Sample records for bin csh fb

  1. Bin Packing

    E-Print Network [OSTI]

    Filipe Brandao

    2012-04-13T23:59:59.000Z

    variants, based on an arc flow formulation with side constraints. Conventional formu- ..... does not allow us to control the number of items we assign to each bin.

  2. Effect of temperature on the microstructure of calcium silicate hydrate (C-S-H)

    SciTech Connect (OSTI)

    Gallucci, E., E-mail: gallucci.emmanuel@ch.sika.com; Zhang, X.; Scrivener, K.L.

    2013-11-15T23:59:59.000Z

    Temperature affects the properties of concrete through its effect on the hydration of cement and its associated microstructural development. This paper focuses on the modifications to C-S-H induced by isothermal curing between 5 and 60 °C. The results show that as the temperature increases (within the range studied) the C/S ratio of C-S-H changes only slightly, with a higher degree of polymerisation of silicate chains, but there is a significant decrease in its bound water content and an increase of apparent density of 25%. This increase seems to come from a different packing of C-S-H at the nanoscale. As a consequence of these changes, the microstructure of the cement paste is much coarser and porous, which explains the lower final strengths obtained by curing at elevated temperatures. -- Highlights: •C-S-H structure studied at the atomic level •Multiple analytical techniques used •Studies conducted at temperatures above and below normal temperatures.

  3. Role of interatomic bonding in the mechanical anisotropy and interlayer cohesion of CSH crystals

    SciTech Connect (OSTI)

    Dharmawardhana, C.C. [Department of Physics and Astronomy, University of Missouri—Kansas City, Kansas City, MO 64110 (United States)] [Department of Physics and Astronomy, University of Missouri—Kansas City, Kansas City, MO 64110 (United States); Misra, A. [Department of Civil, Environmental, and Architectural Engineering, University of Kansas, Lawrence, KS 66045 (United States)] [Department of Civil, Environmental, and Architectural Engineering, University of Kansas, Lawrence, KS 66045 (United States); Aryal, S.; Rulis, P. [Department of Physics and Astronomy, University of Missouri—Kansas City, Kansas City, MO 64110 (United States)] [Department of Physics and Astronomy, University of Missouri—Kansas City, Kansas City, MO 64110 (United States); Ching, W.Y., E-mail: ccdxz8@mail.umkc.edu [Department of Physics and Astronomy, University of Missouri—Kansas City, Kansas City, MO 64110 (United States)

    2013-10-15T23:59:59.000Z

    Atomic scale properties of calcium silicate hydrate (CSH), the main binding phase of hardened Portland cement, are not well understood. Over a century of intense research has identified almost 50 different crystalline CSH minerals which are mainly categorized by their Ca/Si ratio. The electronic structure and interatomic bonding in four major CSH crystalline phases with structures close to those found in hardened cement are investigated via ab initio methods. Our result reveals the critical role of hydrogen bonding and importance of specifying precise locations for water molecules. Quantitative analysis of contributions from different bond types to the overall cohesion shows that while the Si-O covalent bonds dominate, the hydrogen bonding and Ca-O bonding are also very significant. Calculated results reveal the correlation between bond topology and interlayer cohesion. The overall bond order density (BOD) is found to be a more critical measure than the Ca/Si ratio in classifying different CSH crystals.

  4. Recycling Bin Guide Locations and prices

    E-Print Network [OSTI]

    Kirschner, Denise

    Recycling Bin Guide Locations and prices Metal Bins Deskside Bins with Side Saddle Rubbermaid Bins.58 for auxiliaries. And Non-Public Areas Public Offices Non-Public Recyclables Recyclables RecyclablesTrash Trash Trash #12;New Recycling Bin Guidelines Frequently Asked Questions (as of December 2008) · Why

  5. FB Line Basis for Interim Operation

    SciTech Connect (OSTI)

    Shedrow, B.

    1998-10-19T23:59:59.000Z

    The safety analysis of the FB-Line Facility indicates that the operation of FB-Line to support the current mission does not present undue risk to the facility and co-located workers, general public, or the environment.

  6. Synthesis and nano-mechanical characterization of calcium-silicate-hydrate (C-S-H) made with 1.5 CaO/SiO{sub 2} mixture

    SciTech Connect (OSTI)

    Foley, Emmy M. [Arizona Public Service, Wintersburg, AZ 85354 (United States)] [Arizona Public Service, Wintersburg, AZ 85354 (United States); Kim, Jung J. [Department of Civil and Environmental Engineering, Sejong University, Seoul 143-747 (Korea, Republic of)] [Department of Civil and Environmental Engineering, Sejong University, Seoul 143-747 (Korea, Republic of); Reda Taha, M.M., E-mail: mrtaha@unm.edu [Department of Civil Engineering, MSC01 1070, 1 University of New Mexico, Albuquerque, NM 87131-0001 (United States)

    2012-09-15T23:59:59.000Z

    In this study, calcium silicate hydrate (C-S-H) is synthesized and characterized. C-S-H slurry was made with calcium oxide (CaO) to micro-silica (SiO{sub 2}) mixture ratio of 1.5 and enough deionized water. The slurry was continuously mixed for 7 days, then the excess water was removed. Two methods of drying were implemented: one method used the standard d-dry technique and the other was equilibrated to 11% relative humidity (RH). The dried powders were characterized using thermo gravimetric analysis (TGA), X-ray diffraction analysis (XRDA), and {sup 29}Si magic angle spinning (MAS) nuclear magnetic resonance (NMR) spectroscopy. The stoichiometric formulas of synthetic C-S-H powders dried to d-dry and 11% RH in this study were approximated as C{sub 1.2}SH{sub 0.7} and C{sub 1.2}SH{sub 2.4} respectively. The powders were then compacted to create specimens with porosities similar to C-S-H in hydrated cement. The specimens underwent nanoindentation to mechanically characterize C-S-H. The experiments provide insight on the nanoscale mechanical characteristics of C-S-H.

  7. Bin Set 1 Calcine Retrieval Feasibility Study

    SciTech Connect (OSTI)

    R. D. Adams; S. M. Berry; K. J. Galloway; T. A. Langenwalter; D. A. Lopez; C. M. Noakes; H. K. Peterson; M. I. Pope; R. J. Turk

    1999-10-01T23:59:59.000Z

    At the Department of Energy's Idaho Nuclear Technology and Engineering Center, as an interim waste management measure, both mixed high-level liquid waste and sodium bearing waste have been solidified by a calculation process and are stored in the Calcine Solids Storage Facilities. This calcined product will eventually be treated to allow final disposal in a national geologic repository. The Calcine Solids Storage Facilities comprise seven ''bit sets.'' Bin Set 1, the first to be constructed, was completed in 1959, and has been in service since 1963. It is the only bin set that does not meet current safe-shutdown earthquake seismic criteria. In addition, it is the only bin set that lacks built-in features to aid in calcine retrieval. One option to alleviate the seismic compliance issue is to transport the calcine from Bin Set 1 to another bin set which has the required capacity and which is seismically qualified. This report studies the feasibility of retrieving the calcine from Bi n Set 1 and transporting it into Bin Set 6 which is located approximately 650 feet away. Because Bin Set 1 was not designed for calcine retrieval, and because of the high radiation levels and potential contamination spread from the calcined material, this is a challenging engineering task. This report presents preconceptual design studies for remotely-operated, low-density, pneumatic vacuum retrieval and transport systems and equipment that are based on past work performed by the Raytheon Engineers and Constructors architectural engineering firm. The designs presented are considered feasible; however, future development work will be needed in several areas during the subsequent conceptual design phase.

  8. 1 Compost Bin Designs 1. Why Compost?

    E-Print Network [OSTI]

    Kaye, Jason P.

    1 Compost Bin Designs 1. Why Compost? Composting livestock manure is an excellent manure management but you are also being environmentally friendly. Composting not only provides the owner with a free source of compost for the yard, garden, and pastures that will benefit plants by slowly releasing nutrients

  9. Joint-Frequency Bins versus Conventional Bin Weather Data in Analysis of HVAC System Operation

    E-Print Network [OSTI]

    Jones, A.; Baltazar, J. C.; Claridge, D. E.

    this study the use of joint-frequency bins has relative added value to the analysis of HVAC system operation depending on whether the system is dominated by ventilation loads....

  10. Interpretations and implications of the top quark rapidity asymmetries A FB t and A FB ?

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Berger, Edmond L.; Cao, Qing-Hong; Chen, Chuan-Ren; Zhang, Hao

    2013-07-01T23:59:59.000Z

    Forward-backward asymmetries AtFB and AlFB are observed in the top-quark t rapidity distribution and in the rapidity distribution of charged leptons l from top-quark decay at the Tevatron proton-antiproton collider, and a charge asymmetry AC is seen in proton-proton collisions at the Large Hadron Collider (LHC). In this paper, we update our previous studies of the Tevatron asymmetries using the most recent data. We provide expectations for AC at the LHC based first on simple extrapolations from the Tevatron, and second based on new physics models that can explain the Tevatron asymmetries. We examine the relationship of the two asymmetries AtFB and AlFB. We show their connection through the (V–A) spin correlation between the charged lepton and the top quark with different polarization states. We show that the ratio of the two asymmetries provides independent insight into the physics interpretation of the top-quark asymmetry. We emphasize the value of the measurement of both asymmetries, and we conclude that a model which produces more right-handed than left-handed top quarks is suggested by the present Tevatron data.

  11. Analysis of Air Conditioning Effectiveness vs. Outdoor Conditions: Traditional Bins or Joint Frequency Bins?

    E-Print Network [OSTI]

    Cohen, B. M.

    1998-01-01T23:59:59.000Z

    are fairly high. Offices that have a lot of sensible heat generation due to lighting and office equipment tend to be high, maybe greater than 0.9. (Other applications, like ice rinks that have internal cooling, can be low or even negative, and do... ratio ranges on the second axis. This form of binning is easily accomplished if a utility like ~in~aker~~ is used to generate the binned data set. INTRODUCTION The factors which should be considered in the specification of heating and air...

  12. adaptive bin framework: Topics by E-print Network

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Lin, Lin; Ying, Lexing; E, Weinan 2011-01-01 163 Multifractal Diffusion Entropy Analysis: Optimal Bin Width of Probability Histograms CERN Preprints Summary: In the framework...

  13. $A^t_{FB}$ Meets LHC

    SciTech Connect (OSTI)

    Hewett, JoAnne L.; /SLAC; Shelton, Jessie; /Yale U.; Spannowsky, Michael; /Oregon U.; Tait, Tim M.P.; /UC, Irvine; Takeuchi, Michihisa; /Heidelberg U.

    2012-02-14T23:59:59.000Z

    The recent Tevatron measurement of the forward-backward asymmetry of the top quark shows an intriguing discrepancy with Standard Model expectations, particularly at large t{bar t} invariant masses. Measurements of this quantity are subtle at the LHC, due to its pp initial state, however, one can define a forward-central-charge asymmetry which captures the physics. We study the capability of the LHC to measure this asymmetry and find that within the SM a measurement at the 5{sigma} level is possible with roughly 60 fb{sup -1} at {radical}s = 14 TeV. If nature realizes a model which enhances the asymmetry (as is necessary to explain the Tevatron measurements), a significant difference from zero can be observed much earlier, perhaps even during early LHC running at {radical}s = 7 TeV. We further explore the capabilities of the 7 TeV LHC to discover resonances or contact interactions which modify the t{bar t} invariant mass distribution using recent boosted top tagging techniques. We find that TeV-scale color octet resonances can be discovered, even with small coupling strengths and that contact interactions can be probed at scales exceeding 6 TeV. Overall, the LHC has good potential to clarify the situation with regards to the Tevatron forward-backward measurement.

  14. Bin-Hash Indexing: A Parallel Method for Fast Query Processing

    E-Print Network [OSTI]

    Gosink, Luke J.

    2008-01-01T23:59:59.000Z

    The Bin-Hash index uses a form of compression, implementedbitmap index. Unfor- tunately the compression strategies forcompression strategies, based upon the binning strategies of the binned bitmap index,

  15. Data Parallel Bin-Based Indexing for Answering Queries on Multi-Core Architectures

    E-Print Network [OSTI]

    Gosink, Luke

    2009-01-01T23:59:59.000Z

    a binned bitmap index. Unfortu- nately, bitmap compressioncompression strategy, based upon the binning techniques of the binned bitmap index,index is that storage concerns for indices are ameliorated through specialized compression

  16. Auslandsbeauftragte / Departmental Coordinators FB 1: Rechts-und Wirtschaftswissenschaften

    E-Print Network [OSTI]

    Haller-Dintelmann, Robert

    @linglit.tu-... Overseas: Dr. Sabine Bartsch (S1|03 189) Tel: 16-4570 | bartsch@linglit.tu-... FB 3: Mathematik Ansprechpartner Studienbüro Internationales: Dr. René Bartsch (S2|15 233) Tel: 16-3587 | rbartsch

  17. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    Teilgebiete der Physik eigenständig untersuchen. learning outcome Art der Prüfung / method of assessment, exam Modulprüfung (MP) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie work Protokolle Journals Lerninhalte Si

  18. Manipulating time-bin qubits with fiber optics components

    E-Print Network [OSTI]

    Felix Bussieres; Yasaman Soudagar; Guido Berlin; Suzanne Lacroix; Nicolas Godbout

    2006-05-06T23:59:59.000Z

    We propose two experimental schemes to implement arbitrary unitary single qubit operations on single photons encoded in time-bin qubits. Both schemes require fiber optics components that are available with current technology.

  19. Blue Laboratory Recycling Bins Thank you for your efforts in greening the NIH!

    E-Print Network [OSTI]

    Baker, Chris I.

    Blue Laboratory Recycling Bins Thank you for your efforts in greening the NIH! Instructions: Please empty the contents of your bin into the larger centralized recycling bins for collection whenever Information: To request a centralized recycling bin or a hamper for large cleanouts, please contact

  20. Data:A3e7d1e2-5415-4cd9-bc91-6fb9fb7fd076 | Open Energy Information

    Open Energy Info (EERE)

    1-6fb9fb7fd076 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...

  1. Constraints to Stop Deforestation FB IV Informatik, Universitat Trier,

    E-Print Network [OSTI]

    Seidl, Helmut

    Constraints to Stop Deforestation H. Seidl FB IV ­ Informatik, Universit¨at Trier, D­54286 Trier, Universitetsparken 1, DK­2100 Copenhagen �, Denmark. rambo@diku.dk Abstract Wadler's deforestation algorithm, deforestation must terminate on all programs. Several techniques exist to ensure termination of de­ forestation

  2. Constraints to Stop HigherOrder Deforestation FB IV Informatik

    E-Print Network [OSTI]

    Seidl, Helmut

    Constraints to Stop Higher­Order Deforestation H. Seidl FB IV ­ Informatik Universit¨at Trier, D of Copenhagen Universitetsparken 1, DK­2100 Copenhagen �, Denmark rambo@diku.dk Abstract Wadler's deforestation in a compiler, it must terminate on all programs. Several techniques to ensure termi­ nation of deforestation

  3. Application of a Diesel Fuel Reformer for Tier 2 Bin 5 Emissions

    Broader source: Energy.gov (indexed) [DOE]

    of a Diesel Fuel Reformer for Tier 2 Bin 5 Emissions APPROACH On-board diesel fuel reformation is being evaluated as an alternative to urea SCR to meet Tier 2 Bin 5 emissions...

  4. Cummins Next Generation Tier 2, Bin 2 Light Truck Diesel engine...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Cummins Next Generation Tier 2, Bin 2 Light Truck Diesel engine Cummins Next Generation Tier 2, Bin 2 Light Truck Diesel engine Discusses plan, baselining, and modeling, for new...

  5. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine |...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    & Publications Vehicle Technologies Office Merit Review 2014: ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel...

  6. Cummins' Next Generation Tier 2, Bin 2 Light Truck Diesel Engine...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Cummins' Next Generation Tier 2, Bin 2 Light Truck Diesel Engine Cummins' Next Generation Tier 2, Bin 2 Light Truck Diesel Engine Development of a new light truck, in-line...

  7. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine |...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Peer Evaluation ace061ruth2011o.pdf More Documents & Publications ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel...

  8. Welcome new and returning residents! Help us make USC greener by recycling! Your Room Recycling Bin

    E-Print Network [OSTI]

    Almor, Amit

    Welcome new and returning residents! Help us make USC greener by recycling! Your Room Recycling Bin Every room is provided with a recycling bin to make it easy for you to recycle while living in University Housing. Use this bin to collect mixed recyclables in your room and take them to your nearest

  9. Selecting the Number of Bins in a Histogram: A Decision Theoretic Approach

    E-Print Network [OSTI]

    Meeden, Glen

    Running Title Number of Bins in a Histogram ABSTRACT In this note we consider the problem of, given a sample, selecting the number of bins in a histogram. A loss function is introduced which reflects a loss function which incorporates the idea that smoother densities require less bins in their histogram

  10. Measurement of the ? ? * distribution of muon pairs with masses between 30 and 500 GeV in 10.4 fb - 1 of p p ¯ collisions

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V.?M.; Abbott, B.; Acharya, B.?S.; Adams, M.; Adams, T.; Agnew, J.?P.; Alexeev, G.?D.; Alkhazov, G.; Alton, A.; Askew, A.; Atkins, S.; Augsten, K.; Avila, C.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D.?V.; Banerjee, S.; Barberis, E.; Baringer, P.; Bartlett, J.?F.; Bassler, U.; Bazterra, V.; Bean, A.; Begalli, M.; Bellantoni, L.; Beri, S.?B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bhat, P.?C.; Bhatia, S.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E.?E.; Borissov, G.; Borysova, M.; Brandt, A.; Brandt, O.; Brock, R.; Bross, A.; Brown, D.; Bu, X.?B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Buszello, C.?P.; Camacho-Pérez, E.; Casey, B.?C.?K.; Castilla-Valdez, H.; Caughron, S.; Chakrabarti, S.; Chan, K.?M.; Chandra, A.; Chapon, E.; Chen, G.; Cho, S.?W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W.?E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Cutts, D.; Das, A.; Davies, G.; de Jong, S.?J.; De La Cruz-Burelo, E.; Déliot, F.; Demina, R.; Denisov, D.; Denisov, S.?P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H.?T.; Diesburg, M.; Ding, P.?F.; Dominguez, A.; Dubey, A.; Dudko, L.?V.; Duperrin, A.; Dutt, S.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V.?D.; Enari, Y.; Evans, H.; Evdokimov, V.?N.; Fauré, A.; Feng, L.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H.?E.; Fortner, M.; Fox, H.; Fuess, S.; Garbincius, P.?H.; Garcia-Bellido, A.; García-González, J.?A.; Gavrilov, V.; Geng, W.; Gerber, C.?E.; Gershtein, Y.; Ginther, G.; Gogota, O.; Golovanov, G.; Grannis, P.?D.; Greder, S.; Greenlee, H.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M.?W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J.?M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A.?P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M.?D.; Hirosky, R.; Hoang, T.; Hobbs, J.?D.; Hoeneisen, B.; Hogan, J.; Hohlfeld, M.; Holzbauer, J.?L.; Howley, I.; Hubacek, Z.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A.?S.; Jabeen, S.; Jaffré, M.; Jayasinghe, A.; Jeong, M.?S.; Jesik, R.; Jiang, P.; Johns, K.; Johnson, E.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A.?W.; Juste, A.; Kajfasz, E.; Karmanov, D.; Katsanos, I.; Kaur, M.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y.?N.; Kiselevich, I.; Kohli, J.?M.; Kozelov, A.?V.; Kraus, J.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V.?A.; Lammers, S.; Lebrun, P.; Lee, H.?S.; Lee, S.?W.; Lee, W.?M.; Lei, X.; Lellouch, J.; Li, D.; Li, H.; Li, L.; Li, Q.?Z.; Li, X.; Lim, J.?K.; Lincoln, D.; Linnemann, J.; Lipaev, V.?V.; Lipton, R.; Liu, H.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Luna-Garcia, R.; Lyon, A.?L.; Maciel, A.?K.?A.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V.?L.; Mansour, J.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C.?L.; Meijer, M.?M.; Melnitchouk, A.; Menezes, D.; Mercadante, P.?G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N.?K.; Mulhearn, M.; Nagy, E.; Narain, M.; Nayyar, R.; Neal, H.?A.; Negret, J.?P.; Neustroev, P.; Nguyen, H.?T.; Nunnemann, T.; Orduna, J.; Osman, N.; Osta, J.; Pal, A.; Parashar, N.; Parihar, V.; Park, S.?K.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Pleier, M.-A.; Podstavkov, V.?M.; Popov, A.?V.; Prewitt, M.; Price, D.; Prokopenko, N.; Qian, J.; Qin, Y.; Quadt, A.; Quinn, B.; Ratoff, P.?N.; Razumov, I.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Sajot, G.; Sánchez-Hernández, A.; Sanders, M.?P.; Santos, A.?S.; Savage, G.; Savitskyi, M.; Sawyer, L.; Scanlon, T.; Schamberger, R.?D.; Scheglov, Y.; Schellman, H.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shaw, S.; Shchukin, A.?A.; Simak, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Snow, G.?R.; Snow, J.; Snyder, S.; Söldner-Rembold, S.; Sonnenschein, L.; Soustruznik, K.; Stark, J.; Stoyanova, D.?A.; Strauss, M.; Suter, L.; Svoisky, P.; Titov, M.; Tokmenin, V.?V.; Tsai, Y.-T.; Tsybychev, D.; Tuchming, B.; Tully, C.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Van Kooten, R.; van Leeuwen, W.?M.; Varelas, N.; Varnes, E.?W.; Vasilyev, I.?A.; Verkheev, A.?Y.; Vertogradov, L.?S.; Verzocchi, M.; Vesterinen, M.; Vilanova, D.; Vokac, P.; Wahl, H.?D.; Wang, M.?H.?L.?S.; Warchol, J.; Watts, G.

    2015-04-01T23:59:59.000Z

    We present a measurement of the distribution of the variable ?*? for muon pairs with masses between 30 and 500 GeV, using the complete run II data set collected by the D0 detector at the Fermilab Tevatron proton-antiproton collider. This corresponds to an integrated luminosity of 10.4 fb?¹ at ?s=1.96 TeV. The data are corrected for detector effects and presented in bins of dimuon rapidity and mass. The variable ?*? probes the same physical effects as the Z/?* boson transverse momentum, but is less susceptible to the effects of experimental resolution and efficiency. These are the first measurements at any collider of the ?*? distributions for dilepton masses away from the Z?l?l? boson mass peak. The data are compared to QCD predictions based on the resummation of multiple soft gluons.

  11. Photography, Tragedy and Osama Bin Laden: Looking at the enemy

    E-Print Network [OSTI]

    Wallace, Jennifer

    2015-01-01T23:59:59.000Z

    , although as I have argued, the occluded television leaves open the space for speculation, for pity and fear and uncertainty. In the second, haphazardly-shot image, the 20 20 spectator, Bin Laden, is also formed by what he sees, the narcissism... and Infinity: An Essay on Exteriority, trans. Alphonso Lingis (Pittsburgh: Duquesne University Press, 1969), 213. vii Emmanuel Levinas, Is It Righteous to Be?: Interviews with Emmanuel Levinas, ed. Jill Robbins (Stanford, California: Stanford University...

  12. Compressed supersymmetry after 1 fb?¹ at the Large Hadron Collider

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    LeCompte, Thomas J.; Martin, Stephen P.

    2012-02-01T23:59:59.000Z

    We study the reach of the Large Hadron Collider with 1 fb?¹ of data at ?s=7 TeV for several classes of supersymmetric models with compressed mass spectra, using jets and missing transverse energy cuts like those employed by ATLAS for summer 2011 data. In the limit of extreme compression, the best limits come from signal regions that do not require more than 2 or 3 jets and that remove backgrounds by requiring more missing energy rather than a higher effective mass.

  13. FB EcoSolutions LLC | Open Energy Information

    Open Energy Info (EERE)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page onYou are now leaving Energy.gov You are now leaving Energy.gov You are being directedAnnualPropertyd8c-a9ae-f8521cbb8489 NoEurope BV Jump to:FAS Technologies LLC Jump to: navigation,FB

  14. v9fb: a remote framebuffer infrastructure of linux

    SciTech Connect (OSTI)

    Kulkarni, Abhishek [Los Alamos National Laboratory; Ionkov, Latchesar [Los Alamos National Laboratory

    2008-01-01T23:59:59.000Z

    v9fb is a software infrastructure that allows extending framebufFer devices in Linux over the network by providing an abstraction to them in the form of a filesystem hierarchy. Framebuffer based graphic devices export a synthetic filesystem which offers a simple and easy-to-use interface for performing common framebuffer operations. Remote framebuffer devices could be accessed over the network using the 9P protocol support in Linux. We describe the infrastructure in detail and review some of the benefits it offers similar to Plan 9 distributed systems. We discuss the applications of this infrastructure to remotely display and run interactive applications on a terminal while ofFloading the computation to remote servers, and more importantly the flexibility it offers in driving tiled-display walls by aggregating graphic devices in the network.

  15. FB-line neutron multiplicity counter operation manual

    SciTech Connect (OSTI)

    Langner, D.G.; Sweet, M.R.; Salazar, S.D.; Kroncke, K.E.

    1997-12-31T23:59:59.000Z

    This manual describes the design features, performance, and operating characteristics for the FB-Line Neutron Multiplicity counter (FBLNMC). The FBLNMC counts neutron multiplicities to quantitatively assay plutonium in many forms, including impure scrap and waste. Monte Carlo neutronic calculations were used to design the high-efficiency (57%) detector that has 113 {sup 3}He tubes in a high-density polyethylene body. The new derandomizer circuit is included in the design to reduce deadtime. The FBLNMC can be applied to plutonium masses in the range from a few tens of grams to 5 kg; both conventional coincidence counting and multiplicity counting can be used as appropriate. This manual gives the performance data and preliminary calibration parameters for the FBLNMC.

  16. Complete genome sequence of Arthrobacter sp. strain FB24

    SciTech Connect (OSTI)

    Nakatsu, C. H.; Barabote, Ravi; Thompson, Sue; Bruce, David; Detter, Chris; Brettin, T.; Han, Cliff F.; Beasley, Federico; Chen, Weimin; Konopka, Allan; Xie, Gary

    2013-09-30T23:59:59.000Z

    Arthrobacter sp. strain FB24 is a species in the genus Arthrobacter Conn and Dimmick 1947, in the family Micrococcaceae and class Actinobacteria. A number of Arthrobacter genome sequences have been completed because of their important role in soil, especially bioremediation. This isolate is of special interest because it is tolerant to multiple metals and it is extremely resistant to elevated concentrations of chromate. The genome consists of a 4,698,945 bp circular chromosome and three plasmids (96,488, 115,507, and 159,536 bp, a total of 5,070,478 bp), coding 4,536 proteins of which 1,257 are without known function. This genome was sequenced as part of the DOE Joint Genome Institute Program.

  17. Cummins Next Generation Tier 2, Bin 2 Light Truck Diesel Engine

    Broader source: Energy.gov (indexed) [DOE]

    equivalent US Tier 2, Bin 2 emissions levels Commercially Viable Solutions - High quality, Great Performance, Low Total Cost of Ownership Program Targets 2010 Nissan Titan...

  18. Fast Object Localization and Pose Estimation in Heavy Clutter for Robotic Bin Picking

    E-Print Network [OSTI]

    Mellor-Crummey, John

    Fast Object Localization and Pose Estimation in Heavy Clutter for Robotic Bin Picking Ming-Yu Liu-based robotic bin-picking system that per- forms detection and 3D pose estimation of objects in an unstructured flexible, and independent robots that can interact with the surrounding environment is a fundamental goal

  19. Maximum Likelihood Estimation of Mixture Densities for Binned and Truncated Multivariate

    E-Print Network [OSTI]

    Smyth, Padhraic

    Maximum Likelihood Estimation of Mixture Densities for Binned and Truncated Multivariate Data in data analysis and machine learning. This paper addresses the problem of fitting mixture densities to multivariate binned and truncated data. The EM approach proposed by McLachlan and Jones (1988

  20. Solid waste bin detection and classification using Dynamic Time Warping and MLP classifier

    SciTech Connect (OSTI)

    Islam, Md. Shafiqul, E-mail: shafique@eng.ukm.my [Dept. of Electrical, Electronic and Systems Engineering, Universiti Kebangsaan Malaysia, Bangi 43600, Selangore (Malaysia); Hannan, M.A., E-mail: hannan@eng.ukm.my [Dept. of Electrical, Electronic and Systems Engineering, Universiti Kebangsaan Malaysia, Bangi 43600, Selangore (Malaysia); Basri, Hassan [Dept. of Civil and Structural Engineering, Universiti Kebangsaan Malaysia, Bangi 43600, Selangore (Malaysia); Hussain, Aini; Arebey, Maher [Dept. of Electrical, Electronic and Systems Engineering, Universiti Kebangsaan Malaysia, Bangi 43600, Selangore (Malaysia)

    2014-02-15T23:59:59.000Z

    Highlights: • Solid waste bin level detection using Dynamic Time Warping (DTW). • Gabor wavelet filter is used to extract the solid waste image features. • Multi-Layer Perceptron classifier network is used for bin image classification. • The classification performance evaluated by ROC curve analysis. - Abstract: The increasing requirement for Solid Waste Management (SWM) has become a significant challenge for municipal authorities. A number of integrated systems and methods have introduced to overcome this challenge. Many researchers have aimed to develop an ideal SWM system, including approaches involving software-based routing, Geographic Information Systems (GIS), Radio-frequency Identification (RFID), or sensor intelligent bins. Image processing solutions for the Solid Waste (SW) collection have also been developed; however, during capturing the bin image, it is challenging to position the camera for getting a bin area centralized image. As yet, there is no ideal system which can correctly estimate the amount of SW. This paper briefly discusses an efficient image processing solution to overcome these problems. Dynamic Time Warping (DTW) was used for detecting and cropping the bin area and Gabor wavelet (GW) was introduced for feature extraction of the waste bin image. Image features were used to train the classifier. A Multi-Layer Perceptron (MLP) classifier was used to classify the waste bin level and estimate the amount of waste inside the bin. The area under the Receiver Operating Characteristic (ROC) curves was used to statistically evaluate classifier performance. The results of this developed system are comparable to previous image processing based system. The system demonstration using DTW with GW for feature extraction and an MLP classifier led to promising results with respect to the accuracy of waste level estimation (98.50%). The application can be used to optimize the routing of waste collection based on the estimated bin level.

  1. Characterization of the Dynamics in the Protonic Conductor CsH2PO4 by 17O Solid-State NMR Spectroscopy and First-Principles Calculations: Correlating Phosphate and Protonic Motion

    E-Print Network [OSTI]

    Kim, Gunwoo; Griffin, John M.; Blanc, Frédéric; Haile, Sossina M.; Grey, Claire P.

    2015-03-03T23:59:59.000Z

    promising class of proton-conducting solid electrolytes for use in fuel cells that operate in an intermediate-temperature range (200 - 600 ºC).1-4 In particular, CsH2PO4, has been intensively studied because of its desirable operating temperature (230 – 260... of the adjacent O3 oxygen atoms (see Figure 1). This O-H separation was based upon the O1-H1 covalent bond length in the X-ray structure.15 Prior to calculation of the NMR parameters, all structures were fully geometry-optimized, with the unit cell parameters...

  2. Top Quark Production Asymmetries AFBt and AFBl

    SciTech Connect (OSTI)

    Berger, Edmond L.; Cao, Qing-Hong; Chen, Chuan-Ren; Yu, Jiang-Hao; Zhang, Hao

    2012-02-01T23:59:59.000Z

    A large forward-backward asymmetry is seen in both the top quark rapidity distribution AFBt and in the rapidity distribution of charged leptons AFBl from top quarks produced at the Tevatron. We study the kinematic and dynamic aspects of the relationship of the two observables arising from the spin correlation between the charged lepton and the top quark with different polarization states. We emphasize the value of both measurements, and we conclude that a new physics model which produces more right-handed than left-handed top quarks is favored by the present data.

  3. {sup 239}Pu Holdup Measurements at Savannah River Site's FB-Line

    SciTech Connect (OSTI)

    Hodge, C.A.

