld, M; Hopkins, W; Horn, D; Hou, S; Howley, I; Hubacek, Z; Hughes, R E; Hurwitz, M; Husemann, U; Hussain, N; Hussein, M; Huston, J; Hynek, V; Iashvili, I; Ilchenko, Y; Illingworth, R; Introzzi, G; Iori, M; Ito, A S; Ivanov, A; Jabeen, S; Jaffr, M; James, E; Jamin, D; Jang, D; Jayasinghe, A; Jayatilaka, B; Jeon, E J; Jesik, R; Jindariani, S; Johns, K; Johnson, M; Jonckheere, A; Jones, M; Jonsson, P; Joo, K K; Joshi, J; Jun, S Y; Jung, A W; Junk, T R; Juste, A; Kaadze, K; Kajfasz, E; Kamon, T; Karchin, P E; Karmanov, D; Kasmi, A; Kasper, P A; Kato, Y; Katsanos, I; Kehoe, R

2012-01-01T23:59:59.000Z

231

Search for the Higgs boson produced in association with a W boson at CDF Run II  

SciTech Connect

We present a search for standard model Higgs boson production in association with a W boson in proton-antiproton collisions (p{bar p} {yields} W{sup {+-}}H {yields} {ell}{nu}b{bar b}) at a center of mass energy of 1.96 TeV. WH candidate events have a signature of a single lepton (E{sup {+-}}/{mu}{sup {+-}}), missing transverse energy, and two jets. The search looks for candidate events in approximately 2.7 fb{sup -1} of data recorded with the CDF II detector. The high-p{sub T} lepton (e,{mu}) in the events provides a distinct signature for triggering and most of the events in the dataset come from high-p{sub t} lepton triggers. Our analysis improves on prior searches by including events recorded on the E{sub T} + 2 Jets trigger with a lepton reconstructed as an isolated high-p{sub T} charged particle. We increase the sample purity by identifying ('tagging') long-lived b-hadrons in jets. A neural network combines distinguishing kinematic information into a function optimized for WH sensitivity. The neural network output distributions are consistent with the standard model background expectations and we set limits upper limits on the rate of Higgs production. We set 95% confidence level upper limits on the WH production cross section times branching ratio for Higgs masses from 100 to 150 GeV/c{sup 2} and express our results as a ratio of the experimental limit to the theoretical Standard Model production rate. Our limits range from 3.6 (4.3 expected) to 61.1 (43.2 expected) for Higgs masses from 100 to 150 GeV/c{sup 2}, respectively.

Slaunwhite, Jason Michael; /Ohio State U.

2009-01-01T23:59:59.000Z

232

CDF measurement of the top quark mass in the lepton + jets channel using the multivariate template method  

SciTech Connect

The authors measure the mass of the top quark using 162 pb{sup -1} of data collected by the CDF experiment at FNAL in Run II. The decay chain t{bar t} {yields} bq{bar q}{bar b}lv is studied using a novel technique called the Multivariate Template Method (MTM). Using this technique they obtain a result of M{sub top} = 179.6{sub -6.3}{sup +6.4} {+-} 6.8 GeV/c{sup 2} for the top quark.

Freeman, John; /Fermilab

2004-12-01T23:59:59.000Z

233

Data:Bebc0cdf-adfc-42a6-beaa-16749e5624c1 | Open Energy Information  

Open Energy Info (EERE)

Bebc0cdf-adfc-42a6-beaa-16749e5624c1 Bebc0cdf-adfc-42a6-beaa-16749e5624c1 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: CenterPoint Energy Effective date: 2013/01/25 End date if known: Rate name: Secondary Service - Greater than 10 kVa, Non-IDR Metered, less than 400 kVa (TC-MGS) Sector: Commercial Description: Delivery Service will be single-phase, 60 hertz, at a standard secondary voltage. Delivery Service will be metered using Company's standard watt-hour Meter provided for this type of Delivery Service. Any other metering option(s) will be provided at an additional charge and/or will be provided by a Meter Owner other than the Company pursuant to Applicable Legal Authorities. Where Delivery Service of the type desired is not available at the Point of Delivery, additional charges and special contract arrangements may be required prior to Delivery Service being furnished, pursuant to Section 6.1.2.2, Construction Services, in this Tariff.

234

Data:40578972-846a-4cdf-8321-8b488ae9cadf | Open Energy Information  

Open Energy Info (EERE)

846a-4cdf-8321-8b488ae9cadf 846a-4cdf-8321-8b488ae9cadf No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Village of Mt Horeb, Wisconsin (Utility Company) Effective date: 2009/04/01 End date if known: Rate name: Cp-2 Large Power Time-of-Day Service Transformer Ownership Discount with Parallel Generation(20kW or less) Sector: Industrial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0753 per kilowatt-hour.

235

Search for new physics in trilepton events and limits on the associated chargino-neutralino production at CDF  

E-Print Network (OSTI)

We perform a search for new physics using final states consisting of three leptons and a large imbalance in transverse momentum resulting from proton-antiproton collisions at 1.96 TeV center-of-mass energy. We use data corresponding to 5.8 fb-1 of integrated luminosity recorded by the CDF II detector at the Tevatron collider. Our main objective is to investigate possible new low-momentum (down to 5 GeV/c) multi-leptonic final states not investigated by LHC experiments. Relative to previous CDF analyses, we expand the geometric and kinematic coverage of electrons and muons and utilize tau leptons that decay hadronically. Inclusion of tau leptons is particularly important for supersymmetry (SUSY) searches. The results are consistent with standard-model predictions. By optimizing our event selection to increase sensitivity to the minimal supergravity (mSUGRA) SUSY model, we set limits on the associated production of chargino and neutralino, the SUSY partners of the electroweak gauge bosons. We exclude cross sections up to 0.1 pb and chargino masses up to 168 GeV/c^2 at 95% CL, for a suited set of mSUGRA parameters. We also exclude a region of the two-dimensional space of the masses of the neutralino and the supersymmetric partner of the tau lepton, not previously excluded at the Tevatron.

CDF Collaboration; T. Aaltonen; S. Amerio; D. Amidei; A. Anastassov; A. Annovi; J. Antos; G. Apollinari; J. A. Appel; T. Arisawa; A. Artikov; J. Asaadi; W. Ashmanskas; B. Auerbach; A. Aurisano; F. Azfar; W. Badgett; T. Bae; A. Barbaro-Galtieri; V. E. Barnes; B. A. Barnett; P. Barria; P. Bartos; M. Bauce; F. Bedeschi; S. Behari; G. Bellettini; J. Bellinger; D. Benjamin; A. Beretvas; A. Bhatti; K. R. Bland; B. Blumenfeld; A. Bocci; A. Bodek; D. Bortoletto; J. Boudreau; A. Boveia; L. Brigliadori; C. Bromberg; E. Brucken; J. Budagov; H. S. Budd; K. Burkett; G. Busetto; P. Bussey; P. Butti; A. Buzatu; A. Calamba; S. Camarda; M. Campanelli; F. Canelli; B. Carls; D. Carlsmith; R. Carosi; S. Carrillo; B. Casal; M. Casarsa; A. Castro; P. Catastini; D. Cauz; V. Cavaliere; M. Cavalli-Sforza; A. Cerri; L. Cerrito; Y. C. Chen; M. Chertok; G. Chiarelli; G. Chlachidze; K. Cho; D. Chokheli; A. Clark; C. Clarke; M. E. Convery; J. Conway; M. Corbo; M. Cordelli; C. A. Cox; D. J. Cox; M. Cremonesi; D. Cruz; J. Cuevas; R. Culbertson; N. d'Ascenzo; M. Datta; P. de Barbaro; L. Demortier; L. Marchese; M. Deninno; F. Devoto; M. D'Errico; A. Di Canto; B. Di Ruzza; J. R. Dittmann; M. D'Onofrio; S. Donati; M. Dorigo; A. Driutti; K. Ebina; R. Edgar; A. Elagin; R. Erbacher; S. Errede; B. Esham; S. Farrington; J. P. Fernndez Ramos; R. Field; G. Flanagan; R. Forrest; M. Franklin; J. C. Freeman; H. Frisch; Y. Funakoshi; C. Galloni; A. F. Garfinkel; P. Garosi; H. Gerberich; E. Gerchtein; S. Giagu; V. Giakoumopoulou; K. Gibson; C. M. Ginsburg; N. Giokaris; P. Giromini; G. Giurgiu; V. Glagolev; D. Glenzinski; M. Gold; D. Goldin; A. Golossanov; G. Gomez; G. Gomez-Ceballos; M. Goncharov; O. Gonzlez Lpez; I. Gorelov; A. T. Goshaw; K. Goulianos; E. Gramellini; S. Grinstein; C. Grosso-Pilcher; R. C. Group; J. Guimaraes da Costa; S. R. Hahn; J. Y. Han; F. Happacher; K. Hara; M. Hare; R. F. Harr; T. Harrington-Taber; K. Hatakeyama; C. Hays; J. Heinrich; M. Herndon; A. Hocker; Z. Hong; W. Hopkins; S. Hou; R. E. Hughes; U. Husemann; M. Hussein; J. Huston; G. Introzzi; M. Iori; A. Ivanov; E. James; D. Jang; B. Jayatilaka; E. J. Jeon; S. Jindariani; M. Jones; K. K. Joo; S. Y. Jun; T. R. Junk; M. Kambeitz; T. Kamon; P. E. Karchin; A. Kasmi; Y. Kato; W. Ketchum; J. Keung; B. Kilminster; D. H. Kim; H. S. Kim; J. E. Kim; M. J. Kim; S. B. Kim; S. H. Kim; Y. K. Kim; Y. J. Kim; N. Kimura; M. Kirby; K. Knoepfel; K. Kondo; D. J. Kong; J. Konigsberg; A. V. Kotwal; M. Kreps; J. Kroll; M. Kruse; T. Kuhr; M. Kurata; A. T. Laasanen; S. Lammel; M. Lancaster; K. Lannon; G. Latino; H. S. Lee; J. S. Lee; S. Leo; S. Leone; J. D. Lewis; A. Limosani; E. Lipeles; A. Lister; H. Liu; Q. Liu; T. Liu; S. Lockwitz; A. Loginov; A. Luc; D. Lucchesi; J. Lueck; P. Lujan; P. Lukens; G. Lungu; J. Lys; R. Lysak; R. Madrak; P. Maestro; S. Malik; G. Manca; A. Manousakis-Katsikakis; F. Margaroli; P. Marino; M. Martnez; K. Matera; M. E. Mattson; A. Mazzacane; P. Mazzanti; R. McNulty; A. Mehta; P. Mehtala; C. Mesropian; T. Miao; D. Mietlicki; A. Mitra; H. Miyake; S. Moed; N. Moggi; C. S. Moon; R. Moore; M. J. Morello; A. Mukherjee; Th. Muller; P. Murat; M. Mussini; J. Nachtman; Y. Nagai; J. Naganoma; I. Nakano; A. Napier; J. Nett; C. Neu; T. Nigmanov; L. Nodulman; S. Y. Noh; O. Norniella; L. Oakes; S. H. Oh; Y. D. Oh; I. Oksuzian; T. Okusawa; R. Orava; L. Ortolan; C. Pagliarone; E. Palencia; P. Palni; V. Papadimitriou; W. Parker; G. Pauletta; M. Paulini; C. Paus; T. J. Phillips; G. Piacentino; E. Pianori; J. Pilot; K. Pitts; C. Plager; L. Pondrom; S. Poprocki; K. Potamianos; F. Prokoshin; A. Pranko; F. Ptohos; G. Punzi; N. Ranjan; I. Redondo Fernndez; P. Renton; M. Rescigno; F. Rimondi; L. Ristori; A. Robson; T. Rodriguez; S. Rolli; M. Ronzani; R. Roser; J. L. Rosner; F. Ruffini; A. Ruiz; J. Russ; V. Rusu; W. K. Sakumoto; Y. Sakurai; L. Santi; K. Sato; V. Saveliev; A. Savoy-Navarro; P. Schlabach; E. E. Schmidt; T. Schwarz; L. Scodellaro; F. Scuri; S. Seidel; Y. Seiya; A. Semenov; F. Sforza; S. Z. Shalhout; T. Shears; P. F. Shepard; M. Shimojima; M. Shochet; I. Shreyber-Tecker; A. Simonenko; K. Sliwa; J. R. Smith; F. D. Snider; V. Sorin; H. Song; M. Stancari; R. St. Denis; D. Stentz; J. Strologas; Y. Sudo; A. Sukhanov; I. Suslov; K. Takemasa; Y. Takeuchi; J. Tang; M. Tecchio; P. K. Teng; J. Thom; E. Thomson; V. Thukral; D. Toback; S. Tokar; K. Tollefson; T. Tomura; D. Tonelli; S. Torre; D. Torretta; P. Totaro; M. Trovato; F. Ukegawa; S. Uozumi; F. Vzquez; G. Velev; C. Vellidis; C. Vernieri; M. Vidal; R. Vilar; J. Vizn; M. Vogel; G. Volpi; P. Wagner; R. Wallny; S. M. Wang; D. Waters; W. C. Wester III; D. Whiteson; A. B. Wicklund; S. Wilbur; H. H. Williams; J. S. Wilson; P. Wilson; B. L. Winer; P. Wittich; S. Wolbers; H. Wolfe; T. Wright; X. Wu; Z. Wu; K. Yamamoto; D. Yamato; T. Yang; U. K. Yang; Y. C. Yang; W. -M. Yao; G. P. Yeh; K. Yi; J. Yoh; K. Yorita; T. Yoshida; G. B. Yu

2013-09-28T23:59:59.000Z

236

Data:60244d05-cdf2-4dfc-8985-9d436828c873 | Open Energy Information  

Open Energy Info (EERE)

4d05-cdf2-4dfc-8985-9d436828c873 4d05-cdf2-4dfc-8985-9d436828c873 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Maui Electric Co Ltd Effective date: 2013/07/01 End date if known: 2013/07/30 Rate name: Maui-SCHEDULE "Q" Purchases From Qualifying Facilities - 100 KW or Less - Single Phase Sector: Commercial Description: Availability: This schedule is available to customers with cogeneration and/or small power production facilities which qualify under the commission's Rules, Chapter 74 of Title 6, Subchapter 2 with a design capacity of 100 kilowatts or less. Such qualifying facilities (QF's) shall be designed to operate properly in parallel with the Company's system without adversely affecting the operations of its customers and without presenting safety hazards to the Company's or other customer's personnel. The customer shall comply with the Company's requirements for customer generation interconnected with the utility system.

237

Automated recovery of dataintensive jobs in D0 and CDF using SAM A. Baranovski* 1 , V. Bartsch 2 , D. Benjamin 4 , K. Genser 1  

E-Print Network (OSTI)

or at the remote computing facili­ ties. Both ways equally benefit from distributed SAM data handling services] is a data handling system that provides the Fer­ milab HEP experiments D0, CDF and MINOS with the means concerns to address in the SAM project. The SAM data handling and its interface have been used to de­ tect

238

Interface between the SAM data handling system and CDF experiment V. Bartsch 1 , A. Baranovski 2 , D. Benjamin 3 , K. Genser 2 , S. Hsu 3 ,  

E-Print Network (OSTI)

data handling because files which are already present at remote sites are analysed first. This howeverInterface between the SAM data handling system and CDF experiment software V. Bartsch 1 , A at Fermilab has recently changed its data handling system. The old data handling system called DFC (Data File

239

Study of the production of the sigma b*+- with the CDF detector at the Tevatron  

SciTech Connect

The composition of matter is a topic in which the man has been interested throughout History. Since the introduction of the atom by Democritus in the 5th century BC until the establishment of the Standard Model, our successful theory that contains our current knowledge on the matter and their interactions, it has come a long way trying to solve this fundamental question. The efforts of many of the greatest minds to perform crucial experiments and develop theoretical models have helped to get deeper insight into the origin of the matter. Today we know that indivisible atoms postulated by Democritus are no longer true, and they are actually composed of a nucleus made of protons and neutrons (nucleons) with orbiting electrons through electromagnetic interactions. Also the nucleons are not fundamental particles but are composed of more fundamental ones called quarks. According to the present state of our knowledge, matter is composed of two types of particles: quarks and leptons. Leptons are believed to be fundamental particles and can occur freely in nature. Quarks are also fundamental particles, and there are no free in nature, but are confined to form hadrons. The hadrons may consist of a quark and an antiquark (mesons) or three quarks or three antiquarks (baryons). These quarks and leptons interact through the exchange of particles called bosons. Figure 1.1 summary the elementary particles in the Standard Model. Despite its enormous success we know that the Standard Model is incomplete. Some of the issues left unresolved by the Standard Model are the mechanism for electroweak symmetry breaking, the mass spectrum of the Standard Model or that the Universe is much more matter than antimatter. That means that it should exist a more general theory which include the Standard Model as a valid approximation for low energy. This more general theory must give answers to the previous unresolved questions. Accumulate more experimental information is crucial to get a deeper understanding of the Standard Model and its limitations. In particular, it is very important the measurement of those observables which they are not able to be calculated from theory by perturbation theory. Particle accelerators have played and play nowadays a major role for past and new physics discoverements and has been for many years the source of many precision measurements. Unprecedent discoveries have been made and are yet to come. These measurements allow to select the models that best fit the results and also they can be used as input for those models to get further predictions. Tevatron has been for many years the highest energy particle collider operational in the world. It is located in the high energy physics laboratory Fermilab in Batavia, in the State of Illinois (USA). Tevatron produce proton-antiproton collisions with an energy of 1.96 TeV at the center of the mass. This thesis is based on the data taken by the CDF II detector, one of the two multipurpose detectors located in the two interaction points at Tevatron. In this thesis a precise measurement of the mass and width of four heavy baryon states are performed. These states are described together by the symbol {Sigma}{sub b}{sup (*){+-}}. They are built by two light quarks and one heavy b quark as it is shown in Fig. 1.2. Baryons containing one bottom quark and two light quarks are described by Heavy Quark Effective Theories (HQET).

Calancha Paredes, Constantino; /Madrid, CIEMAT /Madrid U.

2011-02-01T23:59:59.000Z

240

Measurement of W-Boson Polarization in Top-quark Decay using the Full CDF Run II Data Set  

E-Print Network (OSTI)

We measure the polarization of W bosons from top-quark (t) decays into final states with a charged lepton and jets, tt --> WbWb --> lvbqqb, using the full Run II data set collected by the CDF II detector. A model-independent method simultaneously determines the fraction of longitudinal (f_0) and right-handed (f_+) W bosons to yield f_0 = 0.726 +/- 0.066 (stat) +/- 0.067 (syst) and f_+ = -0.045 +/- 0.044 (stat) +/- 0.058 (syst) with a correlation coefficient of -0.69. Additional results are presented under various standard model assumptions. No significant discrepencies with the standard model are observed.

CDF Collaboration

2012-11-19T23:59:59.000Z

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


241

Combined search for the standard model Higgs boson decaying to a bb pair using the full CDF data set  

E-Print Network (OSTI)

We combine the results of searches for the standard model Higgs boson based on the full CDF Run II data set obtained from sqrt(s) = 1.96 TeV p-pbar collisions at the Fermilab Tevatron corresponding to an integrated luminosity of 9.45/fb. The searches are conducted for Higgs bosons that are produced in association with a W or Z boson, have masses in the range 90-150 GeV/c^2, and decay into bb pairs. An excess of data is present that is inconsistent with the background prediction at the level of 2.5 standard deviations (the most significant local excess is 2.7 standard deviations).

CDF Collaboration

2012-07-06T23:59:59.000Z

242

$W$ boson polarization measurement in the $t\\bar{t}$ dilepton channel using the CDF II Detector  

SciTech Connect

We present a measurement of W boson polarization in top-quark decays in t{bar t} events with decays to dilepton final states using 5.1 fb{sup -1} integrated luminosity in p{bar p} collisions collected by the CDF II detector at the Tevatron. A simultaneous measurement of the fractions of longitudinal (f{sub 0}) and right-handed (f{sub +}) W bosons yields the results f{sub 0} = 0.71{sub -0.17}{sup +0.18}(stat) {+-} 0.06(syst) and f{sub +} = -0.07 {+-} 0.09(stat) {+-} 0.03(syst). Combining this measurement with our previous result based on single lepton final states, we obtain f{sub 0} = 0.84 {+-} 0.09(stat) {+-} 0.05(syst) and f{sub +} = -0.16 {+-} 0.05(stat) {+-} 0.04(syst). The results are consistent with standard model expectation.

Aaltonen, T.; /Helsinki Inst. of Phys.; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U. /Fermilab; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Arisawa, T.; /Waseda U.; Artikov, A.; /Dubna, JINR /Texas A-M

2012-05-01T23:59:59.000Z

243

Inclusive Search for Standard Model Higgs Boson Production in the WW Decay Channel using the CDF II Detector  

E-Print Network (OSTI)

We present a search for standard model (SM) Higgs boson production using ppbar collision data at sqrt(s) = 1.96 TeV, collected with the CDF II detector and corresponding to an integrated luminosity of 4.8 fb-1. We search for Higgs bosons produced in all processes with a significant production rate and decaying to two W bosons. We find no evidence for SM Higgs boson production and place upper limits at the 95% confidence level on the SM production cross section (sigma(H)) for values of the Higgs boson mass (m_H) in the range from 110 to 200 GeV. These limits are the most stringent for m_H > 130 GeV and are 1.29 above the predicted value of sigma(H) for mH = 165 GeV.

The CDF Collaboration; T. Aaltonen

2010-01-25T23:59:59.000Z

244

Search for the Higgs boson in the all-hadronic final state using the CDF II detector  

E-Print Network (OSTI)

We report on a search for the production of the Higgs boson decaying to two bottom quarks accompanied by two additional quarks. The data sample used corresponds to an integrated luminosity of approximately 4\\,\\invfb\\, of \\ppbar\\, collisions at $\\sqrt{s}=1.96$\\,TeV recorded by the CDF II experiment. This search includes twice the integrated luminosity of the previous published result, uses analysis techniques to distinguish jets originating from light flavor quarks and those from gluon radiation, and adds sensitivity to a Higgs boson produced by vector boson fusion. We find no evidence of the Higgs boson and place limits on the Higgs boson production cross section for Higgs boson masses between 100\\,\\gevcc\\, and 150\\,\\gevcc\\, at the 95% confidence level. For a Higgs boson mass of 120\\,\\gevcc\\, the observed (expected) limit is 10.5\\,(20.0) times the predicted Standard Model cross section.

CDF Collaboration

2011-01-31T23:59:59.000Z

245

Search for the Production of Gluinos and Squarks with the CDF II Experiment at the Tevatron Collider  

SciTech Connect

This thesis reports on two searches for the production of squarks and gluinos, supersymmetric partners of the Standard Model (SM) quarks and gluons, using the CDF detector at the Tevatron {radical}s = 1.96 TeV p{bar p} collider. An inclusive search for squarks and gluinos pair production is performed in events with large E{sub T} and multiple jets in the final state, based on 2 fb{sup -1} of CDF Run II data. The analysis is performed within the framework of minimal supergravity (mSUGRA) and assumes R-parity conservation where sparticles are produced in pairs. The expected signal is characterized by the production of multiple jets of hadrons from the cascade decays of squarks and gluinos and large missing transverse energy E{sub T} from the lightest supersymmetric particles (LSP). The measurements are in good agreement with SM predictions for backgrounds. The results are translated into 95% confidence level (CL) upper limits on production cross sections and squark and gluino masses in a given mSUGRA scenario. An upper limit on the production cross section is placed in the range between 1 pb and 0.1 pb, depending on the gluino and squark masses considered. The result of the search is negative for gluino and squark masses up to 392 GeV/c{sup 2} in the region where gluino and squark masses are close to each other, gluino masses up to 280 GeV/c{sup 2} regardless of the squark mass, and gluino masses up to 423 GeV=c2 for squark masses below 378 GeV/c{sup 2}. These results are compatible with the latest limits on squark/gluino production obtained by the D0 Collaboration and considerably improve the previous exclusion limits from direct and indirect searches at LEP and the Tevatron. The inclusive search is then extended to a scenario where the pair production of sbottom squarks is dominant. The new search is performed in a generic MSSM scenario with R-parity conservation. A specific SUSY particle mass hierarchy is assumed such that the sbottom decays exclusively as {tilde b}{sub 1} {yields} b{sub {tilde {chi}}{sub 1}{sup 0}}. The expected signal for direct sbottom pair production is characterized by the presence of two jets of hadrons from the hadronization of the bottom quarks and E=T from the two LSPs in the final state. The events are selected with large E{sub T} and two energetic jets in the final state, and at least one jet is required to be associated with a b quark. The measurements are in good agreement with SM predictions for backgrounds. The results are translated into 95% CL exclusion limits on production cross sections and sbottom and neutralino masses in the given MSSM scenario. Cross sections down to 0.1 pb are excluded for the sbottom mass range considered. Sbottom masses up to 230 GeV/c{sup 2} are excluded at 95% CL for neutralino masses below 70 GeV/c{sup 2}. This analysis increases the previous CDF limit by more than 40 GeV/c{sup 2}. The sensitivity of both the inclusive and the exclusive search is dominated by systematic effects and the results of the two analyses can be considered as conclusive for CDF Run II. With the new energy frontier of the newly commissioned Large Hadron Collider in Geneva, the experience from Tevatron will be of crucial importance in the developing of effective strategies to search for SUSY in the next era of particle physics experiments.