    2001-06-20T23:59:59.000Z

    Plutonium holdup measurements were conducted in the dry cabinets of FB-Line at the Savannah River Site. This report will discuss the methodology, measurements, assumptions, calculations, and corrections.

  4. Strategies for In-Cylinder Reductions to Reach Bin 2 and LEV...

    Broader source: Energy.gov (indexed) [DOE]

    Strategies for In-Cylinder Reductions to Reach Bin 2 and LEVIII Air System Management to Reduce NOx and PM and Improve Fuel Economy Poster Location P-03 Robert Czarnowski, John...

  5. For some, Bin Laden's death harkens to Hitler's 66 years ago

    E-Print Network [OSTI]

    Belogay, Eugene A.

    For some, Bin Laden's death harkens to Hitler's 66 years ago By SCOTT EYMAN Palm Beach Post Staff images of frantic joy marking the end of World War II and the death of Adolf Hitler. The comparison

  6. A possible mechanism for ENSO turnabouts Bin Wang*, Renguang Wu, Roger Lukas, and Soon-Il An*

    E-Print Network [OSTI]

    Wang, Bin

    1 A possible mechanism for ENSO turnabouts Bin Wang*, Renguang Wu, Roger Lukas, and Soon-Il An to J. Climate July 8, 1999

  7. A CMOS Low Power Biohybrid Lamprey Robot Controller Design Yong-Bin Kim

    E-Print Network [OSTI]

    Ayers, Joseph

    , industrial, and scientific applications for autonomous robots that can operate adaptively in unpredictable or dangerous work efforts ranging from industrial to field applications. There is a strong demand for consumerA CMOS Low Power Biohybrid Lamprey Robot Controller Design Yong-Bin Kim Department of Electrical

  8. On Compress-Forward without Wyner-Ziv Binning for Relay Networks

    E-Print Network [OSTI]

    Zhong, Peng; Vu, Mai

    2011-01-01T23:59:59.000Z

    Noisy network coding is recently proposed for the general multi-source network by Lim, Kim, El Gamal and Chung. This scheme builds on compress-forward (CF) relaying but involves three new ideas, namely no Wyner-Ziv binning, relaxed simultaneous decoding and message repetition. In this paper, using the two-way relay channel as the underlining example, we analyze the impact of each of these ideas on the achievable rate region of relay networks. First, CF without binning but with joint decoding of both the message and compression index can achieve a larger rate region than the original CF scheme for multi-destination relay networks. With binning and successive decoding, the compression rate at each relay is constrained by the weakest link from the relay to a destination; but without binning, this constraint is relaxed. Second, simultaneous decoding of all messages over all blocks without uniquely decoding the compression indices can remove the constraints on compression rate completely, but is still subject to t...

  9. Sliding Mode Flow Rate Observer Design Song Liu and Bin Yao

    E-Print Network [OSTI]

    Yao, Bin

    pressure measurements and unavoidable modelling uncertainties. This paper proposes a sliding mode dynamicSliding Mode Flow Rate Observer Design Song Liu and Bin Yao School of Mechanical Engineering rate from fluid pressure dynamic equations usually results in poor estimates due to the very noisy

  10. Automated Modelling of Cartridge Valve Flow Mapping Song Liu and Bin Yao

    E-Print Network [OSTI]

    Yao, Bin

    Automated Modelling of Cartridge Valve Flow Mapping Song Liu and Bin Yao Abstract-- Proportional poppet-type cartridge valves are the key elements of the energy saving programmable valves, which have significantly saving energy usage. Unlike costly conventional four-way valves, the cartridge valve has simple

  11. Data Dependent Jitter (DDJ) Characterization Methodology Kyung Ki Kim, Yong-Bin Kim, Fabrizio Lombardi

    E-Print Network [OSTI]

    Ayers, Joseph

    Data Dependent Jitter (DDJ) Characterization Methodology Kyung Ki Kim, Yong-Bin Kim, Fabrizio-mail: kkkim@ece.neu.edu, ybk@ece.neu.edu, Lombardi@ece.neu.edu Abstract A new jitter model is developed using Matlab and Spice to analyze Data Dependent Jitter (DDJ) in serial data integrated circuits

  12. What can you recycle at MIT? All Paper in desk side and blue-top bins

    E-Print Network [OSTI]

    Seager, Sara

    What can you recycle at MIT? All Paper in desk side and blue-top bins Bottles, Cans and Containers Paper Computer Monitors / Electronics contact recycling@mit.edu Aluminum cans & foil Glass Bottles All Centers (DMC's) For more information: Working Group Recycling Committee at http

  13. User`s manual for BINIAC: A computer code to translate APET bins

    SciTech Connect (OSTI)

    Gough, S.T.

    1994-03-01T23:59:59.000Z

    This report serves as the user`s manual for the FORTRAN code BINIAC. BINIAC is a utility code designed to format the output from the Defense Waste Processing Facility (DWPF) Accident Progression Event Tree (APET) methodology. BINIAC inputs the accident progression bins from the APET methodology, converts the frequency from occurrences per hour to occurrences per year, sorts the progression bins, and converts the individual dimension character codes into facility attributes. Without the use of BINIAC, this process would be done manually at great time expense. BINIAC was written under the quality assurance control of IQ34 QAP IV-1, revision 0, section 4.1.4. Configuration control is established through the use of a proprietor and a cognizant users list.

  14. Make Model SPECS ACURA ILX (Model Year 2013) 2.0L 4, auto stk [P] ULEV II / Bin 5 45

    E-Print Network [OSTI]

    II / Bin 5 42 BMW 328i (Model Year 2013) 2.0L 4, auto stk [P] Bin 5 / ULEV II 42 BMW 328i (Model Year 2013) 2.0L 4, manual [P] ULEV II / Bin 5 43 BMW 328i XDRIVE (Model Year 2013) 2.0L 4, auto stk Awd [P] ULEV II / Bin 5 41 BMW 335i (Model Year 2013) 3.0L 6, auto stk [P] ULEV II / Bin 5 41 BMW 528i (Model

  15. Quantum secret sharing based on modulated high-dimensional time-bin entanglement

    SciTech Connect (OSTI)

    Takesue, Hiroki [NTT Basic Research Laboratories, NTT Corporation, 3-1 Morinosato Wakamiya, Atsugi, Kanagawa, 243-0198 (Japan); CREST, Japan Science and Technology Agency, 4-1-8 Honcho, Kawaguchi, Saitama, 332-0012 (Japan); Inoue, Kyo [NTT Basic Research Laboratories, NTT Corporation, 3-1 Morinosato Wakamiya, Atsugi, Kanagawa, 243-0198 (Japan); Department of Electrical, Electronics and Information Engineering, Osaka University, 2-1 Yamadaoka, Suita, Osaka, 565-0871 (Japan); CREST, Japan Science and Technology Agency, 4-1-8 Honcho, Kawaguchi, Saitama, 332-0012 (Japan)

    2006-07-15T23:59:59.000Z

    We propose a scheme for quantum secret sharing (QSS) that uses a modulated high-dimensional time-bin entanglement. By modulating the relative phase randomly by {l_brace}0,{pi}{r_brace}, a sender with the entanglement source can randomly change the sign of the correlation of the measurement outcomes obtained by two distant recipients. The two recipients must cooperate if they are to obtain the sign of the correlation, which is used as a secret key. We show that our scheme is secure against intercept-and-resend (IR) and beam splitting attacks by an outside eavesdropper thanks to the nonorthogonality of high-dimensional time-bin entangled states. We also show that a cheating attempt based on an IR attack by one of the recipients can be detected by changing the dimension of the time-bin entanglement randomly and inserting two 'vacant' slots between the packets. Then, cheating attempts can be detected by monitoring the count rate in the vacant slots. The proposed scheme has better experimental feasibility than previously proposed entanglement-based QSS schemes.

  16. Scalable boson-sampling with time-bin encoding using a loop-based architecture

    E-Print Network [OSTI]

    Keith R. Motes; Alexei Gilchrist; Jonathan P. Dowling; Peter P. Rohde

    2014-03-17T23:59:59.000Z

    We present an architecture for arbitrarily scalable boson-sampling using two nested fiber loops. The architecture has fixed experimental complexity, irrespective of the size of the desired interferometer, whose scale is limited only by fiber and switch loss rates. The architecture employs time-bin encoding, whereby the incident photons form a pulse train, which enters the loops. Dynamically controlled loop coupling ratios allow the construction of the arbitrary linear optics interferometers required for boson-sampling. The architecture employs only a single point of interference and may thus be easier to stabilize than other approaches. The scheme has polynomial complexity and could be realized using demonstrated present-day technologies.

  17. Measurement of the anomalous like-sign dimuon charge asymmetry with 9 fb?¹ of pp? collisions

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; Aoki, M.; Arov, M.; Askew, A.; Åsman, B.; Atramentov, O.; Avila, C.; BackusMayes, J.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Barreto, J.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Beale, S.; Bean, A.; Begalli, M.; Begel, M.; Belanger-Champagne, C.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bezzubov, V. A.; Bhat, P. C.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Brooijmans, G.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Burnett, T. H.; Buszello, C. P.; Calpas, B.; Camacho-Pérez, E.; Carrasco-Lizarraga, M. A.; Casey, B. C. K.; Castilla-Valdez, H.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Croc, A.; Cutts, D.; Das, A.; Davies, G.; De, K.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demarteau, M.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dorland, T.; Dubey, A.; Dudko, L. V.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Evdokimov, V. N.; Facini, G.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Garcia-Bellido, A.; Gavrilov, V.; Gay, P.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A.; Grannis, P. D.; Greder, S.; Greenlee, H.; Greenwood, Z. D.; Gregores, E. M.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Guo, F.; Gutierrez, G.; Gutierrez, P.; Haas, A.; Hagopian, S.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hohlfeld, M.; Hubacek, Z.; Huske, N.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jamin, D.; Jayasinghe, A.; Jesik, R.; Johns, K.; Johnson, M.; Johnston, D.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A. W.; Juste, A.; Kaadze, K.; Kajfasz, E.; Karmanov, D.; Kasper, P. A.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kirby, M. H.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kulikov, S.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Kvita, J.; Lammers, S.; Landsberg, G.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lellouch, J.; Li, L.; Li, Q. Z.; Lietti, S. M.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, Y.; Liu, Z.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Lubatti, H. J.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Mackin, D.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Maravin, Y.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N. K.; Muanza, G. S.; Mulhearn, M.; Nagy, E.; Naimuddin, M.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Novaes, S. F.; Nunnemann, T.; Obrant, G.; Orduna, J.; Osman, N.; Osta, J.; Otero y Garzón, G. J.; Padilla, M.; Pal, A.; Parashar, N.; Parihar, V.; Park, S. K.; Parsons, J.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, K.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Piegaia, R.; Pleier, M.-A.; Podesta-Lerma, P. L. M.; Podstavkov, V. M.; Polozov, P.; Popov, A. V.; Prewitt, M.; Price, D.; Prokopenko, N.; Protopopescu, S.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M. S.; Ranjan, K.; Ratoff, P. N.; Razumov, I.; Renkel, P.; Rijssenbeek, M.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Safronov, G.; Sajot, G.; Salcido, P.; Sánchez-Hernández, A.; Sanders, M. P.; Sanghi, B.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schliephake, T.; Schlobohm, S.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shchukin, A. A.; Shivpuri, R. K.; Simak, V.; Sirotenko, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Smith, K. J.

    2011-09-01T23:59:59.000Z

    We present an updated measurement of the anomalous like-sign dimuon charge asymmetry Absl for semileptonic b-hadron decays in 9.0 fb?¹ of pp? collisions recorded with the D0 detector at a center-of-mass energy of ?s=1.96 TeV at the Fermilab Tevatron collider. We obtain Absl=(-0.787±0.172(stat)±0.093(syst))%. This result differs by 3.9 standard deviations from the prediction of the standard model and provides evidence for anomalously large CP violation in semileptonic neutral B decay. The dependence of the asymmetry on the muon impact parameter is consistent with the hypothesis that it originates from semileptonic b-hadron decays.

  18. Development of an aerosol microphysical module: Aerosol Two-dimensional bin module for foRmation and Aging Simulation (ATRAS)

    SciTech Connect (OSTI)

    Matsui, H.; Koike, Makoto; Kondo, Yutaka; Fast, Jerome D.; Takigawa, M.

    2014-09-30T23:59:59.000Z

    Number concentrations, size distributions, and mixing states of aerosols are essential parameters for accurate estimation of aerosol direct and indirect effects. In this study, we developed an aerosol module, designated Aerosol Two-dimensional bin module for foRmation and Aging Simulation (ATRAS), that can represent these parameters explicitly by considering new particle formation (NPF), black carbon (BC) aging, and secondary organic aerosol (SOA) processes. A two-dimensional bin representation is used for particles with dry diameters from 40 nm to 10 µm to resolve both aerosol size (12 bins) and BC mixing state (10 bins) for a total of 120 bins. The particles with diameters from 1 to 40 nm are resolved using an additional 8 size bins to calculate NPF. The ATRAS module was implemented in the WRF-chem model and applied to examine the sensitivity of simulated mass, number, size distributions, and optical and radiative parameters of aerosols to NPF, BC aging and SOA processes over East Asia during the spring of 2009. BC absorption enhancement by coating materials was about 50% over East Asia during the spring, and the contribution of SOA processes to the absorption enhancement was estimated to be 10 – 20% over northern East Asia and 20 – 35% over southern East Asia. A clear north-south contrast was also found between the impacts of NPF and SOA processes on cloud condensation nuclei (CCN) concentrations: NPF increased CCN concentrations at higher supersaturations (smaller particles) over northern East Asia, whereas SOA increased CCN concentrations at lower supersaturations (larger particles) over southern East Asia. Application of ATRAS to East Asia also showed that the impact of each process on each optical and radiative parameter depended strongly on the process and the parameter in question. The module can be used in the future as a benchmark model to evaluate the accuracy of simpler aerosol models and examine interactions between NPF, BC aging, and SOA processes under different meteorological conditions and emissions.

  19. Application of the BINS superheated drop detector spectrometer to the {sup 9}Be(p,xn) neutron energy spectrum determination

    SciTech Connect (OSTI)

    Di Fulvio, A.; Ciolini, R.; Mirzajani, N.; Romei, C.; D'Errico, F. [Dipartimento di Ingegneria Meccanica, Nucleare e della Produzione, Universita di Pisa, Pisa (Italy); Bedogni, R. [INFN, Laboratori Nazionali di Frascati, Frascati (Roma) (Italy); Esposito, J.; Zafiropoulos, D.; Colautti, P. [INFN, Laboratori Nazionali di Legnaro, Legnaro (Padova) (Italy)

    2013-07-18T23:59:59.000Z

    In the framework of TRASCO-BNCT project, a Bubble Interactive Neutron Spectrometer (BINS) device was applied to the characterization of the angle-and energy-differential neutron spectra generated by the {sup 9}Be(p,xn)reaction. The BINS spectrometer uses two superheated emulsion detectors, sequentially operated at different temperatures and thus provides a series of six sharp threshold responses, covering the 0.1-10 MeV neutron energy range. Spectrum unfolding of the data was performed by means of MAXED code. The obtained angle, energy-differential spectra were compared with those measured with a Bonner sphere spectrometer, a silicon telescope spectrometer and literature data.

  20. Two-electron coherence and time-bin entanglement detection in electron quantum optics

    E-Print Network [OSTI]

    E. Thibierge; D. Ferraro; B. Roussel; C. Cabart; A. Marguerite; G. Fève; P. Degiovanni

    2015-03-25T23:59:59.000Z

    Engineering and studying few-electron states in ballistic conductors is a key step towards understanding entanglement in quantum electronic systems. In this Letter, we introduce the intrinsic two-electron coherence of an electronic source in quantum Hall edge channels and relate it to two-electron wavefunctions and to current noise in an Hanbury Brown--Twiss interferometer. Inspired by the analogy with photon quantum optics, we propose to measure the intrinsic two-electron coherence of a source using low-frequency current correlation measurements at the output of a Franson interferometer. To illustrate this protocol, we discuss how it can distinguish between a time-bin entangled pure state and a statistical mixture of time shifted electron pairs.

  1. Hurricane Disturbance Alters Secondary Forest Recovery in Puerto Rico Dan F.B. Flynn1,7

    E-Print Network [OSTI]

    Uriarte, Maria

    Hurricane Disturbance Alters Secondary Forest Recovery in Puerto Rico Dan F.B. Flynn1,7 , Mar, Statesboro, GA 30460, U.S.A. 4 Institute for Tropical Ecosystem Studies, University of Puerto Rico, San Juan, Puerto Rico 00931, U.S.A. 5 Department of Biology, University of Puerto Rico, San Juan, Puerto Rico 00931

  2. http://www.ngs.noaa.gov/cgi-bin/ds_pid.prl/1[7/2/2010 2:26:29 PM] The NGS Data Sheet

    E-Print Network [OSTI]

    Ahmad, Sajjad

    DATASHEETS http://www.ngs.noaa.gov/cgi-bin/ds_pid.prl/1[7/2/2010 2:26:29 PM] The NGS Data Sheet See Report By GR1938 HISTORY - 1957 MONUMENTED CGS #12;DATASHEETS http://www.ngs.noaa.gov/cgi-bin/ds_pid.prl

  3. Why the Properties of El Nio Changed During the Late 1970s Bin Wang and Soon-Il An

    E-Print Network [OSTI]

    Wang, Bin

    1 Why the Properties of El Niño Changed During the Late 1970s Bin Wang and Soon-Il An School. Following the abrupt North Pacific climate shift in the mid-1970s, the period, amplitude, spatial structure in several El Niño characteristics are nearly synchronized with the decadal climate shift. While the decadal

  4. Impact of Secondary Eyewall Heating on Tropical Cyclone Intensity Change* XIAQIONG ZHOU, BIN WANG, XUYANG GE, AND TIM LI

    E-Print Network [OSTI]

    Wang, Bin

    Impact of Secondary Eyewall Heating on Tropical Cyclone Intensity Change* XIAQIONG ZHOU, BIN WANG is to explore the factors that might influence the intensity change of tropical cyclones (TCs) associated. Introduction Concentric eyewalls usually refer to two or more quasi-circular eyewalls separated by a convective

  5. Hydrogen-doped cubic diamond and the crystal structure of n-diamond Bin Wen a,b,

    E-Print Network [OSTI]

    Melnik, Roderick

    Hydrogen-doped cubic diamond and the crystal structure of n-diamond Bin Wen a,b, , Roderick Melnik. In particular, hydrogen concen- tration dependent elastic constants and lattice parameters for the H-doped diamond have been analyzed. Our results indicate that when the hydrogen concentration is less than 19 at

  6. Speech Enhancement of Spectral Magnitude Bin Trajectories using Gaussian Mixture-Model based Minimum Mean-Square Error Estimators

    E-Print Network [OSTI]

    Speech Enhancement of Spectral Magnitude Bin Trajectories using Gaussian Mixture-Model based mean-square error es- timators have been applied to speech enhancement in the tem- poral, transform (e estimator for 8 kHz telephone-quality speech. Index Terms: Speech enhancement, minimum mean-square er- ror

  7. Performance evaluation of source extraction in wireless sensor networks Hong-Bin Chen a,b,*, Chi Kong Tse a

    E-Print Network [OSTI]

    Tse, Chi K. "Michael"

    Performance evaluation of source extraction in wireless sensor networks Hong-Bin Chen a,b,*, Chi wireless sensor networks are evaluated. The sensor observations are assumed to be linear instantaneous: Available online 6 May 2008 Keywords: Wireless sensor network Blind source separation Cluster Performance

  8. Segmentation and Tracking of Mesoscale Eddies in Numeric Ocean Models Vishal Sood, Bin John, Ramprasad Balasubramanian and Amit Tandon*

    E-Print Network [OSTI]

    Tandon, Amit

    Segmentation and Tracking of Mesoscale Eddies in Numeric Ocean Models Vishal Sood, Bin John suggested that the mesoscale eddies and mesoscale features play a strong role in carrying heat poleward oceanographers an invaluable tool to assess mesoscale eddies and the Lagrangian characteristics of this mesoscale

  9. Characterization of transport and retention of biocolloids in unsaturated soils Tammo S. Steenhuis, Annette Dathe, Yuniati Zevi, Jennifer L. Smith, Bin Gao, Stephen B. Shaw,

    E-Print Network [OSTI]

    Walter, M.Todd

    , Annette Dathe, Yuniati Zevi, Jennifer L. Smith, Bin Gao, Stephen B. Shaw, Dilkushi DeAlwis, Samary Amaro, unsaturated porous media, pathogens. Pathogenic microbes including bacteria, viruses and protozoa have been

  10. The Dalhousie Guide to Waste Management on Campus Look for the four bin system around campus designated for paper, recyclables, organics and garbage.

    E-Print Network [OSTI]

    Brownstone, Rob

    for the four bin system around campus designated for paper, recyclables, organics.) · Ceramics · Potato chip bags & candy wrappers · Styrofoam Not acceptable: · Organics · Recyclables and dry. Organic Waste No liquids. Garbage Reconsider all waste for potential reuse before discarding

  11. Data:Ef07654d-404e-4e40-b090-b31b94f1fb1f | Open Energy Information

    Open Energy Info (EERE)

    e40-b090-b31b94f1fb1f 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...

  12. Data:Aa979968-ab20-4f1e-86a4-991fb0096e62 | Open Energy Information

    Open Energy Info (EERE)

    91fb0096e62 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....

  13. Data:4ca3ff7e-6b85-42c9-bb84-4e9616fb6e55 | Open Energy Information

    Open Energy Info (EERE)

    5-42c9-bb84-4e9616fb6e55 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...

  14. Data:5583703c-bd83-4fca-a385-34941e21fb14 | Open Energy Information

    Open Energy Info (EERE)

    5-34941e21fb14 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...

  15. Search for Sneutrino Production in e? Final States in 5.3??fb(?1) of pp-bar Collisions at s?=1.96??TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Clutter, Justace Randall; McGivern, Carrie Lynne; Sekaric, Jadranka; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Abolins, M.; Acharya, B. S.; Adams, M.; Adams, T.

    2010-11-05T23:59:59.000Z

    We report the results of a search for R parity violating (RPV) interactions leading to the production of supersymmetric sneutrinos decaying into e? final states using 5.3??fb(?1) of integrated luminosity collected by the ...

  16. Data:26f8315a-f068-43a6-8731-d726fb8fea9e | Open Energy Information

    Open Energy Info (EERE)

    1-d726fb8fea9e 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...

  17. Data:Ad2aa9e0-be41-4f30-853f-b60505435ca2 | Open Energy Information

    Open Energy Info (EERE)

    f-b60505435ca2 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...

  18. Techniques for Profile Binning and Analysis of Eigenvector Composite Spectra: Comparing Hbeta and MgII 2800 as Virial Estimators

    E-Print Network [OSTI]

    Sulentic, Jack W; del Olmo, Ascension; Plauchu-Frayn, Ilse

    2013-01-01T23:59:59.000Z

    We review the basic techniques for extracting information about quasar structure and kinematics from the broad emission lines in quasars. We consider which lines can most effectively serve as virial estimators of black hole mass. At low redshift the Balmer lines,particularly broad H beta, are the lines of choice. For redshifts greater than 0.7 - 0.8 one can follow H beta into the IR windows or find an H beta surrogate. We explain why UV CIV 1549 is not a safe virial estimator and how MgII 2800 serves as the best virial surrogate for H beta up to the highest redshift quasar known at z ~ 7. We show how spectral binning in a parameter space context (4DE1) makes possible a more effective comparison of H beta and MgII. It also helps to derive more accurate mass estimates from appropriately binned spectra and, finally, to map the dispersion in black hole mass and Eddington ratio across the quasar population. FWHM MgII is about 20% smaller than FWHM H beta in the majority of type 1 AGN requiring correction when comp...

  19. Measurement of the W boson helicity in top quark decays using 5.4 fb?¹ of pp? collision data

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; et al

    2011-02-01T23:59:59.000Z

    We present a measurement of the helicity of the W boson produced in top quark decays using tt¯ decays in the l+jets and dilepton final states selected from a sample of 5.4 fb?¹ of collisions recorded using the D0 detector at the Fermilab Tevatron pp? collider. We measure the fractions of longitudinal and right-handed W bosons to be f?=0.669±0.102[±0.078(stat.)±0.065(syst.)] and f?=0.023±0.053[±0.041(stat.)±0.034(syst.)], respectively. This result is consistent at the 98% level with the standard model. A measurement with f? fixed to the value from the standard model yields f?=0.010±0.037[±0.022(stat.)±0.030(syst.)].

  20. Measurement of the W boson helicity in top quark decays using 5.4 fb?¹ of pp? collision data

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; Ancu, L. S.; Aoki, M.; Arnoud, Y.; Arov, M.; Askew, A.; Åsman, B.; Atramentov, O.; Avila, C.; BackusMayes, J.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Barreto, J.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Beale, S.; Bean, A.; Begalli, M.; Begel, M.; Belanger-Champagne, C.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bezzubov, V. A.; Bhat, P. C.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Bolton, T. A.; Boos, E. E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Brooijmans, G.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Burnett, T. H.; Buszello, C. P.; Calpas, B.; Camacho-Pérez, E.; Carrasco-Lizarraga, M. A.; Casey, B. C. K.; Castilla-Valdez, H.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B.; Christoudias, T.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Croc, A.; Cutts, D.; ?wiok, M.; Das, A.; Davies, G.; De, K.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demarteau, M.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Dominguez, A.; Dorland, T.; Dubey, A.; Dudko, L. V.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Evdokimov, V. N.; Facini, G.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Gadfort, T.; Garcia-Bellido, A.; Gavrilov, V.; Gay, P.; Geist, W.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A.; Grannis, P. D.; Greder, S.; Greenlee, H.; Greenwood, Z. D.; Gregores, E. M.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guo, F.; Gutierrez, G.; Gutierrez, P.; Haas, A.; Hagopian, S.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hohlfeld, M.; Hossain, S.; Hubacek, Z.; Huske, N.; Hynek, V.; Iashvili, I.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jain, S.; Jamin, D.; Jesik, R.; Johns, K.; Johnson, M.; Johnston, D.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Juste, A.; Kaadze, K.; Kajfasz, E.; Karmanov, D.; Kasper, P. A.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Khatidze, D.; Kirby, M. H.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Kvita, J.; Lammers, S.; Landsberg, G.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lellouch, J.; Li, L.; Li, Q. Z.; Lietti, S. M.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, Y.; Liu, Z.; Lobodenko, A.; Lokajicek, M.; Love, P.; Lubatti, H. J.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Mackin, D.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Maravin, Y.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Mondal, N. K.; Muanza, G. S.; Mulhearn, M.; Nagy, E.; Naimuddin, M.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Novaes, S. F.; Nunnemann, T.; Obrant, G.; Orduna, J.; Osman, N.; Osta, J.; Otero y Garzón, G. J.; Owen, M.; Padilla, M.; Pangilinan, M.; Parashar, N.; Parihar, V.; Park, S. K.; Parsons, J.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, K.; Peters, Y.; Petrillo, G.; Pétroff, P.; Piegaia, R.; Piper, J.; Pleier, M.-A.; Podesta-Lerma, P. L. M.; Podstavkov, V. M.; Pol, M.-E.; Polozov, P.; Popov, A. V.; Prewitt, M.; Price, D.; Protopopescu, S.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M. S.; Ranjan, K.; Ratoff, P. N.; Razumov, I.; Renkel, P.; Rich, P.; Rijssenbeek, M.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Royon, C.; Rubinov, P.; Ruchti, R.; Safronov, G.; Sajot, G.; Sánchez-Hernández, A.; Sanders, M. P.; Sanghi, B.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schliephake, T.; Schlobohm, S.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shchukin, A. A.; Shivpuri, R. K.; Simak, V.; Sirotenko, V.; Skubic, P.; Slattery, P.; Smirnov, D.

    2011-02-01T23:59:59.000Z

    We present a measurement of the helicity of the W boson produced in top quark decays using tt¯ decays in the ?+jets and dilepton final states selected from a sample of 5.4??fb?¹ of collisions recorded using the D0 detector at the Fermilab Tevatron pp? collider. We measure the fractions of longitudinal and right-handed W bosons to be f?=0.669±0.102[±0.078(stat.)±0.065(syst.)] and f?=0.023±0.053[±0.041(stat.)±0.034(syst.)], respectively. This result is consistent at the 98% level with the standard model. A measurement with f? fixed to the value from the standard model yields f?=0.010±0.037[±0.022(stat.)±0.030(syst.)].

  1. Data:Cd13dc44-d0d6-46f0-bb39-fb84b30f7517 | Open Energy Information

    Open Energy Info (EERE)

    Cd13dc44-d0d6-46f0-bb39-fb84b30f7517 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading......

  2. Data:C66838d5-85f3-4a7e-89f4-5264fb348fa7 | Open Energy Information

    Open Energy Info (EERE)

    >> Category:Categories Retrieved from "http:en.openei.orgwindex.php?titleData:C66838d5-85f3-4a7e-89f4-5264fb348fa7&oldid620419" Category: Utility Rates What links...

  3. Non-linear adaptive robust control of electro-hydraulic systems driven by double-rod actuators BIN YAO{*. FANPING BU{ and GEORGE T. C. CHIU{

    E-Print Network [OSTI]

    Yao, Bin

    Non-linear adaptive robust control of electro-hydraulic systems driven by double-rod actuators BIN may be subjected to non-smooth and discontinuous non- linearities due to control input saturation of hydraulic dynamics which demands the use of non-linear control, hydraulic servosystems also have large

  4. The Dalhousie Guide to Waste Management on Campus Look for the four bin system around campus designated for paper, recyclables, organics and garbage.

    E-Print Network [OSTI]

    Brownstone, Rob

    for the four bin system around campus designated for paper, recyclables, organics.) · Ceramics · Potato chip bags & candy wrappers · Styrofoam Not acceptable: · Organics · Recyclables. For personal cell phone disposal, visit: call2recycle.ca · Employees can request office related e-waste

  5. On the Modeling and Analysis of Jitter in ATE Using Matlab Kyung Ki Kim, Jing Huang, Yong-Bin Kim, Fabrizio Lombardi

    E-Print Network [OSTI]

    Ayers, Joseph

    On the Modeling and Analysis of Jitter in ATE Using Matlab Kyung Ki Kim, Jing Huang, Yong-Bin Kim This paper presents a new jitter component analysis method for mixed mode VLSI chip testing in Automatic Test. The Matlab simulation shows how jitter components combine and how the total jitter depends on the jitter

  6. Modal Bin Hybrid Model: A Surface Area Consistent, Triple Moment Sectional Method for Use in Process-oriented Modeling of Atmospheric Aerosols

    SciTech Connect (OSTI)

    Kajino, Mizuo; Easter, Richard C.; Ghan, Steven J.

    2013-09-10T23:59:59.000Z

    A triple moment sectional method, Modal Bin Hybrid Model (MBHM), has been developed. In addition to number and mass (volume), surface area is predicted (and preserved), which is important for gas-to-particle mass transfer and light extinction cross section. The performance of MBHM was evaluated against double moment sectional (DMS) methods with various size resolutions up to BIN256 (BINx: x is number of sections over three orders of magnitude in size, ?logD = 3/x) for simulating evolution of particles under simultaneously occurring nucleation, condensation and coagulation processes. Because MBHM gives a physically consistent form of the intra-sectional distributions, errors and biases of MBHM at BIN4-8 resolution were almost equivalent to those of DMS at BIN16-32 resolution for various important variables such as the moments Mk (k: 0, 2, 3), dMk/dt, and the number and volume of particles larger than a certain diameter. Another important feature of MBHM is that only a single bin is adequate to simulate full aerosol dynamics for particles whose size distribution can be approximated by a single lognormal mode. This flexibility is useful for process-oriented (multi category and/or mixing state) modeling: primary aerosols whose size parameters would not differ substantially in time and space can be expressed by a single or a small number of modes, whereas secondary aerosols whose size changes drastically from one to several hundred nanometers can be expressed by a number of modes. Added dimensions can be applied to MBHM to represent mixing state or photo-chemical age for aerosol mixing state studies.