De Lorenzo, Gianluca; /Barcelona, IFAE

2010-05-01T23:59:59.000Z

246

Measurement of the Top-Quark Mass in All-Hadronic Decays in p pbar Collisions at CDF II  

E-Print Network (OSTI)

We present a measurement of the top-quark mass, $M_{\\mathrm{top}}$, in the all-hadronic decay channel $t\\bar{t} \\to W^+b W^- \\bar{b} \\to q_1\\bar{q}_2 b q_3 \\bar{q}_4 \\bar{b}$. The analysis is performed using 310 pb$^{-1}$ of $\\sqrt{s}$=1.96 TeV $p\\bar{p}$ collisions collected with the CDF II detector using a multi-jet trigger. The mass measurement is based on an event-by-event likelihood which depends on both the sample purity and the value of the top-quark mass, using 90 possible jet-to-parton assignments in the six-jet final state. The joint likelihood of 290 selected events yields a value of $M_{\\mathrm{top}}$=177.1 $\\pm$ 4.9 (stat.) $\\pm$ 4.7 (syst.) GeV/$c^2$.

T. Aaltonen

2006-12-12T23:59:59.000Z

247

Measurement of the Top Quark Mass at CDF Using the Template Method in the Lepton + Jets Channel  

SciTech Connect

A measurement of the top quark mass in p{bar p} collisions at {radical}s = 1.96 TeV is presented. The analysis uses a template method, in which the overconstrained kinematics of the Lepton+Jets channel of the t{bar t} system are used to measure a single quantity, the reconstructed top quark mass, that is strongly correlated with the true top quark mass. in addition, the dijet mass of the hadronically decaying W boson is used to constrain in situ the uncertain jet energy scale in the CDF detector. Two-dimensional probability density functions are derived using a kernel density estimate-based machinery. Using 1.9 fb{sup -1} of data, the top quark mass is measured to be 171.8{sub -1.9}{sup +1.9}(stat.) {+-} 1.0(syst.)GeV/c{sup 2}.

Adelman, Jahred A.; /Chicago U.

2008-05-01T23:59:59.000Z

248

Search for standard model Higgs boson production in association with a W boson using a matrix element technique at CDF in pp? collisions at ?s=1.96??TeV  

E-Print Network (OSTI)

This paper presents a search for standard model Higgs boson production in association with a W boson using events recorded by the CDF experiment in a data set corresponding to an integrated luminosity of 5.6??fb[superscript ...

Gomez-Ceballos, Guillelmo

249

Data:B371dca1-cdf8-45e8-9322-efac7a0b58e6 | Open Energy Information  

Open Energy Info (EERE)

1dca1-cdf8-45e8-9322-efac7a0b58e6 1dca1-cdf8-45e8-9322-efac7a0b58e6 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Nebraska Public Power District Effective date: 2013/01/01 End date if known: Rate name: Area Lighting MV 250 W Metered 722 Sector: Lighting Description: To area lighting of farmyards, backyards, patios, parking lots, storage yards, trailer courts, industrial sites, schools, churches, apartments, businesses, and many other applications where lighting is needed for identification, merchandising, environment, aesthetics, safety, protection, or convenience. Equipment Rental Charge means the district will install, own, operate, and maintain the lighting equipment.

250

Data:Cdf00df9-f526-48ce-a99f-9022156ab935 | Open Energy Information  

Open Energy Info (EERE)

Cdf00df9-f526-48ce-a99f-9022156ab935 Cdf00df9-f526-48ce-a99f-9022156ab935 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: El Paso Electric Co Effective date: 2012/05/01 End date if known: Rate name: 250W HPSV 27500 lumen - floodlight on existing wood pole Sector: Lighting Description: This rate is available to customers who desire overhead outdoor lighting service under the conditions specified herein. Source or reference: http://www.epelectric.com/files/html/Rates/TX_Tariff_Schedules/TX_Sch_No._28_Area_Lighting.pdf Source Parent: Comments The rate is subject to the Military Base Discount Recovery Factor adjustments (only applicable to military organizations).

251

Data:6cdf94d5-d609-4140-af6a-fd3cb32bce38 | Open Energy Information  

Open Energy Info (EERE)

cdf94d5-d609-4140-af6a-fd3cb32bce38 cdf94d5-d609-4140-af6a-fd3cb32bce38 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Harmon Electric Assn Inc Effective date: 2008/10/01 End date if known: Rate name: 100 Watt HPS Sector: Lighting Description: * Available to all customers for illumination of outdoor areas at any point on or near the Association's distribution lines. The cost of purchased power adjustment will be computed using 70kWh per light per month. Source or reference: Rate binder # 4 Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh)

252

Data:A48bff6d-efe4-4086-a37c-df737516de87 | Open Energy Information  

Open Energy Info (EERE)

bff6d-efe4-4086-a37c-df737516de87 bff6d-efe4-4086-a37c-df737516de87 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Delaware Electric Cooperative Effective date: 2011/02/01 End date if known: Rate name: Lighting Service--Schedule L-1 HP Sodium Vapor Lamp-Post Top Luminaire (100w) RSL 10" Sector: Lighting Description: Available to Members, governments, agencies, public and private organizations desiring Electric Delivery or Electric Supply and Delivery Services through unmetered services for roadway and area lighting. Source or reference: http://www.delaware.coop/my-services/residential/billing/rates

253

Data:4c459d43-3f52-44c4-bef8-ade076cdf621 | Open Energy Information  

Open Energy Info (EERE)

3-3f52-44c4-bef8-ade076cdf621 3-3f52-44c4-bef8-ade076cdf621 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Broad River Electric Coop, Inc Effective date: 2012/07/01 End date if known: Rate name: Schedule L2, Carrige, 1 Light Per 6 Sector: Lighting Description: * Applicable to any consumers of the Cooperative receiving service under rate schedules 10,20,and 80. Subdivision street lighting must be any BREC decorative special (B) 100-Watt HPS or 175-watt MV fixture. Subject to sales tax. Source or reference: Rate binder # 4(Illinios State University) Source Parent: Comments Applicability Demand (kW)

254

Data:3c461b87-cdf8-4a2c-afbe-0021e556ef3c | Open Energy Information  

Open Energy Info (EERE)

c461b87-cdf8-4a2c-afbe-0021e556ef3c c461b87-cdf8-4a2c-afbe-0021e556ef3c No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Schuyler, Nebraska (Utility Company) Effective date: 2013/01/01 End date if known: Rate name: Irrigation Service- No Control (Less than 10 Hp) Sector: Commercial Description: The irrigation season is generally seven months, between March 15 and October 14. The Department of Utilities may disconnect the transformers between October 15 and March 14 to reduce power loss. At locations where the Department has provided facilities for irrigation service, the Customer may use the

255

Data:01960cdf-5324-466a-b6be-b30615ad18c2 | Open Energy Information  

Open Energy Info (EERE)

cdf-5324-466a-b6be-b30615ad18c2 cdf-5324-466a-b6be-b30615ad18c2 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Broad River Electric Coop, Inc Effective date: 2012/07/01 End date if known: Rate name: Rate Code 60,100 Watt Sector: Lighting Description: * All-night outdoor lighting service using overhead conductors and Cooperative standard package bracket mounted luminaries on 30 foot,Class 7, wood poles. Subject to sales tax . Source or reference: Rate binder # 4(Illinios State University) Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh)

256

Data:3d277e87-54df-4115-b50f-859cdf6eaaa7 | Open Energy Information  

Open Energy Info (EERE)

7e87-54df-4115-b50f-859cdf6eaaa7 7e87-54df-4115-b50f-859cdf6eaaa7 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Sulphur Springs Valley E C Inc Effective date: 2013/03/18 End date if known: Rate name: Street Lighting: 100 Watt HPS - Single/Wood Sector: Lighting Description: Customer provided Facilities and Cooperative Owned and Maintained Lighting Service. Source or reference: http://www.ssvec.org/wp-content/uploads/downloads/2013/03/SSVEC-Rates-03.18.13.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh):

257

Data:287d7eda-44e8-44ad-b5f8-6c6595a57cdf | Open Energy Information  

Open Energy Info (EERE)

44e8-44ad-b5f8-6c6595a57cdf 44e8-44ad-b5f8-6c6595a57cdf No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Public Service Co of Colorado Effective date: 2012/07/01 End date if known: Rate name: COMMERCIAL OUTDOOR AREA LIGHTING SERVICE - SCHEDULE CAL - 250w Sector: Lighting Description: Applicable within all territory served for outdoor area lighting of customer's property where such service can be provided directly from existing secondary distribution lines of the Company. Not applicable for lighting of public streets or highways. This rate schedule is subject to all applicable Electric Rate Adjustments as on file and in effect in this tariff.

258

Data:Fe881325-eb71-45ad-a4cd-f2fe3c28f436 | Open Energy Information  

Open Energy Info (EERE)

325-eb71-45ad-a4cd-f2fe3c28f436 325-eb71-45ad-a4cd-f2fe3c28f436 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Orange County Rural E M C Effective date: 2012/01/01 End date if known: Rate name: Rate 101- 2012 Rate Schedule for Standard Service Sector: Residential Description: Wholesale Power Cost Tracker changes quarterly. Available to any member of the REMC located on its lines for standard service whose installed capacity does not exceed 50KVA. Source or reference: http://www.orangecountyremc.org/electricrates.html Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):

259

Data:310e1cdf-d331-4b4a-a73b-d53772076220 | Open Energy Information  

Open Energy Info (EERE)

cdf-d331-4b4a-a73b-d53772076220 cdf-d331-4b4a-a73b-d53772076220 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Groton, South Dakota (Utility Company) Effective date: End date if known: Rate name: Schedule B - Interruptible Power (House meter) (Dual Heat & Heat Storage Units) Rates Sector: Residential Description: Schedule B - Interruptible Power (Dual Heat & Heat Storage Units) Rates #1 House Meter - Above Rate Schedule A Source or reference: http://city.grotonsd.gov/electric.html Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh)

260

Data:7e822ac8-cdf1-4fca-81c5-63426a4fc983 | Open Energy Information  

Open Energy Info (EERE)

ac8-cdf1-4fca-81c5-63426a4fc983 ac8-cdf1-4fca-81c5-63426a4fc983 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Groton Dept of Utilities Effective date: 2008/10/01 End date if known: Rate name: Street and Area Lighting Service(250 W Floodlight-HPS)-Overhead Sector: Commercial Description: pplicable to public or private customers for standard street and area lighting installations provided and maintained by the Department to render 4,000 annual hours of lighting. Overhead installation is a light fixture attached to an existing overhead distribution system pole. Underground installation is a light fixture attached to a new pole served from an existing underground distribution system.

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


261

Data:6eb38ab5-ce1e-4573-98c5-08286cdf6473 | Open Energy Information  

Open Energy Info (EERE)

8ab5-ce1e-4573-98c5-08286cdf6473 8ab5-ce1e-4573-98c5-08286cdf6473 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Mankato, Kansas (Utility Company) Effective date: 2008/01/13 End date if known: Rate name: Commercial- Meter Horsepower option(Over 200kwh) Sector: Commercial Description: All territory served by the city for electric service supplied to one customer conducting a gainful enterprise through one meter, and whose usage is less than 150,000kWh per year. Source or reference: Rates Binder A Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months):

262

Data:60d45368-cdf0-4eb6-b62d-4a3175069a10 | Open Energy Information  

Open Energy Info (EERE)

8-cdf0-4eb6-b62d-4a3175069a10 8-cdf0-4eb6-b62d-4a3175069a10 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Louisville Electric System Effective date: 2012/11/01 End date if known: Rate name: Lighting- 200W HPS Sector: Lighting Description: Source or reference: ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous 1 2 3 Next >> Seasonal/Monthly Demand Charge Structures

263

Data:3253e4af-ccbd-4b70-a894-4cdf54cc19de | Open Energy Information  

Open Energy Info (EERE)

af-ccbd-4b70-a894-4cdf54cc19de af-ccbd-4b70-a894-4cdf54cc19de No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Indiana Michigan Power Co (Michigan) Effective date: 2013/01/01 End date if known: Rate name: ECLS - 70 Watt HPS Sector: Lighting Description: Energy Conversation Lighting Service Available for streetlighting service to municipalities, counties, and other governmental subdivisions. This rate is applicable for service that is supplied through new or rebuilt streetlight systems, including extension of streetlighting systems to additional locations where service is requested by customer.

264

Combined CDF and D0 Searches for the Standard Model Higgs Boson Decaying to Two Photons with up to 8.2 fb^-1  

E-Print Network (OSTI)

We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in ppbar collisions at the Fermilab Tevatron at sqrt{s}=1.96 TeV, focusing on the decay H\\rightarrow\\gamma\\gamma. We compute upper limits on the Higgs boson production cross section times the decay branching fraction in the range 100Higgs boson. With datasets corresponding to 7.0 fb-1 (CDF) and 8.2 fb-1 (D0), the 95% C.L. upper limits on Higgs boson production is a factor of 10.5 times the SM cross section for a Higgs boson mass of 115 GeV/c^2.

Physics, the Tevatron New

2011-01-01T23:59:59.000Z

265

Combined CDF and D0 Searches for the Standard Model Higgs Boson Decaying to Two Photons with up to 8.2 fb^-1  

Science Conference Proceedings (OSTI)

We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV, focusing on the decay H {yields} {gamma}{gamma}. We compute upper limits on the Higgs boson production cross section times the decay branching fraction in the range 100 Higgs boson. With datasets corresponding to 7.0 fb{sup -1} (CDF) and 8.2 fb{sup -1} (D0), the 95% C.L. upper limits on Higgs boson production is a factor of 10.5 times the SM cross section for a Higgs boson mass of 115 GeV/c{sup 2}.

Not Available

2011-07-01T23:59:59.000Z

266

Combined CDF and D0 Searches for the Standard Model Higgs Boson Decaying to Two Photons with up to 8.2 fb^-1  

E-Print Network (OSTI)

We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in ppbar collisions at the Fermilab Tevatron at sqrt{s}=1.96 TeV, focusing on the decay H\\rightarrow\\gamma\\gamma. We compute upper limits on the Higgs boson production cross section times the decay branching fraction in the range 100Higgs boson. With datasets corresponding to 7.0 fb-1 (CDF) and 8.2 fb-1 (D0), the 95% C.L. upper limits on Higgs boson production is a factor of 10.5 times the SM cross section for a Higgs boson mass of 115 GeV/c^2.

The CDF Collaboration; the D0 Collaboration; the Tevatron New Physics; Higgs Working Group

2011-07-25T23:59:59.000Z

267

Data:0712890b-d074-47a7-ae2f-5252cdf28ec1 | Open Energy Information  

Open Energy Info (EERE)

b-d074-47a7-ae2f-5252cdf28ec1 b-d074-47a7-ae2f-5252cdf28ec1 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Lincoln Electric Coop, Inc Effective date: 2012/03/19 End date if known: Rate name: Area Lighting - 1000 Watt MV Sector: Lighting Description: Source or reference: http://www.lincolnelectric.coop/PDF/schedule-hsecuritylightservice.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous

268

Data:Cd725df4-9c89-4cdf-a138-aaa1e0952ed6 | Open Energy Information  

Open Energy Info (EERE)

25df4-9c89-4cdf-a138-aaa1e0952ed6 25df4-9c89-4cdf-a138-aaa1e0952ed6 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Cleveland, Tennessee (Utility Company) Effective date: 2011/04/01 End date if known: Rate name: residential rate-- schedule RS(Hydro Allocation Credit) Sector: Residential Description: Hydro Allocation credit: $1.60 per month The reported energy charges shall be decreased or increased in accordance with the current Adjustment Addendum published by TVA. Source or reference: http://www.clevelandutilities.com/PDF/2011JulyElectricRates.pdf Source Parent: Comments Applicability

269

Data:5ba1930f-20ff-4e2d-88ff-cdf31599c2c5 | Open Energy Information  

Open Energy Info (EERE)

930f-20ff-4e2d-88ff-cdf31599c2c5 930f-20ff-4e2d-88ff-cdf31599c2c5 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Northern Rio Arriba E Coop Inc Effective date: 2013/05/20 End date if known: Rate name: Residential Time of Use-14 (PRC Rate No. 14) Sector: Residential Description: Source or reference: http://www.noraelectric.org/rates/rates.cfm Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous

270

Data:B8b43aa2-41ee-4c93-9454-6a07cdf09741 | Open Energy Information  

Open Energy Info (EERE)

aa2-41ee-4c93-9454-6a07cdf09741 aa2-41ee-4c93-9454-6a07cdf09741 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City Utilities of Springfield Effective date: 2011/10/01 End date if known: Rate name: Dual Electric Feed second source from same substation Sector: Description: Under this Rider A, City Utilities will provide the customer with electric service from a second independent source. The second source can be either from a second feeder of the same substation or from a feeder of a different substation, however, the first and second source must have a common metering point with one meter. Line construction, if any, is subject to the Extension Policy.

271

Data:Bca02fd5-855d-495d-9fb7-91f0cdf37c63 | Open Energy Information  

Open Energy Info (EERE)

Bca02fd5-855d-495d-9fb7-91f0cdf37c63 Bca02fd5-855d-495d-9fb7-91f0cdf37c63 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Russell, Massachusetts (Utility Company) Effective date: 2009/01/01 End date if known: Rate name: RESIDENTIAL SERVICE SCHEDULE R1 Sector: Residential Description: Additional Info: Availability: To residential customers for all domestic uses in individual residences or apartments. Minimum Bill: $5.00. Flat rate buy = Distribution + Transmission + Generation. Flat rate Adjustment = TAC + ECS + PPA. Source or reference: http://www.townofrussell.us/ElectricRates.html

272

Top-quark mass measurement in events with jets and missing transverse energy using the full CDF data set  

E-Print Network (OSTI)

We present a measurement of the top-quark mass using the full data set of Tevatron $\\sqrt{s} = 1.96$ TeV proton-antiproton collisions recorded by the CDF II detector, corresponding to an integrated luminosity of \\invfb{8.7}. The analysis uses events with one semileptonic $t$ or $\\bar{t}$ decay, but without detection of the electron or muon. We select events with significant missing transverse energy and multiple jets. We veto events containing identified electrons or muons. We obtain distributions of the top-quark masses and the invariant mass of the two jets from $W$-boson decays from data and compare these to templates derived from signal and background samples to extract the top-quark mass and the energy scale of the calorimeter jets with {\\it in situ} calibration. A likelihood fit of the templates from signal and background events to the data yields the top-quark mass, $\\mtop = \\gevcc{\\measStatSyst{173.93}{1.64}{0.87}}$. This result is the most precise measurement to date of the mass of the top quark in this event topology.

CDF Collaboration

2013-05-15T23:59:59.000Z

273

Search for the Higgs boson in the all-hadronic final state using the CDF II detector  

E-Print Network (OSTI)

We report on a search for the production of the Higgs boson decaying to two bottom quarks accompanied by two additional quarks. The data sample used corresponds to an integrated luminosity of approximately 4 fb${-1}$ of $p\\bar{p}$ collisions at \\surd s = 1.96 TeV recorded by the CDF II experiment. This search includes twice the data of the previous published result, uses new analysis techniques to distinguish jets originating from light flavor quarks and those from gluon radiation, and adds sensitivity to a Higgs boson produced by vector boson fusion. We find no evidence of the Higgs boson and place limits on the Higgs boson production cross-section for Higgs boson masses between 100 GeV/c$^{2}$ and 150 GeV/c$^{2}$ at 95% confidence level. For a Higgs boson mass of 120 GeV/c$^{2}$ the observed (expected) limit is 10.5 (20.0) times the predicted Standard Model cross-section.

Aaltonen, T

2011-01-01T23:59:59.000Z

274

Search for Third Generation Squarks in the Missing Transverse Energy plus Jet Sample at CDF Run II  

Science Conference Proceedings (OSTI)

The twentieth century leaves behind one of the most impressive legacies, in terms of human knowledge, ever achieved. In particular the StandardModel (SM) of particle physics has proven to be one of the most accurate descriptions of Nature. The level of accuracy of some theoretical predictions has never been attained before. It includes the electromagnetic interaction, and the weak and strong force, developing the Lagrangian from symmetry principles. There are two different types of fundamental constituents of Nature, in the framework of the Standard Model: bosons and fermions. Bosons are those particles responsible for carrying the interactions among the fermions, which constitute matter. Fermions are divide into six quarks and six leptons, forming a three-folded structure. All these fermions and bosons have an antimatter partner. However, several difficulties point along with the idea that the Standard Model is only an effective low energy theory. These limitations include the difficulty to incorporate gravity and the lack of justification to fine tuning of some perturbative corrections. Moreover, some regions of the theory are not understood, like the mass spectrum of the Standard Model or the mechanism for electroweak symmetry breaking. Supersymmetry is a newer theoretical framework, thought to adress the problems found in the Standard Model, while preserving all its predictive power. It introduces a new symmetry that relates a new boson to each SM fermion and a new fermion to each SM boson. In this way, for every existing boson in the SM it must exist a fermionic super-partner (named with a sufix ino), and likewise, for every fermion a bosonic super-partner (named with a prefix s) must also exist. Moreover, another symmetry called R-parity is introduced to prevent baryon and lepton number violating interactions. If R-parity is conserved, super-particles can only be pair-produced and they cannot decay completely in SM particles. This implies the existence of a lightest SUSY particle (LSP) which would provide a candidate for cold dark matter, that account for 23% of the universe content, as strongly suggested by recent astrophysical data [1]. The Tevatron is a hadron collider operating at Fermilab, USA. This accelerator provides proton-antiproton (p{bar p}) collisions with a center of mass energy of {radical}s = 1.96 TeV. CDF and D0 are the detectors built to analyse the products of the collisions provided by the Tevatron. Both experiments have produced a very significant scientific output in the last few years, like the discovery of the top quark or the measurement of the B{sub s} mixing. The Tevatron experiments are also reaching sensitivity to the SM Higgs boson. The scientific program of CDF includes a broad spectrum on searches for physics signatures beyond the Standard Model. Tevatron is still the energy frontier, what means an unique opportunity to produce a discovery in physic beyond the Standard Model. The analyses presented in this thesis focus on the search for third generation squarks in the missing transverse energy plus jets final state. The production of sbottom ({tilde b}) and stop ({tilde t}) quarks could be highly enhanced at the Tevatron, giving the possibility of discovering new physics or limiting the parameter space available in the theory. No signal is found over the predicted Standard Model background in both searches. Instead, 95% confidence level limits are set on the production cross section, and then translated into the mass plane of the hypothetical particles. This thesis sketches the basic theory concepts of the Standard Model and the Minimal Supersymmetric Extension in Chapter 2. Chapter 3, describes the Tevatron and CDF. Based on the CDF subsystems information, Chapter 4 and 5 describe the analysis objet reconstruction and the heavy flavor tagging tools. The development of the analyses is shown in Chapter 6 and Chapter 7. Finally, Chapter 8 is devoted to discuss the results and conclusions of this work, and future prospects.

Vidal Marono, Miguel; /Madrid, CIEMAT /Madrid U.

2010-03-01T23:59:59.000Z

275

Experimental Study of W Z Intermediate Bosons Associated Production with the CDF Experiment at the Tevatron Collider  

Science Conference Proceedings (OSTI)

Studying WZ associated production at the Fermilab Tevatron Collider is of great importance for two main reasons. On the one hand, this process would be sensitive to anomalies in the triple gauge couplings such that any deviation from the value predicted by the Standard Model would be indicative of new physics. In addition, by choosing to focus on the final state where the Z boson decays to b{bar b} pairs, the event topology would be the same as expected for associated production of a W and a Standard Model light Higgs boson (m{sub H} {approx}< 135 GeV) which decays into b{bar b} pairs most of times. The process WH {yields} W b{bar b} has an expected {sigma} {center_dot} B about five times lower than WZ {yields} Wb{bar b} for m{sub H} {approx_equal} 120 GeV. Therefore, observing this process would be a benchmark for an even more difficult search aiming at discovering the light Higgs in the WH {yields} Wb{bar b} process. After so many years of Tevatron operation only a weak WZ signal was recently observed in the full leptonic decay channel, which suffers from much less competition from background. Searching for the Z in the b{bar b} decay channel in this process is clearly a very challenging endeavour. In the work described in this thesis, WZ production is searched for in a final state where the W decays leptonically to an electron-neutrino pair or a muon-neutrino pair, with associated production of a jet pair consistent with Z decays. A set of candidate events is obtained by applying appropriate cuts to the parameters of events collected by wide acceptance leptonic triggers. To improve the signal fraction of the selected events, an algorithm was used to tag b-flavored jets by means of their content of long lived b-hadrons and corrections were developed to the jet algorithm to improve the b-jet energy resolution for a better reconstruction of the Z mass. In order to sense the presence of a signal one needs to estimate the amount of background. The relative content of heavy flavor jets in the dominant W+multijet background is assumed as predicted by theory. This technique was originally developed in CDF to measure the t{bar t} production cross section in the final state with W + 3 or more jets. This thesis was conceived as the first attempt within CDF to apply a customized version of it to look for evidence of diboson production in the final state with aW and two jets. Extracting the signal in this channel is very hard since with such a small number of jets the background is two orders of magnitude greater than the signal. Moreover, since the signal to background ratio is very small, the expected sensitivity depends critically on the theoretical uncertainties on the amount of background. While work is in progress to understand this background more reliably, this analysis provides an estimate of the achievable upper limit on the WZ production cross section.

Pozzobon, Nicola; /Pisa U.

2007-09-01T23:59:59.000Z

276

Search for MSSM Higgs decaying to tau pairs in ppbar collision at s**(1/2) = 1.96 TeV at CDF  

SciTech Connect

This thesis presents the search for neutral Minimal Supersymmetric extension of Standard Model (MSSM) Higgs bosons decaying to tau pairs where one of the taus decays leptonically, and the other one hadronically. CDF Run II data with L{sub int} = 310 pb{sup -1} are used. There is no evidence of MSSM Higgs existence, which results in the upper limits on {sigma}(p{bar p} {yields} {phi}) x BR({phi} {yields} {tau}{tau}) in m{sub A} range between 115 and 250 GeV. These limits exclude some area in tan {beta} vs m{sub A} parameter space.

Jang, Dongwook; /Rutgers U., Piscataway

2006-05-01T23:59:59.000Z

277

s042.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

I I (J P ) = 1 2 (0 - ) Quantum numbers not measured. Values shown are quark-model predictions. See also the B ± /B 0 ADMIXTURE and B ± /B 0 /B 0 s /b-baryon AD- MIXTURE sections. See the Note "Production and Decay of b-flavored Hadrons" at the beginning of the B ± Particle Listings and the Note on "B 0 -B 0 Mixing" near the end of the B 0 Particle Listings. B 0 MASS B 0 MASS B 0 MASS B 0 MASS The fit uses m B + , (m B 0 - m B + ), and m B 0 to determine m B + , m B 0 , and the mass difference. VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5279.50± 0.30 OUR FIT 5279.50± 0.30 OUR FIT 5279.50± 0.30 OUR FIT 5279.50± 0.30 OUR FIT 5279.5 ± 0.5 OUR AVERAGE 5279.5 ± 0.5 OUR AVERAGE 5279.5 ± 0.5 OUR AVERAGE 5279.5 ± 0.5 OUR AVERAGE 5279.63± 0.53 ± 0.33 1 ACOSTA 06 CDF p p at 1.96 TeV 5279.1 ± 0.7 ± 0.3 135 2 CSORNA 00 CLE2 e + e - → Υ(4S) 5281.3 ± 2.2 ± 1.4 51 ABE 96B CDF p p at 1.8 TeV * * * We do not use the following data for

278

s042.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

0 0 I (J P ) = 1 2 (0 - ) Quantum numbers not measured. Values shown are quark-model predictions. See also the B ± /B 0 ADMIXTURE and B ± /B 0 /B 0 s /b-baryon AD- MIXTURE sections. See the Note "Production and Decay of b-flavored Hadrons" at the beginning of the B ± Particle Listings and the Note on "B 0 -B 0 Mixing" near the end of the B 0 Particle Listings. B 0 MASS B 0 MASS B 0 MASS B 0 MASS The fit uses m B + , (m B 0 - m B + ), and m B 0 to determine m B + , m B 0 , and the mass difference. VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5279.50± 0.33 OUR FIT 5279.50± 0.33 OUR FIT 5279.50± 0.33 OUR FIT 5279.50± 0.33 OUR FIT 5279.5 ± 0.5 OUR AVERAGE 5279.5 ± 0.5 OUR AVERAGE 5279.5 ± 0.5 OUR AVERAGE 5279.5 ± 0.5 OUR AVERAGE 5279.63± 0.53 ± 0.33 1 ACOSTA 06 CDF p p at 1.96 TeV 5279.1 ± 0.7 ± 0.3 135 2 CSORNA 00 CLE2 e + e - → Υ(4S) 5281.3 ± 2.2 ± 1.4 51 ABE 96B CDF p p at 1.8 TeV * * * We do not use the following data for

279

s086.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

s s I (J P ) = 0(0 - ) I , J, P need confirmation. Quantum numbers shown are quark- model predictions. B 0 s MASS B 0 s MASS B 0 s MASS B 0 s MASS VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5366.77± 0.24 OUR FIT 5366.77± 0.24 OUR FIT 5366.77± 0.24 OUR FIT 5366.77± 0.24 OUR FIT 5366.7 ± 0.4 OUR AVERAGE 5366.7 ± 0.4 OUR AVERAGE 5366.7 ± 0.4 OUR AVERAGE 5366.7 ± 0.4 OUR AVERAGE Error includes scale factor of 1.3. See the ideogram below. 5366.90± 0.28± 0.23 1 AAIJ 12E LHCB p p at 7 TeV 5364.4 ± 1.3 ± 0.7 LOUVOT 09 BELL e + e - → Υ(5S) 5366.01± 0.73± 0.33 2 ACOSTA 06 CDF p p at 1.96 TeV 5369.9 ± 2.3 ± 1.3 32 3 ABE 96B CDF p p at 1.8 TeV 5374 ± 16 ± 2 3 ABREU 94D DLPH e + e - → Z 5359 ± 19 ± 7 1 3 AKERS 94J OPAL e + e - → Z 5368.6 ± 5.6 ± 1.5 2 BUSKULIC 93G ALEP e + e - → Z * * * We do not use the following data for averages, fits, limits, etc. * * * 5370 ± 1 ± 3 DRUTSKOY 07A BELL Repl. by LOUVOT 09 5370 ± 40 6 4 AKERS 94J OPAL e + e - → Z 5383.3

280

s041.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

3 3 Page 1 NODE=S041 B ± I (J P ) = 1 2 (0 - ) Quantum numbers not measured. Values shown are quark-model NODE=S041 predictions. See also the B ± /B 0 ADMIXTURE and B ± /B 0 /B 0 s /b-baryon AD- MIXTURE sections. B ± MASS B ± MASS B ± MASS B ± MASS NODE=S041M The fit uses m B + , (m B 0 - m B + ), and m B 0 to determine m B + , m B 0 , NODE=S041M and the mass difference. NODE=S041M VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5279.26 ± 0.17 OUR FIT 5279.26 ± 0.17 OUR FIT 5279.26 ± 0.17 OUR FIT 5279.26 ± 0.17 OUR FIT NEW [5279.25 ± 0.17 MeV OUR 2012 FIT] 5279.25 ± 0.26 OUR AVERAGE 5279.25 ± 0.26 OUR AVERAGE 5279.25 ± 0.26 OUR AVERAGE 5279.25 ± 0.26 OUR AVERAGE 5279.38 ± 0.11 ± 0.33 1 AAIJ 12E LHCB p p at 7 TeV 5279.10 ± 0.41 ± 0.36 2 ACOSTA 06 CDF p p at 1.96 TeV 5279.1 ± 0.4 ± 0.4 526 3 CSORNA 00 CLE2 e + e - → Υ(4S) 5279.1 ± 1.7 ± 1.4 147 ABE 96B CDF p p at 1.8 TeV * * * We do not use the following data for averages, fits, limits, etc.

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


281

s086.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

6 6 B 0 s I (J P ) = 0(0 - ) I , J, P need confirmation. Quantum numbers shown are quark- NODE=S086 model predictions. B 0 s MASS B 0 s MASS B 0 s MASS B 0 s MASS NODE=S086M NODE=S086M VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5366.77 ± 0.24 OUR FIT 5366.77 ± 0.24 OUR FIT 5366.77 ± 0.24 OUR FIT 5366.77 ± 0.24 OUR FIT 5366.7 ± 0.4 OUR AVERAGE 5366.7 ± 0.4 OUR AVERAGE 5366.7 ± 0.4 OUR AVERAGE 5366.7 ± 0.4 OUR AVERAGE Error includes scale factor of 1.3. See the ideogram below. 5366.90 ± 0.28 ± 0.23 1 AAIJ 12E LHCB p p at 7 TeV 5364.4 ± 1.3 ± 0.7 LOUVOT 09 BELL e + e - → Υ(5S) 5366.01 ± 0.73 ± 0.33 2 ACOSTA 06 CDF p p at 1.96 TeV 5369.9 ± 2.3 ± 1.3 32 3 ABE 96B CDF p p at 1.8 TeV 5374 ± 16 ± 2 3 ABREU 94D DLPH e + e - → Z 5359 ± 19 ± 7 1 3 AKERS 94J OPAL e + e - → Z 5368.6 ± 5.6 ± 1.5 2 BUSKULIC 93G ALEP e + e - → Z * * * We do not use the following data for averages, fits, limits, etc. * * * 5370 ± 1 ± 3 DRUTSKOY 07A BELL Repl. by LOUVOT 09 OCCUR=2

282

s041.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

± ± I (J P ) = 1 2 (0 - ) Quantum numbers not measured. Values shown are quark-model predictions. See also the B ± /B 0 ADMIXTURE and B ± /B 0 /B 0 s /b-baryon AD- MIXTURE sections. B ± MASS B ± MASS B ± MASS B ± MASS The fit uses m B + , (m B 0 - m B + ), and m B 0 to determine m B + , m B 0 , and the mass difference. VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5279.13± 0.31 OUR FIT 5279.13± 0.31 OUR FIT 5279.13± 0.31 OUR FIT 5279.13± 0.31 OUR FIT 5279.1 ± 0.4 OUR AVERAGE 5279.1 ± 0.4 OUR AVERAGE 5279.1 ± 0.4 OUR AVERAGE 5279.1 ± 0.4 OUR AVERAGE 5279.10± 0.41 ± 0.36 1 ACOSTA 06 CDF p p at 1.96 TeV 5279.1 ± 0.4 ± 0.4 526 2 CSORNA 00 CLE2 e + e - → Υ(4S) 5279.1 ± 1.7 ± 1.4 147 ABE 96B CDF p p at 1.8 TeV * * * We do not use the following data for averages, fits, limits, etc. * * * 5278.8 ± 0.54± 2.0 362 ALAM 94 CLE2 e + e - → Υ(4S) 5278.3 ± 0.4 ± 2.0 BORTOLETTO92 CLEO e + e - → Υ(4S) 5280.5 ± 1.0 ± 2.0 3 ALBRECHT 90J ARG e + e - → Υ(4S)

283

Data:Bba65cdf-29db-46e3-97b9-e4b9a711aa93 | Open Energy Information  

Open Energy Info (EERE)

Bba65cdf-29db-46e3-97b9-e4b9a711aa93 Bba65cdf-29db-46e3-97b9-e4b9a711aa93 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Piedmont Electric Member Corp Effective date: 2011/01/01 End date if known: Rate name: Small General Service Three Phase Sector: Commercial Description: AVAILABILITY: This Schedule is available in all territory served by the Cooperative, subject to the Cooperative's established Service Rules and Regulations and applicability stated herein. REPS MONTHLY RATE:In addition to all other charges stated in the Monthly Rate of the Schedule with which this Rider is used, the following charges shall also apply:Commercial $ 4.03 (INCLUDED IN THE FIXED MONTHLY CHARGE.)

284

Data:15e8aa65-850d-43a7-b064-3d9195aa7cdf | Open Energy Information  

Open Energy Info (EERE)

aa65-850d-43a7-b064-3d9195aa7cdf aa65-850d-43a7-b064-3d9195aa7cdf No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Public Service Co of NM Effective date: 2011/08/21 End date if known: Rate name: 1A Residential within Santa Fe Sector: Residential Description: The rates on this Schedule are available for single-family houses, individual farm units, individual apartments, or separate living quarters ordinarily designated and recognized as single-family living quarters for primarily domestic or home use. Service under this Schedule is not available for commercial rooming houses, multiple trailer parks, commercial, professional, or business establishments and the like, which shall be served under another applicable commercial Rate Schedule. All service shall be delivered at a single service location to be designated by the Company.

285

Measurement of the top-quark pair production cross-section in events with two leptons and bottom-quark jets using the full CDF data set  

E-Print Network (OSTI)

We present a measurement of the top-quark pair production cross-section in proton-antiproton collisions at $\\sqrt{s}$=1.96 TeV. The data were collected at the Fermilab Tevatron by the CDF II detector and correspond to an integrated luminosity of 8.8 fb$^{-1}$, representing the complete CDF Run II data set. We select events consistent with the production of top-quark pairs by requiring the presence of two reconstructed leptons, an imbalance in the total event transverse momentum, and jets. At least one jet is required to be identified as consistent with the fragmentation of a bottom quark using a secondary-vertex-finding algorithm. The 246 candidate events are estimated to have a signal purity of 91%. We measure a cross section of $\\sigma_{\\ttbar}$ = 7.09 $\\pm$ 0.84 pb, assuming a top-quark mass of 172.5 GeV/$c^{2}$. The results are consistent with the standard model as predicted by next-to-leading-order calculations.

CDF Collaboration

2013-04-30T23:59:59.000Z

286

Data:8ddac2a0-3c8e-4fb7-9ff4-44308cdf0d45 | Open Energy Information  

Open Energy Info (EERE)

ddac2a0-3c8e-4fb7-9ff4-44308cdf0d45 ddac2a0-3c8e-4fb7-9ff4-44308cdf0d45 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Escanaba, Michigan (Utility Company) Effective date: 2012/07/01 End date if known: Rate name: City Water Heating Energy Rate Commercial Sector: Commercial Description: To any customer for separately metered controlled water heating, subject to such wiring rules and regulations as are established by the utility. For as long as the City has costs associated with the ownership of the power plant, these costs shall be recovered through the following power plant cost adjustment factor:$0.01000 for all kWh, all service classes. State of Michigan P.A. 295, of Public Acts 2008, commonly referred to as the Clean, Renewable and Efficient Energy Act mandates the electric utility collect the following charges from each electric utility customer: Commercial $0.00200/kWh. The sum of these charges is reflected in adjustments to the energy charge.

287

Data:3b11cdf4-ffa2-4daa-9437-e7bf7087b14e | Open Energy Information  

Open Energy Info (EERE)

cdf4-ffa2-4daa-9437-e7bf7087b14e cdf4-ffa2-4daa-9437-e7bf7087b14e No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Oconto Falls Water & Light Comm Effective date: 2007/10/13 End date if known: Rate name: Ms-1 Street and Yard Lighting Service Overhead 150 W HPS Sector: Lighting Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0847 per kilowatt-hour.

288

Data:F532263c-df1d-44a9-aa8a-c997f3f8ebf4 | Open Energy Information  

Open Energy Info (EERE)

3c-df1d-44a9-aa8a-c997f3f8ebf4 3c-df1d-44a9-aa8a-c997f3f8ebf4 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Raton Public Service Company Effective date: End date if known: Rate name: Commercial- Three Phase Sector: Commercial Description: To all three phase commercial and all industrial customers in the RPS service area for lighting, heating, and power purposes. Source or reference: Rates Binder A Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

289

Data:Baae5be0-3b57-494c-8cdf-79c57d3de482 | Open Energy Information  

Open Energy Info (EERE)

Baae5be0-3b57-494c-8cdf-79c57d3de482 Baae5be0-3b57-494c-8cdf-79c57d3de482 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Minnesota Power Inc Effective date: 2013/01/01 End date if known: Rate name: RESIDENTIAL CONTROLLED ACCESS ELECTRIC SERVICE Sector: Residential Description: APPLICATION To electric service for residential customers for controlled energy storage or other loads which will be energized only for the time period between 11 p.m. and 7 a.m. daily. Service is subject to Company's Electric Service Regulations and any applicable riders. TYPE OF SERVICE Single phase, 60 hertz, voltages of 120 to 240 volts, supplied through one meter at one point of delivery.

290

Data:695c5a3c-df53-4f70-821d-bed84f9ea53b | Open Energy Information  

Open Energy Info (EERE)

c5a3c-df53-4f70-821d-bed84f9ea53b c5a3c-df53-4f70-821d-bed84f9ea53b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Athens Utility Board Effective date: 2011/04/01 End date if known: Rate name: General Power Rate-Schedule GSB Sector: Industrial Description: For customers having a peak demand greater than 5,000 kW and less than or equal to 15,000 kW. The Fuel Charge is .02356 Source or reference: http://www.aub.org/rate_power_ci.php Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage

291

Search for electroweak single top quark production with cdf in proton - anti-proton collisions at s**(1/2) = 1.96-TeV  

Science Conference Proceedings (OSTI)

In this thesis two searches for electroweak single top quark production with the CDF experiment have been presented, a cutbased search and an iterated discriminant analysis. Both searches find no significant evidence for electroweak single top production using a data set corresponding to an integrated luminosity of 162 pb{sup -1} collected with CDF. Therefore limits on s- and t-channel single top production are determined using a likelihood technique. For the cutbased search a likelihood function based on lepton charge times pseudorapidity of the non-bottom jet was used if exactly one bottom jet was identified in the event. In case of two identified bottom jets a likelihood function based on the total number of observed events was used. The systematic uncertainties have been treated in a Bayesian approach, all sources of systematic uncertainties have been integrated out. An improved signal modeling using the MadEvent Monte Carlo program matched to NLO calculations has been used. The obtained limits for the s- and t-channel single top production cross sections are 13.6 pb and 10.1 pb, respectively. To date, these are most stringent limits published for the s- and the t-channel single top quark production modes.

Walter, Thorsten; /Karlsruhe U., EKP

2005-06-01T23:59:59.000Z

292

Combined CDF and D0 Upper Limits on Standard Model Higgs Boson Production with up to 8.2 fb-1 of Data  

E-Print Network (OSTI)

We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in p-pbar collisions at the Fermilab Tevatron at sqrt(s)=1.96 TeV. The results presented here include those channels which are most sensitive to Higgs bosons with mass between 130 and 200 GeV/c^2, namely searches targeted at Higgs boson decays to W+W-, although acceptance for decays into tau+tau- and gamma gamma is included. Compared to the previous Tevatron Higgs search combination, more data have been added and the analyses have been improved to gain sensitivity. We use the MSTW08 parton distribution functions and the latest gg to H theoretical cross section predictions when testing for the presence of a SM Higgs boson. With up to 7.1 fb-1 of data analyzed at CDF, and up to 8.2 fb-1 at D0, the 95% C.L. upper limits on Higgs boson production is a factor of 0.54 times the SM cross section for a Higgs boson mass of 165 GeV/c^2. We exclude at the 95% C.L. the region 158

The CDF; D0 Collaborations; the TEVNPHWG Working Group

2011-03-16T23:59:59.000Z

293

Combined CDF and D0 Upper Limits on Standard Model Higgs Boson Production with up to 8.2 fb$^{-1}$ of Data  

Science Conference Proceedings (OSTI)

We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV. The results presented here include those channels which are most sensitive to Higgs bosons with mass between 130 and 200 GeV/c{sup 2}, namely searches targeted at Higgs boson decays to W{sup +}W{sup -}, although acceptance for decays into {tau}{sup |+} {tau}{sup -} and {gamma}{gamma} is included. Compared to the previous Tevatron Higgs search combination, more data have been added and the analyses have been improved to gain sensitivity. We use the MSTW08 parton distribution functions and the latest gg {yields} H theoretical cross section predictions when testing for the presence of a SM Higgs boson. With up to 7.1 fb{sup -1} of data analyzed at CDF, and up to 8.2 fb{sup -1} at D0, the 95% C.L. upper limits on Higgs boson production is a factor of 0.54 times the SM cross section for a Higgs boson mass of 165 GeV/c{sup 2}. We exclude at the 95% C.L. the region 158 < m{sub H} < 173 GeV/c{sup 2}.

Aaltonen, T.; Abazov, V.M.; Abbott, B.; Abolins, M.; Acharya, B.S.; Adams, M.; Adams, T.; Adelman, J.; Aguilo, E.; Alexeev, G.D.; Alkhazov, G.; /Helsinki Inst. of Phys. /Dubna, JINR /Oklahoma U. /Michigan State U. /Tata Inst. /Illinois U., Chicago /Florida State U. /Chicago U., EFI /Simon Fraser U. /York U., Canada /St. Petersburg, INP /Illinois U., Urbana /Sao Paulo, IFT /Munich U. /University Coll. London /Oxford U. /St. Petersburg, INP /Duke U. /Kyungpook Natl. U. /Chonnam Natl. U. /Florida U. /Osaka City U.

2011-03-01T23:59:59.000Z

294

Combined CDF and D0 Upper Limits on Standard Model Higgs-Boson Production with 2.1 - 5.4 fb-1 of Data  

SciTech Connect

We combine results from CDF and D0 on direct searches for a standard model (SM) Higgs boson (H) in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV. Compared to the previous Tevatron Higgs search combination more data have been added and some previously used channels have been reanalyzed to gain sensitivity. We use the latest parton distribution functions and gg {yields} H theoretical cross sections when comparing our limits to the SM predictions. With 2.0-4.8 fb{sup -1} of data analyzed at CDF, and 2.1-5.4 fb{sup -1} at D0, the 95% C.L. upper limits on Higgs boson production are a factor of 2.70 (0.94) times the SM cross section for a Higgs boson mass of m{sub H} = 115 (165) GeV/c{sup 2}. The corresponding median upper limits expected in the absence of Higgs boson production are 1.78 (0.89). The mass range excluded at 95% C.L. for a SM Higgs is 163 < m{sub H} < 166 GeV/c{sup 2}, with an expected exclusion of 159 < m{sub H} < 168 GeV/c{sup 2}.

Collaboration, The CDF; Collaboration, the D0; Physics, the Tevatron New; Group, Higgs Working

2009-11-01T23:59:59.000Z

295

Combined CDF and D0 Upper Limits on Standard Model Higgs-Boson Production with up to 6.7 fb$^{-1}$ of Data  

SciTech Connect

We combine results from CDF and D0 on direct searches for the standard model (SM) Higgs boson (H) in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV. Compared to the previous Tevatron Higgs search combination more data have been added, additional new channels have been incorporated, and some previously used channels have been reanalyzed to gain sensitivity. We use the latest parton distribution functions and gg {yields} H theoretical cross sections when comparing our limits to the SM predictions. With up to 5.9 fb{sup -1} of data analyzed at CDF, and up to 6.7 fb{sup -1} at D0, the 95% C.L. upper limits on Higgs boson production are factors of 1.56 and 0.68 the values of the SM cross section for a Higgs boson mass of m{sub H} = 115 GeV/c{sup 2} and 165 GeV/c{sup 2}. We exclude, at the 95% C.L., a new and larger region at high mass between 158 < m{sub H} < 175 GeV/c{sup 2}.

2010-07-01T23:59:59.000Z

296

Combined CDF and D0 Searches for the Standard Model Higgs Boson Decaying to Two Photons with up to 8.2 fb^-1  

SciTech Connect

We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV, focusing on the decay H {yields} {gamma}{gamma}. We compute upper limits on the Higgs boson production cross section times the decay branching fraction in the range 100 < m{sub H} < 150 GeV/c{sup 2}, and we interpret the results in the context of the standard model. We use the MSTW08 parton distribution functions and the latest theoretical cross section predictions when testing for the presence of a SM Higgs boson. With datasets corresponding to 7.0 fb{sup -1} (CDF) and 8.2 fb{sup -1} (D0), the 95% C.L. upper limits on Higgs boson production is a factor of 10.5 times the SM cross section for a Higgs boson mass of 115 GeV/c{sup 2}.

Not Available

2011-07-01T23:59:59.000Z

297

Data:1bc4cdf7-f06d-4886-b201-242a87e9c9c0 | Open Energy Information  

Open Energy Info (EERE)

bc4cdf7-f06d-4886-b201-242a87e9c9c0 bc4cdf7-f06d-4886-b201-242a87e9c9c0 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: PUD No 3 of Mason County Effective date: 2009/04/01 End date if known: Rate name: OH 100 Watt HPS (8,500 Lumen) Lamp METERED Sector: Lighting Description: Source or reference: http://www.masonpud3.org/rates/outdoorLights.aspx Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous

298

Data:Cdf138c6-8065-4fdd-bd88-d1e7aa4df658 | Open Energy Information  

Open Energy Info (EERE)

Cdf138c6-8065-4fdd-bd88-d1e7aa4df658 Cdf138c6-8065-4fdd-bd88-d1e7aa4df658 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Village of Muscoda, Wisconsin (Utility Company) Effective date: 2010/10/26 End date if known: Rate name: Rg-1 Residential Service Three Phase Sector: Residential Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0844 per kilowatt-hour.