  7. Combined search for the Standard Model Higgs boson using up to 4.9 fb[superscript ?1] of pp collision data at ?s = 7 TeV with the ATLAS detector at the LHC

    E-Print Network [OSTI]

    Taylor, Frank E.

    A combined search for the Standard Model Higgs boson with the ATLAS experiment at the LHC using datasets corresponding to integrated luminosities from 1.04 fb[superscript ?1] to 4.9 fb[superscript ?1] of pp collisions ...

  8. 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]

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

    2011-07-25T23:59:59.000Z

    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.

  9. Interpretations and implications of the top quark rapidity asymmetries A FB t and A FB ?

    SciTech Connect (OSTI)

    Berger, Edmond L.; Cao, Qing-Hong; Chen, Chuan-Ren; Zhang, Hao

    2013-07-01T23:59:59.000Z

    Forward-backward asymmetries AtFB and AlFB are observed in the top-quark t rapidity distribution and in the rapidity distribution of charged leptons l from top-quark decay at the Tevatron proton-antiproton collider, and a charge asymmetry AC is seen in proton-proton collisions at the Large Hadron Collider (LHC). In this paper, we update our previous studies of the Tevatron asymmetries using the most recent data. We provide expectations for AC at the LHC based first on simple extrapolations from the Tevatron, and second based on new physics models that can explain the Tevatron asymmetries. We examine the relationship of the two asymmetries AtFB and AlFB. We show their connection through the (V–A) spin correlation between the charged lepton and the top quark with different polarization states. We show that the ratio of the two asymmetries provides independent insight into the physics interpretation of the top-quark asymmetry. We emphasize the value of the measurement of both asymmetries, and we conclude that a model which produces more right-handed than left-handed top quarks is suggested by the present Tevatron data.

  10. SM71A-2 Ginzburg-Landau Model for Whistler Wave Amplification... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 2 3/10/05 11:47 AM

    E-Print Network [OSTI]

    Ng, Chung-Sang

    SM71A-2 Ginzburg-Landau Model for Whistler Wave Amplification... http://www.agu.org/cgi-bin/SFgate/SFgate?language Fall Meeting New Search #12;SM71A-2 Ginzburg-Landau Model for Whistler Wave Amplification... http://www.agu.org/cgi-bin/SFgate/SFgate?language" ------------------------------ HR: 0830h AN: SM71A-23 TI: Ginzburg-Landau Model for Whistler Wave Amplification, Saturation

  11. Year GBClass Make Model M/M/Specs EmisStd City Hiwy Green Score 2014 01_TS AUDI TT ROADSTER QUATTRO 2.0L 4, auto Awd [P] ULEV II / Bin 5 22 31 42

    E-Print Network [OSTI]

    Derisi, Joseph

    Year GBClass Make Model M/M/Specs EmisStd City Hiwy Green Score 2014 01_TS MERCEDES-BENZ SMART FORTWO (CONVERTIBLE) 1.0L 3, auto [P] ULEV II / Bin 5 34 38 53 2014 01_TS MERCEDES-BENZ SMART FORTWO (COUPE) 1.0L 3, auto [P] ULEV II / Bin 5 34 38 53 2014 01_TS MERCEDES

  12. 222-S Laboratory analytical report for tank 241-C-106, grab samples 6C-96-1 through 6C-96-16 {ampersand} 6C-96-17-FB

    SciTech Connect (OSTI)

    Esch, R.A.

    1996-08-06T23:59:59.000Z

    This document is the analytical report for grab samples 6C-96-1through 6C-96-16 and 6C-96-17-FB from tank 241-C-106.

  13. bin.dvi

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:Energy: Grid Integration Redefining What'sis Taking Over OurThe Iron4 Self-Scrubbing Coal(tm): An IntegratedEffectsIntegration of

  14. Search for Randall-Sundrum Gravitons in Dielectron and Diphoton Final States with 5.4fb-1 of D0 Data

    SciTech Connect (OSTI)

    Zhou, Ning; /Columbia U.

    2010-03-01T23:59:59.000Z

    A search for the lightest Kaluza-Klein mode of the graviton in the Randall-Sundrum model with a warped extra dimension is performed in the dielectron and diphoton channels. The data set used for the search corresponds to 5.4 fb{sup -1} of data from p{bar p} collisions at a center-of-mass energy of 1.96 TeV, collected with the D0 detector at the Fermilab Tevatron between July 2002 and Summer 2009. We search for resonances in the invariant mass spectrum of two electromagnetic showers from the decay of the graviton to either electron-positron pairs or photon pairs. To optimize the sensitivity, the dielectron and diphoton channels are analyzed separately, then the results are combined together in the end. We also investigate whether, due to the unique spin-2 nature of the graviton, the angular distribution of the final state particles can be used to significantly enhance the sensitivity of the search. We set 95% confidence level upper limits on the graviton production cross section times branching fraction into electron-positron pairs of between {approx} 7 fb and {approx} 0.5 fb for a range of graviton masses from 220 GeV and 1050 GeV, respectively. Compared with Randall-Sundrum model predictions, these results correspond to lower limits on the lightest graviton mass between 440 GeV and 1040 GeV, for the dimensionless graviton coupling to the Standard Model fields k/{bar M}{sub Pl} in the range from 0.01 to 0.1. In addition, for coupling k/{bar M}{sub Pl} of 0.01, gravitons with masses between 460 GeV and 560 GeV are also excluded at 95% confidence level. These results represent the most sensitive limits to date.

  15. Combination of CDF and D0 results on the mass of the top quark using up to 9.7 fb$^{-1}$ at the Tevatron

    E-Print Network [OSTI]

    Tevatron Electroweak Working Group

    2014-07-12T23:59:59.000Z

    We summarize the current top-quark mass measurements from the CDF and D0 experiments at Fermilab. We combine published Run I (1992--1996) results with the most precise published and preliminary Run II (2001--2011) measurements based on data corresponding to up to 9.7 fb$^{-1}$ of $p\\bar{p}$ collisions. Taking correlations of uncertainties into account, and combining the statistical and systematic uncertainties, the resulting preliminary Tevatron average mass of the top quark is $M_{top} = 174.34 \\pm 0.64 ~GeV/c^2$, corresponding to a relative precision of 0.37%.

  16. A study of the air flow rates and their effects on bin drying sorghum grain with unheated air in South Texas

    E-Print Network [OSTI]

    Aldred, William H

    1956-01-01T23:59:59.000Z

    with the foot storage spoon use not availablo to hold their grain for s mors favorable market. Furthermore, only a limited amount of a~nial storage vss available at that time, These oonditions disolosed the need for infox- mstion consuming pxoesdurss.../ustment of the air flow to the desired rates was controlled bp two sliding gates in the latexal ss shown in Figure 5. Bzxcyle ports were installed in each bin at two levels ? one foot. from the bottom snd halfway between the bottom and the toy, This per- mitted...

  17. 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]

    The CDF; D0 Collaborations; the TEVNPHWG Working Group

    2011-08-16T23:59:59.000Z

    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

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

    SciTech Connect (OSTI)

    Not Available

    2011-07-01T23:59:59.000Z

    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}.

  19. Interplay between the lattice and spin degrees of freedom in (Sr1-xCax)3Ru2O7 Jin Peng,1 Zhe Qu,1 Bin Qian,1,2,3 David Fobes,1 Tijiang Liu,1 Xiaoshan Wu,2 H. M. Pham,4 Leonard Spinu,4 and

    E-Print Network [OSTI]

    Spinu, Leonard

    Bin Qian,1,2,3 David Fobes,1 Tijiang Liu,1 Xiaoshan Wu,2 H. M. Pham,4 Leonard Spinu,4 and Z. Q. Mao1

  20. Measurement of the W boson helicity in top quark decays using 5.4 fb$^{\\boldsymbol{-1}}$ of $\\boldsymbol{p\\bar{p}}$ collision data

    SciTech Connect (OSTI)

    Abazov, Victor Mukhamedovich; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma U.; Acharya, Bannanje Sripath; /Tata Inst.; Adams, Mark Raymond; /Illinois U., Chicago; Adams, Todd; /Florida State U.; Alexeev, Guennadi D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Augustana Coll., Sioux Falls; Alverson, George O.; /Northeastern U.; Alves, Gilvan Augusto; /Rio de Janeiro, CBPF; Ancu, Lucian Stefan; /Nijmegen U. /Fermilab

    2010-11-01T23:59:59.000Z

    We present a measurement of the helicity of the W boson produced in top quark decays using t{bar t} decays in the {ell}+jets and dilepton final states selected from a sample of 5.4 fb{sup -1} of collisions recorded using the D0 detector at the Fermilab Tevatron p{bar p} collider. We measure the fractions of longitudinal and right-handed W bosons to be f{sub 0} = 0.669 {+-} 0.102 [{+-}0.078 (stat.) {+-} 0.065 (syst.)] and f{sub +} = 0.023 {+-} 0.053 [{+-}0.041 (stat.){+-}0.034 (syst.)], respectively. This result is consistent at the 98% level with the standard model. A measurement with f{sub 0} fixed to the value from the standard model yields f{sub +} = 0.010 {+-} 0.037 [{+-}0.022 (stat.) {+-} 0.030 (syst.)].

  1. Search for $WH$ associated production in 5.3 fb$^{-1}$ of $p\\bar{p}$ collisions at the Fermilab Tevatron

    SciTech Connect (OSTI)

    Abazov, Victor Mukhamedovich; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma U.; Acharya, Bannanje Sripath; /Tata Inst.; Adams, Mark Raymond; /Illinois U., Chicago; Adams, Todd; /Florida State U.; Alexeev, Guennadi D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Augustana Coll., Sioux Falls; Alverson, George O.; /Northeastern U.; Alves, Gilvan Augusto; /Rio de Janeiro, CBPF; Ancu, Lucian Stefan; /Nijmegen U. /Fermilab

    2010-12-01T23:59:59.000Z

    We present a search for associated production of Higgs and W bosons in p{bar p} collisions at a center of mass energy of {radical}s = 1.96 TeV in 5.3 fb{sup -1} of integrated luminosity recorded by the D0 experiment. Multivariate analysis techniques are applied to events containing one lepton, an imbalance in transverse energy, and one or two b-tagged jets to discriminate a potential WH signal from standard model backgrounds. We observe good agreement between data and background, and set an upper limit of 4.5 (at 95% confidence level and for m{sub H} = 115 GeV) on the ratio of the WH cross section multiplied by the branching fraction of H {yields} b{bar b} to its standard model prediction. A limit of 4.8 is expected from simulation.

  2. Measurement of the WZ and ZZ production cross sections using leptonic final states in 8.6 fb?¹ of pp? collisions

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Aoki, M.; Askew, A.; Åsman, B.; Atkins, S.; Atramentov, O.; Augsten, K.; Avila, C.; BackusMayes, J.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Barreto, J.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Bean, A.; Begalli, M.; Belanger-Champagne, C.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bezzubov, V. A.; Bhat, P. C.; Bhatia, S.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Brooijmans, G.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Burnett, T. H.; Buszello, C. P.; Calpas, B.; Camacho-Pérez, E.; Carrasco-Lizarraga, M. A.; Casey, B. C. K.; Castilla-Valdez, H.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Croc, A.; Cutts, D.; Das, A.; Davies, G.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dorland, T.; Dubey, A.; Dudko, L. V.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Evdokimov, V. N.; Facini, G.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Garcia-Bellido, A.; García-Guerra, G. A.; Gavrilov, V.; Gay, P.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A.; Grannis, P. D.; Greder, S.; Greenlee, H.; Greenwood, Z. D.; Gregores, E. M.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Haas, A.; Hagopian, S.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hohlfeld, M.; Hubacek, Z.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jamin, D.; Jayasinghe, A.; Jesik, R.; Johns, K.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A. W.; Juste, A.; Kaadze, K.; Kajfasz, E.; Karmanov, D.; Kasper, P. A.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kulikov, S.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Lammers, S.; Landsberg, G.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lellouch, J.; Li, H.; Li, L.; Li, Q. Z.; Lietti, S. M.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Lubatti, H. J.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Mackin, D.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Maravin, Y.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N. K.; Muanza, G. S.; Mulhearn, M.; Nagy, E.; Naimuddin, M.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Novaes, S. F.; Nunnemann, T.; Obrant, G.; Orduna, J.; Osman, N.; Osta, J.; Oteroy y Garzón, G. J.; Padilla, M.; Pal, A.; Parashar, N.; Parihar, V.; Park, S. K.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Piegaia, R.; Pleier, M.-A.; Podesta-Lerma, P. L. M.; Podstavkov, V. M.; Polozov, P.; Popov, A. V.; Prewitt, M.; Price, D.; Prokopenko, N.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M. S.; Ranjan, K.; Ratoff, P. N.; Razumov, I.; Renkel, P.; Rijssenbeek, M.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Safronov, G.; Sajot, G.; Salcido, P.; Sánchez-Hernández, A.; Sanders, M. P.; Sanghi, B.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schliephake, T.; Schlobohm, S.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shchukin, A. A.; Shivpuri, R. K.; Simak, V.; Sirotenko, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Smith, K. J.; Snow, G. R.; Snow, J.; Snyder, S.; Söldner-Rembold, S.; Sonnenschein, L.; Soustruznik, K.; Stark, J.

    2012-06-01T23:59:59.000Z

    We study the processes pp??WZ?l±?l?l? and pp??ZZ?l?l???¯, where l=e or ?. Using 8.6 fb?¹ of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron collider, we measure the WZ production cross section to be 4.50+0.63–0.66 pb which is consistent with, but slightly larger than, the prediction of the standard model. The ZZ cross section is measured to be 1.64±0.46 pb, in agreement with a prediction of the standard model. Combination with an earlier analysis of the ZZ?l?l?l?l? channel yields a ZZ cross section of 1.44+0.35–0.34 pb.

  3. Measurement of direct CP violation parameters in B±?J/?K± and B±?J/??± decays with 10.4??fb-1 of Tevatron data

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Agnew, J. P.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Askew, A.; Atkins, S.; Augsten, K.; Avila, C.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Bean, A.; Beattie, M.; Begalli, M.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bhat, P. C.; Bhatia, S.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Brandt, A.; Brandt, O.; Brock, R.; Bross, A.; Brown, D.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Buszello, C. P.; Camacho-Pérez, E.; Casey, B. C. K.; Castilla-Valdez, H.; Caughron, S.; Chakrabarti, S.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Cho, S. W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Cutts, D.; Das, A.; Davies, G.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dubey, A.; Dudko, L. V.; Duperrin, A.; Dutt, S.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, V. N.; Feng, L.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Garbincius, P. H.; Garcia-Bellido, A.; García-González, J. A.; Gavrilov, V.; Geng, W.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Grannis, P. D.; Greder, S.; Greenlee, H.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hart, B.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hogan, J.; Hohlfeld, M.; Howley, I.; Hubacek, Z.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jayasinghe, A.; Holzbauer, J.; Jeong, M. S.; Jesik, R.; Jiang, P.; Johns, K.; Johnson, E.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A. W.; Juste, A.; Kajfasz, E.; Karmanov, D.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kiselevich, I.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Lammers, S.; Lamont, I.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lei, X.; Lellouch, J.; Li, D.; Li, H.; Li, L.; Li, Q. Z.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, H.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Mansour, J.; Martínez-Ortega, J.; Mason, N.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N. K.; Mulhearn, M.; Nagy, E.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Nguyen, H. T.; Nunnemann, T.; Orduna, J.; Osman, N.; Osta, J.; Pal, A.; Parashar, N.; Parihar, V.; Park, S. K.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Pleier, M.-A.; Podstavkov, V. M.; Popov, A. V.; Prewitt, M.; Price, D.; Prokopenko, N.; Qian, J.; Quadt, A.; Quinn, B.; Ratoff, P. N.; Razumov, I.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Sajot, G.; Sánchez-Hernández, A.; Sanders, M. P.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shaw, S.; Shchukin, A. A.; Simak, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Snow, G. R.; Snow, J.; Snyder, S.; Söldner-Rembold, S.; Sonnenschein, L.; Soustruznik, K.; Stark, J.; Stoyanova, D. A.; Strauss, M.; Suter, L.; Svoisky, P.; Titov, M.; Tokmenin, V. V.; Tsai, Y.-T.; Tsybychev, D.; Tuchming, B.; Tully, C.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Van Kooten, R.; van Leeuwen, W. M.; Varelas, N.; Varnes, E. W.; Vasilyev, I. A.; Verkheev, A. Y.; Vertogradov, L. S.; Verzocchi, M.; Vesterinen, M.; Vilanova, D.; Vokac, P.; Wahl, H. D.; Wang, M. H. L. S.; Warchol, J.; Watts, G.; Wayne, M.; Weichert, J.; Welty-Rieger, L.; Williams, M. R. J.; Wilson, G. W.; Wobisch, M.; Wood, D. R.; Wyatt, T. R.; Xie, Y.; Yamada, R.; Yang, S.; Yasuda, T.; Yatsunenko, Y. A.; Ye, W.; Ye, Z.; Yin, H.; Yip, K.; Youn, S. W.

    2013-06-01T23:59:59.000Z

    We present a measurement of the direct CP-violating charge asymmetry in B± mesons decaying to J/?K± and J/??± where J/? decays to ?+??, using the full run II data set of 10.4??fb?1 of proton-antiproton collisions collected using the D0 detector at the Fermilab Tevatron Collider. A difference in the yield of B? and B+ mesons in these decays is found by fitting to the difference between their reconstructed invariant mass distributions resulting in asymmetries of AJ/?K=[0.59±0.37]%, which is the most precise measurement to date, and AJ/??=[?4.2±4.5]%. Both measurements are consistent with standard model predictions.

  4. A measurement of the $WZ$ and $ZZ$ production cross sections using leptonic final states in 8.6 fb$^{-1}$ of $p\\bar{p}$ collisions

    SciTech Connect (OSTI)

    Abazov, Victor Mukhamedovich; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma U.; Acharya, Bannanje Sripath; /Tata Inst.; Adams, Mark Raymond; /Illinois U., Chicago; Adams, Todd; /Florida State U.; Alexeev, Guennadi D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Augustana Coll., Sioux Falls; Alverson, George O.; /Northeastern U.; Aoki, Masato; /Fermilab; Askew, Andrew Warren; /Florida State U. /Stockholm U.

    2012-01-01T23:59:59.000Z

    We study the processes p{bar p} {yields} WZ {yields} {ell}{nu}{ell}{sup +}{ell}{sup -} and p{bar p} {yields} ZZ {yields} {ell}{sup +}{ell}{sup -}{nu}{bar {nu}}, where {ell} = e or {mu}. Using 8.6 fb{sup -1} of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron collider, we measure the WZ production cross section to be 4.50{sub -0.66}{sup +0.63} pb which is consistent with, but slightly above a prediction of the standard model. The ZZ cross section is measured to be 1.64 {+-} 0.46 pb, in agreement with a prediction of the standard model. Combination with an earlier analysis of the ZZ {yields} {ell}{sup +}{ell}{sup -}{ell}{sup +}{ell}{sup -} channel yields a ZZ cross section of 1.44{sub -0.34}{sup +0.35} pb.

  5. Search for Diphoton Events with Large Missing Transverse Energy in 6.3 fb-1 of ppbar Collisions using the D0 Detector at the Fermilab Tevatron Collider

    SciTech Connect (OSTI)

    Cooke, Mark Stephen; /Columbia U.

    2010-09-01T23:59:59.000Z

    A search for diphoton events with large missing transverse energy produced in p{bar p} collisions at {radical}s = 1.96 TeV is presented. The data were collected with the D0 detector at the Fermilab Tevatron Collider between 2002 and 2010, and correspond to 6.3 fb{sup -1} of integrated luminosity. The observed missing transverse energy distribution is well described by the Standard Model prediction, and 95% C.L. limits are derived on two realizations of theories beyond the Standard Model. In a gauge mediated supersymmetry breaking scenario, the breaking scale {Lambda} is excluded for {Lambda} < 124 TeV. In a universal extra dimension model including gravitational decays, the compactification radius R{sub c} is excluded for R{sub c}{sup -1} < 477 GeV.

  6. A search for resonant production of tt? pairs in 4.8 fb-1 of integrated luminosity of pp? collisions at ?s=1.96 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    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.; Annovi, A [Frascati; Antos, J [Comenius U.; Apollinari, G [Fermilab; Appel, J A [Fermilab; Apresyan, A [Purdue U.; Arisawa, T [Waseda U.; Dubna, JINR

    2011-10-27T23:59:59.000Z

    We search for resonant production of tt? pairs in 4.8 fb-1 integrated luminosity of pp? collision data at ?s = 1.96 TeV in the lepton+jets decay channel, where one top quark decays leptonically and the other hadronically. A matrix element reconstruction technique is used; for each event a probability density function (pdf) of the tt? candidate invariant mass is sampled. These pdfs are used to construct a likelihood function, whereby the cross section for resonant tt? production is estimated, given a hypothetical resonance mass and width. The data indicate no evidence of resonant production of tt? pairs. A benchmark model of leptophobic Z' ? tt? is excluded with mZ' < 900 GeV at 95% confidence level.

  7. Search for the Standard Model Higgs Boson in Associated WH Production in 9.7 fb?¹ of pp? Collisions with the D0 Detector

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Askew, A.; Atkins, S.; Augsten, K.; Avila, C.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Bean, A.; Begalli, M.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bhat, P. C.; Bhatia, S.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Buszello, C. P.; Camacho-Pérez, E.; Casey, B. C. K.; Castilla-Valdez, H.; Caughron, S.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Croc, A.; Cutts, D.; Das, A.; Davies, G.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dubey, A.; Dudko, L. V.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Evdokimov, V. N.; Facini, G.; Feng, L.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Garcia-Bellido, A.; García-González, J. A.; García-Guerra, G. A.; Gavrilov, V.; Gay, P.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A.; Grannis, P. D.; Greder, S.; Greenlee, H.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Hagopian, S.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hogan, J.; Hohlfeld, M.; Howley, I.; Hubacek, Z.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jayasinghe, A.; Jeong, M. S.; Jesik, R.; Jiang, P.; Johns, K.; Johnson, E.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A. W.; Juste, A.; Kaadze, K.; Kajfasz, E.; Karmanov, D.; Kasper, P. A.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kiselevich, I.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kulikov, S.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Lammers, S.; Landsberg, G.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lei, X.; Lellouch, J.; Li, D.; Li, H.; Li, L.; Li, Q. Z.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, H.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Lubatti, H. J.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Maravin, Y.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N. K.; Mulhearn, M.; Nagy, E.; Naimuddin, M.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Nguyen, H. T.; Nunnemann, T.; Orduna, J.; Osman, N.; Osta, J.; Padilla, M.; Pal, A.; Parashar, N.; Parihar, V.; Park, S. K.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Pleier, M.-A.; Podesta-Lerma, P. L. M.; Podstavkov, V. M.; Popov, A. V.; Prewitt, M.; Price, D.; Prokopenko, N.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M. S.; Ranjan, K.; Ratoff, P. N.; Razumov, I.; Renkel, P.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Sajot, G.; Salcido, P.; Sánchez-Hernández, A.; Sanders, M. P.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schlobohm, S.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shaw, S.; Shchukin, A. A.; Shivpuri, R. K.; Simak, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Smith, K. J.; Snow, G. R.; Snow, J.; Snyder, S.; Söldner-Rembold, S.; Sonnenschein, L.; Soustruznik, K.; Stark, J.; Stoyanova, D. A.; Strauss, M.; Suter, L.; Svoisky, P.; Takahashi, M.; Titov, M.; Tokmenin, V. V.; Tsai, Y.-T.; Tschann-Grimm, K.; Tsybychev, D.; Tuchming, B.; Tully, C.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Van Kooten, R.; van Leeuwen, W. M.; Varelas, N.; Varnes, E. W.

    2012-09-01T23:59:59.000Z

    We present a search for the standard model Higgs boson in final states with a charged lepton (electron or muon), missing transverse energy, and two or three jets, at least one of which is identified as a b-quark jet. The search is primarily sensitive to WH?l?bb¯ production and uses data corresponding to 9.7 fb?¹ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron pp¯ Collider at ?s=1.96 TeV. We observe agreement between the data and the expected background. For a Higgs boson mass of 125 GeV, we set a 95% C.L. upper limit on the production of a standard model Higgs boson of 5.2×?SM, where ?SM is the standard model Higgs boson production cross section, while the expected limit is 4.7×?SM.

  8. Search for the Standard Model Higgs Boson in Associated WH Production in 9.7 fb?¹ of pp? Collisions with the D0 Detector

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Askew, A.; et al

    2012-09-01T23:59:59.000Z

    We present a search for the standard model Higgs boson in final states with a charged lepton (electron or muon), missing transverse energy, and two or three jets, at least one of which is identified as a b-quark jet. The search is primarily sensitive to WH?l?bb¯ production and uses data corresponding to 9.7 fb?¹ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron pp¯ Collider at ?s=1.96 TeV. We observe agreement between the data and the expected background. For a Higgs boson mass of 125 GeV, we set a 95% C.L. upper limit on the production ofmore »a standard model Higgs boson of 5.2×?SM, where ?SM is the standard model Higgs boson production cross section, while the expected limit is 4.7×?SM.« less

  9. Measurement of direct CP violation parameters in B(±)?J/?K(±) and B(±)?J/??(±) decays with 10.4??fb(?1) of Tevatron data

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Chen, G.; Clutter, Justace Randall; Sekaric, Jadranka; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Agnew, J. P.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Askew, A.

    2013-06-12T23:59:59.000Z

    Measurement of direct CP violation parameters in B#1; ! J=cK#1; and B#1; ! J=c#1;#1; decays with 10:4 fb#2;1 of Tevatron data V.M. Abazov,31 B. Abbott,66 B. S. Acharya,25 M. Adams,45 T. Adams,43 J. P. Agnew,40 G.D. Alexeev,31 G. Alkhazov,35 A. Alton..., Seattle, Washington 98195, USA (Received 8 April 2013; published 12 June 2013) We present a measurement of the direct CP-violating charge asymmetry in B#1; mesons decaying to J=cK#1; and J=c#1;#1; where J=c decays to #2;þ#2;#2;, using the full run II data...

  10. Search for Doubly-charged Higgs Boson Production in the Decay H++ H-- ---> mu+ mu+ mu- mu- with 1.1 fb**(-1) at D0 Detector

    SciTech Connect (OSTI)

    Kim, Tae Jeong; /Korea U.

    2007-06-01T23:59:59.000Z

    This work presents a search for the pair production of doubly-charged Higgs bosons in the process p{bar p} {yields} H{sup ++}H{sup --} {yields} {mu}{sup +}{mu}{sup +}{mu}{sup -}{mu}{sup -} using the data corresponding to an integrated luminosity of about 1.1 fb{sup -1}. This is the complete dataset of RunIIa taken from April 19, 2002 to February 22, 2006 by the D0 experiment at the Fermilab Tevatron Collider. In the absence of significant excess above standard model background, 95% confidence level mass limits of M(H{sub L}{sup {+-}{+-}}) > 150 GeV and M(H{sub R}{sup {+-}{+-}}) > 126.5 GeV are set for left-handed and right-handed doubly-charged Higgs bosons respectively assuming a 100% branching ratio into muons.

  11. Measurement of the CP-violating phase ?sJ/?? using the flavor-tagged decay Bs0?J/ ?? in 8 fb?¹ of pp? collisions

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; Aoki, M.; Arov, M.; Askew, A.; Åsman, B.; Atkins, S.; Atramentov, O.; Augsten, K.; Avila, C.; BackusMayes, J.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Barreto, J.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Bean, A.; Begalli, M.; Begel, M.; Belanger-Champagne, C.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bezzubov, V. A.; Bhat, P. C.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Brooijmans, G.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Burnett, T. H.; Buszello, C. P.; Calpas, B.; Camacho-Pérez, E.; Carrasco-Lizarraga, M. A.; Casey, B. C. K.; Castilla-Valdez, H.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Croc, A.; Cutts, D.; Das, A.; Davies, G.; De, K.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demarteau, M.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dorland, T.; Dubey, A.; Dudko, L. V.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Evdokimov, V. N.; Facini, G.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Garcia-Bellido, A.; García-Guerra, G. A.; Gavrilov, V.; Gay, P.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A.; Grannis, P. D.; Greder, S.; Greenlee, H.; Greenwood, Z. D.; Gregores, E. M.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Haas, A.; Hagopian, S.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hohlfeld, M.; Hubacek, Z.; Huske, N.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jamin, D.; Jayasinghe, A.; Jesik, R.; Johns, K.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A. W.; Juste, A.; Kaadze, K.; Kajfasz, E.; Karmanov, D.; Kasper, P. A.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kulikov, S.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Kvita, J.; Lammers, S.; Landsberg, G.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lellouch, J.; Li, L.; Li, Q. Z.; Lietti, S. M.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Lubatti, H. J.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Mackin, D.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Maravin, Y.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N. K.; Muanza, G. S.; Mulhearn, M.; Nagy, E.; Naimuddin, M.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Novaes, S. F.; Nunnemann, T.; Obrant, G.; Orduna, J.; Osman, N.; Osta, J.; Otero y Garzón, G. J.; Padilla, M.; Pal, A.; Parashar, N.; Parihar, V.; Park, S. K.; Parsons, J.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, K.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Piegaia, R.; Pleier, M.-A.; Podesta-Lerma, P. L. M.; Podstavkov, V. M.; Polozov, P.; Popov, A. V.; Prewitt, M.; Price, D.; Prokopenko, N.; Protopopescu, S.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M. S.; Ranjan, K.; Ratoff, P. N.; Razumov, I.; Renkel, P.; Rijssenbeek, M.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Safronov, G.; Sajot, G.; Salcido, P.; Sánchez-Hernández, A.; Sanders, M. P.; Sanghi, B.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schliephake, T.; Schlobohm, S.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shchukin, A. A.; Shivpuri, R. K.; Simak, V.; Sirotenko, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Smith, K. J.

    2012-02-01T23:59:59.000Z

    We report an updated measurement of the CP-violating phase, ?sJ/??, and the decay-width difference for the two mass eigenstates, ??s, from the flavor-tagged decay B0s?J/??. The data sample corresponds to an integrated luminosity of 8.0 fb?¹ accumulated with the D0 detector using pp? collisions at ?s=1.96 TeV produced at the Fermilab Tevatron collider. The 68% Bayesian credibility intervals, including systematic uncertainties, are ??s=0.163+0.065?0.064 ps?¹ and ?sJ/??=?0.55+0.38?0.36. The p-value for the Standard Model point is 29.8%.

  12. 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]

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

    2011-09-20T23:59:59.000Z

    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

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

    SciTech Connect (OSTI)

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

    2011-07-01T23:59:59.000Z

    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}.

  14. 11/12/11 Journal of Geophysical Research -Atmospheres: Editors' Highlight 1/1www.agu.org/cgi-bin/highlights/highlights.cgi?action=show&doi=10.1029/20

    E-Print Network [OSTI]

    Jimenez, Jose-Luis

    11/12/11 Journal of Geophysical Research - Atmospheres: Editors' Highlight 1/1www.agu.org/cgi-bin/highlights/highlights.cgi?action=show&doi=10.1029/20 ©2011. American Geophysical Union. All Rights Reserved. AGU: Jo nal of Geoph ical Re ea ch

  15. Four-Field Model for Dispersive Field-Line Resonances in Collision... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 2 3/10/05 11:46 AM

    E-Print Network [OSTI]

    Ng, Chung-Sang

    Four-Field Model for Dispersive Field-Line Resonances in Collision... http://www.agu.org/cgi-bin/SFgate/SFgate?language" ------------------------------ HR: 1330h AN: SM22A-13 TI: Four-Field Model for Dispersive Field-Line Resonances in Collisionless theoretical model is proposed for dispersive field-line resonances in magnetospheric plasmas. The model

  16. Four-Field Model for Dispersive Field-Line Resonances in the Colli... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 2 3/10/05 11:44 AM

    E-Print Network [OSTI]

    Ng, Chung-Sang

    Four-Field Model for Dispersive Field-Line Resonances in the Colli... http://www.agu.org/cgi-bin/SFgate/SFgate?language: 10:45h AN: SM21B-08 TI: Four-Field Model for Dispersive Field-Line Resonances in the Collisionless. Recently, we have proposed a new theoretical model for FLRs in collisionless magnetospheric plasmas

  17. Measurement of the inclusive isolated prompt photons cross section in pp collisions at ?s = 7 TeV with the ATLAS detector using 4.6 fb[superscript -1

    E-Print Network [OSTI]

    Taylor, Frank E.