299

Data:C8a5a188-e949-4cdf-87d1-b860d766f6ef | Open Energy Information  

Open Energy Info (EERE)

a5a188-e949-4cdf-87d1-b860d766f6ef a5a188-e949-4cdf-87d1-b860d766f6ef No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Hartford Electric Effective date: 2005/07/01 End date if known: Rate name: Cp-4 Large Industrial Power I Time-of-Day Service Primary Metering (transmission side of transformer) Discount Sector: Industrial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0452 per kilowatt-hour.

300

Search for the Standard Model Higgs Boson Decaying to a bb? Pair in Events with No Charged Leptons and Large Missing Transverse Energy using the Full CDF Data Set  

E-Print Network (OSTI)

We report on a search for the standard model Higgs boson produced in association with a vector boson in the full data set of proton-antiproton collisions at ?s=1.96??TeV recorded by the CDF II detector at the Tevatron, ...

Gomez-Ceballos, Guillelmo

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


301

e-mail:abe@kz.tsukuba.ac.jp) http://www.kz.tsukuba.ac.jp/~abe/  

E-Print Network (OSTI)

://unit.aist.go.jp/energy/index.htm (1) (2)(SOFC) (1) (http://unit.aist.go.jp/energy/energy-int/) (2)(SOFC) (http://unit.aist.go.jp/energy/groups/tfs.htm) (1) (2) () () (SOFC+GT) () () 70% 8090% f f cell F)/( U nQ V ?= 1.04 V () CH4+2H2O4H2+CO2 4H2+2O2 4H2O SOFC SOFC1kW 10,000 kWSOFC 50% SOFC (CH4+2H2O4H2+CO2) (4H2+2O2 4H2O) 2.5 20% 40 45

Tanaka, Jiro

302

Search for gluino and squark production in multi-jets plus missing transverse energy final states at the Tevatron using the CDF detector  

SciTech Connect

In this thesis, the results of the search for squarks and gluinos in multiple jets plus missing transverse energy final states have been presented. No evidence of these new particles have been found in 371 pb{sup -1} of CDF Run II data. New limits have been set which exclude gluino masses below 220 GeV and, in the region where M{sub {tilde g}} {approx} M{sub {tilde q}}, masses below 380 GeV/c{sup 2} are excluded. These limits are valid in a mSUGRA scenario with tan {beta} = 5, A = 0 and {mu} < 0 assuming the lightest four squark flavours degenerate in mass. To obtain these results a careful study of the beam conditions and their contribution to events with E{sub T} final states has been performed. Special attention has been taken in studying the different SM backgrounds and their normalizations at NLO. Dedicated cuts have been introduced to remove the background processes and main discriminating variables have been optimized for different signal regions. The different systematic uncertainties have also been considered. This is the first time that this search is performed at CDF Run II and the results presented here show significant improvements with respect to the constraints from previous experiments. Thus, this analysis has established the procedure to continue searching for squarks and gluinos with the new data samples that CDF is collecting from Tevatron. Some improvements may also be implemented by considering other hadron final states with different jet multiplicities. This could help extending the sensitivity of the analysis to regions where gluino and squark masses are not similar. At the forthcoming LHC, the search for squarks and gluinos in this inclusive channel constitutes one of the first analyses to be performed. The E{sub T} and multiple jets final states are present in multiple decay modes of many models beyond the SM. The experience from Tevatron in working on an hadron collider environment will be useful for these kind of studies aiming to discover the presence of supersymmetric processes.

Portell i Bueso, Xavier; /Barcelona, IFAE

2007-01-01T23:59:59.000Z

303

Data:45b9e743-233f-4ba6-a322-7cdf17e17827 | Open Energy Information  

Open Energy Info (EERE)

Data Data Edit with form History Facebook icon Twitter icon » Data:45b9e743-233f-4ba6-a322-7cdf17e17827 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Hertford, North Carolina (Utility Company) Effective date: 2009/02/01 End date if known: Rate name: Economic Development- Peak Demand Sector: Commercial Description: To new loads of commercial and industrial customers or new load expansions of existing industrial and commercial customers at least 200 kW annual peak demand. Demand Charges: All Coincident Peak: $19.49/kW All Excess Demand: $1.41/kW All rkVA of Demand: $0.18/rkVA

304

A Search for the Higgs Boson Produced in Association with $Z\\to \\ell^+\\ell^-$ Using the Matrix Element Method at CDF II  

E-Print Network (OSTI)

We present a search for associated production of the standard model (SM) Higgs boson and a $Z$ boson where the $Z$ boson decays to two leptons and the Higgs decays to a pair of $b$ quarks in $p\\bar{p}$ collisions at the Fermilab Tevatron. We use event probabilities based on SM matrix elements to construct a likelihood function of the Higgs content of the data sample. In a CDF data sample corresponding to an integrated luminosity of 2.7 fb$^{-1}$ we see no evidence of a Higgs boson with a mass between 100 GeV$/c^2$ and 150 GeV$/c^2$. We set 95% confidence level (C.L.) upper limits on the cross-section for $ZH$ production as a function of the Higgs boson mass $m_H$; the limit is 8.2 times the SM prediction at $m_H = 115$ GeV$/c^2$.

The CDF Collaboration; T. Aaltonen

2009-08-25T23:59:59.000Z

305

Search for the standard model Higgs boson decaying to a bb pair in events with two oppositely-charged leptons using the full CDF data set  

E-Print Network (OSTI)

We present a search for the standard model Higgs boson produced in association with a Z boson in data collected with the CDF II detector at the Tevatron, corresponding to an integrated luminosity of 9.45/fb. In events consistent with the decay of the Higgs boson to a bottom-quark pair and the Z boson to electron or muon pairs, we set 95% credibility level upper limits on the ZH production cross section times the H -> bb branching ratio as a function of Higgs boson mass. At a Higgs boson mass of 125 GeV/c^2 we observe (expect) a limit of 7.1 (3.9) times the standard model value.

CDF Collaboration

2012-07-06T23:59:59.000Z

306

Combined CDF and D0 Upper Limits on Standard Model Higgs Boson Production with up to 8.6 fb-1 of Data  

Science Conference Proceedings (OSTI)

We combine results from CDF and D0 on direct searches for the standard model (SM) Higgs boson (H) in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV. Compared to the previous Tevatron Higgs boson search combination more data have been added, additional channels have been incorporated, and some previously used channels have been reanalyzed to gain sensitivity. We use the MSTW08 parton distribution functions and the latest theoretical cross sections when comparing our limits to the SM predictions. With up to 8.2 fb{sup -1} of data analyzed at CDF and up to 8.6 fb{sup -1} at D0, the 95% C.L. our upper limits on Higgs boson production are factors of 1.17, 1.71, and 0.48 times the values of the SM cross section for Higgs bosons of mass m{sub H} = 115 GeV/c{sup 2}, 140 GeV/c{sup 2}, and 165 GeV/c{sup 2}, respectively. The corresponding median upper limits expected in the absence of Higgs boson production are 1.16, 1.16, and 0.57. There is a small ({approx} 1{sigma}) excess of data events with respect to the background estimation in searches for the Higgs boson in the mass range 125 < m{sub H} < 155 GeV/c{sup 2}. We exclude, at the 95% C.L., a new and larger region at high mass between 156 < m{sub H} < 177 GeV/c{sup 2}, with an expected exclusion region of 148 < m{sub H} < 180 GeV/c{sup 2}.

CDF, The; Collaborations, D0; Phenomena, the Tevatron New; Group, Higgs Working

2011-07-01T23:59:59.000Z

307

Combined CDF and D0 Upper Limits on Standard Model Higgs Boson Production with up to 8.6 fb-1 of Data  

E-Print Network (OSTI)

We combine results from CDF and D0 on direct searches for the standard model (SM) Higgs boson (H) in ppbar collisions at the Fermilab Tevatron at sqrt{s}=1.96 TeV. Compared to the previous Tevatron Higgs boson search combination more data have been added, additional channels have been incorporated, and some previously used channels have been reanalyzed to gain sensitivity. We use the MSTW08 parton distribution functions and the latest theoretical cross sections when comparing our limits to the SM predictions. With up to 8.2 fb-1 of data analyzed at CDF and up to 8.6 fb-1 at D0, the 95% C.L. our upper limits on Higgs boson production are factors of 1.17, 1.71, and 0.48 times the values of the SM cross section for Higgs bosons of mass m_H=115 GeV/c^2, 140 GeV/c^2, and 165 GeV/c^2, respectively. The corresponding median upper limits expected in the absence of Higgs boson production are 1.16, 1.16, and 0.57. There is a small (approx. 1 sigma) excess of data events with respect to the background estimation in searches for the Higgs boson in the mass range 125

The CDF; D0 Collaborations; the Tevatron New Phenomena; Higgs Working Group

2011-07-27T23:59:59.000Z

308

Data:F9c409c0-ca4b-49d9-81d6-21c120cdf0b6 | Open Energy Information  

Open Energy Info (EERE)

c0-ca4b-49d9-81d6-21c120cdf0b6 c0-ca4b-49d9-81d6-21c120cdf0b6 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Delmarva Power (Maryland) Effective date: 2011/07/08 End date if known: Rate name: OUTDOOR LIGHTING "OL" High Pressure Sodium 150W Sector: Lighting Description: there are many different classifications for different structures for lights. The monthly charge here is for the existing pole. Click on the link for other structures. Source or reference: http://www.delmarva.com/_res/documents/DPLMdMasterTariff.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW):

309

Updated search for the standard model Higgs boson in events with jets and missing transverse energy using the full CDF data set  

E-Print Network (OSTI)

We present an updated search for the Higgs boson produced in association with a vector boson in the final state with missing transverse energy and two jets. We use the full CDF data set corresponding to an integrated luminosity of 9.45 fb${}^{-1}$ at a proton-antiproton center-of-mass energy of $\\sqrt{s}=1.96$ TeV. New to this analysis is the inclusion of a $b$-jet identification algorithm specifically optimized for $H\\to b\\bar{b}$ searches. Across the Higgs boson mass range $90 \\le m_H \\le 150$ GeV$/c^2$, the expected 95% credibility level upper limits on the $V H$ production cross section times the $H\\to b\\bar{b}$ branching fraction are improved by an average of 14% relative to the previous analysis. At a Higgs boson mass of 125 GeV$/c^2$, the observed (expected) limit is 3.06 (3.33) times the standard model prediction, corresponding to one of the most sensitive searches to date in this final state.

CDF Collaboration; T. Aaltonen; S. Amerio; D. Amidei; A. Anastassov; A. Annovi; J. Antos; G. Apollinari; J. A. Appel; T. Arisawa; A. Artikov; J. Asaadi; W. Ashmanskas; B. Auerbach; A. Aurisano; F. Azfar; W. Badgett; T. Bae; A. Barbaro-Galtieri; V. E. Barnes; B. A. Barnett; P. Barria; P. Bartos; M. Bauce; F. Bedeschi; S. Behari; G. Bellettini; J. Bellinger; D. Benjamin; A. Beretvas; A. Bhatti; K. R. Bland; B. Blumenfeld; A. Bocci; A. Bodek; D. Bortoletto; J. Boudreau; A. Boveia; L. Brigliadori; C. Bromberg; E. Brucken; J. Budagov; H. S. Budd; K. Burkett; G. Busetto; P. Bussey; P. Butti; A. Buzatu; A. Calamba; S. Camarda; M. Campanelli; F. Canelli; B. Carls; D. Carlsmith; R. Carosi; S. Carrillo; B. Casal; M. Casarsa; A. Castro; P. Catastini; D. Cauz; V. Cavaliere; M. Cavalli-Sforza; A. Cerri; L. Cerrito; Y. C. Chen; M. Chertok; G. Chiarelli; G. Chlachidze; K. Cho; D. Chokheli; M. A. Ciocci; A. Clark; C. Clarke; M. E. Convery; J. Conway; M. Corbo; M. Cordelli; C. A. Cox; D. J. Cox; M. Cremonesi; D. Cruz; J. Cuevas; R. Culbertson; N. d'Ascenzo; M. Datta; P. De Barbaro; L. Demortier; M. Deninno; F. Devoto; M. d'Errico; A. Di Canto; B. Di Ruzza; J. R. Dittmann; M. D'Onofrio; S. Donati; M. Dorigo; A. Driutti; K. Ebina; R. Edgar; A. Elagin; R. Erbacher; S. Errede; B. Esham; R. Eusebi; S. Farrington; J. P. Fernandez Ramos; R. Field; G. Flanagan; R. Forrest; M. Franklin; J. C. Freeman; H. Frisch; Y. Funakoshi; A. F. Garfinkel; P. Garosi; H. Gerberich; E. Gerchtein; S. Giagu; V. Giakoumopoulou; K. Gibson; C. M. Ginsburg; N. Giokaris; P. Giromini; G. Giurgiu; V. Glagolev; D. Glenzinski; M. Gold; D. Goldin; A. Golossanov; G. Gomez; G. Gomez-Ceballos; M. Goncharov; O. Gonzalez Lopez; I. Gorelov; A. T. Goshaw; K. Goulianos; E. Gramellini; S. Grinstein; C. Grosso-Pilcher; R. C. Group; J. Guimaraes da Costa; S. R. Hahn; J. Y. Han; F. Happacher; K. Hara; M. Hare; R. F. Harr; T. Harrington-Taber; K. Hatakeyama; C. Hays; J. Heinrich; M. Herndon; A. Hocker; Z. Hong; W. Hopkins; S. Hou; R. E. Hughes; U. Husemann; J. Huston; G. Introzzi; M. Iori; A. Ivanov; E. James; D. Jang; B. Jayatilaka; E. J. Jeon; S. Jindariani; M. Jones; K. K. Joo; S. Y. Jun; T. R. Junk; M. Kambeitz; T. Kamon; P. E. Karchin; A. Kasmi; Y. Kato; W. Ketchum; J. Keung; B. Kilminster; D. H. Kim; H. S. Kim; J. E. Kim; M. J. Kim; S. B. Kim; S. H. Kim; Y. K. Kim; Y. J. Kim; N. Kimura; M. Kirby; K. Knoepfel; K. Kondo; D. J. Kong; J. Konigsberg; A. V. Kotwal; M. Kreps; J. Kroll; M. Kruse; T. Kuhr; M. Kurata; A. T. Laasanen; S. Lammel; M. Lancaster; K. Lannon; G. Latino; H. S. Lee; J. S. Lee; S. Leo; S. Leone; J. D. Lewis; A. Limosani; E. Lipeles; T. Liu; Q. Liu; T. Liu; S. Lockwitz; A. Loginov; D. Lucchesi; J. Lueck; P. Lujan; P. Lukens; G. Lungu; J. Lys; R. Lysak; R. Madrak; P. Maestro; S. Malik; G. Manca; A. Manousakis-Katsikakis; F. Margaroli; P. Marino; M. Martinez; K. Matera; M. E. Mattson; A. Mazzacane; P. Mazzanti; R. McNulty; A. Mehta; P. Mehtala; C. Mesropian; T. Miao; D. Mietlicki; A. Mitra; H. Miyake; S. Moed; N. Moggi; C. S. Moon; R. Moore; M. J. Morello; A. Mukherjee; Th. Muller; P. Murat; M. Mussini; J. Nachtman; Y. Nagai; J. Naganoma; I. Nakano; A. Napier; J. Nett; C. Neu; T. Nigmanov; L. Nodulman; S. Y. Noh; O. Norniella; L. Oakes; S. H. Oh; Y. D. Oh; I. Oksuzian; T. Okusawa; R. Orava; L. Ortolan; C. Pagliarone; E. Palencia; P. Palni; V. Papadimitriou; W. Parker; G. Pauletta; M. Paulini; C. Paus; T. J. Phillips; G. Piacentino; E. Pianori; J. Pilot; K. Pitts; C. Plager; L. Pondrom; S. Poprocki; K. Potamianos; F. Prokoshin; A. Pranko; F. Ptohos; G. Punzi; N. Ranjan; I. Redondo Fernandez; P. Renton; M. Rescigno; T. Riddick; F. Rimondi; L. Ristori; A. Robson; T. Rodriguez; S. Rolli; M. Ronzani; R. Roser; J. L. Rosner; F. Ruffini; A. Ruiz; J. Russ; V. Rusu; A. Safonov; W. K. Sakumoto; Y. Sakurai; L. Santi; K. Sato; V. Saveliev; A. Savoy-Navarro; P. Schlabach; E. E. Schmidt; T. Schwarz; L. Scodellaro; F. Scuri; S. Seidel; Y. Seiya; A. Semenov; F. Sforza; S. Z. Shalhout; T. Shears; P. F. Shepard; M. Shimojima; M. Shochet; I. Shreyber-Tecker; A. Simonenko; P. Sinervo; K. Sliwa; J. R. Smith; F. D. Snider; V. Sorin; H. Song; M. Stancari; R. St. Denis; B. Stelzer; O. Stelzer-Chilton; D. Stentz; J. Strologas; Y. Sudo; A. Sukhanov; I. Suslov; K. Takemasa; Y. Takeuchi; J. Tang; M. Tecchio; P. K. Teng; J. Thom; E. Thomson; V. Thukral; D. Toback; S. Tokar; K. Tollefson; T. Tomura; D. Tonelli; S. Torre; D. Torretta; P. Totaro; M. Trovato; F. Ukegawa; S. Uozumi; F. Vaquez; G. Velev; C. Vellidis; C. Vernieri; M. Vidal; R. Vilar; J. Vizan; M. Vogel; G. Volpi; P. Wagner; R. Wallny; S. M. Wang; A. Warburton; D. Waters; W. C. Wester III; D. Whiteson; A. B. Wicklund; S. Wilbur; H. H. Williams; J. S. Wilson; P. Wilson; B. L. Winer; P. Wittich; S. Wolbers; H. Wolfe; T. Wright; X. Wu; Z. Wu; K. Yamamoto; D. Yamato; T. Yang; U. K. Yang; Y. C. Yang; W. -M. Yao; G. P. Yeh; K. Yi

2013-01-18T23:59:59.000Z

310

Developement of a same-side kaon tagging algorithm of B^0_s decays for measuring delta m_s at CDF II  

SciTech Connect

The authors developed a Same-Side Kaon Tagging algorithm to determine the production flavor of B{sub s}{sup 0} mesons. Until the B{sub s}{sup 0} mixing frequency is clearly observed the performance of the Same-Side Kaon Tagging algorithm can not be measured on data but has to be determined on Monte Carlo simulation. Data and Monte Carlo agreement has been evaluated for both the B{sub s}{sup 0} and the high statistics B{sup +} and B{sup 0} modes. Extensive systematic studies were performed to quantify potential discrepancies between data and Monte Carlo. The final optimized tagging algorithm exploits the particle identification capability of the CDF II detector. it achieves a tagging performance of {epsilon}D{sup 2} = 4.0{sub -1.2}{sup +0.9} on the B{sub s}{sup 0} {yields} D{sub s}{sup -} {pi}{sup +} sample. The Same-Side Kaon Tagging algorithm presented here has been applied to the ongoing B{sub s}{sup 0} mixing analysis, and has provided a factor of 3-4 increase in the effective statistical size of the sample. This improvement results in the first direct measurement of the B{sub s}{sup 0} mixing frequency.

Menzemer, Stephanie; /Heidelberg U.

2006-06-01T23:59:59.000Z

311

A Search for the Higgs Boson Produced in Association with $Z\\to \\ell^+\\ell^-$ Using the Matrix Element Method at CDF II  

SciTech Connect

We present a search for associated production of the standard model (SM) Higgs boson and a Z boson where the Z boson decays to two leptons and the Higgs decays to a pair of b quarks in p{bar p} collisions at the Fermilab Tevatron. We use event probabilities based on SM matrix elements to construct a likelihood function of the Higgs content of the data sample. In a CDF data sample corresponding to an integrated luminosity of 2.7 fb{sup -1} we see no evidence of a Higgs boson with a mass between 100 GeV/c{sup 2} and 150 GeV/c{sup 2}. We set 95% confidence level (C.L.) upper limits on the cross-section for ZH production as a function of the Higgs boson mass m{sub H}; the limit is 8.2 times the SM prediction at m{sub H} = 115 GeV/c{sup 2}.

Aaltonen, T.; /Helsinki Inst. of Phys.; Adelman, J.; /Chicago U., EFI; Akimoto, T.; /Tsukuba U.; Alvarez Gonzalez, B.; /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U.; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Apresyan, A.; /Purdue U. /Waseda U.

2009-08-01T23:59:59.000Z

312

s041.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

± ± I (J P ) = 1 2 (0 - ) Quantum numbers not measured. Values shown are quark-model predictions. See also the B ± /B 0 ADMIXTURE and B ± /B 0 /B 0 s /b-baryon AD- MIXTURE sections. B ± MASS B ± MASS B ± MASS B ± MASS The fit uses m B + , (m B 0 - m B + ), and m B 0 to determine m B + , m B 0 , and the mass difference. VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5279.0±0.5 OUR FIT 5279.0±0.5 OUR FIT 5279.0±0.5 OUR FIT 5279.0±0.5 OUR FIT 5279.1±0.5 OUR AVERAGE 5279.1±0.5 OUR AVERAGE 5279.1±0.5 OUR AVERAGE 5279.1±0.5 OUR AVERAGE 5279.1±0.4 ±0.4 526 1 CSORNA 00 CLE2 e + e - → Υ(4S) 5279.1±1.7 ±1.4 147 ABE 96B CDF p p at 1.8 TeV * * * We do not use the following data for averages, fits, limits, etc. * * * 5278.8±0.54 ±2.0 362 ALAM 94 CLE2 e + e - → Υ(4S) 5278.3±0.4 ±2.0 BORTOLETTO92 CLEO e + e - → Υ(4S) 5280.5±1.0 ±2.0 2 ALBRECHT 90J ARG e + e - → Υ(4S) 5275.8±1.3 ±3.0 32 ALBRECHT 87C ARG e + e - → Υ(4S) 5278.2±1.8

313

Citation: W.-M. Yao  

NLE Websites -- All DOE Office Websites (Extended Search)

B B 0 I (J P ) = 1 2 (0 - ) Quantum numbers not measured. Values shown are quark-model predictions. See also the B ± /B 0 ADMIXTURE and B ± /B 0 /B 0 s /b-baryon AD- MIXTURE sections. See the Note "Production and Decay of b-flavored Hadrons" at the beginning of the B ± Particle Listings and the Note on "B 0 -B 0 Mixing" near the end of the B 0 Particle Listings. B 0 MASS B 0 MASS B 0 MASS B 0 MASS The fit uses m B + , (m B 0 - m B + ), and m B 0 to determine m B + , m B 0 , and the mass difference. VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5279.4 ± 0.5 OUR FIT 5279.4 ± 0.5 OUR FIT 5279.4 ± 0.5 OUR FIT 5279.4 ± 0.5 OUR FIT 5279.3 ± 0.7 OUR AVERAGE 5279.3 ± 0.7 OUR AVERAGE 5279.3 ± 0.7 OUR AVERAGE 5279.3 ± 0.7 OUR AVERAGE 5279.1 ± 0.7 ± 0.3 135 1 CSORNA 00 CLE2 e + e - → Υ(4S) 5281.3 ± 2.2 ± 1.4 51 ABE 96B CDF p p at 1.8 TeV * * * We do not use the following data for averages, fits, limits, etc. * * * 5279.2 ± 0.54 ± 2.0 340

314

s042.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

0 0 I (J P ) = 1 2 (0 - ) Quantum numbers not measured. Values shown are quark-model predictions. See also the B ± /B 0 ADMIXTURE and B ± /B 0 /B 0 s /b-baryon AD- MIXTURE sections. See the Note "Production and Decay of b-flavored Hadrons" at the beginning of the B ± Particle Listings and the Note on "B 0 -B 0 Mixing" near the end of the B 0 Particle Listings. B 0 MASS B 0 MASS B 0 MASS B 0 MASS The fit uses m B + , (m B 0 - m B + ), and m B 0 to determine m B + , m B 0 , and the mass difference. VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5279.4± 0.5 OUR FIT 5279.4± 0.5 OUR FIT 5279.4± 0.5 OUR FIT 5279.4± 0.5 OUR FIT 5279.3± 0.7 OUR AVERAGE 5279.3± 0.7 OUR AVERAGE 5279.3± 0.7 OUR AVERAGE 5279.3± 0.7 OUR AVERAGE 5279.1± 0.7 ± 0.3 135 1 CSORNA 00 CLE2 e + e - → Υ(4S) 5281.3± 2.2 ± 1.4 51 ABE 96B CDF p p at 1.8 TeV * * * We do not use the following data for averages, fits, limits, etc. * * * 5279.2± 0.54 ± 2.0 340

315

Citation: D.E. Groom  

NLE Websites -- All DOE Office Websites (Extended Search)

± ± I (J P ) = 1 2 (0 - ) Quantum numbers not measured. Values shown are quark-model predictions. See also the B ± /B 0 ADMIXTURE and B ± /B 0 /B 0 s /b-baryon AD- MIXTURE sections. B ± MASS B ± MASS B ± MASS B ± MASS The fit uses m B + , (m B 0 - m B + ), and m B 0 to determine m B + , m B 0 , and the mass difference. VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5279.0±0.5 OUR FIT 5279.0±0.5 OUR FIT 5279.0±0.5 OUR FIT 5279.0±0.5 OUR FIT 5279.1±0.5 OUR AVERAGE 5279.1±0.5 OUR AVERAGE 5279.1±0.5 OUR AVERAGE 5279.1±0.5 OUR AVERAGE 5279.1±0.4 ±0.4 526 1 CSORNA 00 CLE2 e + e - → Υ(4S) 5279.1±1.7 ±1.4 147 ABE 96B CDF p p at 1.8 TeV * * * We do not use the following data for averages, fits, limits, etc. * * * 5278.8±0.54 ±2.0 362 ALAM 94 CLE2 e + e - → Υ(4S) 5278.3±0.4 ±2.0 BORTOLETTO92 CLEO e + e - → Υ(4S) 5280.5±1.0 ±2.0 2 ALBRECHT 90J ARG e + e - → Υ(4S) 5275.8±1.3 ±3.0 32 ALBRECHT 87C ARG e + e - → Υ(4S) 5278.2±1.8

316

s042.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

0 0 I (J P ) = 1 2 (0 - ) Quantum numbers not measured. Values shown are quark-model predictions. See also the B ± /B 0 ADMIXTURE and B ± /B 0 /B 0 s /b-baryon AD- MIXTURE sections. See the Note "Production and Decay of b-flavored Hadrons" at the beginning of the B ± Particle Listings and the Note on "B 0 -B 0 Mixing and CP Violation in B Decay" near the end of the B 0 Particle Listings. B 0 MASS B 0 MASS B 0 MASS B 0 MASS The fit uses m B + , (m B 0 - m B + ), and m B 0 to determine m B + , m B 0 , and the mass difference. VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5279.4±0.5 OUR FIT 5279.4±0.5 OUR FIT 5279.4±0.5 OUR FIT 5279.4±0.5 OUR FIT 5279.3±0.7 OUR AVERAGE 5279.3±0.7 OUR AVERAGE 5279.3±0.7 OUR AVERAGE 5279.3±0.7 OUR AVERAGE 5279.1±0.7 ±0.3 135 1 CSORNA 00 CLE2 e + e - → Υ(4S) 5281.3±2.2 ±1.4 51 ABE 96B CDF p p at 1.8 TeV * * * We do not use the following data for averages, fits, limits, etc. *

317

s042.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

0 0 I (J P ) = 1 2 (0 - ) Quantum numbers not measured. Values shown are quark-model predictions. See also the B ± /B 0 ADMIXTURE and B ± /B 0 /B 0 s /b-baryon AD- MIXTURE sections. See the Note "Production and Decay of b-flavored Hadrons" at the beginning of the B ± Particle Listings and the Note on "B 0 -B 0 Mixing and CP Violation in B Decay" near the end of the B 0 Particle Listings. B 0 MASS B 0 MASS B 0 MASS B 0 MASS The fit uses m B + , (m B 0 - m B + ), and m B 0 to determine m B + , m B 0 , and the mass difference. VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 5279.4±0.5 OUR FIT 5279.4±0.5 OUR FIT 5279.4±0.5 OUR FIT 5279.4±0.5 OUR FIT 5279.3±0.7 OUR AVERAGE 5279.3±0.7 OUR AVERAGE 5279.3±0.7 OUR AVERAGE 5279.3±0.7 OUR AVERAGE 5279.1±0.7 ±0.3 135 1 CSORNA 00 CLE2 e + e - → Υ(4S) 5281.3±2.2 ±1.4 51 ABE 96B CDF p p at 1.8 TeV * * * We do not use the following data for averages, fits, limits, etc. *

318

A Study of The Standard Model Higgs, WW and ZZ Production in Dilepton Plus Missing Transverse Energy Final State at CDF Run II  

SciTech Connect

We report on a search for Standard Model (SM) production of Higgs to WW* in the two charged lepton (e, {mu}) and two neutrino final state in p{bar p} collisions at a center of mass energy {radical}s = 1.96 TeV. The data were collected with the CDF II detector at the Fermilab Tevatron and correspond to an integrated luminosity of 1.9fb{sup -1}. The Matrix Element method is developed to calculate the event probability and to construct a likelihood ratio discriminator. There are 522 candidates observed with an expectation of 513 {+-} 41 background events and 7.8 {+-} 0.6 signal events for Higgs mass 160GeV/c{sup 2} at next-to-next-to-leading logarithmic level calculation. The observed 95% C.L. upper limit is 0.8 pb which is 2.0 times the SM prediction while the median expected limit is 3.1{sub -0.9}{sup +1.3} with systematics included. Results for 9 other Higgs mass hypotheses ranging from 110GeV/c{sup 2} to 200GeV/c{sup 2} are also presented. The same dilepton plus large transverse energy imbalance (E{sub T}) final state is used in the SM ZZ production search and the WW production study. The observed significance of ZZ {yields} ll{nu}{nu} channel is 1.2{sigma}. It adds extra significance to the ZZ {yields} 4l channel and leads to a strong evidence of ZZ production with 4.4 {sigma} significance. The potential improvement of the anomalous triple gauge coupling measurement by using the Matrix Element method in WW production is also studied.

Hsu, Shih-Chieh; /UC, San Diego

2008-06-01T23:59:59.000Z

319

Search for the standard model Higgs boson produced in association with a $W^{\\pm}$ boson with 7.5 fb$^{-1}$ integrated luminosity at CDF  

Science Conference Proceedings (OSTI)

We present a search for the standard model Higgs boson produced in association with a W{sup {+-}} boson. This search uses data corresponding to an integrated luminosity of 7.5fb{sup -1} collected by the CDF detector at the Tevatron. We select WH{yields}{ell}vb{bar b} candidate events with two jets, large missing transverse energy, and exactly one charged lepton. We further require that at least one jet be identified to originate from a bottom quark. Discrimination between the signal and the large background is achieved through the use of a Bayesian artificial neural network. The number of tagged events and their distributions are consistent with the standard model expectations. We observe no evidence for a Higgs boson signal and set 95% C.L. upper limits on the WH production cross section times the branching ratio to decay to b{bar b}pairs, {sigma}(p{bar p}{yields}W{sup {+-}}H)xB(H{yields}b{bar b}), relative to the rate predicted by the standard model. For the Higgs boson mass range of 100 to 150 GeV/c{sup 2} we set observed (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For 115 GeV/c{sup 2} the upper limit is 3.64 (2.78). The combination of the present search with an independent analysis that selects events with three jets yields more stringent limits ranging from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For 115 and 125 GeV/c{sup 2} the upper limits are 2.65 (2.60) and 4.36 (3.69), respectively.

Aaltonen, T.; /Helsinki Inst. of Phys.; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U. /Fermilab; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Arisawa, T.; /Waseda U.; Artikov, A.; /Dubna, JINR /Texas A-M

2012-06-01T23:59:59.000Z

320

Optimization of the signal selection of exclusively reconstructed decays of B0 and B/s mesons at CDF-II  

SciTech Connect

The work presented in this thesis is mainly focused on the application in a {Delta}m{sub s} measurement. Chapter 1 starts with a general theoretical introduction on the unitarity triangle with a focus on the impact of a {Delta}m{sub s} measurement. Chapter 2 then describes the experimental setup, consisting of the Tevatron collider and the CDF II detector, that was used to collect the data. In chapter 3 the concept of parameter estimation using binned and unbinned maximum likelihood fits is laid out. In addition an introduction to the NeuroBayes{reg_sign} neural network package is given. Chapter 4 outlines the analysis steps walking the path from the trigger level selection to fully reconstructed B mesons candidates. In chapter 5 the concepts and formulas that form the ingredients to an unbinned maximum likelihood fit of {Delta}m{sub s} ({Delta}m{sub d}) from a sample of reconstructed B mesons are discussed. Chapter 6 then introduces the novel method of using neural networks to achieve an improved signal selection. First the method is developed, tested and validated using the decay B{sup 0} {yields} D{pi}, D {yields} K{pi}{pi} and then applied to the kinematically very similar decay B{sub s} {yields} D{sub s}{pi}, D{sub s} {yields} {phi}{pi}, {phi} {yields} KK. Chapter 7 uses events selected by the neural network selection as input to an unbinned maximum likelihood fit and extracts the B{sup 0} lifetime and {Delta}m{sub d}. In addition, an amplitude scan and an unbinned maximum likelihood fit of {Delta}m{sub s} is performed, applying the neural network selection developed for the decay channel B{sub s} {yields} D{sub s}{pi}, D{sub s} {yields} {phi}{pi}, {phi} {yields} KK. Finally chapter 8 summarizes and gives an outlook.

Doerr, Christian; /Karlsruhe U., EKP

2006-06-01T23:59:59.000Z

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


321

Data:Bfc5a30a-2da7-4aac-b8e8-54f72a4d8cdf | Open Energy Information  

Open Energy Info (EERE)

Bfc5a30a-2da7-4aac-b8e8-54f72a4d8cdf Bfc5a30a-2da7-4aac-b8e8-54f72a4d8cdf No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Painesville, Ohio (Utility Company) Effective date: 1990/07/01 End date if known: Rate name: Roadway Lighting-Mercury vapor-400 watts-Outside Corporate Limits Sector: Lighting Description: For the purpose of paying the expenses of conducting and managing the Electric Division, Utilities Department of the City, the City Manager is hereby authorized and directed to charge the following rates for furnishing electric current for outdoor lights, which rates are hereby adopted, for all utility bills issued on and after July 1, 1990

322

Data:67cdf3c6-fcc4-4b0e-ae80-a5d3d1f3e056 | Open Energy Information  

Open Energy Info (EERE)

cdf3c6-fcc4-4b0e-ae80-a5d3d1f3e056 cdf3c6-fcc4-4b0e-ae80-a5d3d1f3e056 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Clintonville, Wisconsin (Utility Company) Effective date: 2006/05/05 End date if known: Rate name: Gs-2 General Time-of-Day Service Single Phase 8am-8pm Sector: Commercial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kWh of sales) is greater or lesser than the base cost of power purchased (per kWh of sales). The base cost of power is $0.0680 per kWh. See schedule PCAC.

323

Search for a Higgs boson in the diphoton final state using the full CDF data set from proton-antiproton collisions at \\surds = 1.96 TeV  

E-Print Network (OSTI)

A search for a narrow Higgs boson resonance in the diphoton mass spectrum is presented based on data corresponding to 10 fb-1 of integrated luminosity from proton-antiproton collisions at \\surds = 1.96 TeV collected by the CDF experiment. In addition to searching for a resonance in the diphoton mass spectrum, we employ a multivariate discriminant technique for the first time in this channel at CDF. No evidence of signal is observed, and upper limits are set on the cross section times branching ratio of the resonant state as a function of Higgs boson mass. The limits are interpreted in the context of the standard model with an expected (observed) limit on the cross section times branching ratio of 9.9 (17.0) times the standard model prediction at the 95% credibility level for a Higgs boson mass of 125 GeV/c2. Moreover, a Higgs boson with suppressed couplings to fermions is excluded for masses below 114 GeV/c2 at the 95% credibility level.

the CDF Collaboration

2012-07-26T23:59:59.000Z

324

Combined CDF and D0 upper limits on $gg\\to H\\to W^+W^-$ and constraints on the Higgs boson mass in fourth-generation fermion models with up to 8.2 fb$^{-1}$ of data  

Science Conference Proceedings (OSTI)

We combine results from searches by the CDF and D0 Collaborations for a standard model Higgs boson (H) in the processes gg {yields} H {yields} W{sup +}W{sup -} and gg {yields} H {yields} ZZ in p{bar p} collisions at the Fermilab Tevatron Collider at {radical}s = 1.96 TeV. With 8.2 fb{sup -1} of integrated luminosity analyzed at CDF and 8.1 fb{sup -1} at D0, the 95% C.L. upper limit on {sigma}(gg {yields} H) x {Beta}(H {yields} W{sup +}W{sup -}) is 1.01 pb at m{sub H} = 120 GeV, 0.40 pb at m{sub H} = 165 GeV, and 0.47 pb at m{sub H} = 200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% Confidence Level a standard-model-like Higgs boson with a mass between 124 and 286 GeV.

Benjamin, Doug; /Tufts U.

2011-08-01T23:59:59.000Z

325

Combined CDF and Dzero Upper Limits on Standard Model Higgs Boson Production at High Mass (155-200 GeV/c2) with 3 fb-1 of data  

E-Print Network (OSTI)

We combine results from CDF and DO searches for a standard model Higgs boson in ppbar collisions at the Fermilab Tevatron, at sqrt{s}=1.96 TeV. With 3.0 fb-1 of data analyzed at CDF, and at DO, the 95% C.L. upper limits on Higgs boson production are a factor of 1.2, 1.0 and 1.3 higher than the SM cross section for a Higgs boson mass of m_{H}=$165, 170 and 175 GeV, respectively. We exclude at 95% C.L. a standard model Higgs boson of m_H=170 GeV. Based on simulation, the ratios of the corresponding median expected upper limit to the Standard Model cross section are 1.2, 1.4 and 1.7. Compared to the previous Higgs Tevatron combination, more data and refined analysis techniques have been used. These results extend significantly the individual limits of each experiment and provide new knowledge on the mass of the standard model Higgs boson beyond the LEP direct searches.

Tevatron New Phenomena; Higgs working group; CDF Collaboration; D0 Collaboration

2008-08-05T23:59:59.000Z

326

Data:Ea9c8db7-2e8a-4b9b-a30f-26e3cdf78e0c | Open Energy Information  

Open Energy Info (EERE)

c8db7-2e8a-4b9b-a30f-26e3cdf78e0c c8db7-2e8a-4b9b-a30f-26e3cdf78e0c No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Borough of Pitcairn, Pennsylvania (Utility Company) Effective date: End date if known: Rate name: Large Power Service Sector: Commercial Description: Availability for commercial or industrial service. Customers shall contract for a definite amount of electrical capacity in kilovolt-amperes which shall be sufficient to meet normal maximum requirements but in no case shall the capacity contracted for be less than 50 kva. The Utility may not be required to supply capacity in excess of that contracted for except by mutual agreement. Contracts will be made in multiples of 25 kva.

327

AusgAbe 03 | 2010 ,,Im Internet surfen ist wie  

E-Print Network (OSTI)

: Jennifer Klingler und Mathias Pusch sind Auszubildende im botanischen garten. ein bericht auf seite 14 ARbeITsPlATZPORTRAIT Azubis im botanischen garten 14 gleICHsTelluNgsbeAuFTRAgTe Ferienfreizeit ,,bella

Schiller, Stephan

328

Search for the standard model Higgs boson produced in association with a Z boson in 7.9 fb[superscript ?1] of p[bar-over p] collisions at ?s = 1.96 TeV using the CDF II detector  

E-Print Network (OSTI)

We present a search for the standard model Higgs boson produced in association with a Z boson, using up to 7.9 fb[superscript ?1] of integrated luminosity from p[bar-over p] collisions collected with the CDF II detector. ...

Gomez-Ceballos, Guillelmo

329

Fermilab Detectors CDF & D0  

NLE Websites -- All DOE Office Websites (Extended Search)

detectors and the need for upgrading to keep up with the advancements of the accelerators. As Fermilab prepares for the future in high-energy physics, the Laboratory must...

330

Search for the standard model Higgs boson decaying to a $b\\bar{b}$ pair in events with no charged leptons and large missing transverse energy using the full CDF data set  

E-Print Network (OSTI)

We report on a search for the standard model Higgs boson produced in association with a vector boson in the full data set of proton-antiproton collisions at $\\sqrt{s} = 1.96$ TeV recorded by the CDF II detector at the Tevatron, corresponding to an integrated luminosity of 9.45 fb$^{-1}$. We consider events having no identified charged lepton, a transverse energy imbalance, and two or three jets, of which at least one is consistent with originating from the decay of a $b$ quark. We place 95% credibility level upper limits on the production cross section times standard model branching fraction for several mass hypotheses between 90 and $150 \\mathrm{GeV}/c^2$. For a Higgs boson mass of $125 \\mathrm{GeV}/c^2$, the observed (expected) limit is 6.7 (3.6) times the standard model prediction.

The CDF Collaboration

2012-07-06T23:59:59.000Z

331

Search for the standard model Higgs boson decaying to a bb pair in events with one charged lepton and large missing transverse energy using the full CDF data set  

E-Print Network (OSTI)

We present a search for the standard model Higgs boson produced in association with a W boson in sqrt(s) = 1.96 TeV p-pbar collision data collected with the CDF II detector at the Tevatron corresponding to an integrated luminosity of 9.45 fb-1. In events consistent with the decay of the Higgs boson to a bottom-quark pair and the W boson to an electron or muon and a neutrino, we set 95% credibility level upper limits on the WH production cross section times the H->bb branching ratio as a function of Higgs boson mass. At a Higgs boson mass of 125 GeV/c2 we observe (expect) a limit of 4.9 (2.8) times the standard model value.

The CDF Collaboration

2012-07-06T23:59:59.000Z

332

Search for Standard Model Higgs Boson Production in Association with a $W$ Boson Using a Matrix Element Technique at CDF in $p\\bar{p}$ Collisions at $\\sqrt{s} = 1.96$ TeV  

Science Conference Proceedings (OSTI)

This paper presents a search for standard model Higgs boson production in association with a W boson using events recorded by the CDF experiment in a dataset corresponding to an integrated luminosity of 5.6 fb{sup -1}. The search is performed using a matrix element technique in which the signal and background hypotheses are used to create a powerful discriminator. The discriminant output distributions for signal and background are fit to the observed events using a binned likelihood approach to search for the Higgs boson signal. We find no evidence for a Higgs boson, and 95% confidence level (C.L.) upper limits are set on {sigma}(p{bar p} {yields} WH) x {Beta}(H {yields} b{bar b}). The observed limits range from 3.5 to 37.6 relative to the standard model expectation for Higgs boson masses between m{sub H} = 100 GeV/c{sup 2} and m{sub H} = 150 GeV/c{sup 2}. The 95% C.L. expected limit is estimated from the median of an ensemble of simulated experiments and varies between 2.9 and 32.7 relative to the production rate predicted by the standard model over the Higgs boson mass range studied.

Aaltonen, T.; /Helsinki Inst. of Phys.; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U. /Fermilab; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Arisawa, T.; /Waseda U.; Artikov, A.; /Dubna, JINR /Texas A-M

2011-12-01T23:59:59.000Z

333

First search at CDF for the Higgs boson decaying to a W-boson pair in proton-antiproton collisions at the center-of-mass energy of 1.96 TeV  

SciTech Connect

By way of retaining the gauge invariance of the Standard Model (SM) and giving masses to the W{sup {+-}} and Z{sup 0} bosons and the fermions, the Higgs mechanism predicts the existence of a neutral scalar bosonic particle, whose mass is not exactly known. The Higgs boson is the only experimentally unconfirmed SM particle to date. This thesis documents a search for the Higgs boson in p{bar p} collisions at {radical}s = 1.96 TeV at the Tevatron, using 360 {+-} pb {sup -1} data collected by the Run II Collider Detector at Fermilab (CDF II), as part of the most important quest for contemporary particle physicists. The search was for a Higgs boson decaying to a pair of W{sup {+-}} bosons, where each W boson decays to an electron, a muon or a tau that further decays to an electron or a muon with associated neutrinos. Events with two charged leptons plus large missing energy were selected in data triggered on a high p{sub t} lepton and compared to the signal and backgrounds modeled using Monte Carlo and jet data. No signal-like excess was observed in data. Therefore, upper limits on the HWW production cross-section in the analyzed mass range were extracted using the binned likelihood maximum from distributions of dilepton azimuthal angle at 95% Bayesian credibility level (CL), as shown in the table below.

Chuang, Shan-Huei S.; /Wisconsin U., Madison

2006-12-01T23:59:59.000Z

334

Data:Ff96b170-68b8-4c17-91fb-374a14958bb7 | Open Energy Information  

Open Energy Info (EERE)

b170-68b8-4c17-91fb-374a14958bb7 b170-68b8-4c17-91fb-374a14958bb7 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Nodak Electric Coop Inc Effective date: 2012/05/20 End date if known: Rate name: GS High Density Three Phase LT Sector: Industrial Description: Available for service to locations in a High Density area. A High Density area is defined as:  An enlargement (generally 160 acres) with 20 or more active locations, or  A cluster of 20 or more active locations, or  A cluster with 10 or more active locations that adjoins an enlargement with 20 or more active locations, or  An area adjacent to an incorporated town with 20 or more active locations. Additional Meters (Off-Peak Included) $ 3.60/Meter/Month Renewable Energy Market Adjustment $0.003/KWH (Added to All Above Energy Rates) Controlled Water Heater Credit $.00736/KWH Applies to the first 1,000 KWHs each month (October-March)

335

Data:Ed96b632-385d-4a71-b9cd-5d62e56186a4 | Open Energy Information  

Open Energy Info (EERE)

b632-385d-4a71-b9cd-5d62e56186a4 b632-385d-4a71-b9cd-5d62e56186a4 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Village of Milan, Ohio (Utility Company) Effective date: 2012/01/01 End date if known: Rate name: General Service- Small- Load Management Sector: Commercial Description: Available to all customers of the Village with measured demands of 50 kW or less. Source or reference: ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

336

Data:E964b96b-50ed-4042-8349-2e8e16c5ea01 | Open Energy Information  

Open Energy Info (EERE)

6b-50ed-4042-8349-2e8e16c5ea01 6b-50ed-4042-8349-2e8e16c5ea01 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Roosevelt Public Power Dist Effective date: End date if known: Rate name: Standby Irrigation Sector: Commercial Description: Annual charge is $107. Source or reference: http://rooseveltppd.com/content/rates Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous

337

Data:B12a96b8-e5dc-4002-a47e-f82fe67c5828 | Open Energy Information  

Open Energy Info (EERE)

b8-e5dc-4002-a47e-f82fe67c5828 b8-e5dc-4002-a47e-f82fe67c5828 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Mille Lacs Energy Cooperative Effective date: End date if known: Rate name: General Service Sector: Residential Description: Availability Available for all non-commercial service Source or reference: Rate Binder A Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >>

338

Data:0f96b428-c03a-4ba1-a057-32dfd99ad4df | Open Energy Information  

Open Energy Info (EERE)

6b428-c03a-4ba1-a057-32dfd99ad4df 6b428-c03a-4ba1-a057-32dfd99ad4df No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Oconomowoc Utilities Effective date: 2007/09/01 End date if known: Rate name: Cp-1 TOD Small Power Optional Time-of-Day Service with Parallel Generation(20kW or less) Sector: Industrial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0598 per kilowatt-hour.

339

Data:5c0c96b5-2969-4436-af89-f7507f9374c7 | Open Energy Information  

Open Energy Info (EERE)

b5-2969-4436-af89-f7507f9374c7 b5-2969-4436-af89-f7507f9374c7 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Menard Electric Coop Effective date: 2012/02/01 End date if known: Rate name: Security Light Service rate SL: 14,400 Lumen High Pressure Sodium Sector: Lighting Description: Dusk to dawn outdoor lighting, other than street lighting for towns and villages. Source or reference: http://www.menard.com/files/rates/rcSL_SecurityLight.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months):

340

Measurement of the t-tbar production cross section in p-pbar collisions at s**(1/2) = 1.96 TeV using lepton+jets events in the CDF detector at Fermilab  

SciTech Connect

The top quark is the most massive fundamental particle observed so far, and the study of its properties is interesting for several reasons ranging from its possible special role in electroweak symmetry breaking to its sensitivity to physics beyond the standard model (SM). In particular, the measurement of the top quark pair production cross section {sigma}{sub t{bar t}} is of interest as a test of QCD predictions. Recent QCD calculations done with perturbation theory to next-to-leading order predict {sigma}{sub t{bar t}} with an uncertainty of less than 15%, which motivate measurements of comparable precision. In this thesis, the author reports a measurement of the cross section for pair production of top quarks in the lepton+jets channel in 318 pb{sup -1} of p{bar p} collision data at {radical}s = 1.96 TeV. The data were recorded between March 2002 and September 2004, during Run II of the Tevatron, by the CDF II detector, a general purpose detector which combines charged particle trackers, sampling calorimeters, and muon detectors. processes in which a W boson is produced in association with several jets with large transverse momentum can be misidentified at t{bar t}, since they have the same signature. In order to separate the t{bar t} events from this background, they develop a method to tag b-jets based on tracking information from the silicon detector. The main event selection requires at least one tight (more restrictive) b tag in the event. As a cross check, they also measure the cross section using events with a loose (less restrictive) b tag and events which have at least two tight or at least two loose b tags. Background contributions from heavy flavor production processes, such as Wb{bar b}, Wc{bar c} or Wc, misidentified W bosons, electroweak processes, single top production, and mistagged jets are estimated using a combination of Monte Carlo calculations and independent measurements in control data samples. An excess over background in the number of events that contain a lepton, missing energy and three or more jets with at least one b-tag is assumed to be a signal of t{bar t} production and is used to measure the production cross section {sigma}{sub t{bar t}}.