    A measurement of the cross section for the production of isolated prompt photons in pp collisions at a center-of-mass energy ?s = 7??TeV is presented. The results are based on an integrated luminosity of 4.6??fb[superscript ...

  18. Search for the Production of Narrow tb-bar Resonances in 1.9 fb-1 of pp-bar Collisions at sqrt[s]=1.96 TeV

    E-Print Network [OSTI]

    Xie, Si

    We present new limits on resonant tb? production in pp? collisions at ?s=1.96??TeV, using 1.9??fb[superscript -1] of data recorded with the CDF II detector at the Fermilab Tevatron. We reconstruct a candidate tb? mass ...

  19. The Tiniest Power Plants http://www.businessweek.com/@@YTkdxWQQ7ju4fB4A/... 1 of 3 5/26/2006 1:09 PM

    E-Print Network [OSTI]

    Lovley, Derek

    was the power source for the buoy's electronics: microbes. Bacteria in the river bottom gobbled up organic.D. Power Ratings Product Reviews Tech Stats Wildstrom: Tech Maven AUTOS Home Page Auto Reviews Classic CarsThe Tiniest Power Plants http://www.businessweek.com/@@YTkdxWQQ7ju4fB4A/... 1 of 3 5/26/2006 1

  20. Search for a Higgs boson in diphoton final states with the D0 detector in 9.6??fb(?1) of pp-bar collisions at s?=1.96??TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Chen, G.; Clutter, Justace Randall; Sekaric, Jadranka; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Askew, A.; Atkins, S.

    2013-09-17T23:59:59.000Z

    We present a search for a Higgs boson decaying into a pair of photons based on 9.6??fb(?1) of pp-bar collisions at s?=1.96??TeV collected with the D0 detector at the Fermilab Tevatron Collider. The search employs multivariate techniques...

  1. Search for Higgs boson production in oppositely charged dilepton and missing energy final states in 9.7??fb(?1) of pp-bar collisions at s?=1.96??TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Chen, Gemma; Clutter, Justace Randall; Sekaric, Jadranka; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Askew, A.; Atkins, S.

    2013-09-17T23:59:59.000Z

    We present a search for the Higgs boson in final states with two oppositely charged leptons and large missing transverse energy as expected in H?WW??????? decays. The events are selected from the full Run II data sample of 9.7??fb(?1) of pp...

  2. Search for t[¯ over t] resonances in the lepton plus jets final state with ATLAS using 4.7??fb[superscript -1] of pp collisions at ?s=7??TeV

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for new particles that decay into top quark pairs (tt? ) is performed with the ATLAS experiment at the LHC using an integrated luminosity of 4.7??fb[superscript -1] of proton–proton (pp) collision data collected ...

  3. A boost for the EW SUSY hunt: monojet-like search for compressed sleptons at LHC14 with 100 fb^-1

    E-Print Network [OSTI]

    Alan Barr; James Scoville

    2015-01-27T23:59:59.000Z

    Current Large Hadron Collider (LHC) analyses are blind to compressed supersymmetry (SUSY) models with sleptons near the lightest super partner (LSP) in mass: $m_{\\tilde{l}} - m_{\\tilde{\\chi}_1^0} \\equiv \\Delta m \\lesssim 60$ GeV. We present a search sensitive to the very compressed range $3~\\text{GeV} 100$ GeV). The sleptons recoil against the jet boosting them and their decay products, making the leptons detectable and providing substantial missing transverse momentum. We use the kinematic variable $m_{\\rm T 2}$ along with a different-flavor control region to reduce the large standard model backgrounds and control systematic uncertainty. We find the analysis should allow LHC14 with $100~\\text{fb}^{-1}$ to search for degenerate left-handed selectrons and smuons in the compressed region up to $m_{\\tilde{l}_L} \\lesssim 150$ GeV. In addition, it should be sensitive to $m_{\\tilde{l}_L} \\lesssim 110$ GeV for the very challenging case of auto-concealed SUSY, in which left-handed sleptons decay to the Kaluza-Klein tower of a modulino LSP which lives in $d=6$ extra dimensions. In both the compressed spectrum and auto-concealed SUSY scenarios this analysis will need more data to improve on LEP2 limits for right-handed sleptons due to their smaller cross sections.

  4. Search for tt¯ resonances in the lepton plus jets final state with ATLAS using 4.7 fb?¹ of pp collisions at ?s=7 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aad, G.; Abajyan, T.; Abbott, B.; Abdallah, J.; Abdel Khalek, S.; Abdelalim, A. A.; Abdinov, O.; Aben, R.; Abi, B.; Abolins, M.; AbouZeid, O. S.; Abramowicz, H.; Abreu, H.; Abulaiti, Y.; Acharya, B. S.; Adamczyk, L.; Adams, D. L.; Addy, T. N.; Adelman, J.; Adomeit, S.; Adragna, P.; Adye, T.; Aefsky, S.; Aguilar-Saavedra, J. A.; Agustoni, M.; Ahlen, S. P.; Ahles, F.; Ahmad, A.; Ahsan, M.; Aielli, G.; Åkesson, T. P. A.; Akimoto, G.; Akimov, A. V.; Alam, M. A.; Albert, J.; Albrand, S.; Aleksa, M.; Aleksandrov, I. N.; Alessandria, F.; Alexa, C.; Alexander, G.; Alexandre, G.; Alexopoulos, T.; Alhroob, M.; Aliev, M.; Alimonti, G.; Alison, J.; Allbrooke, B. M. M.; Allison, L. J.; Allport, P. P.; Allwood-Spiers, S. E.; Almond, J.; Aloisio, A.; Alon, R.; Alonso, A.; Alonso, F.; Altheimer, A.; Alvarez Gonzalez, B.; Alviggi, M. G.; Amako, K.; Amelung, C.; Ammosov, V. V.; Amor Dos Santos, S. P.; Amorim, A.; Amoroso, S.; Amram, N.; Anastopoulos, C.; Ancu, L. S.; Andari, N.; Andeen, T.; Anders, C. F.; Anders, G.; Anderson, K. J.; Andreazza, A.; Andrei, V.; Anduaga, X. S.; Angelidakis, S.; Anger, P.; Angerami, A.; Anghinolfi, F.; Anisenkov, A.; Anjos, N.; Annovi, A.; Antonaki, A.; Antonelli, M.; Antonov, A.; Antos, J.; Anulli, F.; Aoki, M.; Aperio Bella, L.; Apolle, R.; Arabidze, G.; Aracena, I.; Arai, Y.; Arce, A. T. H.; Arfaoui, S.; Arguin, J-F.; Argyropoulos, S.; Arik, E.; Arik, M.; Armbruster, A. J.; Arnaez, O.; Arnal, V.; Artamonov, A.; Artoni, G.; Arutinov, D.; Asai, S.; Ask, S.; Åsman, B.; Asquith, L.; Assamagan, K.; Astalos, R.; Astbury, A.; Atkinson, M.; Auerbach, B.; Auge, E.; Augsten, K.; Aurousseau, M.; Avolio, G.; Axen, D.; Azuelos, G.; Azuma, Y.; Baak, M. A.; Baccaglioni, G.; Bacci, C.; Bach, A. M.; Bachacou, H.; Bachas, K.; Backes, M.; Backhaus, M.; Backus Mayes, J.; Badescu, E.; Bagnaia, P.; Bai, Y.; Bailey, D. C.; Bain, T.; Baines, J. T.; Baker, O. K.; Baker, S.; Balek, P.; Balli, F.; Banas, E.; Banerjee, P.; Banerjee, Sw.; Banfi, D.; Bangert, A.; Bansal, V.; Bansil, H. S.; Barak, L.; Baranov, S. P.; Barber, T.; Barberio, E. L.; Barberis, D.; Barbero, M.; Bardin, D. Y.; Barillari, T.; Barisonzi, M.; Barklow, T.; Barlow, N.; Barnett, B. M.; Barnett, R. M.; Baroncelli, A.; Barone, G.; Barr, A. J.; Barreiro, F.; Barreiro Guimarães da Costa, J.; Bartoldus, R.; Barton, A. E.; Bartsch, V.; Basye, A.; Bates, R. L.; Batkova, L.; Batley, J. R.; Battaglia, A.; Battistin, M.; Bauer, F.; Bawa, H. S.; Beale, S.; Beau, T.; Beauchemin, P. H.; Beccherle, R.; Bechtle, P.; Beck, H. P.; Becker, K.; Becker, S.; Beckingham, M.; Becks, K. H.; Beddall, A. J.; Beddall, A.; Bedikian, S.; Bednyakov, V. A.; Bee, C. P.; Beemster, L. J.; Beermann, T. A.; Begel, M.; Behar Harpaz, S.; Belanger-Champagne, C.; Bell, P. J.; Bell, W. H.; Bella, G.; Bellagamba, L.; Bellomo, M.; Belloni, A.; Beloborodova, O.; Belotskiy, K.; Beltramello, O.; Benary, O.; Benchekroun, D.; Bendtz, K.; Benekos, N.; Benhammou, Y.; Benhar Noccioli, E.; Benitez Garcia, J. A.; Benjamin, D. P.; Benoit, M.; Bensinger, J. R.; Benslama, K.; Bentvelsen, S.; Berge, D.; Bergeaas Kuutmann, E.; Berger, N.; Berghaus, F.; Berglund, E.; Beringer, J.; Bernat, P.; Bernhard, R.; Bernius, C.; Bernlochner, F. U.; Berry, T.; Bertella, C.; Bertin, A.; Bertolucci, F.; Besana, M. I.; Besjes, G. J.; Besson, N.; Bethke, S.; Bhimji, W.; Bianchi, R. M.; Bianchini, L.; Bianco, M.; Biebel, O.; Bieniek, S. P.; Bierwagen, K.; Biesiada, J.; Biglietti, M.; Bilokon, H.; Bindi, M.; Binet, S.; Bingul, A.; Bini, C.; Biscarat, C.; Bittner, B.; Black, C. W.; Black, J. E.; Black, K. M.; Blair, R. E.; Blanchard, J.-B.; Blazek, T.; Bloch, I.; Blocker, C.; Blocki, J.; Blum, W.; Blumenschein, U.; Bobbink, G. J.; Bobrovnikov, V. S.; Bocchetta, S. S.; Bocci, A.; Boddy, C. R.; Boehler, M.; Boek, J.; Boek, T. T.; Boelaert, N.; Bogaerts, J. A.; Bogdanchikov, A.; Bogouch, A.; Bohm, C.; Bohm, J.; Boisvert, V.; Bold, T.; Boldea, V.; Bolnet, N. M.; Bomben, M.; Bona, M.; Boonekamp, M.; Bordoni, S.; Borer, C.; Borisov, A.; Borissov, G.; Borjanovic, I.; Borri, M.; Borroni, S.; Bortfeldt, J.; Bortolotto, V.; Bos, K.; Boscherini, D.; Bosman, M.; Boterenbrood, H.; Bouchami, J.; Boudreau, J.; Bouhova-Thacker, E. V.; Boumediene, D.; Bourdarios, C.; Bousson, N.; Boutouil, S.; Boveia, A.; Boyd, J.; Boyko, I. R.; Bozovic-Jelisavcic, I.; Bracinik, J.; Branchini, P.; Brandt, A.; Brandt, G.; Brandt, O.; Bratzler, U.; Brau, B.; Brau, J. E.; Braun, H. M.; Brazzale, S. F.; Brelier, B.; Bremer, J.; Brendlinger, K.; Brenner, R.; Bressler, S.; Bristow, T. M.; Britton, D.; Brochu, F. M.; Brock, I.; Brock, R.; Broggi, F.; Bromberg, C.; Bronner, J.; Brooijmans, G.; Brooks, T.; Brooks, W. K.; Brown, G.; Bruckman de Renstrom, P. A.; Bruncko, D.; Bruneliere, R.; Brunet, S.; Bruni, A.; Bruni, G.; Bruschi, M.; Bryngemark, L.

    2013-07-01T23:59:59.000Z

    A search for new particles that decay into top quark pairs (tt¯) is performed with the ATLAS experiment at the LHC using an integrated luminosity of 4.7 fb?¹ of proton–proton (pp ) collision data collected at a center-of-mass energy ?s =7 TeV . In the tt¯ ?WbWb decay, the lepton plus jets final state is used, where one W boson decays leptonically and the other hadronically. The tt¯ system is reconstructed using both small-radius and large-radius jets, the latter being supplemented by a jet substructure analysis. A search for local excesses in the number of data events compared to the Standard Model expectation in the tt¯ invariant mass spectrum is performed. No evidence for a tt¯ resonance is found and 95% credibility-level limits on the production rate are determined for massive states predicted in two benchmark models. The upper limits on the cross section times branching ratio of a narrow Z' resonance range from 5.1 pb for a boson mass of 0.5 TeV to 0.03 pb for a mass of 3 TeV. A narrow leptophobic topcolor Z' resonance with a mass below 1.74 TeV is excluded. Limits are also derived for a broad color-octet resonance with ?/m=15.3% . A Kaluza–Klein excitation of the gluon in a Randall–Sundrum model is excluded for masses below 2.07 TeV.

  5. Search for a Standard Model-like Higgs boson decaying into WW to l nu qqbar in exclusive jet bins in pp collisions at sqrt s = 8 TeV

    E-Print Network [OSTI]

    CMS Collaboration

    2015-01-01T23:59:59.000Z

    A search for a Standard Model Higgs boson decaying into the WW final state is performed with an integrated luminosity of up to 19.3~${\\rm fb}^{-1}$ of pp collisions at $\\sqrt{s}$~=~8~TeV in the high mass region $600 < m_{\\rm H} < 1000$~GeV.

  6. y12 disc 1954 FB

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:Energy: Grid Integration Redefining What'sis Taking Over OurThe Iron4 Self-Scrubbing:,, ,Development1U CO1) 1 Winter FuelsYOURxinyufuUpdraft

  7. Search for the standard model Higgs boson produced in association with a W± boson with 7.5 fb?¹ integrated luminosity at CDF

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aaltonen, T.; Álvarez González, B.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J. A.; Arisawa, T.; et al

    2012-08-01T23:59:59.000Z

    We present a search for the standard model Higgs boson produced in association with a W± boson. This search uses data corresponding to an integrated luminosity of 7.5 fb?¹ collected by the CDF detector at the Tevatron. We select WH?l?bb¯ 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 withmore »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 bb¯ pairs, ?(pp¯?W±H)×B(H?bb¯), relative to the rate predicted by the standard model. For the Higgs boson mass range of 100 to 150 GeV/c² we set observed (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For 115 GeV/c² 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/c² the upper limits are 2.65 (2.60) and 4.36 (3.69), respectively.« less

  8. Search for the standard model Higgs boson produced in association with a W± boson with 7.5 fb?¹ integrated luminosity at CDF

    SciTech Connect (OSTI)

    Aaltonen, T.; Álvarez González, B.; Amerio, S.; 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.; Bisello, D.; Bizjak, I.; 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.; Buzatu, A.; Calamba, A.; Calancha, C.; Camarda, S.; Campanelli, M.; Campbell, M.; Canelli, F.; Carls, B.; Carlsmith, D.; Carosi, R.; Carrillo, S.; Carron, 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.; Chlebana, F.; Cho, K.; Chokheli, D.; Chung, W. H.; Chung, Y. S.; Ciocci, M. A.; Clark, A.; Clarke, C.; Compostella, G.; Convery, M. E.; Conway, J.; Corbo, M.; Cordelli, M.; Cox, C. A.; Cox, D. J.; Crescioli, F.; Cuevas, J.; Culbertson, R.; Dagenhart, D.; d’Ascenzo, N.; Datta, M.; de Barbaro, P.; Dell’Orso, M.; Demortier, L.; Deninno, M.; Devoto, F.; d’Errico, M.; Di Canto, A.; Di Ruzza, B.; Dittmann, J. R.; D’Onofrio, M.; Donati, S.; Dong, P.; Dorigo, M.; Dorigo, T.; Ebina, K.; Elagin, A.; Eppig, A.; Erbacher, R.; Errede, S.; Ershaidat, N.; Eusebi, R.; Farrington, S.; Feindt, M.; Fernandez, J. P.; Field, R.; Flanagan, G.; Forrest, R.; Frank, M. J.; Franklin, M.; Freeman, J. C.; Funakoshi, Y.; Furic, I.; Gallinaro, M.; Garcia, J. E.; Garfinkel, A. F.; Garosi, P.; Gerberich, H.; Gerchtein, E.; Giagu, S.; Giakoumopoulou, V.; Giannetti, P.; Gibson, K.; Ginsburg, C. M.; Giokaris, N.; Giromini, P.; Giurgiu, G.; Glagolev, V.; Glenzinski, D.; Gold, M.; Goldin, D.; Goldschmidt, N.; Golossanov, A.; Gomez, G.; Gomez-Ceballos, G.; Goncharov, M.; González, O.; Gorelov, I.; Goshaw, A. T.; Goulianos, K.; Grinstein, S.; Grosso-Pilcher, C.; Group, R. C.; Guimaraes da Costa, J.; Hahn, S. R.; Halkiadakis, E.; Hamaguchi, A.; Han, J. Y.; Happacher, F.; Hara, K.; Hare, D.; Hare, M.; Harr, R. F.; Hatakeyama, K.; Hays, C.; Heck, M.; Heinrich, J.; Herndon, M.; Hewamanage, S.; Hocker, A.; Hopkins, W.; Horn, D.; Hou, S.; Hughes, R. E.; Hurwitz, M.; Husemann, U.; Hussain, N.; 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.; Kamon, T.; Karchin, P. E.; Kasmi, A.; Kato, Y.; Ketchum, W.; Keung, J.; Khotilovich, V.; 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.; Klimenko, S.; Knoepfel, K.; Kondo, K.; Kong, D. J.; Konigsberg, J.; Kotwal, A. V.; Kreps, M.; Kroll, J.; Krop, D.; Kruse, M.; Krutelyov, V.; Kuhr, T.; Kurata, M.; Kwang, S.; Laasanen, A. T.; Lami, S.; Lammel, S.; Lancaster, M.; Lander, R. L.; Lannon, K.; Lath, A.; Latino, G.; LeCompte, T.; Lee, E.; Lee, H. S.; Lee, J. S.; Lee, S. W.; Leo, S.; Leone, S.; Lewis, J. D.; Limosani, A.; Lin, C.-J.; Lindgren, M.; Lipeles, E.; Lister, A.; Litvintsev, D. O.; Liu, C.; Liu, H.; Liu, Q.; Liu, T.; Lockwitz, S.; Loginov, A.; Lucchesi, D.; Lueck, J.; Lujan, P.; Lukens, P.; Lungu, G.; Lys, J.; Lysak, R.; Madrak, R.; Maeshima, K.; Maestro, P.; Malik, S.; Manca, G.; Manousakis-Katsikakis, A.; Margaroli, F.; Marino, C.; Martínez, M.; Mastrandrea, P.; Matera, K.; Mattson, M. E.; Mazzacane, A.; Mazzanti, P.; McFarland, K. S.; McIntyre, P.; McNulty, R.; Mehta, A.; Mehtala, P.; Mesropian, C.; Miao, T.; Mietlicki, D.; Mitra, A.; Miyake, H.; Moed, S.; Moggi, N.; Mondragon, M. N.; Moon, C. S.; Moore, R.; Morello, M. J.; Morlock, J.; Movilla Fernandez, P.; Mukherjee, A.; Muller, Th.; Murat, P.; Mussini, M.; Nachtman, J.; Nagai, Y.; Naganoma, J.; Nakano, I.; Napier, A.; Nett, J.; Neu, C.; Neubauer, M. S.; Nielsen, J.; Nodulman, L.; Noh, S. Y.; Norniella, O.; Oakes, L.; Oh, S. H.; Oh, Y. D.; Oksuzian, I.; Okusawa, T.; Orava, R.; Ortolan, L.; Pagan Griso, S.; Pagliarone, C.; Palencia, E.; Papadimitriou, V.; Paramonov, A. A.; Patrick, J.; Pauletta, G.; Paulini, M.; Paus, C.; Pellett, D. E.; Penzo, A.; 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.; Rahaman, A.; Ramakrishnan, V.; Ranjan, N.; Redondo, I.; Renton, P.; Rescigno, M.; Riddick, T.; Rimondi, F.; Ristori, L.; Robson, A.; Rodrigo, T.; Rodriguez, T.; Rogers, E.; Rolli, S.; Roser, R.; Ruffini, F.; Ruiz, A.; Russ, J.; Rusu, V.; Safonov, A.; Sakumoto, W. K.

    2012-08-01T23:59:59.000Z

    We present a search for the standard model Higgs boson produced in association with a W± boson. This search uses data corresponding to an integrated luminosity of 7.5 fb?¹ collected by the CDF detector at the Tevatron. We select WH?l?bb¯ 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 bb¯ pairs, ?(pp¯?W±H)×B(H?bb¯), relative to the rate predicted by the standard model. For the Higgs boson mass range of 100 to 150 GeV/c² we set observed (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For 115 GeV/c² 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/c² the upper limits are 2.65 (2.60) and 4.36 (3.69), respectively.

  9. Search for the standard model Higgs boson produced in association with a W± boson with 7.5 fb?¹ integrated luminosity at CDF

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aaltonen, T.; Álvarez González, B.; Amerio, S.; 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.; Bisello, D.; Bizjak, I.; 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.; Buzatu, A.; Calamba, A.; Calancha, C.; Camarda, S.; Campanelli, M.; Campbell, M.; Canelli, F.; Carls, B.; Carlsmith, D.; Carosi, R.; Carrillo, S.; Carron, 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.; Chlebana, F.; Cho, K.; Chokheli, D.; Chung, W. H.; Chung, Y. S.; Ciocci, M. A.; Clark, A.; Clarke, C.; Compostella, G.; Convery, M. E.; Conway, J.; Corbo, M.; Cordelli, M.; Cox, C. A.; Cox, D. J.; Crescioli, F.; Cuevas, J.; Culbertson, R.; Dagenhart, D.; d’Ascenzo, N.; Datta, M.; de Barbaro, P.; Dell’Orso, M.; Demortier, L.; Deninno, M.; Devoto, F.; d’Errico, M.; Di Canto, A.; Di Ruzza, B.; Dittmann, J. R.; D’Onofrio, M.; Donati, S.; Dong, P.; Dorigo, M.; Dorigo, T.; Ebina, K.; Elagin, A.; Eppig, A.; Erbacher, R.; Errede, S.; Ershaidat, N.; Eusebi, R.; Farrington, S.; Feindt, M.; Fernandez, J. P.; Field, R.; Flanagan, G.; Forrest, R.; Frank, M. J.; Franklin, M.; Freeman, J. C.; Funakoshi, Y.; Furic, I.; Gallinaro, M.; Garcia, J. E.; Garfinkel, A. F.; Garosi, P.; Gerberich, H.; Gerchtein, E.; Giagu, S.; Giakoumopoulou, V.; Giannetti, P.; Gibson, K.; Ginsburg, C. M.; Giokaris, N.; Giromini, P.; Giurgiu, G.; Glagolev, V.; Glenzinski, D.; Gold, M.; Goldin, D.; Goldschmidt, N.; Golossanov, A.; Gomez, G.; Gomez-Ceballos, G.; Goncharov, M.; González, O.; Gorelov, I.; Goshaw, A. T.; Goulianos, K.; Grinstein, S.; Grosso-Pilcher, C.; Group, R. C.; Guimaraes da Costa, J.; Hahn, S. R.; Halkiadakis, E.; Hamaguchi, A.; Han, J. Y.; Happacher, F.; Hara, K.; Hare, D.; Hare, M.; Harr, R. F.; Hatakeyama, K.; Hays, C.; Heck, M.; Heinrich, J.; Herndon, M.; Hewamanage, S.; Hocker, A.; Hopkins, W.; Horn, D.; Hou, S.; Hughes, R. E.; Hurwitz, M.; Husemann, U.; Hussain, N.; 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.; Kamon, T.; Karchin, P. E.; Kasmi, A.; Kato, Y.; Ketchum, W.; Keung, J.; Khotilovich, V.; 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.; Klimenko, S.; Knoepfel, K.; Kondo, K.; Kong, D. J.; Konigsberg, J.; Kotwal, A. V.; Kreps, M.; Kroll, J.; Krop, D.; Kruse, M.; Krutelyov, V.; Kuhr, T.; Kurata, M.; Kwang, S.; Laasanen, A. T.; Lami, S.; Lammel, S.; Lancaster, M.; Lander, R. L.; Lannon, K.; Lath, A.; Latino, G.; LeCompte, T.; Lee, E.; Lee, H. S.; Lee, J. S.; Lee, S. W.; Leo, S.; Leone, S.; Lewis, J. D.; Limosani, A.; Lin, C.-J.; Lindgren, M.; Lipeles, E.; Lister, A.; Litvintsev, D. O.; Liu, C.; Liu, H.; Liu, Q.; Liu, T.; Lockwitz, S.; Loginov, A.; Lucchesi, D.; Lueck, J.; Lujan, P.; Lukens, P.; Lungu, G.; Lys, J.; Lysak, R.; Madrak, R.; Maeshima, K.; Maestro, P.; Malik, S.; Manca, G.; Manousakis-Katsikakis, A.; Margaroli, F.; Marino, C.; Martínez, M.; Mastrandrea, P.; Matera, K.; Mattson, M. E.; Mazzacane, A.; Mazzanti, P.; McFarland, K. S.; McIntyre, P.; McNulty, R.; Mehta, A.; Mehtala, P.; Mesropian, C.; Miao, T.; Mietlicki, D.; Mitra, A.; Miyake, H.; Moed, S.; Moggi, N.; Mondragon, M. N.; Moon, C. S.; Moore, R.; Morello, M. J.; Morlock, J.; Movilla Fernandez, P.; Mukherjee, A.; Muller, Th.; Murat, P.; Mussini, M.; Nachtman, J.; Nagai, Y.; Naganoma, J.; Nakano, I.; Napier, A.; Nett, J.; Neu, C.; Neubauer, M. S.; Nielsen, J.; Nodulman, L.; Noh, S. Y.; Norniella, O.; Oakes, L.; Oh, S. H.; Oh, Y. D.; Oksuzian, I.; Okusawa, T.; Orava, R.; Ortolan, L.; Pagan Griso, S.; Pagliarone, C.; Palencia, E.; Papadimitriou, V.; Paramonov, A. A.; Patrick, J.; Pauletta, G.; Paulini, M.; Paus, C.; Pellett, D. E.; Penzo, A.; 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.; Rahaman, A.; Ramakrishnan, V.; Ranjan, N.; Redondo, I.; Renton, P.; Rescigno, M.; Riddick, T.; Rimondi, F.; Ristori, L.; Robson, A.; Rodrigo, T.; Rodriguez, T.; Rogers, E.; Rolli, S.; Roser, R.; Ruffini, F.; Ruiz, A.; Russ, J.; Rusu, V.; Safonov, A.; Sakumoto, W. K.

    2012-08-01T23:59:59.000Z

    We present a search for the standard model Higgs boson produced in association with a W± boson. This search uses data corresponding to an integrated luminosity of 7.5 fb?¹ collected by the CDF detector at the Tevatron. We select WH?l?bb¯ 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 bb¯ pairs, ?(pp¯?W±H)×B(H?bb¯), relative to the rate predicted by the standard model. For the Higgs boson mass range of 100 to 150 GeV/c² we set observed (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For 115 GeV/c² 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/c² the upper limits are 2.65 (2.60) and 4.36 (3.69), respectively.

  10. Measurement of the Forward-Backward Charge Asymmetry($A_{FB}$) using $p\\bar{p}\\rightarrow Z/\\gamma*\\rightarrow e^+e^-$ events in $\\sqrt{S} = 1.96$ TeV

    SciTech Connect (OSTI)

    Yin, Hang; /Sci. Tech. U., Beijing

    2010-06-01T23:59:59.000Z

    This dissertation describes a measurement of the forward-backward asymmetry(A{sub FB}) in p{bar p} {yields} Z/{gamma}* {yields} ee events using 5.0 fb{sup -1} data collected by the D0 detector at the Fermilab Tevatron. The AFB is measured as a function of the invariant mass of the electron-positron pair. Along with obtaining normalized differential cross section 1/{sigma} x d{sigma}/dM and Z to light quark couplings, we measured the Standard Model(SM) fundamental parameter, the effective weak mixing angle sin{sup 2} {theta}{sub eff}{sup lept}, with an unprecedented precise in light quark sector, namely the single D0 measurement has surpassed the LEP combination of four experiment results of inclusive hadronic charge asymmetry.

  11. Search for Randall-Sundrum gravitons in the dielectron and diphoton final states with 5.4fb$^{-1}$ of data from $p\\bar{p}$ collisions at $\\sqrt{s}=1.96$ TeV

    SciTech Connect (OSTI)

    Abazov, Victor Mukhamedovich; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma U.; Abolins, Maris A.; /Michigan State U.; Acharya, Bannanje Sripath; /Tata Inst.; Adams, Mark Raymond; /Illinois U., Chicago; Adams, Todd; /Florida State U.; Aguilo, Ernest; /York U., Canada; Alexeev, Guennadi D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Augustana Coll., Sioux Falls; Alverson, George O.; /Northeastern U. /Rio de Janeiro, CBPF

    2010-04-01T23:59:59.000Z

    Using 5.4 fb{sup -1} of integrated luminosity from p{bar p} collisions at {radical}s = 1.96 TeV collected by the D0 detector at the Fermilab Tevatron Collider, we search for decays of the lightest Kaluza-Klein mode of the graviton in the Randall-Sundrum model to ee and {gamma}{gamma}. We set 95% C.L. lower limits on the mass of the lightest graviton between 560 GeV and 1050 GeV for values of the coupling k/{bar M}{sub Pl} between 0.01 and 0.1.

  12. Search for sneutrino production in $e\\mu$ final states in 5.3 fb$^{-1}$ of $p\\bar{p}$ collisions at $\\sqrt(s) =1.96$ TeV

    SciTech Connect (OSTI)

    Abazov, Victor Mukhamedovich; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma U.; Abolins, Maris A.; /Michigan State U.; Acharya, Bannanje Sripath; /Tata Inst.; Adams, Mark Raymond; /Illinois U., Chicago; Adams, Todd; /Florida State U.; Alexeev, Guennadi D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Augustana Coll., Sioux Falls; Alverson, George O.; /Northeastern U.; Alves, Gilvan Augusto; /Rio de Janeiro, CBPF /Nijmegen U.

    2010-07-01T23:59:59.000Z

    We report the results of a search for R parity violating (RPV) interactions leading to the production of supersymmetric sneutrinos decaying into e{mu} final states using 5.3 fb{sup -1} of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron Collider. Having observed no evidence for production of e{mu} resonances, we set direct bounds on the RPV couplings {lambda}{prime}{sub 311} and {lambda}{sub 312} as a function of sneutrino mass.

  13. Combined search for the Standard Model Higgs boson using up to 4.9 fb(-1) of pp collision data at root s=7 TeV with the ATLAS detector at the LHC

    SciTech Connect (OSTI)

    Aad G.; Abbott, B; Abdallah, J; Khalek, SA; Abdelalim, AA; Abdesselam, A; Abdinov, O; Abi, B; Abolins, M; AbouZeid, OS; Abramowicz, H; Abreu, H; Acerbia, E; Acharya, BS; Adamczyk, L; Adams, DL; Addy, TN; Adelman, J; Aderholz, M; Adomeit, S; Adragna, P; Ad

    2012-03-29T23:59:59.000Z

    A combined search for the Standard Model Higgs boson with the ATLAS experiment at the LHC using datasets corresponding to integrated luminosities from 1.04 fb{sup -1} to 4.9 fb{sup -1} of pp collisions collected at {radical}s = 7 TeV is presented. The Higgs boson mass ranges 112.9-115.5 GeV, 131-238 GeV and 251-466 GeV are excluded at the 95% confidence level (CL), while the range 124-519 GeV is expected to be excluded in the absence of a signal. An excess of events is observed around m{sub H} {approx} 126 GeV with a local significance of 3.5 standard deviations ({sigma}). The local significances of H {yields} {gamma}{gamma}, H {yields} ZZ{sup (*)} {yields} {ell}{sup +}{ell}{sup -}{ell}{prime}{sup +}{ell}{prime}{sup -} and H {yields} WW{sup (*)} {yields} {ell}{sup +}{nu}{ell}{prime}{sup -}{bar {nu}}, the three most sensitive channels in this mass range, are 2.8{sigma}, 2.1{sigma} and 1.4{sigma}, respectively. The global probability for the background to produce such a fluctuation anywhere in the explored Higgs boson mass range 110-600 GeV is estimated to be {approx}1.4% or, equivalently, 2.2{sigma}.