Palencia, Enrique; /Cantabria Inst. of Phys. /Cantabria U., Santander

2006-12-01T23:59:59.000Z

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


341

A search for the Standard Model Higgs boson in the process $ZH \\rightarrow \\ell^{+} \\ell^{-} b \\bar{b}$ in $4.1\\unit{fb^{-1}}$ OF CDF~II DATA}  

SciTech Connect

The standard model of particle physics provides a detailed description of a universe in which all matter is composed of a small number of fundamental particles, which interact through the exchange of force - carrying gauge bosons (the photon, W{sup {+-}}, Z and gluons). The organization of the matter and energy in this universe is determined by the effects of three forces; the strong, weak, and electromagnetic. The weak and electromagnetic forces are the low energy manifestations of a single electro-weak force, while the strong force binds quarks into protons and neutrons. The standard model does not include gravity, as the effect of this force on fundamental particles is negligible. Four decades of experimental tests, spanning energies from a few electron-volts (eV) up to nearly two TeV, confirm that the universe described by the standard model is a reasonable approximation of our world. For example, experiments have confirmed the existence of the top quark, the W{sup {+-}} and the Z bosons, as predicted by the standard model. The latest experimental averages for the masses of the top quark, W{sup {+-}} and Z are respectively 173.1 {+-} 0.6(stat.) {+-} 1.1(syst.), 80.399 {+-} 0.023 and 91.1876 {+-} 0.0021 GeV/c{sup 2}. The SM is a gauge field theory of zero mass particles. However, the SM is able to accommodate particles with non-zero mass through the introduction of a theoretical Higgs field which permeates all of space. Fermions gain mass through interactions with this field, while the longitudinal components of the massive W{sup {+-}} and Z are the physical manifestations of the field itself. Introduction of the Higgs field, directly leads to the predicted existence of an additional particle, the Higgs boson. The Higgs boson is the only particle of the standard model that has not been observed, and is the only unconfirmed prediction of the theory. The standard model describes the properties of the Higgs boson in terms of its mass, which is a free parameter in the theory. Experimental evidence suggests that the Higgs mass has a value between 114.4 and 186 GeV/c{sup 2}. Particles with a mass in this range can be produced in collisions of less massive particles accelerated to near the speed of light. Currently, one of only a few machines capable of achieving collision energies large enough to potentially produce a standard model Higgs boson is the Tevatron proton-antiproton collider located at Fermi National Accelerator Laboratory in Batavia, Illinois. This dissertation describes the effort to observe the standard model Higgs in Tevatron collisions recorded by the Collider Detector at Fermilab (CDF) II experiment in the ZH {yields} {ell}{sup +}{ell}{sup -}b{bar b} production and decay channel. In this process, the Higgs is produced along with a Z boson which decays to a pair of electrons or muons (Z {yields} {ell}{sup +}{ell}{sup -}), while the Higgs decays to a bottom anti-bottom quark pair (H {yields} b{bar b}). A brief overview of the standard model and Higgs theory is presented in Chapter 2. Chapter 3 explores previous searches for the standard model Higgs at the Tevatron and elsewhere. The search presented in this dissertation expands upon the techniques and methods developed in previous searches. The fourth chapter contains a description of the Tevatron collider and the CDF II detector. The scope of the discussion in Chapter 4 is limited to the experimental components relevant to the current ZH {yields} {ell}{sup +}{ell}{sup -}b{bar b} search. Chapter 5 presents the details of object reconstruction; the methods used to convert detector signals into potential electrons, muons or quarks. Chapter six describes the data sample studied for the presence of a ZH {yields} {ell}{sup +}{ell}{sup -}b{bar b} signal and details the techniques used to model the data. The model accounts for both signal and non-signal processes (backgrounds) which are expected to contribute to the observed event sample. Chapters 7 and 8 summarize the event selection applied to isolate ZH {yields} {ell}{sup +}{ell}{sup -}b{bar b} candidate events

Shalhout, Shalhout Zaki; /Wayne State U.

2010-05-01T23:59:59.000Z

342

Data:66a9d240-3606-43d3-9abe-d2c666033c6b | Open Energy Information  

Open Energy Info (EERE)

3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of North Little Rock, Arkansas (Utility Company) Effective date: 20120901 End date if known: Rate name:...

343

Exclusive Dijet production from CDF2LHC  

E-Print Network (OSTI)

Exclusive dijet production at the Tevatron can be used as a benchmark to establish predictions on exclusive diffractive Higgs production, a process with a much smaller cross section. Exclusive dijet production in Double Pomeron Exchange processes, including diffractive Higgs production with measurements at the Tevatron and predictions for the Large Hadron Collider are presented. Using new data from the Tevatron and dedicated diffractive triggers, no excess over a smooth falling distribution for exclusive dijet events could be found. Upper limits on the exclusive dijet production cross section are presented and compared to current theoretical predictions.

Michele Gallinaro; for the CDF collaboration

2005-04-05T23:59:59.000Z

344

B mixing and CP violation at CDF  

SciTech Connect

The mixing of the neutral {bold B} mesons and the violation of CP symmetry in the {bold B} sector can be investigated at the Tevatron proton-antiproton collider. The most severe challenge that these measurements pose is tagging the flavor of a B meson at production. Here we present in detail the method of same side tagging (SST), which is used to obtain new measurement of the {ital B}{sup 0} mass difference {Delta}{ital m{sub d}} = 0.446 {+-} 0.057({ital stat}) + 0. 034 - 0.031({ital syst}) ps{sup -1}. The significance of SST and other tagging methods for physics during Run II of the Tevatron is discussed.

Boudreau, J. [Pittsburgh Univ., PA (United States)

1996-11-01T23:59:59.000Z

345

Determination of W boson helicity fractions in top quark decays in p anti-p collisions at CDF Run II and production of endcap modules for the ATLAS Silicon Tracker  

SciTech Connect

The thesis presented here includes two parts. The first part discusses the production of endcap modules for the ATLAS SemiConductor Tracker at the University of Geneva. The ATLAS experiment is one of the two multi-purpose experiments being built at the LHC at CERN. The University of Geneva invested extensive efforts to create an excellent and efficient module production site, in which 655 endcap outer modules were constructed. The complexity and extreme requirements for 10 years of LHC operation with a high resolution, high efficiency, low noise tracking system resulted in an extremely careful, time consuming production and quality assurance of every single module. At design luminosity about 1000 particles will pass through the tracking system each 25 ns. In addition to requiring fast tracking techniques, the high particle flux causes significant radiation damage. Therefore, modules have to be constructed within tight and accurate mechanical and electrical specification. A description of the ATLAS experiment and the ATLAS Semiconductor tracker is presented, followed by a detailed overview of the module production at the University of Geneva. My personal contribution to the endcap module production at the University of Geneva was taking part, together with other physicists, in selecting components to be assembled to a module, including hybrid reception tests, measuring the I-V curve of the sensors and the modules at different stages of the production, thermal cycling the modules and performing electrical readout tests as an initial quality assurance of the modules before they were shipped to CERN. An elaborated description of all of these activities is given in this thesis. At the beginning of the production period the author developed a statistics package which enabled us to monitor the rate and quality of the module production. This package was then used widely by the ATLAS SCT institutes that built endcap modules of any type, and kept being improved and updated. The production monitoring and summary using this package is shown in this thesis. The second part of the thesis reports a measurement of the fraction of longitudinal and right-handed helicity states of W bosons in top quark decays. This measurement was done using 955 pb{sup -1} of data collected with the CDF detector at the TEvatron, where protons and anti-protons are collided with a center-of-mass energy of 1.96 TeV. the helicity fraction measurements take advantage of the fact that the angular distribution of the W boson decay products depends on the helicity state of the W which they originate from. They analyze t{bar t} events in the 'lepton+jets' channel and look at the leptonic side of decay. They construct templates for the distribution of cos{theta}*, the angle between the charged lepton and the W flight direction in the rest frame of the top quark. Using Monte Carlo techniques, they construct probability distributions ('templates') for cos{theta}* in the case of left-handed, longitudinal and right-handed Ws and a template for the background model. They extract the W helicity fractions using an unbinned likelihood fitter based on the information of these templates. The Standard Model predicts the W helicity fractions to be about 70% longitudinal and 30% left-handed, while the fraction of right-handed W bosons in top decays is highly suppressed and vanishes when neglecting the mass of the b quark.

Moed, Shulamit; /Geneva U.

2007-01-01T23:59:59.000Z

346

APPENDIX A-BES-0 to User Agreement No. NP-09-  

E-Print Network (OSTI)

Materials Sciences (CNMS), High Flux Isotope Reactor (HFIR), Shared Research Equipment User Facility (Sha performed at HFIR and/or SNS, the following provisions shall apply. Where the following provisions) for use at the Spallation Neutron Source (SNS) or the High Flux Isotope Reactor (HFIR). CONTRACTOR

347

Detection of the 6 November 1997 Ground Level Event by Abe D. Falcone, for Milagro Collaboration  

E-Print Network (OSTI)

for approximately one year in 1997/98, was sensitive to solar proton and neutron fluxes above ~4 GeV. Milagrito and other neutron monitors. An analysis, based on preliminary effective area estimates, indicates photomultiplier tubes (228 PMTs for the prototype, Milagrito). This energy range overlaps that of neutron monitors

California at Santa Cruz, University of

348

Next-to-next-to-leading order soft gluon corrections in top quark hadroproduction.  

E-Print Network (OSTI)

by the Division of Nuclear Physics of the Office of High Energy and Nuclear Physics of the U.S. Department of Energy under Contract No. DE-AC-03-76SF00098. References [1] CDF Collaboration, F. Abe et al., Phys. Rev. Lett. 74, 2626 (1995); D0 Collaboration, S... of Cambridge, Madingley Road, Cambridge CB3 0HE, UK bNuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA and Physics Department, University of California at Davis, Davis, CA 95616, USA Abstract We calculate next...

Kidonakis, Nikolaos; Vogt, Ramona

349

Data:F96b42f3-f536-4df3-9bd4-8871e9e3d5c6 | Open Energy Information  

Open Energy Info (EERE)

b42f3-f536-4df3-9bd4-8871e9e3d5c6 b42f3-f536-4df3-9bd4-8871e9e3d5c6 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Maui Electric Co Ltd Effective date: 2013/07/01 End date if known: 2013/07/30 Rate name: Maui-SCHEDULE "Q" Purchases From Qualifying Facilities - 100 KW or Less - Three Phase Sector: Commercial Description: Availability: This schedule is available to customers with cogeneration and/or small power production facilities which qualify under the commission's Rules, Chapter 74 of Title 6, Subchapter 2 with a design capacity of 100 kilowatts or less. Such qualifying facilities (QF's) shall be designed to operate properly in parallel with the Company's system without adversely affecting the operations of its customers and without presenting safety hazards to the Company's or other customer's personnel. The customer shall comply with the Company's requirements for customer generation interconnected with the utility system.

350

s027.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

Free Free Quark Searches A REVIEW GOES HERE - Check our WWW List of Reviews Quark Production Cross Section - Accelerator Searches Quark Production Cross Section - Accelerator Searches Quark Production Cross Section - Accelerator Searches Quark Production Cross Section - Accelerator Searches X-SECT CHG MASS ENERGY (cm 2 ) (e/3) (GeV) (GeV) BEAM EVTS DOCUMENT ID TECN <1.3E- 36 ± 2 45-84 130-172 e + e - 0 ABREU 97D DLPH <2.E- 35 + 2 250 1800 p p 0 1 ABE 92J CDF <1.E- 35 + 4 250 1800 p p 0 1 ABE 92J CDF <3.8E- 28 14.5A 28 Si-Pb 0 2 HE 91 PLAS <3.2E- 28 14.5A 28 Si-Cu 0 2 HE 91 PLAS <1.E- 40 ± 1,2 <10 p,ν,ν 0 BERGSMA 84B CHRM <1.E- 36 ± 1,2 <9 200 µ 0 AUBERT 83C SPEC <2.E- 10 ± 2,4 1-3 200 p 0 3 BUSSIERE 80 CNTR <5.E- 38 + 1,2 >5 300 p 0 4,5 STEVENSON 79 CNTR <1.E- 33 ± 1 <20 52 p p 0 BASILE 78 SPEC <9.E- 39 ± 1,2 <6 400 p 0 4 ANTREASYAN 77 SPEC <8.E- 35 + 1,2 <20 52 p p 0 6 FABJAN

351

s027.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

Free Free Quark Searches NODE=S027 A REVIEW GOES HERE - Check our WWW List of Reviews NODE=S027 Quark Production Cross Section - Accelerator Searches Quark Production Cross Section - Accelerator Searches Quark Production Cross Section - Accelerator Searches Quark Production Cross Section - Accelerator Searches NODE=S027C NODE=S027C X-SECT CHG MASS ENERGY (cm 2 ) (e/3) (GeV) (GeV) BEAM EVTS DOCUMENT ID TECN <1.3E- 36 ± 2 45-84 130-172 e + e - 0 ABREU 97D DLPH <2.E- 35 + 2 250 1800 p p 0 1 ABE 92J CDF OCCUR=2 <1.E- 35 + 4 250 1800 p p 0 1 ABE 92J CDF <3.8E- 28 14.5A 28 Si-Pb 0 2 HE 91 PLAS OCCUR=2 <3.2E- 28 14.5A 28 Si-Cu 0 2 HE 91 PLAS <1.E- 40 ± 1,2 <10 p,ν,ν 0 BERGSMA 84B CHRM <1.E- 36 ± 1,2 <9 200 µ 0 AUBERT 83C SPEC <2.E- 10 ± 2,4 1-3 200 p 0 3 BUSSIERE 80 CNTR <5.E- 38 + 1,2 >5 300 p 0 4,5 STEVENSON 79 CNTR <1.E- 33 ± 1 <20 52 p p 0 BASILE 78 SPEC <9.E- 39 ± 1,2 <6 400

352

Press Pass - Press Release - CDF B_s  

NLE Websites -- All DOE Office Websites (Extended Search)

8 8 September 13, 2006 Media Contacts: Fermilab - Mike Perricone, mikep@fnal.gov, 630-840-3351 CERN - James Gillies, James.gillies@cern.ch, + 41 22 76 74101 For immediate release Fermilab contributions help CMS magnet reach full field at CERN Tests show CMS detector will be ready for data at European particle physics laboratory BATAVIA, Illinois - Scientists of the U.S. Department of Energy/Office of Science's Fermi National Accelerator Laboratory and collaborators of the US/CMS project have joined colleagues from around the world in announcing that the world's largest superconducting solenoid magnet has reached full field strength in tests at CERN, the European Particle Physics Laboratory. Weighing in at more than 13,000 tons, the Compact Muon Solenoid experiment's magnet is built around a 20-foot-diameter, nearly 43-foot-long superconducting solenoid - a wire coil with multiple loops, which generates a magnetic field when electricity passes through it. The CMS solenoid generates a magnetic field of 4 Tesla, some 100,000 times stronger than the Earth's magnetic field, and stores 2.5 gigajoules of energy, enough to melt nearly 20 tons of gold. Superconductivity is achieved by chilling the coil to a temperature near absolute zero, where virtually all electrical resistance vanishes. Extremely high electrical current can then be used to generate a powerful magnetic field.

353

SCIPP 07/12 CDF/PUB/EXOTIC/PUBLIC/8837  

E-Print Network (OSTI)

FERMILAB-CONF-09-675-E Search for a Low Mass Standard Model Higgs Boson at D? in ppbar Collisions combined searches for the Low Mass Standard Model Higgs boson at a center-of-mass energy of s =1.96 Te Collider Physics Symposium, Evian : France (2009)" #12;Search for a Low Mass Standard Model Higgs Boson

California at Santa Cruz, University of

354

Aging in the large CDF axial drift chamber  

DOE Green Energy (OSTI)

The Central Outer Tracker (COT) is a large axial drift chamber in the Collider Detector at Fermilab operating with a gas mixture that is 50/50 argon/ethane with an admixture of 1.7% isopropanol. In its first two years of operation the COT showed unexpected aging with the worst parts of the chamber experiencing a gain loss of {approx}50% for an accumulated charge of {approx}35 mC/cm. By monitoring the pulse height of hits on good tracks, it was possible to determine the gain as a function of time and location in the chamber. In addition, the currents of the high voltage supplies gave another monitor of chamber gain and its dependence on the charge deposition rate. The aging was worse on the exhaust end of the chamber consistent with polymer buildup as the gas flows through the chamber. The distribution in azimuth suggests that aging is enhanced at lower temperatures, but other factors such as gas flow patterns may be involved. Elemental and molecular analysis of the sense wires found a coating that is mostly carbon and hydrogen with a small amount of oxygen; no silicon or other contaminants were identified. High resolution electron microscope pictures of the wire surface show that the coating is smooth with small sub-micron nodules. In the course of working with the chamber gas system, we discovered a small amount of O{sub 2} is enough to reverse the aging. Operating the chamber with {approx}100 ppm of O{sub 2} reversed almost two years of gain loss in less than 10 days while accumulating {le} 2 mC/cm.

Allspach, D.; Ambrose, D.; Binkley, M.; /Fermilab; Bromberg, C.; /Michigan State U.; Burkett, K.; Kephart, R.; Madrak, R.; Miao, T.; Mukherjee, A.; Roser, R.; Wagner, R.L. /Fermilab

2004-12-01T23:59:59.000Z

355

Analysis of B [sigma] flavor oscillations at CDF  

E-Print Network (OSTI)

The search for and the study of flavor oscillations in the neutral B,B, meson system is an experimentally challenging endeavor. This constitutes a flagship analysis of the Tevatron proton-antiproton collider physics program. ...

Leonardo, Nuno Teotnio Viegas Guerreiro

2007-01-01T23:59:59.000Z

356

Triggering on B-jets at CDF II  

Science Conference Proceedings (OSTI)

In this paper we present a trigger algorithm able to select online events enriched of b-jets. This feature is of central interest in order to extend the physics reach for standard model and minimal super symmetric model Higgs decaying into a pair of b-quarks. The algorithm fully exploits the recently upgraded CDFII tracking system and Level 2 CALorimeter cluster finder. These upgrades are necessary to cope with Tevatron increasing luminosity and provide new and refined trigger primitives that are the key elements of our algorithm together with the already existing silicon vertex trigger. A b-hadron can travel some millimeters before decaying and the trigger algorithm exploits this characteristic by searching for tracks displaced with respect to the primary vertex and matched to energetic jets of particles. We discuss the study and the optimization of the algorithm, its technical implementation as well as its performance. The new trigger provides an efficient selection for Higgs decaying into a pair of b-quarks and runs up to high luminosity with an acceptable occupancy of the available bandwidth.

Amerio, Silvia; /Padua U. /INFN, Padua; Casarsa, Massimo; /Fermilab; Cortiana, Giorgio; /Padua U. /INFN, Padua; Donini, Julien; /Padua U. /INFN, Padua; Lucchesi, Donatella; /Padua U. /INFN, Padua; Pagan Griso, Simone; /Padua U. /INFN, Padua

2009-01-01T23:59:59.000Z

357

Data:19bf399a-be80-4574-997d-760bfe855491 | Open Energy Information  

Open Energy Info (EERE)

be80-4574-997d-760bfe855491 be80-4574-997d-760bfe855491 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Clintonville, Wisconsin (Utility Company) Effective date: 2006/05/05 End date if known: Rate name: Cp-2 Large Power Time-of-Day Service Transformer Ownership Discount with Parallel Generation(20kW or less) Sector: Industrial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kWh of sales) is greater or lesser than the base cost of power purchased (per kWh of sales). The base cost of power is $0.0680 per kWh. See schedule PCAC.

358

s091.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

c c I (J P ) = 0(0 - ) I, J, P need confirmation. Quantum numbers shown are quark-model predictions. B ± c MASS B ± c MASS B ± c MASS B ± c MASS VALUE (GeV) DOCUMENT ID TECN COMMENT 6.2745± 0.0018 OUR AVERAGE 6.2745± 0.0018 OUR AVERAGE 6.2745± 0.0018 OUR AVERAGE 6.2745± 0.0018 OUR AVERAGE 6.2737± 0.0013 ± 0.0016 1 AAIJ 12AV LHCB p p at 7 TeV 6.2756± 0.0029 ± 0.0025 2 AALTONEN 08M CDF p p at 1.96 TeV 6.300 ± 0.014 ± 0.005 2 ABAZOV 08T D0 p p at 1.96 TeV 6.4 ± 0.39 ± 0.13 3 ABE 98M CDF p p at 1.8 TeV * * * We do not use the following data for averages, fits, limits, etc. * * * 6.2857± 0.0053 ± 0.0012 2 ABULENCIA 06C CDF Repl. by AALTONEN 08M 6.32 ± 0.06 4 ACKERSTAFF 98O OPAL e + e - → Z 1 AAIJ 12AV uses the B(c) + → J/ψ π + mode and also measures the mass difference M(B(c) + ) - M(B + ) = 994.6 ± 1.3 ± 0.6 MeV/c 2 . 2 Measured using a fully reconstructed decay mode of B c → J/ψ π. 3 ABE 98M observed 20.4 + 6.2 - 5.5 events

359

Alloy Design of 9% Cr Steel for High Efficiency Ultra-Supercritical ...  

Science Conference Proceedings (OSTI)

Presentation Title, Alloy Design of 9% Cr Steel for High Efficiency Ultra- Supercritical Power Plants. Author(s), Fujio Abe. On-Site Speaker (Planned), Fujio Abe.

360

Data:B44abe17-bea1-4a77-8752-77ad27b7776a | Open Energy Information  

Open Energy Info (EERE)

7-bea1-4a77-8752-77ad27b7776a 7-bea1-4a77-8752-77ad27b7776a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Mascoutah, Illinois (Utility Company) Effective date: 2011/05/01 End date if known: Rate name: Municipal Street Lighting Service- Rate 6: Mercury Vapor, 11000 Lumen, 250 watts, Class A Sector: Lighting Description: Class A: Sodium Vapor or Mercury Vapor Lamps, owned and operated by Municipality. Source or reference: Rates Binder 1, Illinois State University Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh):

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


361

Data:31c93993-08e1-4096-abe1-50fb4ebe4dd3 | Open Energy Information  

Open Energy Info (EERE)

Clean Energy Analysis Low Emission Development Strategies Oil & Gas Smart Grid Solar U.S. OpenLabs Utilities Water Wind Page Actions View form View source History View New Pages...

362

Data:0c463386-a7f7-467a-bee0-224e7c5fde8a | Open Energy Information  

Open Energy Info (EERE)

Large Power Service LP-1 Sector: Commercial Description: Available to Texas Eastern Pipeline Company. Minimum Charge of 1.00 per KVA of installed transformer capacity Source or...

363

Data:F36c9062-8dc9-45c2-9731-abe3f5430e0c | Open Energy Information  

Open Energy Info (EERE)

Lighting Description: APPLICABILITY: Applicable for street, roadway, and general area lighting service under the provisions of the Company's standard contract for such service....

364

Data:6dc1030a-abed-4dfe-b2f9-d75fab35a251 | Open Energy Information  

Open Energy Info (EERE)

LIGHT SERVICE (400W MH) Sector: Lighting Description: Additional fees for poles and transformers may apply Source or reference: ISU Documentation Source Parent: Comments...

365

Anomalous Temperature Dependence of Solvent-Enhanced Dye Diffusion In Polymer T. Graves-Abe, F. Pschenitzka, J.C. Sturm  

E-Print Network (OSTI)

to pattern full color polymer Organic Light-Emitting Diode (OLED) displays is to print dye from a pre. INTRODUCTION The desire to fabricate large-area Organic Light-Emitting Diode (OLED) displays has been a central

366

Data:6d3ca0ab-abe4-4ee6-a1fe-23e3ef5cbab9 | Open Energy Information  

Open Energy Info (EERE)

name: General Service Demand - Load Factor 65%-69% Sector: Commercial Description: Total Energy Charge Usage charge + Power cost adjustment charge 0.10611 0.06127 0.04484...

367

Search for the Higgs Boson Produced in Association with a W Boson at CDF Run II.  

E-Print Network (OSTI)

??We present a search for standard model Higgs boson production in association with a W boson in proton-antiproton collisions (pp? ? WH ? ??bb?) at (more)

Slaunwhite, Jason M.

2009-01-01T23:59:59.000Z

368

Evaluation of candidate photomultiplier tubes for the upgrade of the CDF end plug calorimeter  

SciTech Connect

The Collider Detector at Fermilab is upgrading its end plug calorimeter from a gas detector system to one using scintillating tiles and wavelength shifting fibers. This tile-fiber calorimeter will be read out through 1,824 photomultiplier tubes. The performance requirements of the calorimeter require that the PMTs have good response to light in the 500 nm region, provide adequate amplification for signals from minimum ionizing particles yet provide linear response for peak anode currents up to 25 mA at a gain of 50,000, and fit into the restricted space at the rear of the plugs. This paper will describe the evaluation process used to determine the adequacy of the commercially available PMTs which appeared to meet these performance requirements.

Koska, W.; Delchamps, S.W.; Freeman, J.; Kinney, W.; Lewis, D.; Limon, P.; Strait, J. [Fermi National Accelerator Lab., Batavia, IL (United States); Fiori, I. [Univ. of Bologna (Italy); Gallinaro, M. [Univ. of Padova (Italy); Shen, Q. [Purdue Univ., West Lafayette, IN (United States)

1994-01-01T23:59:59.000Z

369

Search for the Higgs Boson in the ZH ? ?^+?-bb? Channel at CDF Run II.  

E-Print Network (OSTI)

??The Standard Model of particle physics is in excellent agreement with the observed phenomena of particle physics. Within the Standard Model, the weak and electromagnetic (more)

Efron, Jonathan Zvi

2007-01-01T23:59:59.000Z

370

Search for the Higgs Boson in the ZH ? ?^+??bb? Channel at CDF Using Novel Multivariate Techniques.  

E-Print Network (OSTI)

??We present a search for the Standard Model Higgs Boson using the process ZH ? ?+??bb?. We use a dataset corresponding to 9.2/fb-1 of integrated (more)

Pilot, Justin Robert

2011-01-01T23:59:59.000Z

371

Search for the Higgs Boson in the ZH ? vvbb? Channel at CDF Run II.  

E-Print Network (OSTI)

??This analysis focuses on a low mass Higgs boson search with 1.7 fb-1 of data. The focus is on Higgs events in which it is (more)

Parks, Brandon Scott

2008-01-01T23:59:59.000Z

372

Search for the Higgs Boson in the ZH->vvbb Channel at CDF Run II  

SciTech Connect

This analysis focuses on a low mass Higgs boson search with 1.7 fb{sup -1} of data. The focus is on Higgs events in which it is produced in association with a W or Z boson. Such events are expected to leave a distinct signature of large missing transverse energy for either a Z {yields} {nu}{nu} decay or a leptonic W decay in which the lepton goes undetected, as well as jets with taggable secondary vertices from the H {yields} b{bar B} decay. Utilizing a new track based technique for removing QCD multi-jet processes as well as a neural network discriminant, an expected limit of 8.3 times the Standard Model prediction at the 95% CL for a Higgs boson mass of 115 GeV/c{sup 2} is calculated, with an observed limit of 8.0*SM.

Parks, Brandon Scott; /Ohio State U.

2008-07-01T23:59:59.000Z

373

Search for Hadronic Resonances of W/Z in Photon Events at CDF  

SciTech Connect

The authors present a study of the p{bar p} {yields} W(Z){gamma} {yields} {gamma}q{bar q} process at the center-of-mass energy {radical}s = 1.96 TeV using data collected by the Collider Detector at Fermilab. The analysis is based on the selection of low transverse momentum photons produced in association with at least two jets. A modification of an existing photon trigger was studied and implemented in the data acquisition system to enhance the sensitivity of this analysis. The data presented are from approximately 184 pb{sup -1} of integrated luminosity collected by this new trigger. A preliminary event sample is obtained requiring a central photon with E{sub T} > 12 GeV and two jets with E{sub T} > 15 GeV. The corresponding efficiency is studied using a Monte Carlo simulation of the W(Z){gamma} {yields} {gamma}q{bar q} based on Standard Model predictions. Monte Carlo estimation of the background is not necessary as it is measured from the data. A more advanced selection based on a Neural Network method improves the signal-to-noise ratio from 1/333 to 1/71, and further optimization of the dijet mass search region increases the ratio to its final value of 1/41. No evidence of a W/Z {yields} q{bar q} peak in the dijet mass distribution is visible when the background contribution is subtracted. Using a fully Bayesian approach, the 95% confidence level upper limit on {sigma}(p{bar p} {yields} W{gamma}) x {Beta}(W {yields} q{bar q}) + {sigma}(p{bar p} {yields} Z{gamma}) x {Beta}(Z {yields} q{bar q}) is calculated to be 54 pb, which is consistent with the Standard Model prediction of 20.5 pb.

Bocci, Andrea; /Rockefeller U.

2005-01-01T23:59:59.000Z

374

Search for standard model Higgs boson production in association with a W boson at CDF  

E-Print Network (OSTI)

We present a search for the standard model Higgs boson production in association with a W boson in proton-antiproton collisions (pp? ?W[superscript ]H???bb? ) at a center of mass energy of 1.96 TeV. The search employs ...

Bauer, Gerry P.

375

B Flavour Tagging with Artificial Neural Networks for the CDF II Experiment  

SciTech Connect

One of the central questions arising from human curiosity has always been what matter is ultimately made of, with the idea of some kind of elementary building-block dating back to the ancient greek philosophers. Scientific activities of multiple generations have contributed to the current best knowledge about this question, the Standard Model of particle physics. According to it, the world around us is composed of a small number of stable elementary particles: Electrons and two different kinds of quarks, called up and down quarks. Quarks are never observed as free particles, but only as bound states of a quark-antiquark pair (mesons) or of three quarks (baryons), summarized as hadrons. Protons and Neutrons, the constituents forming the nuclei of all chemical elements, are baryons made of up and down quarks. The electron and the electron neutrino - a nearly massless particle without electric charge - belong to a group called leptons. These two quarks and two leptons represent the first generation of elementary particles. There are two other generations of particles, which seem to have similar properties as the first generation except for higher masses, so there are six quarks and six leptons altogether. They were around in large amounts shortly after the beginning of the universe, but today they are only produced in high energetic particle collisions. Properties of particles are described by quantum numbers, for example charge or spin. For every type of particle, a corresponding antiparticle exists with the sign of all charges swapped, but similar properties otherwise. The Standard Model is a very successful theory, describing the properties of all known particles and the interactions between them. Many of its aspects have been tested in various experiments at very high precision. Although none of these experimental tests has shown a significant deviation from the corresponding Standard Model prediction, the theory can not be complete yet: Cosmological aspects like gravity, dark matter and dark energy are not described, and open questions remain in the sector of neutrino masses and neutrino oscillations. Also no answer has been given to the question of matter-antimatter asymmetry observed in the contemporary universe. Assuming that the Big Bang created equal amounts of matter and antimatter, there must be effects where nature treats matter and antimatter somehow different. This can happen through a mechanism called CP violation, which has been observed within the Standard Model, but not in the necessary order of magnitude. For all these reasons, the search for New Physics - theories beyond the Standard Model - is one of the main objectives of modern particle physics. In this global effort, flavour physics is the field of transitions between the different types of quarks, called quark flavours, wherein the examination of B meson oscillations and the search for CP violation in B{sub s}{sup 0} meson decays set the stage for the work presented in this thesis.

Schmidt, Andreas; /Karlsruhe U., EKP

2010-01-01T23:59:59.000Z

376

Search for the Higgs boson in the ZH to llbb channel at CDF Run II  

SciTech Connect

The Standard Model of particle physics is in excellent agreement with the observed phenomena of particle physics. Within the Standard Model, the weak and electromagnetic forces are successfully combined. However, this combination is only valid if the masses of the force carriers of the weak force, the Z and W bosons, are massless. In fact, these two particles are the second and third most massive observed elementary particles. Within the minimal Standard Model, the Higgs mechanism is introduced to reconcile this contradiction. Conclusive proof of this theory would come with the discovery of the Higgs boson.

Efron, Jonathan Zvi; /Ohio State U.

2007-08-01T23:59:59.000Z

377

Search for hadronic resonance in multijet final states with the CDF detector  

SciTech Connect

This thesis describes a search for a new hadronic resonance in 3.2 fb{sup -1} of data using the Collider Detector at Fermilab. The Fermilab Tevatron accelerator collides beams of protons and antiprotons at a center of mass energy of {radical}s = 1.96 TeV. A unique approach is presented to extract multijet resonances from the large QCD background. Although the search is model independent, a pair produced supersymmetric gluino decaying through R-parity violation into three partons each is used to test our sensitivity to new physics. We measure these partons as jets, and require a minimum of six jets in an event. We make use of the kinematic features and correlations and use an ensemble of jet combinations to distinguish signal from multijet QCD backgrounds. Our background estimates also include all-hadronic t{bar t} decays that have a signature similar to signal. We observe no significant excess in an invariant mass range of 77 GeV/c{sup 2} to 240 GeV/c{sup 2} and place 95% C.L. limits on {sigma}(p{bar p} {yields} {tilde g}{tilde g} {yields} 3jets + 3jets) as a function of gluino invariant mass.

Seitz, Claudia; /Rutgers U., Piscataway

2011-01-01T23:59:59.000Z

378

The CDF-II tau physics program triggers, tau ID and preliminary results  

SciTech Connect

The study of processes containing {tau} leptons in the final state will play an important role at Tevatron Run II. Such final states will be relevant both for electroweak studies and measurements as well as in searches for physics beyond the Standard Model. The present paper discusses the physics opportunities and challenges related to the implementation of new set of triggers able to select events containing tau candidates in the final state. They illustrate, in particular, the physics capabilities for a variety of new physics scenarios such as supersymmetry (SUSY), SUSY with Rp-parity violation, with Bilinear parity violation or models with the violation of lepton flavor. Finally, they present the first Run II results obtained using some of the described tau triggers.

C. Pagliarone et al.

2003-11-03T23:59:59.000Z

379

BARTLT SUBROUTINE BARTLT (VAR,DF,N,CH2,CH2CDF ...  

Science Conference Proceedings (OSTI)

... EPS,IFLAG,CDFY) CDFX = 0.5*(1.0+SIGN(CDFY,X)) RETURN C END *CENSCL SUBROUTINE CENSCL (X,W,N1,N2,IOPT,ITER,P1TAIL,CENTER ...

2012-07-27T23:59:59.000Z

380

THE ARROW FRAMEWORK FOR A BUILDING OBJECT WAREHOUSE Leonard Newnham1  

E-Print Network (OSTI)

. [Par96a] Parand, F., The Construction Information Gateway Demonstrator, CIBSE Journal, vol. [Par96b

Amor, Robert

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


381

For Physicists  

NLE Websites -- All DOE Office Websites (Extended Search)

CDF Leo Bellantoni Sum 99 CKM Doug Glenzinski Sum 99 CDF Rick Tesarek Sum 99 CDF Hogan Nguyen June 98 KTeVCKM Peter Wilson June 98 CDF Sergei Nagaitsev Jun 98 Accel Steve Vejcik...

382

Data:F590e4f9-fe5e-4b8a-be3d-ab2b59c121de | Open Energy Information  

Open Energy Info (EERE)

rate Sector: Residential Description: Closed to New Accounts Energy adjustment base average 0.054kwh (E.A. base would vary each month based on projected power costs. Source...

383

Search for the standard model Higgs boson produced in association with top quarks using the full CDF data set  

E-Print Network (OSTI)

A search is presented for the standard model Higgs boson produced in association with top quarks using the full Run II proton-antiproton collision data set, corresponding to 9.45 inverse fb, collected by the Collider Detector at Fermilab. No significant excess over the expected background is observed, and 95% credibility-level upper bounds are placed on the cross section sigma(t\\bar{t}H --> lepton + missing transverse energy + jets). For a Higgs boson mass of 125 GeV, we expect to set a limit of 12.6, and observe a limit of 20.5 times the standard model rate. This represents the most sensitive search for a standard model Higgs boson in this channel to date.

The CDF Collaboration

2012-08-13T23:59:59.000Z

384

Measurement of the WW+WZ Production Cross Section Using the Lepton+Jets Final State at CDF II  

SciTech Connect

We report two complementary measurements of the diboson (WW + WZ) cross section in the final state consisting of an electron or muon, missing transverse energy, and jets, performed using p{bar p} collision data at {radical}s = 1.96 TeV collected by the Collider Detector at Fermilab. The first method uses the dijet invariant mass distribution while the second method uses more of the kinematic information in the event through matrix-element calculations of the signal and background processes and has a higher sensitivity. The result from the second method has a signal significance of 5.4{sigma} and is the first observation of WW + WZ production using this signature. Combining the results from both methods gives {sigma}{sub WW+WZ} = 16.0 {+-} 3.3 pb, in agreement with the standard model prediction.

Aaltonen, T.; /Helsinki Inst. of Phys.; Adelman, J.; /Chicago U., EFI; Alvarez Gonzalez, B.; /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U.; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Apresyan, A.; /Purdue U.; Arisawa, T.; /Waseda U. /Dubna, JINR

2009-11-01T23:59:59.000Z

385

A Search For The Sm Higgs Boson In The Process Zhllbb In 4.1/fb Of Cdf Ii Data.  

E-Print Network (OSTI)

??This dissertation presents a search for the standard model (SM) Higgs boson in the associated production process ZH ? l+l- bb using 4.1fb-1 of Tevatron (more)

Shalhout, Shalhout Zaki

2010-01-01T23:59:59.000Z

386

X-Ray Diffraction Study of MBE-Grown CaF2-CdF2 Superlattices on ...  

Science Conference Proceedings (OSTI)

About this Abstract. Meeting, 13th International Conference on Defects-- Recognition, Imaging and Physics in Semiconductors. Symposium, 13th International...

387

Search for the Higgs boson in the all-hadronic final state using the CDF II detector  

E-Print Network (OSTI)

We report on a search for the production of the Higgs boson decaying to two bottom quarks accompanied by two additional quarks. The data sample used corresponds to an integrated luminosity of approximately 4??fb[superscript ...

Bauer, Gerry P.

388

Search for the Standard Model Higgs Boson Produced in Association with Top Quarks Using the Full CDF Data Set  

E-Print Network (OSTI)

A search is presented for the standard model Higgs boson produced in association with top quarks using the full Run II proton-antiproton collision data set, corresponding to 9.45??fb[superscript -1], collected by the ...

Gomez-Ceballos, Guillelmo

389

Search for standard model Higgs boson production in association with a W boson using a neural network discriminant at CDF  

E-Print Network (OSTI)

We present a search for standard model Higgs boson production in association with a W boson in proton-antiproton collisions (pp??W[superscript ]H???bb?) at a center of mass energy of 1.96 TeV. The search employs data ...

Xie, Si

390

Search for the standard model Higgs boson produced in association with top quarks using the full CDF data set  

Science Conference Proceedings (OSTI)

A search is presented for the standard model Higgs boson produced in association with top quarks using the full Run II proton-antiproton collision data set, corresponding to 9.45 fb{sup -1}, collected by the Collider Detector at Fermilab. No significant excess over the expected background is observed, and 95% credibility-level upper bounds are placed on the cross section {sigma}(t{bar t}H {yields} lepton + missing transverse energy + jets). For a Higgs boson mass of 125 GeV/c{sup 2}, we expect to set a limit of 12.6, and observe a limit of 20.5 times the standard model rate. This represents the most sensitive search for a standard model Higgs boson in this channel to date.

Aaltonen, T.; /Helsinki Inst. of Phys.; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U. /Fermilab; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Arisawa, T.; /Waseda U.; Artikov, A.; /Dubna, JINR /Texas A-M

2012-08-01T23:59:59.000Z

391

Supporting Computational Data Model Representation with High-performance I/O in Parallel netCDF  

E-Print Network (OSTI)

staycompetitive Argonne Leadership Computing Facility industry@alcf.anl.gov #12;MIRA RANKS third on the TOP500, and create more accurate models for your business with Mira, the ALCF's new petascale IBM Blue Gene/Q system, ALCF Science Director CUTTING-EDGE SUPERCOMPUTING KEEPS YOU COMPETITIVE A key driver of our nation

Choudhary, Alok

392

Using Drell-Yan to probe the underlying event in Run II at Collider Detector at Fermilab (CDF)  

SciTech Connect

We study the behavior of charged particles produced in association with Drell-Yan lepton-pairs in the region of the Z-boson in proton-antiproton collisions at 1.96 TeV. We use the direction of the Z-boson in each event to define 'toward', 'away', and 'transverse' regions. For Drell-Yan production (excluding the leptons) both the 'toward' and 'transverse' regions are very sensitive to the 'underlying event', which is defined as everything except the two hard scattered components. The data are corrected to the particle level and are then compared with several PYTHIA models (with multiple parton interactions) and HERWIG (without multiple parton interactions) at the particle level (i.e. generator level). The data are also compared with a previous analysis on the behavior of the 'underlying event' in high transverse momentum jet production. The goal is to produce data that can be used by the theorists to tune and improve the QCD Monte-Carlo models of the 'underlying event' that are used to simulate hadron-hadron collisions.

Kar, Deepak; /Florida U.

2008-12-01T23:59:59.000Z

393

Fermilab Today | Result of the Week Archive | 2004  

NLE Websites -- All DOE Office Websites (Extended Search)

4 December 16, 2004 DZero Search for a Light Higgs Boson DZero DZero December 9, 2004 How Small is an Electron? CDF CDF December 3, 2004 CDF Sees Charmed Beauty Meson in a New...

394

Ethnicity, Employment and Migration  

E-Print Network (OSTI)

ABCDEG][CF]5 >EFG][ABCDEGJ[ACF][BCF][CDF][ CEF][CFG] >EFG][ABCDEG][ACFJ[CDF][CEF][CFG] >EFG][ABCDEGJ[ACF][BCF][CEF][CFG] 1EFGJ[ABCDEGJ[ACF][BCFJ[CDF][CFG] 1EFG][ABCDEGJ[ACF][

Wilson, Franklin D.; Tienda, Marta

1988-01-01T23:59:59.000Z

395

Fermilab Today  

NLE Websites -- All DOE Office Websites (Extended Search)

CDF control room. NAME: Harvard University HOME TOWN: Cambridge, MA MASCOT: Harvard Pilgrim SCHOOL COLORS: Crimson PARTICLE PHYSICS COLLABORATIONS: ATLAS, CDF, MINOS, NOvA and...

396

For Physicists  

NLE Websites -- All DOE Office Websites (Extended Search)

1211 University of Pisa CDF CERN Wade Fisher 505 - 809 Princeton University DZero Michigan State University Ricardo Eusebi 406 - 809 University of Rochester CDF Texas A & M...

397

Development and validation of compressible mixture viscous fluid algorithm applied to predict the evolution of inertial fusion energy chamber gas and the impact of gas on direct-drive target survival  

E-Print Network (OSTI)

green) and thermal energy (gray) . . . . . . . . . . .is the temperature of the thermal energy of the system at abe exchanged with the thermal energy and dissipated through

Martin, Robert Scott

2011-01-01T23:59:59.000Z

398

Slide 1  

NLE Websites -- All DOE Office Websites (Extended Search)

MRCSP Michigan Basin Test Site Jacqueline Gerst, Battelle Regional Carbon Sequestration Partnerships Annual Review November 16-19, 2009 2 Acknowledgements- Project Team Abed...

399

A High Frequency Isolated Current-fed Bidirectional DC/AC Converter For Grid-Tied Energy Storage System  

E-Print Network (OSTI)

AC Converter for Grid-tied Energy Storage System Xiaolei Hu,resources, grid-tied energy storage systems voltage to abe increasingly incorporated. Energy storage devices allows

King Jet, Tseng

2013-01-01T23:59:59.000Z

400

PowerPoint Presentation  

NLE Websites -- All DOE Office Websites (Extended Search)

Owners Engineer Perspective * McAbee Construction * Pilot fab and installation * EPRI o Technical Advisor o Cost Share o Independent Performance Evaluation and Techno-...

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


401

PowerPoint Presentation  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

- Chuck Herman and Guy Sliker * NGK - Hiroyuke Abe * EPRI funders (Con Edison, CPS Energy, HECO, Hydro One, NYISO, SDG&E, and TVA) 3 2009 Electric Power Research...

402

Measurement of the difference of CP--violating asymmetries in $D^0 \\to K^+K^-$ and $D^0 \\to \\pi^+\\pi^-$ decays at CDF  

Science Conference Proceedings (OSTI)

We report a measurement of the difference (D/Acp) between time-integrated-violating asymmetries in D{sup 0} K{sup +}K{sup -} and D{sup 0} {pi}{sup +}{pi}{sup -} decays reconstructed in the full data set of proton-antiproton collisions collected by the Collider Detector at Fermilab, corresponding to 9.7 fb{sup -1} of integrated luminosity. The strong decay D*{sup +} D{sup 0}{pi}{sup +} is used to identify the charm meson at production as D{sup 0} or ['D]{sup 0}. We measure D/Acp = (-0.62 0.21 /stat 0.10 /syst)%, which differs from zero by 2.7 Gaussian standard deviations. This result supports similar evidence for violation in charm-quark obtained in proton-proton collisions.

Aaltonen, T.; /Helsinki Inst. of Phys.; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U. /Fermilab; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Arisawa, T.; /Waseda U.; Artikov, A.; /Dubna, JINR /Texas A-M

2012-07-01T23:59:59.000Z

403

Data:52cdf4fe-b6ca-4ac3-a860-bd9b3ff64e82 | Open Energy Information  

Open Energy Info (EERE)

fe-b6ca-4ac3-a860-bd9b3ff64e82 fe-b6ca-4ac3-a860-bd9b3ff64e82 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Elroy, Wisconsin (Utility Company) Effective date: 2009/01/22 End date if known: Rate name: Cp-2 Large Power Service between 100kW and 500kW Demand Transformer Ownership Discount Sector: Industrial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0510 per kilowatt-hour.

404

Data:1c2cdf4a-fbb6-4b3d-9e7d-8d289f34238c | Open Energy Information  

Open Energy Info (EERE)

a-fbb6-4b3d-9e7d-8d289f34238c a-fbb6-4b3d-9e7d-8d289f34238c No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Black Warrior Elec Member Corp Effective date: 2013/09/01 End date if known: Rate name: Outdoor Lighting Service (250 W Mercury Vapor) Sector: Lighting Description: Source or reference: ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous

405

Data:Cdf08225-b220-41ff-9b6a-b30f56c8ae49 | Open Energy Information  

Open Energy Info (EERE)

8225-b220-41ff-9b6a-b30f56c8ae49 8225-b220-41ff-9b6a-b30f56c8ae49 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Northern States Power Co - Wisconsin Effective date: 2011/01/01 End date if known: Rate name: Experimental Advanced Renewable Energy Purchase Service Wind Tier 1: 100 kW (at less than 200 amps) Sector: Description: Effective In All territories served by the Company. Definition: Distributed generation facilities are electricity generators owned by the customer, located R close to the point of energy consumption, and small in scale, usually no more than the existing load of the customer. Availability The advanced renewable energy tariff is available to retail customers who own small distributed generation facilities that are powered by a renewable resource and placed in initial service after January 1, 2012, or who executed an advanced renewable energy contract prior to January 1, 2012. maximum size project per customer is: Wind: * Tier 1: 100 kw * Tier 2: 2 MW * Tier 3: 5 MW (Community-based Projects) Community-based Limits The Community-based Project Category is only applicable to the Biomass/Biogas and Wind technology categories and will be fully subscribed when 5 MW of capacity has been subscribed. In addition, the Community-based Category is applicable only to projects owned by local units of government (Village, City, Town or County), or to projects majority-owned by existing retail customers that choose to join together to develop a joint project.

406

Data:8c6cdf6b-6965-4b54-9386-ed4d405615c7 | Open Energy Information  

Open Energy Info (EERE)

b-6965-4b54-9386-ed4d405615c7 b-6965-4b54-9386-ed4d405615c7 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Mascoutah, Illinois (Utility Company) Effective date: 2011/05/01 End date if known: Rate name: Customer Area Lighting Service- Rate 7: Directional Lighting, Quartz, 500 Watt Sector: Lighting Description: Source or reference: Rates Binder 1, Illinois State University Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category:

407

Data:Df1cdf6a-6509-4f6b-82f4-95923849b2ad | Open Energy Information  

Open Energy Info (EERE)

a-6509-4f6b-82f4-95923849b2ad a-6509-4f6b-82f4-95923849b2ad No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Walton Electric Member Corp Effective date: 2006/06/01 End date if known: Rate name: Cobrahead- HPS 250 Watt Gray Sector: Lighting Description: Source or reference: http://www.waltonemc.com/commercial/ Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >> << Previous

408

Data:9235f77b-f320-4bda-9e2e-cdf2a6f52836 | Open Energy Information  

Open Energy Info (EERE)

Elec Coop, Inc Effective date: 20120101 End date if known: Rate name: Outdoor & Street Light 400 W ( Energy Only, Owned and Maintained by Member) Sector: Lighting...