  14. Adaptation of the modified Bouc–Wen model to compensate for hysteresis in respiratory motion for the list-mode binning of cardiac SPECT and PET acquisitions: Testing using MRI

    SciTech Connect (OSTI)

    Dasari, Paul K. R.; Shazeeb, Mohammed Salman [Department of Radiology, Division of Nuclear Medicine, University of Massachusetts Medical School, Worcester, Massachusetts 01655 and Department of Biomedical Engineering, Worcester Polytechnic Institute, Worcester, Massachusetts 01609 (United States); Könik, Arda; Lindsay, Clifford; Mukherjee, Joyeeta M.; Johnson, Karen L.; King, Michael A., E-mail: Michael.King@umassmed.edu [Department of Radiology, Division of Nuclear Medicine, University of Massachusetts Medical School, Worcester, Massachusetts 01655 (United States)

    2014-11-01T23:59:59.000Z

    Purpose: Binning list-mode acquisitions as a function of a surrogate signal related to respiration has been employed to reduce the impact of respiratory motion on image quality in cardiac emission tomography (SPECT and PET). Inherent in amplitude binning is the assumption that there is a monotonic relationship between the amplitude of the surrogate signal and respiratory motion of the heart. This assumption is not valid in the presence of hysteresis when heart motion exhibits a different relationship with the surrogate during inspiration and expiration. The purpose of this study was to investigate the novel approach of using the Bouc–Wen (BW) model to provide a signal accounting for hysteresis when binning list-mode data with the goal of thereby improving motion correction. The study is based on the authors’ previous observations that hysteresis between chest and abdomen markers was indicative of hysteresis between abdomen markers and the internal motion of the heart. Methods: In 19 healthy volunteers, they determined the internal motion of the heart and diaphragm in the superior–inferior direction during free breathing using MRI navigators. A visual tracking system (VTS) synchronized with MRI acquisition tracked the anterior–posterior motions of external markers placed on the chest and abdomen. These data were employed to develop and test the Bouc–Wen model by inputting the VTS derived chest and abdomen motions into it and using the resulting output signals as surrogates for cardiac motion. The data of the volunteers were divided into training and testing sets. The training set was used to obtain initial values for the model parameters for all of the volunteers in the set, and for set members based on whether they were or were not classified as exhibiting hysteresis using a metric derived from the markers. These initial parameters were then employed with the testing set to estimate output signals. Pearson’s linear correlation coefficient between the abdomen, chest, average of chest and abdomen markers, and Bouc–Wen derived signals versus the true internal motion of the heart from MRI was used to judge the signals match to the heart motion. Results: The results show that the Bouc–Wen model generated signals demonstrated strong correlation with the heart motion. This correlation was slightly larger on average than that of the external surrogate signals derived from the abdomen marker, and average of the abdomen and chest markers, but was not statistically significantly different from them. Conclusions: The results suggest that the proposed model has the potential to be a unified framework for modeling hysteresis in respiratory motion in cardiac perfusion studies and beyond.

  15. Search for diphoton events with large missing transverse energy in 6.3 fb$^{-1}$ of $\\mathbf{p\\bar{p}}$ collisions at $\\mathbf{\\sqrt{s}=1.96}$~TeV

    SciTech Connect (OSTI)

    Abazov, Victor Mukhamedovich; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma U.; Abolins, Maris A.; /Michigan State U.; Acharya, Bannanje Sripath; /Tata Inst.; Adams, Mark Raymond; /Illinois U., Chicago; Adams, Todd; /Florida State U.; Alexeev, Guennadi D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Augustana Coll., Sioux Falls; Alverson, George O.; /Northeastern U.; Alves, Gilvan Augusto; /Rio de Janeiro, CBPF /Nijmegen U.

    2010-08-01T23:59:59.000Z

    We report a search for diphoton events with large missing transverse energy produced in p{bar p} collisions at {radical}s = 1.96 TeV. The data were collected with the D0 detector at the Fermilab Tevatron Collider, and correspond to 6.3 fb{sup -1} of integrated luminosity. The observed missing transverse energy distribution is well described by the standard model prediction, and 95% C.L. limits are derived on two realizations of theories beyond the standard model. In a gauge mediated supersymmetry breaking scenario, the breaking scale {Lambda} is excluded for {Lambda} < 124 TeV. In a universal extra dimension model including gravitational decays, the compactification radius R{sub c} is excluded for R{sub c}{sup -1} < 477 GeV.

  16. Search for $ZH \\rightarrow \\ell^+\\ell^-b\\bar{b}$ production in $4.2$~fb$^{-1}$ of $p\\bar{p}$ collisions at $\\sqrt{s}=1.96~\\TeV$

    SciTech Connect (OSTI)

    Abazov, Victor Mukhamedovich; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma U.; Abolins, Maris A.; /Michigan State U.; Acharya, Bannanje Sripath; /Tata Inst.; Adams, Mark Raymond; /Illinois U., Chicago; Adams, Todd; /Florida State U.; Alexeev, Guennadi D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Augustana Coll., Sioux Falls; Alverson, George O.; /Northeastern U.; Alves, Gilvan Augusto; /Rio de Janeiro, CBPF /Nijmegen U.

    2010-08-01T23:59:59.000Z

    We present a search for the standard model Higgs boson produced in association with a Z boson in 4.2 fb{sup -1} of p{bar p} collisions, collected with the D0 detector at the Fermilab Tevatron at {radical}s = 1.96 TeV. Selected events contain one reconstructed Z {yields} {ell}{sup +}{ell}{sup -} candidate and at least two jets, including at least one b-tagged jet. In the absence of an excess over the background expected from other standard model processes, limits on the ZH cross section multiplied by the branching ratios are set. The limit at M{sub H} = 115 GeV is a factor of 5.9 larger than the standard model prediction.

  17. Search for a heavy neutral gauge boson in the dielectron channel with 5.4~fb$^{-1}$ of $\\mathbf{p\\bar{p}}$ collisions at $\\mathbf{\\sqrt{s} = 1.96}$~TeV

    SciTech Connect (OSTI)

    Abazov, Victor Mukhamedovich; Abazov, V.; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma U.; Abolins, Maris A.; /Michigan State U.; Acharya, Bannanje Sripath; /Tata Inst.; Adams, Mark Raymond; /Illinois U., Chicago; Adams, Todd; /Florida State U.; Alexeev, Guennadi D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Augustana Coll., Sioux Falls; Alverson, George O.; /Northeastern U. /Rio de Janeiro, CBPF /Nijmegen U.

    2010-08-01T23:59:59.000Z

    We report the results of a search for a heavy neutral gauge boson Z' decaying into the dielectron final state using data corresponding to an integrated luminosity of 5.4 fb{sup -1} collected by the D0 experiment at the Fermilab Tevatron Collider. No significant excess above the standard model prediction is observed in the dielectron invariant-mass spectrum. We set 95% C.L. upper limits on {sigma}(p{bar p} {yields} Z') x BR(Z' {yields} ee) depending on the dielectron invariant mass. These cross section limits are used to determine lower mass limits for Z' bosons in a variety of models with standard model couplings and variable strength.

  18. A search for resonant production of tt? pairs in 4.8 fb-1 of integrated luminosity of pp? collisions at ?s=1.96 TeV

    SciTech Connect (OSTI)

    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.; Annovi, A [Frascati; Antos, J [Comenius U.; Apollinari, G [Fermilab; Appel, J A [Fermilab; Apresyan, A [Purdue U.; Arisawa, T [Waseda U.; Dubna, JINR

    2011-10-27T23:59:59.000Z

    We search for resonant production of tt? pairs in 4.8 fb-1 integrated luminosity of pp? collision data at ?s = 1.96 TeV in the lepton+jets decay channel, where one top quark decays leptonically and the other hadronically. A matrix element reconstruction technique is used; for each event a probability density function (pdf) of the tt? candidate invariant mass is sampled. These pdfs are used to construct a likelihood function, whereby the cross section for resonant tt? production is estimated, given a hypothetical resonance mass and width. The data indicate no evidence of resonant production of tt? pairs. A benchmark model of leptophobic Z' ? tt? is excluded with mZ' < 900 GeV at 95% confidence level.

  19. Search for the Standard Model Higgs Boson in ZH?l?l?bb? Production with the D0 Detector in 9.7 fb?¹ of pp? Collisions at ?s=1.96 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Askew, A.; Atkins, S.; Augsten, K.; Avila, C.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Bean, A.; Begalli, M.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bhat, P. C.; Bhatia, S.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Buszello, C. P.; Camacho-Pérez, E.; Casey, B. C. K.; Castilla-Valdez, H.; Caughron, S.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Croc, A.; Cutts, D.; Das, A.; Davies, G.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dubey, A.; Dudko, L. V.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Evdokimov, V. N.; Facini, G.; Feng, L.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Garcia-Bellido, A.; García-González, J. A.; García-Guerra, G. A.; Gavrilov, V.; Gay, P.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A.; Grannis, P. D.; Greder, S.; Greenlee, H.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Hagopian, S.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hogan, J.; Hohlfeld, M.; Howley, I.; Hubacek, Z.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jayasinghe, A.; Jeong, M. S.; Jesik, R.; Jiang, P.; Johns, K.; Johnson, E.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A. W.; Juste, A.; Kaadze, K.; Kajfasz, E.; Karmanov, D.; Kasper, P. A.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kiselevich, I.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kulikov, S.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Lammers, S.; Landsberg, G.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lei, X.; Lellouch, J.; Li, D.; Li, H.; Li, L.; Li, Q. Z.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, H.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Lubatti, H. J.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Maravin, Y.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N. K.; Mulhearn, M.; Nagy, E.; Naimuddin, M.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Nguyen, H. T.; Nunnemann, T.; Orduna, J.; Osman, N.; Osta, J.; Padilla, M.; Pal, A.; Parashar, N.; Parihar, V.; Park, S. K.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Pleier, M.-A.; Podesta-Lerma, P. L. M.; Podstavkov, V. M.; Popov, A. V.; Prewitt, M.; Price, D.; Prokopenko, N.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M. S.; Ranjan, K.; Ratoff, P. N.; Razumov, I.; Renkel, P.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Sajot, G.; Salcido, P.; Sánchez-Hernández, A.; Sanders, M. P.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schlobohm, S.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shaw, S.; Shchukin, A. A.; Shivpuri, R. K.; Simak, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Smith, K. J.; Snow, G. R.; Snow, J.; Snyder, S.; Söldner-Rembold, S.; Sonnenschein, L.; Soustruznik, K.; Stark, J.; Stoyanova, D. A.; Strauss, M.; Suter, L.; Svoisky, P.; Takahashi, M.; Titov, M.; Tokmenin, V. V.; Tsai, Y.-T.; Tschann-Grimm, K.; Tsybychev, D.; Tuchming, B.; Tully, C.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Van Kooten, R.; van Leeuwen, W. M.; Varelas, N.; Varnes, E. W.

    2012-09-01T23:59:59.000Z

    We present a search for the standard model (SM) Higgs boson produced in association with a Z boson in 9.7 fb?¹ of pp? collisions collected with the D0 detector at the Fermilab Tevatron Collider at ?s=1.96 TeV. Selected events contain one reconstructed Z?e?e? or Z????? candidate and at least two jets, including at least one jet identified as likely to contain a b quark. To validate the search procedure, we also measure the cross section for ZZ production in the same final state. It is found to be consistent with its SM prediction. We set upper limits on the ZH production cross section times branching ratio for H?bb? at the 95% C.L. for Higgs boson masses 90?MH?150 GeV. The observed (expected) limit for MH=125 GeV is 7.1 (5.1) times the SM cross section.

  20. Search for the Standard Model Higgs Boson in ZH?l?l?bb? Production with the D0 Detector in 9.7 fb?¹ of pp? Collisions at ?s=1.96 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Askew, A.; et al

    2012-09-01T23:59:59.000Z

    We present a search for the standard model (SM) Higgs boson produced in association with a Z boson in 9.7 fb?¹ of pp? collisions collected with the D0 detector at the Fermilab Tevatron Collider at ?s=1.96 TeV. Selected events contain one reconstructed Z?e?e? or Z????? candidate and at least two jets, including at least one jet identified as likely to contain a b quark. To validate the search procedure, we also measure the cross section for ZZ production in the same final state. It is found to be consistent with its SM prediction. We set upper limits on the ZHmore »production cross section times branching ratio for H?bb? at the 95% C.L. for Higgs boson masses 90?MH?150 GeV. The observed (expected) limit for MH=125 GeV is 7.1 (5.1) times the SM cross section.« less

  1. Search for a Standard Model Higgs boson in the H -> ZZ -> llnunu decay channel using 4.7 fb-1 of sqrt(s) = 7 TeV data with the ATLAS detector

    E-Print Network [OSTI]

    ATLAS Collaboration

    2012-05-30T23:59:59.000Z

    A search for a heavy Standard Model Higgs boson decaying via H -> ZZ -> llnunu, where l represents electrons or muons, is presented. It is based on proton-proton collision data at sqrt(s) = 7 TeV, collected by the ATLAS experiment at the LHC during 2011 and corresponding to an integrated luminosity of 4.7 fb^-1. The data agree with the expected Standard Model backgrounds. Upper limits on the Higgs boson production cross section are derived for Higgs boson masses between 200 GeV and 600 GeV and the production of a Standard Model Higgs boson with a mass in the range 319 - 558 GeV is excluded at the 95% confidence level.

  2. Measurement of the CP-violating phase ?sJ/?? using the flavor-tagged decay Bs0?J/ ?? in 8 fb?¹ of pp? collisions

    SciTech Connect (OSTI)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; Aoki, M.; Arov, M.; Askew, A.; Åsman, B.; Atkins, S.; Atramentov, O.; Augsten, K.; Avila, C.; BackusMayes, J.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Barreto, J.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Bean, A.; Begalli, M.; Begel, M.; Belanger-Champagne, C.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bezzubov, V. A.; Bhat, P. C.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Brooijmans, G.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Burnett, T. H.; Buszello, C. P.; Calpas, B.; Camacho-Pérez, E.; Carrasco-Lizarraga, M. A.; Casey, B. C. K.; Castilla-Valdez, H.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Croc, A.; Cutts, D.; Das, A.; Davies, G.; De, K.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demarteau, M.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dorland, T.; Dubey, A.; Dudko, L. V.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Evdokimov, V. N.; Facini, G.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Garcia-Bellido, A.; García-Guerra, G. A.; Gavrilov, V.; Gay, P.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A.; Grannis, P. D.; Greder, S.; Greenlee, H.; Greenwood, Z. D.; Gregores, E. M.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Haas, A.; Hagopian, S.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hohlfeld, M.; Hubacek, Z.; Huske, N.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jamin, D.; Jayasinghe, A.; Jesik, R.; Johns, K.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A. W.; Juste, A.; Kaadze, K.; Kajfasz, E.; Karmanov, D.; Kasper, P. A.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kulikov, S.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Kvita, J.; Lammers, S.; Landsberg, G.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lellouch, J.; Li, L.; Li, Q. Z.; Lietti, S. M.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Lubatti, H. J.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Mackin, D.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Maravin, Y.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N. K.; Muanza, G. S.; Mulhearn, M.; Nagy, E.; Naimuddin, M.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Novaes, S. F.; Nunnemann, T.; Obrant, G.; Orduna, J.; Osman, N.; Osta, J.; Otero y Garzón, G. J.; Padilla, M.; Pal, A.; Parashar, N.; Parihar, V.; Park, S. K.; Parsons, J.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, K.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Piegaia, R.; Pleier, M.-A.; Podesta-Lerma, P. L. M.; Podstavkov, V. M.; Polozov, P.; Popov, A. V.; Prewitt, M.; Price, D.; Prokopenko, N.; Protopopescu, S.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M. S.; Ranjan, K.; Ratoff, P. N.; Razumov, I.; Renkel, P.; Rijssenbeek, M.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Safronov, G.; Sajot, G.; Salcido, P.; Sánchez-Hernández, A.; Sanders, M. P.; Sanghi, B.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schliephake, T.; Schlobohm, S.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shchukin, A. A.; Shivpuri, R. K.; Simak, V.; Sirotenko, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Smith, K. J.

    2012-02-01T23:59:59.000Z

    We report an updated measurement of the CP-violating phase, ?sJ/??, and the decay-width difference for the two mass eigenstates, ??s, from the flavor-tagged decay B0s?J/??. The data sample corresponds to an integrated luminosity of 8.0 fb?¹ accumulated with the D0 detector using pp? collisions at ?s=1.96 TeV produced at the Fermilab Tevatron collider. The 68% Bayesian credibility intervals, including systematic uncertainties, are ??s=0.163+0.065?0.064 ps?¹ and ?sJ/??=?0.55+0.38?0.36. The p-value for the Standard Model point is 29.8%.

  3. 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]

    Gomez-Ceballos, Guillelmo

    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. ...

  4. Search for Higgs boson production in oppositely charged dilepton and missing energy final states in 9.7 fb-1 of ppbar collisions at sqrts = 1.96 TeV

    E-Print Network [OSTI]

    D0 Collaboration

    2013-01-07T23:59:59.000Z

    We present a search for Higgs boson in final states with two oppositely charged leptons and large missing transverse energy as expected in H -> WW -> lvlv decays. The events are selected from the full Run II data sample of 9.7 fb-1 of ppbar collisions collected with the D0 detector at the Fermilab Tevatron Collider at sqrt s = 1.96 TeV. To validate our search methodology, we measure the non-resonant W W production cross section and find sigma_WW = 11.6 +/- 0.7 pb, in agreement with the standard model prediction. In the Higgs boson search, no significant excess above the background expectation is observed. Upper limits at the 95% confidence level on the Higgs boson production cross section are therefore derived. Within the standard model, the Higgs boson mass range 159 Higgs boson production cross sections 4.1 times larger than the standard model expectation, which is compatible with the presence of a Higgs boson at this mass. Within a theoretical framework with a fourth generation of fermions, the mass range 125 Higgs boson couplings, which yields an exclusion of fermiophobic Higgs boson production cross sections 3.1 times larger than the expectation for MH = 125 GeV.

  5. Search for a Higgs boson in diphoton final states with the D0 detector in 9.6 fb-1 of p-pbar collisions at sqrt(s)=1.96 TeV

    E-Print Network [OSTI]

    D0 Collaboration

    2013-01-22T23:59:59.000Z

    We present a search for a Higgs boson decaying into a pair of photons based on 9.6 fb-1 of p-pbar collisions at sqrt(s)=1.96 TeV collected with the D0 detector at the Fermilab Tevatron Collider. The search employs multivariate techniques to discriminate signal from the non-resonant background and is separately optimized for a standard model and a fermiophobic Higgs boson. No significant excess of data above the background prediction is observed and upper limits on the product of the cross section and branching fraction are derived at the 95% confidence level as a function of Higgs boson mass. For a standard model Higgs boson with mass of 125 GeV, the observed (expected) upper limits are a factor of 12.8 (8.7) above the standard model prediction. The existence of a fermiophobic Higgs boson with mass in the 100-113 GeV range is excluded at the 95% confidence level.

  6. 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]

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

    2008-08-05T23:59:59.000Z

    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.

  7. Search for the Standard Model Higgs boson in the decay channel H -> ZZ((*)) -> 4l with 4.8 fb(-1) of pp collision data at root s=7 TeV with ATLAS

    SciTech Connect (OSTI)

    Aad G.; Abbott B.; Abdallah J.; Khalek S. Abdel; Abdelalim A. A.; Abdesselam A.; Abdinov O.; Abi B.; Abolins M.; AbouZeid U. S.; Abramowicz H.; Abreu H.; Acerbi E.; Acharya B. S.; Adamczyk L.; Adams D. L.; Addy T. N.; Adelman J.; et al.

    2012-04-12T23:59:59.000Z

    This Letter presents a search for the Standard Model Higgs boson in the decay channel H {yields} ZZ{sup (*)} {yields} {ell}{sup +}{ell}{sup -}{ell}{prime}{sup +}{ell}{prime}{sup -}, where {ell}, {ell}{prime} = e or {mu}, using proton-proton collisions at {radical}s = 7 TeV recorded with the ATLAS detector and corresponding to an integrated luminosity of 4.8 fb{sup -1}. The four-lepton invariant mass distribution is compared with Standard Model background expectations to derive upper limits on the cross section of a Standard Model Higgs boson with a mass between 110 GeV and 600 GeV. The mass ranges 134-156 GeV, 182-233 GeV, 256-265 GeV and 268-415 GeV are excluded at the 95% confidence level. The largest upward deviations from the background-only hypothesis are observed for Higgs boson masses of 125 GeV, 244 GeV and 500 GeV with local significances of 2.1, 2.2 and 2.1 standard deviations, respectively. Once the look-elsewhere effect is considered, none of these excesses are significant.

  8. Universitt Konstanz FB Informatik und Informationswissenschaft

    E-Print Network [OSTI]

    Reiterer, Harald

    show that search is no alternative to navigation on websites. But a search function is necessary to let Vertriebskanals von DaimlerChrysler zur Erlangung des akademischen Grades eines Master of Science (M.ScChrysler - Search and Exploration in complex Information Spaces exemplified by the Digital Sales Channel of Daimler

  9. y12 1950-55 FB

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:Energy: Grid Integration Redefining What'sis Taking Over OurThe Iron4 Self-Scrubbing:,, ,Development1U CO1) 1 Winter FuelsYOURxinyufuUpdraft

  10. hescore_2012_bins | Department of Energy

    Energy Savers [EERE]

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page onYou are now leaving Energy.gov You are now leaving Energy.gov You are being directedAnnual Siteof Energy 2, 2015Visiting8.pdfand Characterization of a Larger Scale

  11. The Search for VH $\\bf\\to$ VWW Standard Model \\\\ Higgs Production in the Trilepton Signature\\\\ with $\\bf5.9\\fb$ of Data from $\\bf\\ppbar$ Collisions \\\\ at $\\bf\\sqrt{s}=1.96$ GeV

    SciTech Connect (OSTI)

    Nett, Jason Michael; /Wisconsin U., Madison

    2010-06-01T23:59:59.000Z

    We present here the search for Standard Model VH {yields} VWW {yields} lll + E{sub T} (missing energy due to neutrinos) production, where V is a W or Z weak vector boson, which uses up to 5.9 fb{sup -1} of integrated luminosity. This analysis has recently added to the CDF high-mass Higgs group three new signal topologies characterized by a tri-lepton signature, which are chosen to isolate the VH {yields} VWW associated production signals in the three-lepton signature. As such, we define three new regions for a WH analysis, a ZH 1-jet analysis, and a ZH {ge} 2-jet analysis with which we expect to contribute an additional {approx} 5.8% (for m{sub H} = 165 GeV) acceptance to the current H {yields} WW dilepton analysis. The ZH trilepton regions are defined by events passing a Z-boson selection: events having at least one lepton pairing (among three possible pairings) with opposite sign, same flavor, and a dilepton invariant mass within [76.0, 106.0] GeV - a {+-} 15 GeV window around the Z-boson mass. The WH trilepton region is then defined as the set of trilepton events that are complement to those chosen by the Z-boson selection. These three new event topologies make a substantial contribution to the H {yields} WW group result. As a measure of the sensitivity of this search, we compute the median expected limit on the at 95% confidence level ('C.L.') on the production cross section (effectively the rate of production) for a Standard Model Higgs boson and report the result as a ratio to the theoretical production cross section. An observed limit ratio of one or less at a given mass would rule out the production of a Standard Model Higgs boson at that mass with 95% confidence. At m{sub H} = 165 GeV, the WH analysis expected limits reach 7.2 times the standard model cross section; the ZH 1-jet analysis is set at 29 times the expected standard model cross section; the ZH {ge} 2-jet analysis is set at 9.9 times the expected standard model cross section; and the combined trilepton analysis is set at 4.9 times the expected standard model cross section. We announce that the combination of this trilepton VH {yields} VWW Higgs boson search and the previous CDF dilepton H {yields} WW search achieves an expected median limit of 1.00 at 165 GeV/c{sup 2}. The expected median limit of 1.00 indicates we anticipate a 50% probability of ruling out the existence of a Standard Model Higgs boson with a mass of 165 GeV/c{sup 2}. This is the first time a single hadron collider experiment has achieved sensitivity to the production of a Standard Model Higgs boson. We do not see evidence for a significant signal of Higgs bosons in the data and place observed limits on the production of a Standard Model Higgs boson of 165 GeV/c{sup 2} at 1.08 times Standard Model production cross section.

  12. Measurement of sin2 ??eff and Z-light quark couplings using the forward-backward charge asymmetry in pp? -> Z/gamma* -> e+e- events with L=5.0 fb-1 at ?s=1.96 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    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.; Alverson, G [Northeastern U.; Alves, G A [Rio de Janeiro, CBPF; Ancu, L S [NIKHEF, Amsterdam; Fermilab

    2011-07-26T23:59:59.000Z

    We measure the mass dependence of the forward-backward charge asymmetry in 157,553 pp? = Z/?* = e+e- interactions, corresponding to 5.0 fb-1 of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron Collider at ?s = 1.96 TeV. The effective weak mixing angle (??eff) from this process involving predominantly the first generation of quarks is extracted as sin2 ??eff = 0.2309 ± 0.0008 (stat.) ± 0.0006 (syst.). We also present the most precise direct measurement of the vector and axial-vector couplings of u and d quarks to the Z boson.

  13. Growth of sheets in 3D confinements - a model for the C-S-H meso 2 structure

    E-Print Network [OSTI]

    Etzold, Merlin A.; McDonald, Peter J.; Routh, Alexander F.

    2014-06-21T23:59:59.000Z

    - and dicalcium silicate surfaces on particle aggre-41 gation [8]. Particle based models have also been used by the group of Ulm to successfully interpret nano42 indentation results [9]. Small-angle neutron scattering data of cement paste has been interpreted... -vectors, both curves show a q?4 dependence which corresponds to203 the experimental Porod regime. The simulated data is compared to experimental small-angle neutron204 scattering data for cement from Allen et al. (dashed) [30]. For large and intermediate...

  14. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    elements 2.1 Teilmodul / submodule FD 2.1 Didactics 2.1 3 ECTS-Punkte / credit points Notwendige zum Modul / further comments Biologiedidaktik 1 sollte möglichst absolviert worden sein. Didactics 1

  15. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    of biology teaching and learning Teilmodul / submodule FD 1.2 Didactics 1.2 3 ECTS-Punkte / credit points of biology teaching and learning Teilmodul / submodule FD 1.2 Didactics 1.2 3 ECTS-Punkte / credit points

  16. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    of biology teaching and learning Teilmodul / submodule FD 1.1 Didactics 1.1 3 ECTS-Punkte / credit points Theoretical and practical basics of biology teaching and learning Teilmodul / submodule FD 1.1 Didactics 1.1 3

  17. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    elements 2.2 Teilmodul / submodule FD 2.2 Didactics 2.2 3 ECTS-Punkte / credit points Notwendige zum Modul / further comments Biologiedidaktik 1 sollte möglichst absolviert worden sein. Didactics 1

  18. FB/SN CRAC Workshops (rates/meetings)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645U.S. DOEThe Bonneville Power AdministrationField8,Dist. Category UC-l 1,EnergyExploringGamma-ray2As

  19. Financial-Based (FB) CRAC (rates/adjustments)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645U.S. DOEThe Bonneville Power AdministrationField8,Dist.New Mexico

  20. Smart Bin for Incompatible Waste Items Arnab Sinha

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    in the context of waste management, where considerable volume of waste is present collectively and there may are performed based on the knowledge available locally without looking up from any external sources. Since, the global identification of objects is avoided, preservation of privacy is ensured, which is a concern

  1. DISS. ETH NO. 16907 Dong-Bin Huang

    E-Print Network [OSTI]

    Richner, Heinz

    Decision-Support #12;#12;DISS. ETH NO. 16907 A Discrete-Event Dynamic Systems Approach for Environmental the cross-scale interdependencies of the urban drainage system and the regional water balance system; (ii Decision-Support A dissertation submitted to the SWISS FEDERAL INSTITUTE OF TECHNOLOGY ZURICH

  2. Challenges of Meeting Tier2 Bin2 Tailpipe Emissions

    Broader source: Energy.gov (indexed) [DOE]

    of emissions solutions Poor consumer image of legacy products Gasolinediesel refinery split will become a challenge if diesel market grows significantly Cetane...

  3. The volatile compound BinBase mass spectral database

    E-Print Network [OSTI]

    Skogerson, Kirsten; Wohlgemuth, Gert; Barupal, Dinesh K; Fiehn, Oliver

    2011-01-01T23:59:59.000Z

    B, Eriksson R: SuperScent-a database of flavors and scents.Sayaed AM: The Pherobase: Database of Insect Pheromones andA public study design database for metabolomics projects.

  4. Data Caching under Number Constraint Himanshu Gupta and Bin Tang

    E-Print Network [OSTI]

    Gupta, Himanshu

    a network graph, the read/write frequencies to the data item by each node, and the cost of caching the data the data item such that the sum of the reading, writing (using an optimal Steiner tree), and storage cost. Here, the cost of reading the data item by a node is defined as the distance to the closest cache node

  5. US Tier 2 Bin 2 Diesel Research Progress

    Broader source: Energy.gov (indexed) [DOE]

    SYSTEM LEVEL 22+ LEVEL 3 LEVEL 4 Variable swirl Advanced EGR EGR bypass Advanced turbo concepts Low Pressure EGR Assisted boosting Variable valve actuation? 16-16.5 CR...

  6. The BMW Approach to Tier2 Bin5

    Broader source: Energy.gov (indexed) [DOE]

    BMW Group BMW Diesel. Wolfgang Mattes DEER 2007 2-Stage Turbocharger (Variable Twin Turbo). Page 10 Engine Small Turbo Big Turbo Intercooler Compressor- Bypass Air Exhaust...

  7. Resonant character of laser-induced formation of particles in a Cs-H2 vapour J. L. Picqu, J. Vergs and R. Vetter

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    . This resonant character confirms the feasibility, which was also pointed out in the case of UF6 mole- cules [4

  8. EXAFS study of Nd(III) uptake by amorphous calcium silicate hydrates (CSH) P. Mandaliev a,b,*, R. Dhn a

    E-Print Network [OSTI]

    Wehrli, Bernhard

    EXAFS study of Nd(III) uptake by amorphous calcium silicate hydrates (C­S­H) P. Mandaliev a,b,*, R Accepted 3 June 2009 Available online 7 June 2009 Keywords: Amorphous calcium silicate hydrate (C Binding mechanisms Molecular level a b s t r a c t Calcium silicate hydrate (C­S­H) phases control

  9. Data:D638d925-23fb-444a-a218-47fb6d7ee905 | Open Energy Information

    Open Energy Info (EERE)

    metered services and Part B-23 is primary metered customers who own their own transformers and distribution service facilities and have a peak demand less than 800 KW. Part...

  10. Data:C4311e31-07fb-463f-b088-a05eb6867164 | Open Energy Information

    Open Energy Info (EERE)

    River Electric Coop Corp Effective date: 20120601 End date if known: Rate name: Cogeneration and small power production power purchase rate schedule over 100 kW Sector:...

  11. Data:1980fb12-686f-41a1-91fb-276aa0f033f4 | Open Energy Information

    Open Energy Info (EERE)

    in fuel and purchased power costs above or below the base amount of .065 per KWH. HYDROPOWER REDUCTION: There shall be a reduction in rate due to power purchased from the...