409

CDF/PUB/EXOTIC/PUBLIC/8887, FERMILAB-PUB-07-567-E, SCIPP 07/15 Search for Standard Model Higgs Bosons Produced in  

E-Print Network (OSTI)

Wayne State University, Detroit, Michigan 48201 58 University of Wisconsin, Madison, Wisconsin 53706 59

California at Santa Cruz, University of

410

Measurement of CP--violating asymmetries in $D^0\\to\\pi^+\\pi^-$ and $D^0\\to K^+K^-$ decays at CDF  

SciTech Connect

We report on a measurement of CP-violating asymmetries (A{sub CP}) in the Cabibbo-suppressed D{sup 0} {yields} {pi}{sup +}{pi}{sup -} and D{sup 0} {yields} K{sup +}K{sup -} decays reconstructed in a data sample corresponding to 5.9 fb{sup -1} of integrated luminosity collected by the upgraded Collider Detector at Fermilab. We use the strong decay D*{sup +} {yields} D{sup 0}{pi}{sup +} to identify the flavor of the charmed meson at production and exploit CP-conserving strong c{bar c} pair-production in p{bar p} collisions. High-statistics samples of Cabibbo-favored D{sup 0} {yields} K{sup -}{pi}{sup +} decays with and without a D*{sup {+-}} tag are used to correct for instrumental effects and significantly reduce systematic uncertainties. We measure A{sub CP}(D{sup 0} {yields} {pi}{sup +}{pi}{sup -}) = (+0.22 {+-} 0.24(stat) {+-} 0.11 (syst))% and A{sub CP}(D{sup 0} {yields} K{sup +}K{sup -}) = (-0.24 {+-} 0.22 (stat) {+-} 0.09 (syst))%, in agreement with CP conservation. These are the most precise determinations from a single experiment to date. Under the assumption of negligible direct CP violation in D{sup 0} {yields} {pi}{sup +}{pi}{sup -} and D{sup 0} {yields} K{sup +}K{sup -} decays, the results provide an upper limit to the CP-violating asymmetry in D{sup 0} mixing, |A{sub CP}{sup ind}(D{sup 0})| < 0.13% at the 90% confidence level.

Aaltonen, T.; /Helsinki Inst. of Phys.; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U. /Fermilab; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Arisawa, T.; /Waseda U.; Artikov, A.; /Dubna, JINR /Texas A-M

2011-11-01T23:59:59.000Z

411

Measurement of R = B(t?Wb)/B(t?Wq) in top-quark-pair decays using lepton+jets events and the full CDF run II dataset  

E-Print Network (OSTI)

We present a measurement of the ratio of the top-quark branching fractions R=B(t?Wb)/ B(t?Wq), where q represents quarks of type b, s, or d, in the final state with a lepton and hadronic jets. The measurement uses ?s=1.96??TeV ...

Gomez-Ceballos, Guillelmo

412

Search for the Higgs boson produced in association with Z-->l^{+}l^{-} using the matrix element method at CDF II  

E-Print Network (OSTI)

We present a search for associated production of the standard model Higgs boson and a Z boson where the Z boson decays to two leptons and the Higgs decays to a pair of b quarks in pp? collisions at the Fermilab Tevatron. ...

Xie, Si

413

Agreement between the California Department of Foresty Firefighters (CDF), Bargaining Unit 8 Firefighter and the State of California, 1999-2001  

E-Print Network (OSTI)

days. Thirteen hours of standby may be scheduled on one dutyall of their assigned standby hours. Overtime Compensation72 Shift Pattern 1 Work Standby Shift Pattern 2 Work Standby

California Department of Foresty Firefighters (CDF), Bargaining Unit 8 Firefighter

1999-01-01T23:59:59.000Z

414

Data:30ca49da-ff76-4152-b19c-ab94cdf836fc | Open Energy Information  

Open Energy Info (EERE)

than 1,300 kW, measured on a 60-minute interval basis. Fixed Monthly Charge Includes a Energy Optimization Surcharge The Company's Net Metering Program is available on a first...

415

Data:B52beee3-2caf-49be-be1d-123a50cdf951 | Open Energy Information  

Open Energy Info (EERE)

three-phase customers who demonstrate to management's satisfaction that the majority of energy usage will occur off-peak. Peak hours shall be determined in the same manner they...

416

Data:1cdf593c-4338-4f5f-a8c7-60fb4bed4a18 | Open Energy Information  

Open Energy Info (EERE)

338-4f5f-a8c7-60fb4bed4a18 338-4f5f-a8c7-60fb4bed4a18 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Trico Electric Cooperative Inc Effective date: 2009/08/01 End date if known: Rate name: General Service-GS 1 Three-Phase Sector: Commercial Description: * Applicable to general service less than 10KW. Subject to tax and power cost adjustment. Source or reference: http://www.trico.coop/images/TRICO_GS1.pdf Source Parent: Comments Energy charge($0.1335/KW)= power supply charge($0.0830)+Access charge($0.0505) Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh)

417

Data:42cdf5d9-7b20-4e16-857b-90c5a46fcac2 | Open Energy Information  

Open Energy Info (EERE)

7b20-4e16-857b-90c5a46fcac2 7b20-4e16-857b-90c5a46fcac2 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Consumers Power, Inc Effective date: 2011/10/01 End date if known: Rate name: 150 W HPS, Metered Sector: Lighting Description: * Applicable to customers who receive dusk to dawn area lighting service. Rate when light is metered through customer service. Source or reference: Rate binder # 4(Illinios State University) Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V):

418

Search for B [0 over subscript s]??[superscript +]?[superscript -] and B[superscript 0]??[superscript +]?[superscript -] decays with the full CDF Run II data set  

E-Print Network (OSTI)

We report on a search for B [0 over subscript s]??[superscript +]?[superscript -] and B[superscript 0]??[superscript +]?[superscript -] decays using proton-antiproton collision data at ?s=1.96??TeV corresponding to ...

Gomez-Ceballos, Guillelmo

419

Fermilab | Science at Fermilab | Experiments & Projects | Energy Frontier |  

NLE Websites -- All DOE Office Websites (Extended Search)

CDF DZero Fermilab involvement with the Large Hadron Collider Intensity Frontier Cosmic Frontier Works in Progress CDF silicon vertex detector being installed in 2001 CDF silicon vertex detector being installed in 2001. Drawing of the CDF detector Drawing of the CDF detector. Energy Frontier CDF How it works CDF is one of two detectors positioned along the four-mile Tevatron accelerator ring. Physicists use the detector to study the array of particles and forces within the atom by recording data about collisions of protons and anti-protons in the machine. The 4,500-ton detector sits more than four stories tall and is composed of more than 1 million individual detector elements. Beams of protons and antiprotons collide at the center of CDF at nearly the speed of light, creating flashes of energy that condense into particles

420

Fermilab Today | Results for the Frontiers | 2013  

NLE Websites -- All DOE Office Websites (Extended Search)

2013 CMS: Higgs and top quarks together March 21, 2013 CDF: CDF finalizes combined Higgs boson results March 15, 2013 MINOS: Does matter matter for neutrino flavor? March 14,...

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


421

Fermilab Today  

NLE Websites -- All DOE Office Websites (Extended Search)

The CDF and DZero experiments are pulling out all of the stops in the race for the Higgs boson. CDF recently upgraded its Higgs analysis efforts, like fine tuning a machine, and...

422

Fermilab Today  

NLE Websites -- All DOE Office Websites (Extended Search)

features Fermilab employees Frontier Science Result: CDF: CDF finalizes its combined Higgs boson results From SLAC Today: Hundreds meet at SLAC to discuss future of U.S. particle...

423

Research in elementary particle physics. Technical progress report, June 1, 1991--May 31, 1992  

Science Conference Proceedings (OSTI)

This report discusses research in the following areas of high energy physics: B meson mixing; CDF response to low energy jets; jet scaling behavior; search for pair produced leptoquarks at CDF; SSC program; quantum field theory; and neural networks. (LSP).

Kirsch, L.E.; Schnitzer, H.J.; Bensinger, J.R.; Blocker, C.A.

1992-08-01T23:59:59.000Z

424

Research in elementary particle physics  

Science Conference Proceedings (OSTI)

This report discusses research in the following areas of high energy physics: B meson mixing; CDF response to low energy jets; jet scaling behavior; search for pair produced leptoquarks at CDF; SSC program; quantum field theory; and neural networks. (LSP).

Kirsch, L.E.; Schnitzer, H.J.; Bensinger, J.R.; Blocker, C.A.

1992-01-01T23:59:59.000Z

425

ARM XDC Datastreams  

NLE Websites -- All DOE Office Websites (Extended Search)

cloud products netCDF File Header Description (Data Object Design File) goes12minnis-acf - GOES-12: 0.3 degree cloud products, ARM Central Facility netCDF File Header...

426

262 t< IX ~ I V I S T A - Springer  

Science Conference Proceedings (OSTI)

preparava de!le ]ami~Is set,ill 7 abe poteva poi esaminaro anehe nella hen polarizzata. II topazio del ]3rasiio mostr6 eosl di posse- der% in ogaana dolle sue

427

HETEROGENEOUS CATALYSIS RESEARCH MEETING  

E-Print Network (OSTI)

production of SNG or Fischer-Tropsch products Therefore, abe trying to obtain from Fischer-Tropsch synthesis? Answer:intermediates in Fischer-Tropsch synthesis? Answer: It was

Authors, Various

2011-01-01T23:59:59.000Z

428

President's Message November 2011  

E-Print Network (OSTI)

in moving us forward with a Facebook page and has planned abe applied to the CAL/AAEM Facebook page to automaticallyof interacting with our chapter Facebook site and links with

Mills, Trevor

2011-01-01T23:59:59.000Z

429

Physics at Tevatron Run II  

E-Print Network (OSTI)

We present recent physics results from the Tevatron Collider experiments CDF and D0. (contribution to Lattice 2004)

Daria Zieminska

2004-11-11T23:59:59.000Z

430

Fermilab Today | Result of the Week Archive | 2003  

NLE Websites -- All DOE Office Websites (Extended Search)

3 3 December 18, 2003 DZero Examines True Nature of New Particle December 11, 2003 Search for Leptoquarks with the CDF Detector December 4, 2003 Search for Leptoquarks with the DZero Detector November 20, 2003 The Hunt for Single Top Continues at CDF November 13, 2003 DZero: Are there exotic Higgs particles? November 6, 2003 CDF reports new new measurement of pomeron production ratio October 30, 2003 DZero: Search for SUSY in final states with three leptons October 23, 2003 CDF, DZero publish combined electroweak results October 16, 2003 Matter-Antimatter Mixing at CDF October 9, 2003 Top Quark Production at DZero October 2, 2003 CDF Observes Mystery Meson September 25, 2003 DZero: Hunting for Higgs Has Begun September 18, 2003 DZero: Particle Pairs and Monojets CDF: The Bulk and The Brane

431

Search for the Standard Model Higgs boson in the diphoton final state in proton-antiproton collisions at a center of mass energy of 1.96 TeV using the CDF II detector.  

E-Print Network (OSTI)

??We present a search for the Standard Model Higgs boson decaying into a pair of photons produced in pp ? collisions with a center of (more)

Bland, Karen Renee.

2012-01-01T23:59:59.000Z

432

Data:B6a000cd-f8d1-418f-b0ce-0ac722b650a0 | Open Energy Information  

Open Energy Info (EERE)

Source or reference: http:www.walllake.comindex.php?localsinglebusiness&nid321&catUtilities Assume net metering (buy sell): No Flat rate buy (kWh): Flat rate sell...

433

First observation of the Bs->K+K- decay mode, and measurement of the B0 and Bs mesons decay-rates into two-body charmless final states at CDF  

SciTech Connect

The authors searched for decays of the type B{sub (s)}{sup 0} {yields} h{sup +}h{prime}{sup -} (where h, h{prime} = K or {pi}) in a sample corresponding to 180 pb{sup -1} of p{bar p} collisions at {radical}s = 1.96 TeV, collected by the upgraded Collider Detector at the Fermilab Tevatron. A total signal of approximately 900 events was reconstructed, and the relative branching fractions ({Beta}) of each decay mode were determined with a likelihood fit.

Tonelli, Diego; /Pisa, Scuola Normale Superiore

2006-11-01T23:59:59.000Z

434

Palm Oil Laboratory Proficiency Testing Program  

Science Conference Proceedings (OSTI)

Lab Proficiency Testing provider for Palm Oil determinations via P4.3 PORIM, P4.1 PORIM, P2.5 PORIM, Cd 1d-92, P4.2 PORIM, Cd 96b-93,

435

Amplitude [Sko94]. Amusement [Rud95b].  

E-Print Network (OSTI)

Version 0.05 Title word cross-reference 2 [Tro99c]. 3 [Ful96b, SB94a, SB94b]. n [Fre93a]. p [De 99]. ? [Abb05b].

Nelson H. F. Beebe; Adic [de -queens [frea

2013-01-01T23:59:59.000Z

436

WIPP Shares Expertise with Salt Club Members | Department of Energy  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Shares Expertise with Salt Club Members Shares Expertise with Salt Club Members WIPP Shares Expertise with Salt Club Members November 26, 2013 - 12:00pm Addthis Carlsbad Field Office’s Abe Van Luik, third from right, examines rock salt taken from the Morsleben mine in Germany. Carlsbad Field Office's Abe Van Luik, third from right, examines rock salt taken from the Morsleben mine in Germany. CARLSBAD, N.M. - EM's Carlsbad Field Office (CBFO) participated in the second meeting of the Nuclear Energy Agency's (NEA) Salt Club and the 4th U.S.-German Workshop on Salt Repository Research, Design & Operation in Berlin. CBFO, which has responsibility for the Waste Isolation Pilot Plant (WIPP) and the National Transuranic (TRU) Program, was represented by International Programs and Policy Advisor Dr. Abe Van Luik.

437

ARM XDC Datastreams  

NLE Websites -- All DOE Office Websites (Extended Search)

Documentation FLUXNET Instrument FLUXNET netCDF File Header Descriptions (Data Object Design Files) External Datastream Descriptions Order Data Comments? We would love to hear...

438

Title Slide  

Science Conference Proceedings (OSTI)

... Software size distributions appear power-law in LOC Smoothed (cdf) data for 21 systems, C, Tcl/Tk and Fortran, combining ...

2011-08-15T23:59:59.000Z

439

Diffractive Production of Jets and Vector Bosons at the Tevatron  

E-Print Network (OSTI)

Recent results on diffractive dijet and vector boson production and exclusive dijet production from the Collider Detector at Fermilab (CDF) experiment are presented.

Kenichi Hatakeyama; for the CDF Collaboration

2008-12-08T23:59:59.000Z

440

A search for the standard model Higgs boson produced in association with a W boson.  

E-Print Network (OSTI)

??We present a search for a standard model Higgs boson produced in association with a W boson using data collected with the CDF II detector (more)

Frank, Martin J., 1983-

2011-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


441

Fermilab Today  

NLE Websites -- All DOE Office Websites (Extended Search)

by his CDF colleagues and by the laboratory community." Read his obituary In Brief Gender, race and science education talk at Fermilab Tuesday Although the number of women...

442

ARM XDC Datastreams  

NLE Websites -- All DOE Office Websites (Extended Search)

NCEPGFS Instrument NCEPGFS netCDF File Header Descriptions (Data Object Design Files) External Datastream Descriptions Order Data Comments? We would love to hear from...

443

ARM XDC Datastreams  

NLE Websites -- All DOE Office Websites (Extended Search)

StreamsMultispectral Thermal Imager Documentation MTI Instrument MTI netCDF File Header Descriptions (Data Object Design Files) External Datastream Descriptions Order Data...

444

Fermilab Today  

NLE Websites -- All DOE Office Websites (Extended Search)

pairs. CDF scientists studied this signature for the first time, developing novel techniques to understand and constrain the backgrounds. Unfortunately, from the perspective of...

445

Particle Event Pictures  

NLE Websites -- All DOE Office Websites (Extended Search)

- Identifying Particles - D0 Detector - CDF Detector - Links Project Contact: Thomas Jordan - jordant@fnal.gov Web Maintainer: qnet-webmaster@fnal.gov Last Update: April 13, 2001...

446

Fermilab Today  

NLE Websites -- All DOE Office Websites (Extended Search)

Institute of Physics), Bottom: Yen-Chu Chen (Academia Sinica), Andy Beretvas, G.P. Yeh (Fermilab) (Click on image for larger version.) CDF Top: Julian Budagov, Guram...

447

Fermilab Today  

NLE Websites -- All DOE Office Websites (Extended Search)

for CDF with Rob Roser. Behind the flowery metaphor hides a long, often daunting, laundry list of responsibilities. Spokespeople are responsible for the proper collection,...

448

Fermilab Today | University of Rochester Profile  

NLE Websites -- All DOE Office Websites (Extended Search)

SCHOOL COLORS: Blue and yellow PARTICLE PHYSICS COLLABORATIONS: MINERvA, CDF, DZero, Compact Muon Solenoid, Large Hadron Collider and LPC. EXPERIMENTS AT FERMILAB: In addition to...

449

Press Pass - Press Release - Higgs mass constraints  

NLE Websites -- All DOE Office Websites (Extended Search)

imagesHiggs-mass-constraints-Aug2008.html Tevatron Experiments Double-Team Higgs Boson Joint CDF, DZero effort lands Fermilab in Higgs territory Batavia, Ill.--Scientists...

450

Fermilab Today  

NLE Websites -- All DOE Office Websites (Extended Search)

comments and suggestions to: today@fnal.gov Feature Tevatron experiments double team Higgs boson Scientists from the CDF and DZero collaborations at DOE's Fermilab have combined...

451

Fermilab Today  

NLE Websites -- All DOE Office Websites (Extended Search)

Today Fermilab Press Release Fermilab experiments narrow allowed mass range for Higgs boson Scientists from the CDF and DZero collaborations at DOE's Fermilab have combined...

452

Searches for SUSY at the Tevatron  

Science Conference Proceedings (OSTI)

This paper presents recent results on Supersymmetry searches in various channels from the CDF and D0 experiments at the Tevatron.

Andrei Nomerotski

1998-01-01T23:59:59.000Z

453

ARM XDC Datastreams  

NLE Websites -- All DOE Office Websites (Extended Search)

StreamsMesoscale Analysis and Prediction System Documentation MAPS Instrument MAPS netCDF File Header Descriptions (Data Object Design Files) External Datastream Descriptions Order...

454

Inquiring Minds  

NLE Websites -- All DOE Office Websites (Extended Search)

CDF and DZero detectors, fewer than a thousand events per second pass the highest trigger level for permanent storage, still producing almost 100 megabytes of data written...

455

INSIDE  

NLE Websites -- All DOE Office Websites (Extended Search)

proton-antiproton collisions at the Tevatron. http:www-cdf.fnal.gov CDMS: Cryogenic Dark Matter Search. A Fermilabuniversity experiment to search for the interaction of dark...

456

Combination of tevatron searches for the standard model Higgs Boson for observing antiferromagnetism and superfluidity  

E-Print Network (OSTI)

We combine searches by the CDF and D0 Collaborations for a Higgs boson decaying to W[superscript +]W[superscript -]. The data correspond to an integrated total luminosity of 4.8 (CDF) and 5.4 (D0) fb[superscript -1] of pp? ...

Bauer, Gerry P.

457

Overhearing in 802.11 mesh networks  

E-Print Network (OSTI)

Total transmission time, uSec Figure 3.17: CDF of the totalTotal transmission time, uSec Figure 3.18: CDF of the totalExOR Total transmission time, uSec (a) Jigsaw testbed, whole

Afanasyev, Mikhail

2009-01-01T23:59:59.000Z

458

Technical and economic assessment of processes for the production of butanol and acetone. Phase two: analysis of research advances. Energy Conversion and Utilization Technologies Program  

DOE Green Energy (OSTI)

The initial objective of this work was to develop a methodology for analyzing the impact of technological advances as a tool to help establish priorities for R and D options in the field of biocatalysis. As an example of a biocatalyzed process, butanol/acetone fermentation (ABE process) was selected as the specific topic of study. A base case model characterizing the technology and economics associated with the ABE process was developed in the previous first phase of study. The project objectives were broadened in this second phase of work to provide parametric estimates of the economic and energy impacts of a variety of research advances in the hydrolysis, fermentation and purification sections of the process. The research advances analyzed in this study were based on a comprehensive literature review. The six process options analyzed were: continuous ABE fermentaton; vacuum ABE fermentation; Baelene solvent extraction; HRI's Lignol process; improved prehydrolysis/dual enzyme hydrolysis; and improved microorganism tolerance to butanol toxicity. Of the six options analyzed, only improved microorganism tolerance to butanol toxicity had a significant positive effect on energy efficiency and economics. This particular process option reduced the base case production cost (including 10% DCF return) by 20% and energy consumption by 16%. Figures and tables.

None

1984-08-01T23:59:59.000Z

459

Characterisation of C-F polymer film formation on the air-bearing surface etched sidewall of fluorine-based plasma interacting with AL2O3-TiC substrate  

Science Conference Proceedings (OSTI)

C-F polymer redeposition is generated on the etched sidewall of the patterned air-bearing surface (ABS). This C-F polymer is a byproduct from fluorine-based plasma using a Surface Technology Systems multiplex-pro air-bearing etch (ABE). The morphology ...

Alonggot Limcharoen, Pichet Limsuwan, Chupong Pakpum, Krisda Siangchaew

2013-01-01T23:59:59.000Z

460

Mutant strain of C. acetobutylicum and process for making butanol  

DOE Patents (OSTI)

A biologically pure asporogenic mutant of Clostridium acetobutylicum is produced by growing sporogenic C. acetobutylicum ATCC 4259 and treating the parent strain with ethane methane sulfonate. The mutant which as been designated C. acetobutylicum ATCC 55025 is useful in an improved ABE fermentation process, and produces high concentrations of butanol and total solvents.

Jain, Mahendra K. (Okemos, MI); Beacom, Daniel (East Lansing, MI); Datta, Rathin (Chicago, IL)

1993-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "abe 96b cdf" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


461

Microstructure and Creep Strength of Welds in Advanced Ferritic Power Plant Steels  

E-Print Network (OSTI)

Microstructure and Creep Strength of Welds in Advanced Ferritic Power Plant Steels Fujio ABE) power plant at 650 o C (923 K).1 Critical issues for the development of ferritic steels for 650 o C USC carried out at 650o C (923 K) for up to about 104 h. The creep crack growth tests were also carried out

Cambridge, University of

462

Ciphertext policy attribute-based encryption from lattices  

Science Conference Proceedings (OSTI)

Sahai and Waters [6] proposed Attribute-Based Encryption (ABE) as a new paradigm of encryption algorithms that allow the sender to set a policy describing who can decrypt a particular ciphertext. In this paper, we first propose a ciphertext policy attribute-based ...

Jiang Zhang; Zhenfeng Zhang; Aijun Ge

2012-05-01T23:59:59.000Z

463

Inclusive jet production at Tevatron  

Science Conference Proceedings (OSTI)

The CDF and D0 Collaborations have measured the inclusive jet cross section using 1992--93 collider data at {radical}s = 1,800 GeV. The D0 measurement is higher than NLO QCD predictions, though within systematic uncertainties. The CDF measurement is in very good agreement with NLO QCD predictions for transverse energies (E{sub T}) below 200 GeV. However it is systemically higher than NLO QCD predictions for E{sub T} above 200 GeV. The CDF measurement of two-jet mass and total transverse energy spectra also show a similar excess above QCD predictions at higher E{sub T}.

Bhatti, A.A.; CDF Collaboration; D0 Collaboration

1995-07-01T23:59:59.000Z

464

Algorithmic [Bar06]. Algorithms [Mae94a, Mae96c]. Amplitude [Sko94]. Amusement [Rud95b]. Analysis  

E-Print Network (OSTI)

Version 0.06 Title word cross-reference 2 [Tro99c]. 3 [Ful96b, SB94a, SB94b]. n [Fre93a]. p [De 99]. ? [Abb05b].-adic [De 99].-Queens [Fre93a]. 1 [TiS96]. 1999 [Ker98].

Nelson H. F. Beebe

2013-01-01T23:59:59.000Z

465

FermiNews - March 7, 2003  

NLE Websites -- All DOE Office Websites (Extended Search)

4 In This Issue: A Visit to Tsukuba CDF Approves First Run II Paper DESY Gets OK on TESLA X-Ray Laser Good-bye, Budget Codes Good Neighbor Policy Calendar and Milestones...

466

ARM - Data Tools  

NLE Websites -- All DOE Office Websites (Extended Search)

govDataData Tools govDataData Tools Data Tools Most ARM data is archived and made available as time-series data in netCDF format. NetCDF (designed by Unidata) is relatively compact, is appendable, is capable of storing descriptive "meta-data" along with measurement data, and is platform-independent. However, the organiza