  12. Data:2fb0f185-fe3e-4fb5-bdaa-5c647d5a18c5 | Open Energy Information

    Open Energy Info (EERE)

    date if known: Rate name: MU-1 - a1b - 250 watt HPS - Painted Bronze Column Sector: Lighting Description: Lamps in enclosed fixtures, mounted on metal or fiberglass columns and...

  13. Top Quark Mass Measurement in the 2 fb -1 Tight Lepton and Isolated Track Sample using

    E-Print Network [OSTI]

    Quigg, Chris

    have been specified (see below). y Part of this work was supported by DARA grant WE2 50 OR 9411. 1 #12

  14. Upgrade of the D0 detector: The Tevatron beyond 2 fb**(-1)

    SciTech Connect (OSTI)

    Quinn, Breese; /Mississippi U.

    2005-01-01T23:59:59.000Z

    Recent performance of Fermilab's Tevatron has exceeded this year's design goals and further accelerator upgrades are underway. The high-luminosity period which follows these improvements is known as Run IIb. The D0 experiment is in the midst of a comprehensive upgrade program designed to enable it to thrive with much higher data rate and occupancy. Extensive modifications of and additions to all levels of the trigger and the silicon tracker are in progress. All upgrade projects are on schedule for installation in the 2005 shutdown.

  15. FOR INFORMATION CONTACT: March 11, 2014 Jess.Beck@noaa.gov FB14-012

    E-Print Network [OSTI]

    in the release of millions barrels of oil into the Gulf of Mexico. After 85 days, the well was successfully Aquaculture in the Gulf of Mexico Comment Period Extended to April 4, 2014 NOAA Fisheries is seeking public for Regulating Offshore Marine Aquaculture in the Gulf of Mexico (Aquaculture Plan). This document considers

  16. Chiral U(1) Flavor Models and Flavored Higgs Doublets: The Top FB Asymmetry

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645U.S. DOE Office511041clothAdvanced Materials Advanced. C o w l i t z CPlasma of theChemistryChicagoFuel CellX I Aand the

  17. Chemomechanics of calcium leaching of cement-based materials at different scales : the role of CH-dissolution and C-S-H degradation on strength and durability performance of materials and structures

    E-Print Network [OSTI]

    Heukamp, Franz H. (Franz Hoyte), 1973-

    2003-01-01T23:59:59.000Z

    Calcium leaching is a durability threat for cement-based materials employed in critical infrastructures, such as Nuclear Waste Storage Systems. This thesis presents a comprehensive study of the material and structural ...

  18. Protein Function Prediction in Proteomics Era Daisuke Kihara, Troy Hawkins, Stan Luban, Bin Li,

    E-Print Network [OSTI]

    Kihara, Daisuke

    , which include a Hidden Markov Model database search [2] or a local motif search [3]. One of the shortcom to draw bio- logical conclusion from them. 1.1 Algorithm of PFP A typical way to use BLAST is to set up even low-scoring se- quence hits by a PSI-BLAST search [6] more extensively [7]. PFP uses Gene Ontology

  19. Equilibrium Defects and Concentrations in Nickel Aluminide Bin Bai* and Gary S. Collins

    E-Print Network [OSTI]

    Collins, Gary S.

    used in aerospace applications. Knowledge of its point defects is needed to understand phenomena by structural point defects: Ni-vacancies (VNi) in Ni-poor alloys and Ni-antisite atoms (NiAl) in Ni-rich alloys at temperatures up to 1300°C. Observation of VNi and NiAl structural defects in Ni-poor and Ni-rich alloys

  20. Identifying anomalous diffusion and melting in dusty plasmas Yan Feng,* J. Goree, and Bin Liu

    E-Print Network [OSTI]

    Goree, John

    is deter- mined by the balance of the energy input and dissipation. As the driven energy input increases Department of Physics and Astronomy, The University of Iowa, Iowa City, Iowa 52242, USA Received 3 June 2010 described as 2D experiments 1,4­8 . Dusty plasma is a driven-dissipative system 1 , and its kinetic energy

  1. Lieber Opa Paul, Ich Bin Auch Ein Experimental Scientist! Doron ZEILBERGER 1

    E-Print Network [OSTI]

    Zeilberger, Doron

    was the inventor of eÆcient verfahrens for the regeneration (recycling) of caoutchouc (rubber). 3. Paul had many solution and the regeneration of rubber waste". 4. He contributed several articles to the famous Ullmann nice. One especially nasty specimen was the great organic chemist Hermann Kolbe, who was Wislicensus

  2. Lieber Opa Paul, Ich Bin Auch Ein Experimental Scientist! Doron ZEILBERGER 1

    E-Print Network [OSTI]

    Zeilberger, Doron

    was the inventor of efficient verfahrens for the regeneration (recycling) of caoutchouc (rubber). 3. Paul had many solution and the regeneration of rubber waste". 4. He contributed several articles to the famous Ullmann. One especially nasty specimen was the great organic chemist Hermann Kolbe, who was Wislicensus

  3. Benefit-based Data Caching in Ad Hoc Networks Bin Tang, Himanshu Gupta, Samir Das

    E-Print Network [OSTI]

    Gupta, Himanshu

    network by reducing the access latency and bandwidth usage. However, designing effi- cient distributed. The computing devices could be conventional computers (e.g., PDA, laptop, or PC) or backbone routing platforms in bandwidth as well as battery energy. The problem of cache placement is particularly challenging when each

  4. #!/usr/bin/python # Program mref.py converts typical .tex file into ...

    E-Print Network [OSTI]

    ... links by reference to MR database using MREF # Written by Bartlomiej Siudeja # Based on script mrefh.py by Jim Pitman pitman@stat.berkeley.edu 10/10/03.

  5. Bin-MAC: A Hybrid MAC for Ultra-Compact Wireless Sensor Nodes Vahid Salmani

    E-Print Network [OSTI]

    Chou, Pai H.

    status monitoring to target tracking. Although many protocols have been proposed in the literature, few

  6. Presentation 2.7: Energy and the Forest Products Industry in Malaysia Zulkifli Bin Ahmad

    E-Print Network [OSTI]

    balanced utilization of oil, gas, hydro & coal To prolong lifespan of Malaysia's oil reserves for future in the production of wood products are collected to be used as raw materials to produce fibre boards

  7. Lieber Opa Paul, Ich Bin Auch Ein Experimental Scientist! Doron ZEILBERGER 1

    E-Print Network [OSTI]

    Zeilberger, Doron

    entitled "Process * *for the production of aqueous caoutchouc solution and the regeneration of rubber (recyc* *ling) of caoutchouc (rubber). 3. Paul had many patents, e.g. US # 844077, issued in 1907

  8. CCooggnniittiivvee aanndd UUssaabbiilliittyy IIssssuueess iinn GGeeoovviissuuaalliizzaattiioonn Terry A. Slocum, Connie Blok, Bin Jiang, Alexandra Koussoulakou,

    E-Print Network [OSTI]

    Montello, Daniel R.

    in Geovisualization. Developments in hardware and software have led to (and will continue to stimulate) novel methods a lifecycle (including design, development, and deployment). Applying usability engineering if they are not developed within a theoretical cognitive framework and iteratively tested using usability engineering

  9. Dilute Acid and Autohydrolysis Pretreatment Bin Yang and Charles E. Wyman

    E-Print Network [OSTI]

    California at Riverside, University of

    to make cellulose and hemi- cellulose susceptible to an enzymatic hydrolysis step for generation 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 Jonathan R. Mielenz (ed.), Biofuels, biological catalysis was substituted for the second thermochemical step to enhance glucose yields from

  10. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    reduced cylinder block weight Aluminum cylinder head for weight and size optimization * Reduced development time and cost to program * Make common with LDD V8 (previous...

  11. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    any confidential, proprietary, or otherwise restricted information. Catalyst optimization for optimal NO 2 NOx & HC conversion varying PGM load on CSC(tm) parts PGM loading...

  12. Resilient Event Triggered Systems with Limited Communication Lichun Li, Bin Hu and Michael Lemmon

    E-Print Network [OSTI]

    Lemmon, Michael

    of critical civil infrastructure, such as the power grid or transportation network, will result in economic systems are integrated over public networks. These public systems also become more vulnerable to malicious of Electrical Engineering, University of Notre Dame, Notre Dame, IN 46556, USA. lli3,bhu2,lemmon@nd.edu Event

  13. Impact of surfactants on pretreatment of corn stover Qing Qing, Bin Yang 1

    E-Print Network [OSTI]

    California at Riverside, University of

    glycol 4000 during water-only or dilute acid pretreatment of corn stover at 140­220 °C were evaluated energy security, trade deficit, environmental, and economic issues that are becoming more urgent in light of declining petroleum reserves and increasing international demand for transportation fuels. However

  14. Relay node placement in large scale wireless sensor networks Jian Tang*, Bin Hao, Arunabha Sen

    E-Print Network [OSTI]

    Tang, Jian "Neil"

    efficient design is needed for prolonging network lifetime. Computer Communications 29 (2006) 490­501 www for a fairly short period of time if operated at high transmission power levels. As a consequence, energy

  15. A Bin Method for Calculating Energy Conservation Retrofit Savings in Commercial Buildings

    E-Print Network [OSTI]

    Thamilseran, S.; Haberl, J. S.

    1994-01-01T23:59:59.000Z

    The calculation of measured energy savings from energy conservation retrofits is an important step in the verification of the success of a retrofit (Claridge et al. 1992). Several methods for calculating the savings from energy conservation...

  16. FIND A BIN, IT ALL GOES IN all types of paper

    E-Print Network [OSTI]

    Thaxton, Christopher S.

    & steel cans, lids, & pans GLASSall bottles & jars PLASTICall plastics #1 - #7, wraps, films, & bags zerow: flatten next to containers, or place in marked dumpsters SPECIAL RECYCLING ITEMS: containers located in student union · cfl bulbs (place in sealed plastic bag) · computer equipment * · techno-trash: thumbdrives

  17. Diurnal Precipitation Regimes in the Global Tropics* KAZUYOSHI KIKUCHI AND BIN WANG

    E-Print Network [OSTI]

    Wang, Bin

    by moderate amplitude and an early morning peak [0600­0900 Local Solar Time (LST)], found primarily Australia, the west coast of America extending from Mexico to Ecuador, the west coast of equatorial Africa's response to solar radiation. Thus, the diurnal cycle provides a good opportunity for testing our

  18. Xylooligomers are strong inhibitors of cellulose hydrolysis by enzymes Qing Qing, Bin Yang 1

    E-Print Network [OSTI]

    California at Riverside, University of

    Carlo analysis decreased subject requirement without sacrificing power. This model provides a useful, the tissues contain the maximum nitrogen load possible for a given depth, so decompression from saturation saturation conditions are relatively sparse and, for ethical reasons, do not ap- proach the severe profiles

  19. Application of a Diesel Fuel Reformer for Tier 2 Bin 5 Emissions

    Broader source: Energy.gov (indexed) [DOE]

    Inlet exhaust gas temperature Warm-up LNT bed Warm-up DOC bed Under floor LNT bed Turbo out Exhaust Temperature 0 20 40 60 80 100 120 140 Time(sec) MAF Ref WHLSPD mph WU...

  20. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine

    Broader source: Energy.gov (indexed) [DOE]

    and Progress Engine Out Emissions and Fuel Economy BSFC held constant via improved turbo match on low CR engine 11 Innovation You Can Depend On(tm) This presentation does not...

  1. A Bin Method for Calculating Energy Conservation Retrofit Savings in Commercial Buildings 

    E-Print Network [OSTI]

    Thamilseran, S.; Haberl, J. S.

    1994-01-01T23:59:59.000Z

    The calculation of measured energy savings from energy conservation retrofits is an important step in the verification of the success of a retrofit (Claridge et al. 1992). Several methods for calculating the savings from energy conservation...

  2. Cummins Next Generation Tier 2, Bin 2 Light Truck Diesel engine

    Broader source: Energy.gov (indexed) [DOE]

    to current diesel Aftertreatment effectiveness improvement Reduction in emission control fuel economy penalty Low impact vehicle integration for OEM application 5...

  3. LNT or Urea SCR Technology: Which is the right technology for TIER 2 BIN 5

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn't YourTransport(FactDepartment ofLetter Report:40PM toLED Lighting5-15Trade |Vessel intopassenger

  4. http://cemp.dri.edu/cgi-bin/cemp_stations.pl?stn=tono&prod=11

    National Nuclear Security Administration (NNSA)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645 3,625 1,006 492 742EnergyOn AprilAElectronic Input Options Gary L. Hirsch SNLMaythe InteriorWaterhepf3 Community

  5. http://cemp.dri.edu/cgi-bin/cemp_stations.pl?stn=tono&prod=11

    National Nuclear Security Administration (NNSA)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645 3,625 1,006 492 742EnergyOn AprilAElectronic Input Options Gary L. Hirsch SNLMaythe InteriorWaterhepf3 Community1

  6. http://frwebgate.access.gpo.gov/cgi-bin/getdoc.cgi?dbname=106_c

    National Nuclear Security Administration (NNSA)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645 3,625 1,006 492 742EnergyOn AprilAElectronic Input Options Gary L. Hirsch SNLMaythemeansI MEDIAN HOUSEHOLD

  7. http://frwebgate.access.gpo.gov/cgi-bin/usc.cgi?ACTION=RETRIEVE

    National Nuclear Security Administration (NNSA)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645 3,625 1,006 492 742EnergyOn AprilAElectronic Input Options Gary L. Hirsch SNLMaythemeansI MEDIAN HOUSEHOLDResources

  8. Cummins Next Generation Tier 2, Bin 2 Light Truck Diesel engine |

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn't Your Destiny: Theof"Wave theJuly 30,Crafty Gifts for theofPhotovoltaics »Indy

  9. Cummins' Next Generation Tier 2, Bin 2 Light Truck Diesel Engine |

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn't Your Destiny: Theof"Wave theJuly 30,Crafty Gifts for theofPhotovoltaicsMay 16,

  10. Challenges of Meeting Tier2 Bin2 Tailpipe Emissions | Department of Energy

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn't Your Destiny: Theof EnergyAdministration-Desertof Energy0 ChairsDepartmentCHALLENGES

  11. US Tier 2 Bin 2 Diesel Research Progress | Department of Energy

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your DensityEnergy U.S.-China Electric Vehicle and Battery TechnologyDepartmentIndia Joint Center forGridUS

  12. Thermodynamic Systems for Tier 2 Bin 2 Diesel Engines | Department of

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn'tOriginEducationVideoStrategic|Industrial Sector,Department of Energythe Use of Lowand

  13. Hmelo, Bin Hu, Alamgir Karim, Martyn McLachlan, and Ron Jones (by phone)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645U.S. DOEThe Bonneville PowerCherries 82981-1cnHigh School football High SchoolBundlesHistory New BrunswickHitting a

  14. Application of a Diesel Fuel Reformer for Tier 2 Bin 5 Emissions |

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn't Your Destiny: The FutureComments from Taras KucmanTransmissionTransmissionApplicationDepartment

  15. Application of a Diesel Fuel Reformer for Tier 2 Bin 5 Emissions |

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn't Your Destiny: The FutureComments from Taras

  16. The BMW Approach to Tier2 Bin5 | Department of Energy

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn'tOriginEducationVideoStrategic| DepartmentDepartment ofTankTest(EAP) Bulletin,(EAP)TheThe BEAMThe

  17. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn't Your Destiny: The Future of1 A Strategic FrameworkRoadmap ANSItheARPA-E MarchfansATNIInnovation

  18. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine | Department of

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn't Your Destiny: The Future of1 A Strategic FrameworkRoadmap ANSItheARPA-E

  19. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine | Department of

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn't Your Destiny: The Future of1 A Strategic FrameworkRoadmap ANSItheARPA-EEnergy 1 DOE Hydrogen

  20. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine | Department of

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn't Your Destiny: The Future of1 A Strategic FrameworkRoadmap ANSItheARPA-EEnergy 1 DOE

  1. Strategies for In-Cylinder Reductions to Reach Bin 2 and LEV III |

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn'tOriginEducationVideoStrategic Safety Goals Strategic Safety Goals July

  2. Quantum Mechanical Metric for Internal Cohesion in Cement Crystals

    E-Print Network [OSTI]

    Dharmawardhana, C. C.; Misra, Anil; Ching, Wai-Yim

    2014-12-05T23:59:59.000Z

    Calcium silicate hydrate (CSH) is the main binding phase of Portland cement, the single most important structural material in use worldwide. Due to the complex structure and chemistry of CSH at various length scales, the focus has progressively...

  3. Cultural Geography and Interregional Contacts in Prehistoric Liangshan (Southwest China)

    E-Print Network [OSTI]

    Hein, Anke Marion

    2013-01-01T23:59:59.000Z

    constricted neck; Type FbI: downward-slanting sides, foot-flaring rim (34), and Type FbI: high neck. A correlationFaII FaII FaII FaII FaII Fb FbI FbI FbI FbI FbI FbI FbI FbI

  4. Measurements of inclusive $W+$jets production rates as a function of jet transverse momentum in $p\\bar{p}$ collisions at $\\sqrt{s}=1.96$~TeV

    SciTech Connect (OSTI)

    Abazov, Victor Mukhamedovich; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma U.; Acharya, Bannanje Sripath; /Tata Inst.; Adams, Mark Raymond; /Illinois U., Chicago; Adams, Todd; /Florida State U.; Alexeev, Guennadi D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Augustana Coll., Sioux Falls; Alverson, George O.; /Northeastern U.; Alves, Gilvan Augusto; /Rio de Janeiro, CBPF; Ancu, Lucian Stefan; /Nijmegen U. /Fermilab

    2011-06-01T23:59:59.000Z

    This Letter describes measurements of inclusive W({yields} e{nu}) + n jet cross sections (n = 1-4), presented as total inclusive cross sections and differentially in the n{sup th} jet transverse momentum. The measurements are made using data corresponding to an integrated luminosity of 4.2 fb{sup -1} collected by the D0 detector at the Fermilab Tevatron Collider, and achieve considerably smaller uncertainties on W+jets production cross sections than previous measurements. The measurements are compared to next-to-leading order perturbative QCD (pQCD) calculations in the n = 1-3 jet multiplicity bins and to leading order pQCD calculations in the 4-jet bin. The measurements are generally in agreement with pQCD predictions, although certain regions of phase space are identified where the calculations could be improved.

  5. Data:Ac6cac7a-3b71-4c12-8fb2-f20fb8bc7e86 | Open Energy Information

    Open Energy Info (EERE)

    Southeastern Power Admin Effective date: 20121001 End date if known: Rate name: Wholesale Power Rate Schedule Pump-1-A Sector: Commercial Description: Availability: This rate...

  6. Data:81fb99fe-5292-4a00-bfbb-2635adf907b7 | Open Energy Information

    Open Energy Info (EERE)

    Time-of-Day: SCHEDULE GS-1 Sector: Commercial Description: Available to customers who use energy storage devices with time-differentiated load characteristics approved by the...

  7. Data:12301c2c-3522-41e3-90fb-88538afc105c | Open Energy Information

    Open Energy Info (EERE)

    Description: Source or reference: http:www.montana-dakota.comdocsdefault-sourcerates-tariffsMTElectric16 Source Parent: http:www.montana-dakota.comrates-and-services...

  8. Data:Eb1c48fb-44a3-4403-98fd-853966861405 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Clay County Electric Coop Corp Effective date: 20130101 End date if known: Rate name:...

  9. Data:78893167-9282-411a-82a4-fb690a5b1409 | Open Energy Information

    Open Energy Info (EERE)

    Irrigation Power Service is applicable to accounts where Member is using an electric motor to lift ground water for the purpose of irrigation. Day- of- Week Irrigation: The...

  10. Data:F3164fcd-c53a-47ee-9427-b84467fb5833 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Dover, Delaware (Utility Company) Effective date: 20080701 End date if known: Rate...

  11. Data:902905fb-8cbb-457d-9db5-352834999c90 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Cuba City, Wisconsin (Utility Company) Effective date: 20091014 End date if known:...

  12. Data:2404fb0c-9501-4897-bc5f-82eecc3f975e | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Burt County Public Power Dist Effective date: 20120101 End date if known: Rate name: Irrigation and Grain...

  13. Data:12819b61-8fb8-4289-afae-af2425c7504d | Open Energy Information

    Open Energy Info (EERE)

    schedule is available for metered outdoor lighting service to any Customer. New or replacement light installations shall be limited to high pressure sodium and metal-halide...

  14. Data:356282ca-87f0-4fb6-a57c-3fc9389866ff | Open Energy Information

    Open Energy Info (EERE)

    furnish, install, and maintain street lighting units. This rate is subject to a Power Cost Adjustment charge per all kWh, that varies on a monthly basis. Source or reference:...

  15. Data:4fb36aea-c051-4565-8491-36181abb11fc | Open Energy Information

    Open Energy Info (EERE)

    Sector: Lighting Description: RULES AND REGULATIONS: Terms and conditions of this electric rate schedule and the General Rules and Regulations govern use of this service....

  16. Data:4a81ff34-3411-46a7-9415-4007405fb196 | Open Energy Information

    Open Energy Info (EERE)

    to purchase and install 2" Sch. 40 electrical grade EPVC conduit and install pre-cast concrete bases for mounting the light poles. Customers should contact GMP's engineering...

  17. Data:6f605d2f-1405-4026-9205-4fb2612dc576 | Open Energy Information

    Open Energy Info (EERE)

    purposes when all service is supplied through a single meter and residences using electricity as the principal source of heat. Source or reference: http:...

  18. Data:764960a6-c576-432f-b6bf-21b862270742 | Open Energy Information

    Open Energy Info (EERE)

    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...

  19. Data:4471b83c-f3ab-4488-b486-fb4bbb915272 | Open Energy Information

    Open Energy Info (EERE)

    Lincoln Electric System Effective date: 20110523 End date if known: Rate name: Cogeneration & Small Power Production Purchase Sector: Commercial Description: To cogeneration...

  20. Data:1207fb35-aa8e-4022-a3ba-c2342fd66991 | Open Energy Information

    Open Energy Info (EERE)

    subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Wheeling Power...

  1. Data:23094a41-b5ae-46fb-953a-8559db175625 | Open Energy Information

    Open Energy Info (EERE)

    process and remains constant during the term that the Customer qualifies for the Rider. TERMS AND CONDITIONS The customer who qualifies for this Rider receives the billing credit...

  2. Data:71fb7fd5-d384-4529-9590-9990446dae0d | 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:...

  3. Data:6943388f-b933-4d62-b208-156017236c8f | Open Energy Information

    Open Energy Info (EERE)

    Rate name: Lighting Rate Schedule No. 8-Owned By District-Standard Roadway Pole - Steel - 38 Ft-100 Watt Sector: Lighting Description: Applicability: Applicable to any type...

  4. '('()%0 1 243 57698A@CB(8EDGF24FB(8AHI8A24P

    E-Print Network [OSTI]

    to share and re-use knowledge between the geographical lo- cations. As O'Leary claims, KM is difficult when knowl- edge flows (e.g. face to face communication) are simply not present (O'Leary, 1998). Selected

  5. Data:1ff143fb-92f7-4639-b337-67d027720178 | Open Energy Information

    Open Energy Info (EERE)

    Description: The Button-Up Weatherization Program offers an incentive for reducing the heat loss of a home. The retail member of Taylor County Rural Electric Cooperative...

  6. Data:7720700d-783d-4c93-b509-fb3110ecea58 | Open Energy Information

    Open Energy Info (EERE)

    Rate name: Residential Sector: Residential Description: Source or reference: ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):...

  7. Data:28430969-c005-40ae-b536-3803ebcf4fb0 | Open Energy Information

    Open Energy Info (EERE)

    Industrial Sector: Industrial Description: Industrial Source or reference: isu documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):...

  8. Superdiffusion and Non-Gaussian Statistics in a Driven-Dissipative 2D Dusty Plasma Bin Liu and J. Goree

    E-Print Network [OSTI]

    Goree, John

    . Goree Department of Physics and Astronomy, The University of Iowa, Iowa City, Iowa 52242, USA (Received media [8], our particles are driven by an external source, and their average kinetic energy is set by a balance of driving forces and dissipation. Random motion is characterized using the mean

  9. Online Bin Coloring Sven O. Krumke ?1 , Willem E. de Paepe 2 , Jorg Rambau 1 , and Leen Stougie ??3

    E-Print Network [OSTI]

    Krumke, Sven O.

    University of Eindhoven, P. O. Box 513, 5600MB Eindhoven, The Netherlands. w.e.d.paepe@tm.tue.nl 3 Department of Mathematics, Technical University of Eindhoven, P. O. Box 513, 5600MB Eindhoven, The Netherlands and Centre

  10. User-Driven Frequency Scaling Arindam Mallik, Student Member, IEEE, Bin Lin, Gokhan Memik, Member, IEEE, Peter Dinda, Member, IEEE,

    E-Print Network [OSTI]

    Kuzmanovic, Aleksandar

    Scaling (DVFS), e.g, those used in current laptop and desktop computers. UDFS dynamically adapts CPU techniques through user studies conducted on a Pentium M laptop running Windows applications. The UDFS scheme supported by Department of Energy Award DE-FG02-05ER25691 and NSF Grants IIS- 0613568, CNS-0551639, CNS

  11. Vehicle Technologies Office Merit Review 2015: ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine

    Broader source: Energy.gov [DOE]

    Presentation given by Cummins at 2015 DOE Hydrogen and Fuel Cells Program and Vehicle Technologies Office Annual Merit Review and Peer Evaluation Meeting about ATP-LD; Cummins next generation tier...

  12. Node Reclamation and Replacement for Long-lived Sensor Networks Bin Tong, Guiling Wang, Wensheng Zhang, and Chuang Wang

    E-Print Network [OSTI]

    Zhang, Wensheng

    surveillance, road condition monitoring, and so on. Hence, many energy conservation schemes [1] were proposed. In particular, the amount of energy that a solar cell can harvest is proportional to its surface area, but it is infeasible to equip a tiny sensor node with a large-size solar cell. The amount of available solar energy

  13. Evolution of Shear-Induced Melting in a Dusty Plasma Yan Feng,* J. Goree, and Bin Liu

    E-Print Network [OSTI]

    Goree, John

    is reached. Melting spreads with a front that propagates at the transverse sound speed. Unexpectedly essentially on a 2D plane include a Wigner lattice of electrons on a liquid-He surface [8], ions confined to a crystalline solid or a liquid [17]. Coulomb repulsion is shielded with a screening length D [27]. Dusty

  14. SET-based nano-circuit simulation and design method using HSPICE Fengming Zhang, Rui Tang, Yong-Bin Kim*

    E-Print Network [OSTI]

    Ayers, Joseph

    on the orthodox theory and the Birth­Death Markov chain is demonstrated and verified with Coulomb characteristics, and increasingly difficult and expensive lithography will arise. To maintain the trend of Moore's Law ARTICLE IN PRESS #12;structure, and the characteristic of periodic current with gate voltage makes

  15. Cooperative Bin-Picking with Time-of-Flight Camera and Impedance Controlled DLR Lightweight Robot III

    E-Print Network [OSTI]

    Blanz, Volker

    is characterized by all-purpose industrial robots replacing man- power for mass production. These robots perform industrial robotic generation will be characterized by highly sensorized light- weight robots

  16. University of Tulsa Technical Report UTULSA-MCS-93-8, May, 1993. A Heuristic for Improved Genetic Bin Packing

    E-Print Network [OSTI]

    Wainwright, Roger L.

    University of Tulsa Technical Report UTULSA-MCS-93-8, May, 1993. A Heuristic for Improved Genetic Sciences, The University of Tulsa, 600 South College Avenue, Tulsa, OK 74104-3189, USA Keywords

  17. Bin Li, John O'Loughlin and Lee Gillam (PI) Department of Computing, FEPS, University of Surrey

    E-Print Network [OSTI]

    Gillam, Lee

    Application-Specific Service Level Agreements: Experiments in Clouds and Grids, In Antonopoulos and Gillam Journal of Grid and Utility Computing (IJGUC) ISSN (Online): 1741-8488 - ISSN (Print): 1741-847X. (In, Oxford, UK. [1] Li, B. and Gillam, L. (2009), Grid Service Level Agreements using Financial Risk Analysis

  18. Energy Consumption Simulation and Analysis of Heat Pump Air Conditioning System in Wuhan by the BIN Method 

    E-Print Network [OSTI]

    Wen, Y.; Zhao, F.

    2006-01-01T23:59:59.000Z

    to simulate the annual energy consumption of groundwater heat pump systems (GWHPS) for an office building in Wuhan. Its annual energy consumption was obtained and compared with the partner of the air source heat pump systems (ASHPS). The results show...

  19. RESEARCH GRANT The Sheikh Saud bin Saqr Al Qasimi Research Grants encourages scholars from a wide range of

    E-Print Network [OSTI]

    Bushman, Frederic

    , access and attitudes to treatment · Reproductive health · Access to antenatal and postnatal care and education · Substance abuse ­ prevalence, treatment, social attitudes, perceptions and education · Health patients · Congenital birth defects and diseases ­ prevalence, education and access to treatment / long

  20. Preparation of BaPbO3 functional ceramics from leaded waste Bin Li, Shen-Gen Zhang*, Kun Zhang,

    E-Print Network [OSTI]

    Volinsky, Alex A.

    -mail: thlibin@sina.com K. Zhang Beijing Nonferrous Metals and Rare Earth Research Institute, Beijing 100012 should be made to process secondary sources, such as waste rare earth pro- ducts [1], tailings [2, USA 123 Rare Met. (2014) 33(5):598­603 RARE METALS DOI 10.1007/s12598-014-0369-1 www

  1. Energy Consumption Simulation and Analysis of Heat Pump Air Conditioning System in Wuhan by the BIN Method

    E-Print Network [OSTI]

    Wen, Y.; Zhao, F.

    2006-01-01T23:59:59.000Z

    to simulate the annual energy consumption of groundwater heat pump systems (GWHPS) for an office building in Wuhan. Its annual energy consumption was obtained and compared with the partner of the air source heat pump systems (ASHPS). The results show...

  2. Shear Viscosity of Two-Dimensional Yukawa Systems in the Liquid State Bin Liu and J. Goree

    E-Print Network [OSTI]

    Goree, John

    with liquids, including liquids near freezing, composed of molecules or particles that interact with a Yukawa a few reports of transport coef- ficients computed for 2D liquids using molecular dynamics (MD simulation uses an equilibrium method to calculate . Under equilibrium conditions, momentum transport arises

  3. frwebgate.access.gpo.gov/cgi-bin/getdoc.cgi?dbname=2008_register&docid=55825.pdf

    Energy Savers [EERE]

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page onYou are now leaving Energy.gov You are now leaving Energy.gov You are being directedAnnual Siteof Energy 2, 2015Visiting8.pdf flash2004-18.pdfflash2007-21Attachment.pdfBPA1-14 for

  4. First Draft Performance Assessment for the H-Area Tank Farm at...

    Office of Environmental Management (EM)

    of Concern COPC Constituent of Potential Concern CPT Cone Penetration Test CRC Cesium Removal Column CSH Calcium Silicate Hydrate CSRA Central Savannah River Area CTS...

  5. Natural Abundance 43Ca NMR Spectroscopy of Tobermorite and Jennite...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    which has limited our ability to understand the structure of, for example, Ca–silicate hydrate (C–S–H). 43Ca nuclear magnetic resonance (NMR) spectroscopy has...

  6. Microsoft Word - NRAP-TRS-III-004-2014_Acid Gas Interactions...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    involves dissolution of key cementitious phases (portlandite and amorphous calcium-silicate-hydrate (C-S-H)), precipitation and dissolution of carbonate species (calcite),...

  7. Nocturnal cold air drainage and pooling in a tropical forest

    E-Print Network [OSTI]

    Goulden, M. L.; Miller, S. D.; da Rocha, H. R.

    2006-01-01T23:59:59.000Z

    line connecting means within 10 percentile bins). NEE as aconnecting means within 10 percentile bins). The frictionbreaking the data into 10-percentile u* bins with the lowest

  8. Deteriorated hardened cement paste structure analyzed by XPS and {sup 29}Si NMR techniques

    SciTech Connect (OSTI)

    Kurumisawa, Kiyofumi, E-mail: kurumi@eng.hokudai.ac.jp [Faculty of Engineering, Hokkaido University, Japan, Kita 13, Nishi 8, Kita-ku, Sapporo, Hokkaido 060-8628 (Japan)] [Faculty of Engineering, Hokkaido University, Japan, Kita 13, Nishi 8, Kita-ku, Sapporo, Hokkaido 060-8628 (Japan); Nawa, Toyoharu [Faculty of Engineering, Hokkaido University, Japan, Kita 13, Nishi 8, Kita-ku, Sapporo, Hokkaido 060-8628 (Japan)] [Faculty of Engineering, Hokkaido University, Japan, Kita 13, Nishi 8, Kita-ku, Sapporo, Hokkaido 060-8628 (Japan); Owada, Hitoshi [Radioactive Waste Management Funding and Research Center, 1-15-7 Tsukishima, Chuo-ku, Tokyo (Japan)] [Radioactive Waste Management Funding and Research Center, 1-15-7 Tsukishima, Chuo-ku, Tokyo (Japan); Shibata, Masahito [Taiheiyo Consultant Co., Ltd., 2-4-2, Ohsaku, Sakura-City, Chiba (Japan)] [Taiheiyo Consultant Co., Ltd., 2-4-2, Ohsaku, Sakura-City, Chiba (Japan)

    2013-10-15T23:59:59.000Z

    In this report, X-ray photoelectron spectroscopy (XPS) and {sup 29}Si-MAS-NMR was used for the evaluation of deteriorated hardened cement pastes. The deterioration by ammonium nitrate solution was accompanied by changes in the pore structure as well as by structural changes in the C–S–H in the hardened cement paste. The CaO/SiO{sub 2} ratio of the C–S–H decreased with the progress of deterioration, there was also polymerization of the silicate in the C–S–H. It was confirmed that the degree of polymerization of silicate of the C–S–H in hardened cement paste can be determined by XPS. It was also shown that the polymerization depends on the structure of the C–S–H. -- Highlights: •The polymerization of silicate of the C–S–H in the HCP can be observed by XPS. •The structure of C–S–H changed with the degree of calcium leaching. •The NMR result about silicate in C–S–H was in good agreement with the XPS result.

  9. Contact Mechanics Based Mechanical Characterization of Portland Cement Paste

    E-Print Network [OSTI]

    Jones, Christopher

    2012-02-14T23:59:59.000Z

    that the calcium silicate hydrate (C-S-H) phase of hydrated portland cement has different properties on the nanometric scale than on the micron scale. Packing density of C-S-H particles is proposed as an explanation for the disparity in the measured results...

  10. Waste Stream Disposal Pharmacy Quick Sheet (6/16/14) Also pharmacy employees must complete SABA "Medication Waste Stream Disposal" Non-hazardous Hazardous Additional Waste

    E-Print Network [OSTI]

    Oliver, Douglas L.

    Additional Waste Disposal Location Green Bins for Non-hazardous waste Black Bins must complete SABA "Medication Waste Stream Disposal" Non-hazardous Hazardous for Hazardous Waste Yellow Trace Chemo Disposal Bin Red Sharps Bins Red

  11. Deploying Systems Interoperability and Customer Choice within Smart Grid

    E-Print Network [OSTI]

    Ghatikar, Girish

    2014-01-01T23:59:59.000Z

    twiki- sggrid/bin/view/SmartGrid/PriorityActionPlanssggrid/bin/view/SmartGrid/TTMeetingOnPriceCommunications The

  12. Data:09f26efc-50f2-4972-9b3d-136c5e29f6fb | Open Energy Information

    Open Energy Info (EERE)

    taking service from the District that voluntarily agree to a Green Power Service Contract. This Rider is not available to those Consumers taking service under Rate...

  13. Data:E3073c8b-9a05-4b3e-98b9-af282fb257da | Open Energy Information

    Open Energy Info (EERE)

    taking service from the District that voluntarily agree to a Green Power Service Contract. This Rider is not available to those accounts taking service under Rate Schedule...

  14. Data:6fff5fb5-dd23-459e-b785-657689fe1805 | Open Energy Information

    Open Energy Info (EERE)

    5-657689fe1805 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...

  15. Data:6fb4284b-4d20-462e-ab5b-28645d3b33ee | Open Energy Information

    Open Energy Info (EERE)

    and to non-residential customers with monthly demands below 20 kW who have thermal energy storage devices andor thermal storage heating systems integrated with resistance...

  16. Data:A43b3d2d-1510-4c41-9cf0-fb4d79eada15 | Open Energy Information

    Open Energy Info (EERE)

    heating installations meeting the Cooperative's space heating equipment, building insulation and wiring specifications, where electric service is also used for lighting and...

  17. Data:4aa54605-4c32-425b-869a-e0458dc940fb | Open Energy Information

    Open Energy Info (EERE)

    * Qualify for special parking privileges under RCW 46.16.381(1) (a through h) or are a blind person as defined in RCW 74.18.020(4), or * Earn an SSDI income, or * Provide a...

  18. Data:53a16080-fb8f-4c59-9ed1-c7e6aa1367e8 | Open Energy Information

    Open Energy Info (EERE)

    not exceeding 20% of the total energy used on the same premises is permitted. Energy Conservation Charge: The bill for service hereunder may be increased or decreased as...

  19. Data:0e56ee97-7536-4baa-8fb1-07e0e7bd1c4c | Open Energy Information

    Open Energy Info (EERE)

    Effective date: 20140110 End date if known: Rate name: Schedule LPC-CBM: Large Power Compression - Coal Bed Methane Sector: Industrial Description: * Demand Charge at...

  20. F2C 1/Photoni Conference 2000/443 Sid em od e O p t ical I nj ection D FB

    E-Print Network [OSTI]

    Choi, Woo-Young

    F2C 1/Photoni� Conference 2000/443 ¦ - / o Sid em od e O p t ical I nj ection � � ë � ÷ ¢ ¯ ¶ � D D ar ed - M od u lated D F B L aser s by Sid a n od e O p tical I nj ection ¨ ] � õ , - µ ¤ , � ì µ

  1. Data:Cc8427b3-92d4-4cac-ade1-5dd9fb0b039c | Open Energy Information

    Open Energy Info (EERE)

    Lighting - Sodium Vapor 100W, Schedule ML Sector: Lighting Description: Available in OTEC service territory for OTEC-owned municipal and highway lighting installed on existing...

  2. Data:Cd308b5a-15fb-406d-8286-91dd8f5367a0 | Open Energy Information

    Open Energy Info (EERE)

    Southeastern Power Admin Effective date: 20121001 End date if known: Rate name: Wholesale Power Rate Schedule Duke-1-E Sector: Commercial Description: Availability: This rate...

  3. Data:F855a9ea-42fb-4f79-8f3b-00cb07862873 | Open Energy Information

    Open Energy Info (EERE)

    Southeastern Power Admin Effective date: 20111001 End date if known: Rate name: Wholesale Power Rate Schedule CEK-1-H: Rate Scenario 1 Sector: Commercial Description:...

  4. Data:7053c52d-767e-468f-b91e-44cfd6eac2b4 | Open Energy Information

    Open Energy Info (EERE)

    Southeastern Power Admin Effective date: 20121001 End date if known: Rate name: Wholesale Power Rate Schedule Santee-1-E Sector: Commercial Description: Availability: This...

  5. Data:8d8fb5e8-f5cf-47a9-818f-79e25991ece5 | Open Energy Information

    Open Energy Info (EERE)

    Authority Effective date: 20140601 End date if known: Rate name: Outdoor Lighting Rates 100Watt Sodium Sector: Lighting Description: Source or reference: http:...

  6. Data:9ec1fa25-759e-4016-b98f-fb63885069a6 | Open Energy Information

    Open Energy Info (EERE)

    if known: Rate name: Residential Sector: Residential Description: Rates are subject to an Energy Cost Adjustment Tracking Factor, determined quarterly, to reflect changes in the...

  7. Data:28f46846-fe31-4929-b9da-46fe9fb19b1e | Open Energy Information

    Open Energy Info (EERE)

    prior to January 1, 2008 in the former Duke Energy Carolinas Nantahala Area in Cherokee, Clay, Graham, Macon, Jackson and, Swain, counties. Existing Pole - 11.77 New pole -...

  8. Data:C33e447d-c5d5-4fca-a848-4fb22127d199 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Clay County Electric Coop Corp (Missouri) Effective date: End date if known: Rate name:...

  9. Data:D7c6cf5b-1e31-4b62-a00c-fb5126171f68 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Platte-Clay Electric Coop, Inc Effective date: 20130101 End date if known: Rate name: MC3 -...

  10. Data:5d43d429-2b6b-4528-9a14-9fb3627352c3 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Platte-Clay Electric Coop, Inc Effective date: 20130101 End date if known: Rate name: SL - 300...

  11. Data:F6fb720f-8469-4546-a22e-53b8e6fd9d92 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Clay County Electric Coop Corp (Missouri) Effective date: 20130101 End date if known:...

  12. Data:B290b061-4c94-4fb6-ac0f-e31b54be277b | Open Energy Information

    Open Energy Info (EERE)

    prior to January 1, 2008 in the former Duke Energy Carolinas Nantahala Area in Cherokee, Clay, Graham, Macon, Jackson and, Swain, counties. Existing Pole - 10.53 New pole - NA...

  13. Data:A8957398-1abb-4fd7-83b3-0db7f4a85fb2 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Clay County Electric Coop Corp (Missouri) Effective date: End date if known: Rate name:...

  14. Data:6fb9ee6d-a1b6-45f8-b914-da6884c29cb1 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Platte-Clay Electric Coop, Inc Effective date: 20130101 End date if known: Rate name: SL - 150...

  15. Data:6ecc1bc5-5ac5-4d32-a5b8-c87ba5cde0fb | Open Energy Information

    Open Energy Info (EERE)

    Approval of the Cooperative must be obtained prior to the installation of any motor having a rated capacity of five horsepower or more. Source or reference: http:...

  16. Data:0115b145-e9cb-4de7-b2a4-a3fb994175e8 | Open Energy Information

    Open Energy Info (EERE)

    capacity does not exceed 75 KVA and where the starting current of the largest motor does not exceed 260 amperes for all uses, and subject to the rules, regulations and...

  17. Data:4b8a5523-bbba-48df-a22a-fb48b1c37a25 | Open Energy Information

    Open Energy Info (EERE)

    *Monthly chage 0 as long as customer meets annual chage of 2,820.00 Max single-phase motor size -10hp Max three-phase motor size -200hp Source or reference: Ilinois State...

  18. Data:9ee239f4-43fb-448d-8b29-8cebd4b3d091 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Lexington, Tennessee (Utility Company) Effective date: 20120701 End date if known:...

  19. Data:4316da82-3f36-459e-9029-d70159b1fb75 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Princeton, Wisconsin (Utility Company) Effective date: 20060914 End date if known:...

  20. Data:E9de3c64-b09e-433c-bb53-47f82fb9ab07 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of River Falls, Wisconsin (Utility Company) Effective date: 20080411 End date if...

  1. Data:450c3051-11e1-451f-b931-4d45a4678ccf | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Princeton, Wisconsin (Utility Company) Effective date: 20060914 End date if known:...

  2. Data:31046076-4a88-43ce-b096-44c74ff5fb64 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Princeton, Wisconsin (Utility Company) Effective date: 20060914 End date if known:...

  3. Data:512a888f-a9fb-44af-b08a-5274d7222162 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Princeton, Wisconsin (Utility Company) Effective date: 20060914 End date if known:...

  4. Data:95fb8b41-baad-44a5-adcf-a7bc64f063ad | Open Energy Information

    Open Energy Info (EERE)

    may request OTEC to leave de-energized existing electrical facilities in place up to five years, excluding transformers, by paying 8.00 per billing period. Temporary re-connection...

  5. Data:Fe4b848d-7e6c-48f7-a6fb-1829e55b4817 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Blue Grass Energy Coop Corp Effective date: 20110601 End date if known: Rate name: 100...

  6. Data:Fb35f172-43df-448e-89dc-6f325c8f232b | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Nemaha-Marshall E C A, Inc Effective date: 20070515 End date if known: Rate name: Private...

  7. Data:5b943e77-c817-4ba9-aee3-dfd4bbbdd0fb | Open Energy Information

    Open Energy Info (EERE)

    Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Blue Earth, Minnesota (Utility Company) Effective date: 20140516 End date if known: Rate name:...

  8. Data:9257ab3c-b68c-4223-9f24-b803fb930852 | Open Energy Information

    Open Energy Info (EERE)

    Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Blue Earth, Minnesota (Utility Company) Effective date: 20140516 End date if known: Rate name:...

  9. Data:90b88357-aed9-419f-b14d-aa2111584b49 | Open Energy Information

    Open Energy Info (EERE)

    Effective date: 20100501 End date if known: Rate name: CommercialIndustrial With Water Heater Sector: Industrial Description: Source or reference: Rate Binder8 (Illinois...

  10. Data:022024da-b4c3-497f-83c9-185340736fb3 | Open Energy Information

    Open Energy Info (EERE)

    (Utility Company) Effective date: 20120101 End date if known: Rate name: COMMERCIAL WATER HEATER CREDIT Sector: Commercial Description: *Must meet criteria for credit. Source...

  11. Data:Ce18419d-c9a8-4262-9b0f-b19dfd989e19 | Open Energy Information

    Open Energy Info (EERE)

    0602 End date if known: Rate name: Rural Residential with approved 40 gallon electric water heater Sector: Residential Description: Source or reference: http:...

  12. Data:7f5485a1-4c26-431f-b7d0-439f843369fd | Open Energy Information

    Open Energy Info (EERE)

    Effective date: 20120501 End date if known: Rate name: Residential With Electric HeaterWater Heater Sector: Residential Description: Source or reference: Rate Binder8 (Illinois...

  13. Data:F778d669-a0c1-4113-8157-fb53b71b085a | Open Energy Information

    Open Energy Info (EERE)

    Energy Market Adjustment 0.003KWH (Added to All Above Energy Rates) Controlled Water Heater Credit .00736KWH Applies to the first 1,000 KWHs each month (October-March)...

  14. TECHNICAL PUBLICATIONS & BOOKS PRESENTED/PUBLISHED GOMES J.S. & ALVES, F.B. (2013): "The Universe of the Oil & Gas Industry From Exploration to Refining", 780

    E-Print Network [OSTI]

    Williams, John M.

    2013-01-01T23:59:59.000Z

    Universe of the Oil & Gas Industry ­ From Exploration to Refining", 780 pages University textbook published by PARTEX Oil & Gas, Lisbon, Portugal. ISBN 9789892037783. GOMES J.S. (2012): "New Technologies in the Oil and Gas Industry", edited by J.S. Gomes, published by INTECH open science (www

  15. Data:E7e3d0ae-0896-469f-b8d0-3bb49b792880 | Open Energy Information

    Open Energy Info (EERE)

    Available only to manufacturers whose Standard Industrial Classification (SIC) codes are between 2000 and 3999 who are exempt from the Connecticut Gross Earnings Tax....

  16. Data:3c4b0554-ceb7-4d2a-a4a1-9fb9bfd76073 | Open Energy Information

    Open Energy Info (EERE)

    shall also apply to security lights in a municipality that are billed under other rate codes (i.e., 20, 57, etc.). Source or reference: http:www.perennialpower.comImages...

  17. Data:6741b13a-3e06-4e8f-b197-82b8d076569d | Open Energy Information

    Open Energy Info (EERE)

    renew until otherwise canceled. Source or reference: http:www.cityofperryok.comFilesCodesCityCode101211.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW):...

  18. Data:4ea9b891-fb98-4604-bc44-c1d3cc3f739e | Open Energy Information

    Open Energy Info (EERE)

    User: over 100,000 KWH monthly Source or reference: http:www.cityofperryok.comFilesCodesCityCode101211.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW):...

  19. Data:3fb74f03-38fc-45b6-8605-9173ad1ddd8b | Open Energy Information

    Open Energy Info (EERE)

    shall also apply to security lights in a municipality that are billed under other rate codes (i.e., 20, 57, etc.). Source or reference: http:www.perennialpower.comImages...

  20. Data:20dbac30-ce96-43e6-a1fb-a9195d99d78e | Open Energy Information

    Open Energy Info (EERE)

    Source or reference: http:precorp.coopwp-contentuploads2014012014-01-10-Rate-Tariffs.pdf Source Parent: http:precorp.coop Comments Applicability Demand (kW) Minimum...

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

    Open Energy Info (EERE)

    LLC Effective date: 20050928 End date if known: Rate name: 2 GS - TOD general service time of use (secondary voltage) Sector: Commercial Description: This rate is applicable on...

  2. Data:52fb1be4-f0b3-40fc-9305-4fdba28f1bef | Open Energy Information

    Open Energy Info (EERE)

    https:www.firstenergycorp.comcontentdamcustomerCustomer%20ChoiceFilesOhiotariffsOE-2012-Electric-Service.pdf Source Parent: Comments Applicability Demand (kW)...

  3. Data:B8a7f039-d881-4033-9f94-ac3d7fb04bbd | Open Energy Information

    Open Energy Info (EERE)

    http:rollinghills.coopwebbuilder.comsitesrollinghills.coopwebbuilder.comfilesratetariffs.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):...

  4. Data:D97fb563-feb6-4f10-ba64-8ae4207cfab0 | Open Energy Information

    Open Energy Info (EERE)

    LLC Effective date: 20050928 End date if known: Rate name: 2 GS - TOD general service time of use (primary voltage) Sector: Commercial Description: This rate is applicable on a...

  5. Data:E70650df-5370-41fb-a364-699a373e3c1c | Open Energy Information

    Open Energy Info (EERE)

    to the Power Cost Adjustment Clause. Source or reference: http:psc.wi.govapps40tariffsviewfile.aspx?typeelectric&id6490 Source Parent: Comments Applicability Demand...

  6. Data:Cf4df18d-588e-46e5-82ad-31a59ea826fb | Open Energy Information

    Open Energy Info (EERE)

    Power Cost Adjustment varies monthly. Source or reference: http:psc.wi.govapps40tariffsviewfile.aspx?typeelectric&id580 Source Parent: Comments Applicability Demand...

  7. Data:4a88561f-b1cf-4dc7-baec-9272b2d731c8 | Open Energy Information

    Open Energy Info (EERE)

    http:rollinghills.coopwebbuilder.comsitesrollinghills.coopwebbuilder.comfilesratetariffs.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):...

  8. Data:5d9d24ff-e250-409a-8757-66fb959a8b19 | Open Energy Information

    Open Energy Info (EERE)

    of: the "Weighted Average Index Price" reflected by the Intercontinental Exchange (ICE) Daily Power Indices for theMid C at peak and off-peak for the month or the largest...

  9. Data:2fb3516c-6c44-4e7a-83ac-c0cb4040d427 | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Loup River Public Power Dist Effective date: 20130115 End date if known: Rate name: Interrupible...

  10. Data:4fb3e2c7-0073-49aa-9499-16230c72e86b | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Perennial Public Power Dist Effective date: 20130101 End date if known: Rate name: IRRIGATION Three Days...

  11. Data:590f419e-bd51-415f-b856-ed5b8f985bef | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Southwest Public Power Dist Effective date: 20130101 End date if known: Rate name: Irrigation: Two-Day...

  12. Data:Eb6d71dc-0939-4c0f-b83d-2f6a247e0bed | Open Energy Information

    Open Energy Info (EERE)

    his service only during the time that the system is experiencing a peak condition. Power will be restored when the peak condition normalizes. Participation in the program is...

  13. Data:Eb1d6c89-9e0d-4025-a68f-b84bbedb81d3 | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Southwest Public Power Dist Effective date: 20130101 End date if known: Rate name: Irrigation: Daily...

  14. Data:1e0e4fb0-5edd-4bcd-99eb-9bee0007052f | Open Energy Information

    Open Energy Info (EERE)

    it is not feasible andor practical to install metered security lighting. New or replacement light installations shall be limited to high pressure sodium lights. Source or...

  15. Data:C5fb4943-64b9-4054-abd3-85968efe96ae | Open Energy Information

    Open Energy Info (EERE)

    done at customer's premises. An additional charge for any costs of repairs andor replacement of damaged facilities, installing protective facilities, and the estimated amount...

  16. Data:85cfbd33-bef5-4bdc-b995-d9fd9fb85e4d | Open Energy Information

    Open Energy Info (EERE)

    schedule is available for metered outdoor lighting service to any Customer. New or replacement light installations shall be limited to high pressure sodium and metal-halide...

  17. Data:Fb6bfa25-64ae-4c87-b424-90fc4e710d89 | Open Energy Information

    Open Energy Info (EERE)

    Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V):...

  18. Data:Bc6ba6cc-57fb-4d29-9412-60fa6b0e3949 | Open Energy Information

    Open Energy Info (EERE)

    who contracts with the Cooperative for a block or blocks of electricity produced from renewable resources provided through the NC GreenPower program. The maximum number of...

  19. Data:35a044a3-0f6b-43fb-85d9-9fedd355d3b9 | Open Energy Information

    Open Energy Info (EERE)

    opposed to a standard meter, other than service rendered under CMLP Electric Thermal Storage Rates or Controlled Domestic Water Heating Rates, will incur an additional charge...

  20. Data:829f535d-4378-468f-b5f9-c767185bde0f | Open Energy Information

    Open Energy Info (EERE)

    0.028 per KWH. Next 140 KWH per KVA @ 0.024 per KWH. Over 470 KWH per KVA @ 0.021 per KWH. Power Cost Adjustment: 0.0001 Primary Meter Discount: 0.40 per KVA. Source or...

  1. Data:9cd27a40-efa6-4d2f-b086-688eaddfca75 | Open Energy Information

    Open Energy Info (EERE)

    purchased power expense is increased or decreased above or below the base purchased power cost of 0.078510kWh sold, flow through to the users such increases or decreases, in...

  2. Data:5f97368e-9814-4f0c-9bcb-c9f7fb6e0b23 | Open Energy Information

    Open Energy Info (EERE)

    0.035 per KWH. Next 140 KWH per KVA @ 0.029 per KWH. Over 470 KWH per KVA @ 0.023 per KWH. Power Cost Adjustment: 0.0001 Source or reference: Rate Binder Kelly 11 ISU...

  3. Data:2ef5d159-8cb2-457f-b444-3d69b4204b10 | Open Energy Information

    Open Energy Info (EERE)

    Governed in more detail by Standard Rules and Regulations of the City. Subject to Power Cost Adjustment, kWh Tax, and Community Tax Credit. Power Cost Adjustment varies month to...

  4. Data:145a51d9-70fb-4b6b-aeec-4e16a012bccf | Open Energy Information

    Open Energy Info (EERE)

    lighting. The utility will furnish, install, and maintain street lighting. The Purchase Cost Adjustment Clause, a charge per all kWh that varies monthly, applies to this rate....

  5. ENERGY ECONOMY CII5fB 81 (R3) (L2) (M2) UDC 728.3 (489) Low-energy houses

    E-Print Network [OSTI]

    a new-type structural element, and to ensure airtightness. Test results of infiltration air change rates range from 0.02 to 0.12 ach, while other tests show less than 15 per cent difference between calculated became prevalent, often with a brick facing, and internal surfaces were panelled. There followed the use

  6. Data:42f0b911-8717-4fb5-a594-82953a8f2ee1 | Open Energy Information

    Open Energy Info (EERE)

    Nonwood Sector: Lighting Description: To all night street lighting service (dusk to daylight) from the overhead systems conforming to the District's standard specifications....

  7. Data:2d46371a-e450-486e-92fb-63b4d2e676ba | Open Energy Information

    Open Energy Info (EERE)

    Sector: Lighting Description: 157 To all night street lighting service (dusk to daylight) from the overhead systems conforming to the District's standard specifications....

  8. Data:389be289-ff10-4a2e-869c-c9487fb1686d | Open Energy Information

    Open Energy Info (EERE)

    customer shall be billed monthly on a net energy basis and shall pay the fixed charge and energy charge specified in the rate schedule under which he is served. If, in any month,...

  9. Data:5cace0ad-0573-4b0f-8fb8-71496494fc5b | Open Energy Information

    Open Energy Info (EERE)

    City Power & Light Co Effective date: 20130101 End date if known: Rate name: Large General Service Space Heating <1000kW Secondary Sector: Description: AVAILABILITY: For...

  10. Data:75aae5fb-c797-4add-b31e-e74010ca4f9d | Open Energy Information

    Open Energy Info (EERE)

    Effective date: 20130701 End date if known: Rate name: Rate 27 - Small Time-Of-Day General Electric Service (Bundled Service Primary Discount Facilities Ownership) Sector:...

  11. Data:4aef1fb6-f088-4162-b0ed-ded8e2596267 | Open Energy Information

    Open Energy Info (EERE)

    W Sector: Lighting Description: RULES AND REGULATIONS: Terms and conditions of this electric rate schedule and the General Rules and Regulations govern use of this service....

  12. Data:912c1872-6fb5-4a25-ab48-fe016d0f6a45 | Open Energy Information

    Open Energy Info (EERE)

    Central Electric Coop Inc Effective date: 20111001 End date if known: Rate name: General Service Rate Shedule B(Three Phase 16-50 KW) Sector: Commercial Description:...

  13. Data:97f7d61d-39c3-4c2e-9e52-85591fb07a1c | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: El Paso Electric Co (New Mexico) Effective date: 20140501 End date if known: Rate name: General Service...

  14. Data:8c9d57ad-eaac-4fb3-8da2-fdab7f4d493f | Open Energy Information

    Open Energy Info (EERE)

    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...

  15. Data:9fb9b87b-58b1-4912-bf96-c9dc6f6562f8 | Open Energy Information

    Open Energy Info (EERE)

    12-bf96-c9dc6f6562f8 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...

  16. Data:16337ee5-241c-435d-8a06-04cff7fb9a92 | Open Energy Information

    Open Energy Info (EERE)

    >> Basic Information Utility name: Cuming County Public Pwr Dist Effective date: 20111214 End date if known: Rate name: Security Lighting Unmetered Lights 100W HPS Sector:...

  17. Data:9944f743-0abb-4c16-9fb2-4fe2571bab84 | Open Energy Information

    Open Energy Info (EERE)

    Information Utility name: Singing River Elec Pwr Assn (Mississippi) Effective date: 20091204 End date if known: Rate name: Industrial Service (750 kW - 2499 kW) Primary Voltage...

  18. Data:9be3db16-e125-45ae-afef-ff8fb999dd27 | Open Energy Information

    Open Energy Info (EERE)

    For these purposes, the "Cost of Production" shall mean the cost of fuel and purchased power, less all payments received by the Austin Utilities as reimbursement for power plant...

  19. Data:3a66dc95-9503-42b6-83b8-7d5a75fb6694 | Open Energy Information

    Open Energy Info (EERE)

    name: PUD No 2 of Grant County Effective date: 20020101 End date if known: Rate name: ALTERNATIVE ENERGY RESOURCES RATE SCHEDULE 13 Sector: Commercial Description: AVAILABLE:...

  20. Data:90ca7196-1455-4069-a5fb-7d65b9f6d3fd | Open Energy Information

    Open Energy Info (EERE)

    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...

  1. Data:43aa7c84-72b4-4d6f-b27f-42a47447c826 | Open Energy Information

    Open Energy Info (EERE)

    matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Bristol Virginia...

  2. Data:872d7b3b-28ab-4046-9d63-4a2794e6fb03 | Open Energy Information

    Open Energy Info (EERE)

    space heating purposes, or for a combination space heating and cooling installation (heat pump). All other electric usage by the customer must be separately metered and billed...

  3. Data:0b0b963f-b6b0-41b4-b1b7-aab331be5afc | Open Energy Information

    Open Energy Info (EERE)

    date: 20090801 End date if known: Rate name: Residential:SINGLE PHASE EARTH(COUPLED HEAT PUMP SERVICE EXPERIMENTAL) Sector: Residential Description: This rate is applicable to...

  4. Data:2cac15b8-fb54-4701-8a31-18a7f4543add | Open Energy Information

    Open Energy Info (EERE)

    application to Company for service under this Rider, 3. Has applied for and received economic development assistance from State or local government or other public agency, 4....

  5. Data:C915ea5f-b581-42ae-abc9-a85634ae0b63 | Open Energy Information

    Open Energy Info (EERE)

    1-42ae-abc9-a85634ae0b63 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...

  6. Data:547fb553-585c-48e3-80ad-9dd9a42e1f13 | Open Energy Information

    Open Energy Info (EERE)

    ad-9dd9a42e1f13 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...

  7. Data:0695a8d3-4547-45fb-836a-4c9250b827ca | Open Energy Information

    Open Energy Info (EERE)

    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...

  8. Data:07595612-c315-4c8a-a671-9f77f7e0a4fb | Open Energy Information

    Open Energy Info (EERE)

    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...

  9. Data:80360d01-3f4d-418f-b6ff-9ee26559094f | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Rural Elec Coop Inc Effective date: End date if known: Rate name: 3 Phase...

  10. Data:2d57e112-efb2-4b70-bc8b-8fda9ae547fb | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp Effective date: 20081001 End date if known: Rate name:...

  11. Data:1f06c3a9-fb2c-4234-a83b-c527755c7472 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp Effective date: 20120101 End date if known: Rate name:...

  12. Data:B898c570-c83d-4d10-891e-6c9fb3ac7f72 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp Effective date: 20081001 End date if known: Rate name: Pole...

  13. Data:3e993494-ff87-4728-b8a9-e8fb7dedf5d3 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp (Tennessee) Effective date: 20140601 End date if known: Rate...

  14. Data:Fb7e7aa0-94fe-45dd-a02d-201fc2ee4bd0 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp (Tennessee) Effective date: 20140601 End date if known: Rate...

  15. Data:26a0fca6-c8b2-43fb-995b-493e85981551 | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Indiana Michigan Power Co (Michigan) Effective date: 20130101 End date if known: Rate name: ECLS -...

  16. Data:437aab84-009f-4fb1-b666-ed5d43c9089f | Open Energy Information

    Open Energy Info (EERE)

    system. APPLICABLE: To firm point-to-point transmission service customers for which power and energy are supplied to the CRSP transmission system at points of interconnection...

  17. Data:C7e6667f-b670-45cf-9eb8-2cb4359e90e3 | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Indiana Michigan Power Co (Michigan) Effective date: 20130101 End date if known: Rate name: ECLS -...

  18. Data:4cf65e73-3ea7-4dff-a563-a52fb0797cbb | Open Energy Information

    Open Energy Info (EERE)

    rate is applicable for service that is supplied through new or rebuilt streetlight systems, including extension of streetlighting systems to additional locations where service...

  19. Data:6d6c822b-888c-423f-b8dc-11514e922c4d | Open Energy Information

    Open Energy Info (EERE)

    Parallel Generation (20 kW or less)- Net Energy Billing Customer-Owned Generation Systems (Greater than 20 kW) Source or reference: http:psc.wi.govapps40tariffs...

  20. Data:5fb276c4-1eb0-46bb-a17a-e2468acd697a | Open Energy Information

    Open Energy Info (EERE)

    rate is applicable for service that is supplied through new or rebuilt streetlight systems, including extension of streetlighting systems to additional locations where service...

  1. Data:55d52ef3-963f-45ad-9f06-c5a900c30fb1 | Open Energy Information

    Open Energy Info (EERE)

    buildings and lighting, sewage treatment facilities, grain elevators and see processors, commercial office buildings, lounges or night clubs, telephone microwave tower, pipeline...

  2. Data:Fb434813-28eb-44a4-ae2e-7b95e553e6e1 | Open Energy Information

    Open Energy Info (EERE)

    Parent: Comments If Company furnishes overhead or underground service to metal or concrete poles in residential subdivision, Customer pays a monthly charge of 1.94 or 3.93...

  3. Data:C7a0d59f-6269-4eb0-90f1-f79fb82efeab | Open Energy Information

    Open Energy Info (EERE)

    Parent: Comments If Company furnishes overhead or underground service to metal or concrete poles in residential subdivision, Customer pays a monthly charge of 1.94 or 3.93...

  4. Data:F5a39f92-e3fa-4974-b6d5-aed9fb6c14ac | Open Energy Information

    Open Energy Info (EERE)

    wood-street lighting standards. Those in subdivisions containing aluminum or concrete standards where the Company has received a contribution from developer or others...

  5. Data:61536f7d-df93-4115-8e79-156fb2e477c7 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc (New Mexico) Effective date: 20120901 End date if known: Rate name: 175 Watt MVL 75 kWh Street...

  6. Data:Fb788c4f-e589-4af0-aeab-8191994f64e7 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc (New Mexico) Effective date: 20120901 End date if known: Rate name: 100 Watt HPS 34 kWh Street...

  7. Data:A5464299-4fb1-49a6-86be-7b6c05c69f57 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Farmers' Electric Coop, Inc (New Mexico) Effective date: 20120501 End date if known: Rate name: Security Light Pole Only...

  8. Data:Ad4911fb-1ccb-4f96-921b-200c770e1d41 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc (New Mexico) Effective date: 20120801 End date if known: Rate name: Commercial and Industrial...

  9. Data:Cd3537d3-fd76-4fa7-9f3f-75d06fb2b0ba | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Tri-County Electric Coop, Inc (New Mexico) Effective date: 20131101 End date if known: Rate name: Industrial Service Rate 45...

  10. Data:Da10b869-2522-4b0f-b7b6-3127ac40ac6b | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Southwestern Electric Coop Inc (New Mexico) Effective date: 20070701 End date if known: Rate name: Commercial Lighting Service...

  11. Data:50bf8666-897e-420e-9296-bc0fb74c7ce2 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc (New Mexico) Effective date: 20120801 End date if known: Rate name: 250 Watt MVL 110 kWh...

  12. Data:95751d3f-b2bb-46c0-9950-b52b07b2d04d | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Tri-County Electric Coop, Inc (New Mexico) Effective date: 20131101 End date if known: Rate name: Public Street Lighting MV...

  13. Data:E5213578-0993-4bca-aaee-c3cfe1fb9d18 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc (New Mexico) Effective date: 20140109 End date if known: Rate name: Residential, Schools,...

  14. Data:B00670fb-e78f-4021-a814-a490e4d1677c | Open Energy Information

    Open Energy Info (EERE)

    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...

  15. Data:5220c34b-4017-4ef2-b1fb-c8a6b8d2cd4f | Open Energy Information

    Open Energy Info (EERE)

    subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Idaho Power Co...

  16. Data:6a188798-a8fb-47e2-a28c-b02d550e3f84 | Open Energy Information

    Open Energy Info (EERE)

    subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Oklahoma...

  17. Data:2f31aa69-c39e-462f-92fb-3b5c7475b93c | Open Energy Information

    Open Energy Info (EERE)

    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...

  18. Data:Ccda57a8-1a6c-455f-b4ca-cc019f0839dd | Open Energy Information

    Open Energy Info (EERE)

    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...

  19. Data:041ac1bb-63e3-40cf-a7f6-95aaa3fb3da1 | Open Energy Information

    Open Energy Info (EERE)

    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...

  20. Data:58d87638-1c49-486d-9f7f-b4fe230db159 | Open Energy Information

    Open Energy Info (EERE)

    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...

  1. Data:C2bfb777-23fe-43fb-817e-539a9942c888 | Open Energy Information

    Open Energy Info (EERE)

    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...

  2. Data:164c9b78-0248-4e1a-8760-fb9847e7671a | Open Energy Information

    Open Energy Info (EERE)

    the availability of replacement parts Source or reference: http:www.cmpco.comYourHomepricingpricingSchedulesdefault.html Source Parent: Comments Applicability Demand (kW)...

  3. Data:28c567a3-08e4-4fb3-806b-c40003a76e0c | Open Energy Information

    Open Energy Info (EERE)

    if known: Rate name: GSB Sector: Industrial Description: *Excessive over contract demand results in a charge of 16.45kw Source or reference: ISU Documentation Source Parent:...

  4. Data:99f9130f-d339-48c5-8078-430fb4e3041c | Open Energy Information

    Open Energy Info (EERE)

    or governmental authority where 120-volt service exists. The cost of service provides for electricity only from existing Northeastern REMC (Northeastern) facilities. Any investment...

  5. Data:155c5dea-18da-4430-b224-2c01c4b70fb9 | Open Energy Information

    Open Energy Info (EERE)

    be as stated in the applicable rate tariff. Under this rider, only the kWh charge for electricity delivered by the Customer is affected. The Customer will pay for all kWh...

  6. Data:Fb7f0ea2-ae62-4a86-b59e-aeebdae3b551 | Open Energy Information

    Open Energy Info (EERE)

    (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...

  7. Data:3d46b2e1-fb0b-4c8d-a648-29fcad737e34 | Open Energy Information

    Open Energy Info (EERE)

    be as stated in the applicable rate tariff. Under this rider, only the kWh charge for electricity delivered by the Customer is affected. The Customer will pay for all kWh...

  8. Data:De1fb01f-d309-4e20-9694-97ded226814c | Open Energy Information

    Open Energy Info (EERE)

    will be determined by the Company. Where the Company deems it impractical to deliver electricity through one service, or where more than one meter has been installed for...

  9. Data:4539f4fd-2323-47e1-8beb-f4fb6df76d58 | Open Energy Information

    Open Energy Info (EERE)

    This schedule is available to separately metered and billed supply of alternating current electricity to any customer including a residential farm where the farm uses are not taken...

  10. Data:A442b48a-53fb-459d-8234-7a0d70af1dd6 | Open Energy Information

    Open Energy Info (EERE)

    net metering energy resource) Company shall measure the difference between the amount of electricity delivered by Company to Customer and the amount of electricity generated by...

  11. Data:1a7c1076-47ed-41c8-8fb4-3b06a99292ff | Open Energy Information

    Open Energy Info (EERE)

    available to new applicants after February 1, 2011. This rate is applicable to the use of electricity for water heating of any customer other than residential, except as noted...

  12. Data:1bd7fbd9-a0f4-457d-8ae7-0fcff075fb06 | Open Energy Information

    Open Energy Info (EERE)

    when all of Customer's service at one location is measured by one meter, and when electricity is used for space andor water heating. Source or reference: http:...

  13. Data:131d3b34-f521-4735-839f-1e0bc97fb1a9 | Open Energy Information

    Open Energy Info (EERE)

    voltage is available, the customer desires to furnish, install and maintain transformers and protective devices, a 2.5% discount will be allowed. All metering will be on...

  14. Data:73d34bb4-9b67-4ede-89da-e7fa254991fb | Open Energy Information

    Open Energy Info (EERE)

    metered services and Part B-23 is primary metered customers who own their own transformers and distribution service facilities and have a peak demand less than 800 KW. Part...

  15. Data:7361fb39-0c07-4e3d-95c3-9e4fbdb40fe9 | Open Energy Information

    Open Energy Info (EERE)

    adjustment. 1% reduction of total charge when metering is at primary voltage and transformers are owned by the City. Source or reference: http:www.cityofwayne.org...

  16. Data:A5b2284c-bb1a-4075-8aa3-7fb21d137e67 | Open Energy Information

    Open Energy Info (EERE)

    discount: Transformer Ownership Discount: Customers who own and maintain their own transformers or substations shall be given a credit of 0.25 per kW of distribution demand....

  17. Data:239dd8c3-2660-4fb5-a10f-200895eb226c | Open Energy Information

    Open Energy Info (EERE)

    ( 250W HPS - Shoebox ) Sector: Lighting Description: Additional fees for poles and transformers may apply Source or reference: ISU Documentation Source Parent: Comments Applicable...

  18. Data:5683ff7b-a387-45ac-b1e2-bf50b83fb3f9 | Open Energy Information

    Open Energy Info (EERE)

    is responsible for procuring, installing and maintaining all necessary wiring, transformers, switches, cut-outs and protection equipment beyond the point of delivery, with...

  19. Data:825019fb-1c94-43f8-8983-e99a01c5af6b | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Aspen, Colorado (Utility Company) Effective date: 20140101 End date if known: 20141231...

  20. Data:2ae66fb5-8162-47d9-b060-4c8b873ebfd6 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Aspen, Colorado (Utility Company) Effective date: 20140101 End date if known: 20141231...

  1. Search for resonant WZ to lvll production using 13 fb^{-1} in \\sqrt{s} = 8 TeV p-p collisions with the ATLAS detector

    E-Print Network [OSTI]

    Loscutoff, Peter Vladimir

    2013-01-01T23:59:59.000Z

    W ? ZZ WZ Rho600 m WZ T , eem [GeV] Events / 20 GeV Events /REGIONS WZ Invariant Mass (GeV) eem channel Entries/40 GeV

  2. Data:Ebcca88e-15be-40fb-af98-7dedc915d3db | Open Energy Information

    Open Energy Info (EERE)

    Public Service Co of NM Effective date: 20130301 End date if known: Rate name: 12 Cogeneration and Small Power Production Secondary Distribution (1A, 1B, 2A, 2B, 3B, 3C, 10A, &...

  3. Data:E229fb12-27d3-47a4-8a10-277f2f939016 | Open Energy Information

    Open Energy Info (EERE)

    matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Alabama Power Co...

  4. Data:638bc389-fb01-4b31-96a5-0c12a8e0261b | Open Energy Information

    Open Energy Info (EERE)

    Sector: Commercial Description: Optional for non-Domestic Service where consumption of energy exceeds 3,500 kWh in any one month, where the Billing Demand is equal to or less...

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

    Open Energy Info (EERE)

    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...

  6. Updated Combination of Searches for the Standard Model Higgs Boson at the D0 Experiment in 9.7 fb-1 of Data

    E-Print Network [OSTI]

    D0 Collaboration

    2012-07-02T23:59:59.000Z

    Searches for standard model Higgs boson production at the D0 experiment in ppbar collisions at sqrt(s)=1.96 TeV are carried out for Higgs boson masses (m_H) in the range 100Higgs boson. In absence of a significant excess above the background expectation, 95% confidence level upper limits are set on the production cross section for a standard model Higgs boson. The upper limits are found to be a factor of 2.11 (0.73) times the predicted standard model cross section for m_H=115 (165) GeV. Under the background-only hypothesis, the corresponding expected limit is 1.46 (0.72) times the standard model prediction. At the same confidence level, these analyses exclude a standard model Higgs boson with a mass in the range 159

  7. Data:0ac74409-f2ac-4fb5-89ca-2b93352f3c66 | Open Energy Information

    Open Energy Info (EERE)

    date: 20110315 End date if known: Rate name: MU-1 - a1b - 1000 watt MV Sector: Lighting Description: Lamps in enclosed fixtures, mounted on metal or fiberglass columns and...

  8. Data:B0993536-b649-466f-b2b7-92bd7d6d30f2 | Open Energy Information

    Open Energy Info (EERE)

    Company) Effective date: 20130701 End date if known: Rate name: Public Street Lighting Service - HPSV Pendant Lamp Fixtures - Ornamental Pole - Residential Sector: Lighting...

  9. Search for the standard model Higgs boson in associated $WH$ production in 9.7 fb$^{-1}$ of $p\\bar{p}$ collisions with the D0 detector

    E-Print Network [OSTI]

    The D0 Collaboration

    2012-09-21T23:59:59.000Z

    We present a search for the standard model Higgs boson in final states with a charged lepton (electron or muon), missing transverse energy, and two or three jets, at least one of which is identified as a $b$-quark jet. The search is primarily sensitive to $WH\\to\\ell\

  10. Type B Accident Investigation Board Report on the September 1, 1999, Plutonium Intakes at the Savannah River Site FB-Line

    Broader source: Energy.gov [DOE]

    This report is an independent product of the Type B Accident Investigation Board appointed by Greg Rudy, Manager, Savannah River Operations Office, U.S. Department of Energy.

  11. Data:F358e502-527d-49b0-b8e7-16ce8282b8fb | Open Energy Information

    Open Energy Info (EERE)

    a renewable or recurring basis, including dedicated energy crops, trees grown for energy production, wood waste and wood residues, plants (including aquatic plants, grasses, and...

  12. Data:53e191c2-04fb-4239-afd6-5e473bfeb11b | Open Energy Information

    Open Energy Info (EERE)

    are Eugene Code 9.6725 and all EWEB policies and procedures pertaining to light pollution, light trespass and glare. Source or reference: http:www.eweb.orgpublic...

  13. Data:A19a75cf-fea0-40fb-a873-890c6266b47a | Open Energy Information

    Open Energy Info (EERE)

    in all territory served by the Corporation to members who have Automated Metering Infrastructure (AMI), as a voluntary alternative to the Corporation's Schedule CS-14, subject to...

  14. Data:E5fb6d06-ca48-45c5-848c-8bfb3d23560d | Open Energy Information

    Open Energy Info (EERE)

    than 100KW and less than 1000KW as defined in the billing demand section of this tariff. 2. In the event that billing demand becomes permanently less than 100kW, the customer...

  15. Data:1e969327-8244-4db7-9c77-1fb5b2244bed | Open Energy Information

    Open Energy Info (EERE)

    greater than 30 KWs as defined in the determination of billing demand section of this tariff. 2. Average monthly energy consumption is equal to greater than 3,000KW based on the...

  16. Data:D80d58fb-40a7-49a9-9c18-62365ea596fd | Open Energy Information

    Open Energy Info (EERE)

    streets. Source or reference: https:www.burlingtonelectric.comELBOassetsTariff%20Sheets%20June%20262009%20revised-1.pdf Source Parent: Comments Applicability Demand...

  17. Data:F6fb5948-6080-45da-b55e-73808fcbb36d | Open Energy Information

    Open Energy Info (EERE)

    Commercial Description: Source or reference: http:www.pioneerelectric.coopdocumentstariff-schedules.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum...

  18. Data:45c71c2d-8c26-40fb-a7e0-fab503a49d1f | Open Energy Information

    Open Energy Info (EERE)

    Stillwater Utilities Authority Effective date: 20120101 End date if known: Rate name: ELECTRIC RATE GENERAL SERVICE Sector: Commercial Description: Production Cost Adjustment...

  19. Data:1fb310f8-db83-498b-b923-d5e0deaa9e09 | Open Energy Information

    Open Energy Info (EERE)

    Sector: Lighting Description: Source or reference: http:www.btes.netindex.phpelectricgeneral-electric-rates-oldlighting-service-rate-schedule Source Parent: Comments...

  20. Data:952ca314-1f91-4bf0-b704-e80630412fb4 | Open Energy Information

    Open Energy Info (EERE)

    entire requirements are taken through a single meter, for all uses excluding crop drying or irrigation. Demand Charge Purchased Power + Distribution Delivery Source or...

  1. Data:Aec094ea-a721-479f-b343-67fe5f637d52 | Open Energy Information

    Open Energy Info (EERE)

    entire requirements are taken through a single meter, for all uses excluding crop drying or irrigation. Demand Charge Purchased Power + Distribution Delivery Source or...

  2. Data:Da05fb7c-7f74-45c0-b1d2-dce609ef66f2 | Open Energy Information

    Open Energy Info (EERE)

    Valley Elec Coop Inc Effective date: End date if known: Rate name: Controlled Grain Drying - Off Season - Subject to Moderate Periods of Control Sector: Residential Description:...

  3. Data:97c39de8-7a02-4cbc-88fb-99fdd5889042 | Open Energy Information

    Open Energy Info (EERE)

    by the U. S. Army Corps of Engineers (Corps) as a precaution to prevent failure of the dams, Southeastern is not able to provide peaking capacity to these customers. Southeastern...

  4. Data:572eb4a7-39fb-45e6-98fd-7544a0fea433 | Open Energy Information

    Open Energy Info (EERE)

    20120101 End date if known: Rate name: RATE SCHEDULE NO. 99 LOAD FORECAST ADJUSTMENT Sector: Description: APPLICABILITY: All customers billed on rate schedules 14, 15, 16, and 85...

  5. Data:7146d5fb-ec7c-48ac-98a8-118f52ea32e2 | Open Energy Information

    Open Energy Info (EERE)

    charge calculated as follows: forecast capacity rate (1.87) + reactive supply (0.046) + regulation and frequency response (0.1897) Energy charge calculated as follows: forecast...

  6. Data:8c31dba9-331f-4d72-8d9b-7d63193fb4e8 | Open Energy Information

    Open Energy Info (EERE)

    B3PI Sector: Commercial Description: Note: 10.00 added to Fixed monthly charge if Remote Read Device is used. Source or reference: Rates Binder 1, Illinois State University...

  7. Data:3aca5136-67e4-4fb6-a05f-3cb32d2e6ccc | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Village of L'Anse, Michigan (Utility Company) Effective date: 20120201 End date if known: Rate name:...

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

    Open Energy Info (EERE)

    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...

  9. Data:16cc1788-21d0-4a0b-8df1-4c91f66fb14a | Open Energy Information

    Open Energy Info (EERE)

    base cost of power (U) is 0.0720 per kilowatt-hour. Parallel Generation (20 kW or less) Net Energy Billing - Available for single-phase and three-phase customers where a part or...

  10. Data:434682d3-1caf-49df-b1fb-06e5d91edec8 | Open Energy Information

    Open Energy Info (EERE)

    base cost of power (U) is 0.0785 per kilowatt-hour. Parallel Generation (20 kW or less) Net Energy Billing - Available for single-phase and three-phase customers where a part or...

  11. Data:4ce60f48-c2ac-449f-b745-9ab1009e8428 | Open Energy Information

    Open Energy Info (EERE)

    9am-9pm 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...

  12. Data:A1729943-9fb7-4246-9d3a-3e3e44e13410 | Open Energy Information

    Open Energy Info (EERE)

    To uses of electrical power on a continuous basis for seasonal agricultural irrigation pumping or agricultural drainage pumping. C. Character of Service: Sixty (60) hertz...

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

    Open Energy Info (EERE)

    terminates, whichever occurs first. Fiberglass Pole Embededded Fixed Monthly Charge Steel Pole Foundation 39.89 Source or reference: http:www.duke-energy.compdfs...

  14. Data:773b7e72-2a29-4a09-b350-1d646e1824fb | Open Energy Information

    Open Energy Info (EERE)

    terminates, whichever occurs first. Fiberglass Pole Embededded Fixed Monthly Charge Steel Pole Foundation 39.26 Source or reference: http:www.duke-energy.compdfs...

  15. Data:Ca94fb47-d744-4b08-b999-6d27c8a05f7e | Open Energy Information

    Open Energy Info (EERE)

    250.00 16' Fiberglass (Black) 300.00 16' Fiberglass (Acorn, Black) 800.00 30' Steel & Sub Base 1325.00 30' Fiberglass with 6' Arm 625.00 30' Fiberglass with 2 - 6' Arm...

  16. Data:0e36e05e-8105-494f-b13f-a5fd48da93d6 | Open Energy Information

    Open Energy Info (EERE)

    250.00 16' Fiberglass (Black) 300.00 16' Fiberglass (Acorn, Black) 800.00 30' Steel & Sub Base 1325.00 30' Fiberglass with 6' Arm 625.00 30' Fiberglass with 2 - 6' Arm...

  17. Data:1cf1eec6-fb89-4f31-9cb0-aa3fae5bce04 | Open Energy Information

    Open Energy Info (EERE)

    250.00 16' Fiberglass (Black) 300.00 16' Fiberglass (Acorn, Black) 800.00 30' Steel & Sub Base 1325.00 30' Fiberglass with 6' Arm 625.00 30' Fiberglass with 2 - 6' Arm...

  18. Data:857c5962-cd32-43e6-b129-4d55e7fb4fcf | Open Energy Information

    Open Energy Info (EERE)

    date: 20130301 End date if known: Rate name: MVS - Closed Offerings - 400 Watt MV Steel Pole Sector: Lighting Description: Source or reference: https:www.swepco.com Source...

  19. Data:8e8569fb-812d-488a-85d7-010fac6de443 | Open Energy Information

    Open Energy Info (EERE)

    2.78 Standard Wood Pole with an Underground Feed, 30-35 feet: 4.24 Direct Burial Steel with an Underground Feed, 30 feet: 4.99 Source or reference: http:...

  20. Data:Fb56ea53-1506-48f1-a795-62ec14804dad | Open Energy Information

    Open Energy Info (EERE)

    250.00 16' Fiberglass (Black) 300.00 16' Fiberglass (Acorn, Black) 800.00 30' Steel & Sub Base 1325.00 30' Fiberglass with 6' Arm 625.00 30' Fiberglass with 2 - 6' Arm...

  1. Data:F3217065-46b0-4e77-b2cb-d45fa34046fb | Open Energy Information

    Open Energy Info (EERE)

    until their contract expires or this rate schedule terminates, whichever occurs first. Steel Pole Fixed Monthly Charge SteelAluminum Pole 42.61 Wood Pole 29.89 Additional...

  2. Data:52c1785f-1cda-4fb8-a8ac-98e3112e9493 | Open Energy Information

    Open Energy Info (EERE)

    date: End date if known: Rate name: Street Lighting ornamental, 400w mv, 30 ft steel pole Sector: Lighting Description: street lighting,ornamental mercury vapor 400 watt...

  3. Data:D3938799-e61a-4550-aaca-c3fb8724a8a7 | Open Energy Information

    Open Energy Info (EERE)

    matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Cleco Power LLC Effective...

  4. Data:B0e9026d-17ec-4618-95e5-682d8e117fb7 | Open Energy Information

    Open Energy Info (EERE)

    pasturage at one Point of Delivery and through one meter. Water pumping or water delivery systems include, but are not limited to, irrigation pumps, pivots, fertilizer pumps,...

  5. Data:292737fc-1c21-4a71-8d84-878ca6e025fb | Open Energy Information

    Open Energy Info (EERE)

    http%3A%2F%2Fpsc.wi.gov%2Fapps40%2Ftariffs%2Fviewfile.aspx%3Ftype%3Delectric%26id%3D5940&eibLmEU9-kDIqSyATb34D4BA&usgAFQjCNHQszMM37DZ2RABeDOYr8qMUj5yA Source Parent: Comments...

  6. Data:8a6072d5-dbda-47fb-a54e-7eb1eb932b74 | Open Energy Information

    Open Energy Info (EERE)

    2 3 Next >> Basic Information Utility name: Slash Pine Elec Member Corp Effective date: 19970201 End date if known: Rate name: Outdoor Lighting 250 Watt HPS Security Light...

  7. Data:Fc63ad02-f0fb-4ded-a90a-32612313be85 | Open Energy Information

    Open Energy Info (EERE)

    Single-phase, 60-cycles, and where available, three-phase, 60 cycles, at available secondary voltages. For prepay accounts, the facilities charge will be increased by 5.00...

  8. Data:54adb3ff-c362-4574-b14b-8b9c0fd2f8fb | Open Energy Information

    Open Energy Info (EERE)

    Power Supply Cost Recovery Factor, Fixed Charge Customer Charge + Energy Optimization. kWh << Previous 1 2 3 Next >> Category:Categories Retrieved from "http:...

  9. Data:0fb798a6-a6bb-45c1-a0f6-6f6727504b4a | Open Energy Information

    Open Energy Info (EERE)

    1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 Comments Fixed charge is facilities charge, energy optimization, and renewable energy standard charge multiplied by 36512. Energy charge is energy...

  10. Data:E00fc87e-6fb1-459c-b964-8747a495d7fe | Open Energy Information

    Open Energy Info (EERE)

    1 1 1 1 1 1 1 1 Dec 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 Comments Energy Optimization: .001780 added onto adjustments. kWh << Previous 1 2 3 Next >>...

  11. Data:F1d01087-996f-41c3-8ffa-e628e4fb6f61 | Open Energy Information

    Open Energy Info (EERE)

    Pole (NLA) 20.85 1220 &When consumer chooses URD service to the light where OH is the EMC preferred method of service. Additional Charges: Street Light Arms and Fixtures A. ARMS...

  12. Data:C1bb69c9-96f2-4d2f-b939-1755bc17809f | Open Energy Information

    Open Energy Info (EERE)

    Energy << Previous 1 2 3 Next >> Basic Information Utility name: Whitewater Valley Rural EMC Effective date: 20110101 End date if known: Rate name: Schedule GS - General Service...

  13. Data:8fd9d4ef-688a-48e0-88fb-3e93108c11d1 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Wild Rice Electric Coop, Inc Effective date: 20120318 End date if known: Rate name:...

  14. Data:Fb4e97fa-6eca-42de-a38f-01fc44fa31f9 | Open Energy Information

    Open Energy Info (EERE)

    within 30 days following the due date, a charge will be assessed. Any customer on a budget or leveled payment plan shall not be assessed for a late payment amount provided that...

  15. Data:Fb19a4b3-1bef-46cb-95e3-015a2272ad0d | Open Energy Information

    Open Energy Info (EERE)

    Effective date: 20090601 End date if known: Rate name: External interraptible service EIS-16 Sector: Industrial Description: Source or reference: Source Parent: Comments...

  16. Data:0e162bce-fb0e-4b37-9243-3fa48ccfb7a1 | Open Energy Information

    Open Energy Info (EERE)

    to either residential or commercial customers for the operation of storage type electric water heaters of standard make and design when used in conjunction with other regular...

  17. Data:Fc1fb8cb-2413-4f2a-bedf-27d0e7dd65b1 | Open Energy Information

    Open Energy Info (EERE)

    if known: Rate name: TDGSA Sector: Commercial Description: Source or reference: ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):...

  18. Data:7da9fb6d-395e-466f-8865-016e956e7d1e | Open Energy Information

    Open Energy Info (EERE)

    Street Lighting- 400 Watt Sector: Lighting Description: Source or reference: *ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):...

  19. Data:90eb1d4f-b204-4b5a-9d73-f04224bf00de | Open Energy Information

    Open Energy Info (EERE)

    name: Street Lighting- D150 Sector: Lighting Description: Source or reference: *ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):...

  20. Data:C2f657fb-1bf4-43a7-bab8-35adf4b59fa0 | Open Energy Information

    Open Energy Info (EERE)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page onYou are now leaving Energy.gov You are now leaving Energy.gov You are being directedAnnualPropertyd8c-a9ae-f8521cbb8489 No revision has been approved for this page.adf4b59fa0 No

  1. Data:Ffe2fb55-352f-473b-a2dd-50ae8b27f0a6 | Open Energy Information

    Open Energy Info (EERE)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page onYou are now leaving Energy.gov You are now leaving Energy.gov You are being directedAnnualPropertyd8c-a9ae-f8521cbb8489 No revision hasda62829c05b No revision has

  2. Search for associated production of z and Higgs bosons in proton-antiproton collisions at 1.96 TeV

    SciTech Connect (OSTI)

    BackusMayes, John Alexander; /Washington U., Seattle

    2010-12-01T23:59:59.000Z

    We present a search for associated production of Z and Higgs bosons in 4.2 fb{sup -1} of {bar p}p collisions at {radical}s = 1.96 TeV, produced in RunII of the Tevatron and recorded by the D0 detector. The search is performed in events containing at least two muons and at least two jets. The ZH signal is distinguished from the expected backgrounds by means of multivariate classifiers known as random forests. Binned random forest output distributions are used in comparing the data to background-only and signal+background hypotheses. No excess is observed in the data, so we set upper limits on ZH production with a 95% confidence level.

  3. An NMR approach to structural proteomics Adelinda Yee*, Xiaoqing Chang*, Antonio Pineda-Lucena*, Bin Wu*, Anthony Semesi*, Brian Le*, Theresa Ramelot

    E-Print Network [OSTI]

    McIntosh, Lawrence P.

    Biophysics, University of Toronto, 101 College Street, Toronto, ON, Canada M5G 1L7; Environmental Molecular of Biochemistry and Molecular Biology, Chemistry, and the Biotechnology Laboratory, 2146 Health Sciences Mall (see ref. 1 and other articles in the same issue). The large number of protein structures expected from

  4. Beitrittserklrung Hiermit erklre ich meinen Beitritt zu Alumni Lbeck Sektion der ,,Gesellschaft der Freunde und Frderer der Universitt zu Lbeck e. V." Ich bin damit einverstanden, dass meine

    E-Print Network [OSTI]

    Lübeck, Universität zu

    Beitrittserklärung Alumni Lübeck Universität zu Lübeck Frau Gabriele Zillmer Ratzeburger Allee 160 23538 Lübeck #12;

  5. Astro-DISC: Data-Intensive Analytics for Astrophysics Julio Lpez, Bin Fu, Eugene Fink, Swapnil Patil, Wittawat Tantisiriroj, Milo Polte, Lin Xiao, Vijay Vasudavan,

    E-Print Network [OSTI]

    Fink, Eugene

    Widefield Array Roadrunner Universe Bluewaters BHCosmo Large Synoptic Survey Tel (LSST) Ultimate Dark Matter

  6. The Dalhousie Employee Guide to Materials Management on Campus Look for the 4 system bins around campus designated for recyclables, paper/cardboard, organics and garbage.

    E-Print Network [OSTI]

    Brownstone, Rob

    can on bid on excess goods for reuse, please visit the Purchasing Department website ( http://purchasing.dal.ca/Surplus all waste for potential reuse before discarding! HAZARDOUS WASTE On-campus, contact Environmental cartons and drink trays Not Acceptable: Coffee cups (garbage) Carbon paper (garbage) Soiled paper

  7. CLICKER AN IPTV REMOTE CONTROL IN YOUR CELL PHONE Rittwik Jana, Yih-Farn Chen, David C Gibbon, Yennun Huang, Serban Jora, John Murray, Bin Wei

    E-Print Network [OSTI]

    Fisher, Kathleen

    device profile selection and content adaptation using a classification algorithm to match the best delivery by a broadband connection. For residential users, IPTV is often provided in conjunction with Video on Demand and may be bundled with Internet services such as Web access and Voice over IP (Vo

  8. Pn Tomographic Velocity and Anisotropy beneath the Iran Region by Yan L, Bin Liu, Shunping Pei, Youshun Sun, M. Nafi Toksz, and Xiangfang Zeng

    E-Print Network [OSTI]

    Sun, Youshun

    - son and McKenzie, 1984; Dewey et al., 1986; Beghoul and Barazangi, 1989; Boulin, 1991). The closure

  9. A note on Hardy-Weinberg equilibrium of VNTR data by using the Federal Bureau of Investigation's fixed-bin method

    SciTech Connect (OSTI)

    Devlin, B.; Risch, N. (Yale Univ., New Haven, CT (United States))

    1992-09-01T23:59:59.000Z

    To fully utilize the information of VNTR data for forensic inference, the probability of observing the matching suspect and evidentiary profile in a reference population is estimated, usually by assuming independence of alleles within and between loci. This assumption has been challenged on the basis of the observation that there is frequently an excess of single-band phenotypes (SBP) in forensic data bases, which could indicate lack of independence. Nevertheless, another explanation is that the excess SBP are artifacts of laboratory methods. In this report the authors examine the excess of SBP for three VNTR loci studied by the FBI (D17S79 and D2S44, for blacks, and D14S13, for Caucasians). The FBI claims that the excess is due to the effect of null alleles; the null alleles are suspected to be small to be detected. The authors estimate the frequency of null alleles for two loci (D17S79 and D14A13) by comparing, for these loci, the data from the FBI data base and the data from the Lifecodes data base. These comparisons yield information on small fragments because Lifecodes uses the restriction enzyme PstI, which yields larger fragments than does HaeIII, which the FBI uses. For D17S19 in blacks, the authors estimate a null allele frequency of 4.4%, and, for D14S13 in Caucasians, they estimate a frequency of 3.0%. The null-allele frequency for D2S44 in blacks is derived similarly, again being based on analysis of DNA cut with HaeIII and PstI; the estimate of the null-allele frequency for this locus is 1.5%. Using these null-allele frequency estimates and a goodness-of-fit test, the authors show that there is no evidence for deviations from Hardy-Weinberg expectations of genotype probabilities at these loci. 20 refs., 1 fig.

  10. The Robustness of the Sum-of-Squares Algorithm for Bin Packing Michael A. Bender Bryan Bradley y Geetha Jagannathan z

    E-Print Network [OSTI]

    Bender, Michael

    of Computer Science, Hofstra University, Hemp- stead, NY 11549, USA, email: pot8os@acm.org. z Department@acm.org. x Department of Computer Science, Hofstra University, Hemp- stead, NY 11549, USA, email: csckzp

  11. The Dalhousie Employee Guide to Materials Management on Campus Look for the 4 system bins around campus designated for recyclables, paper/cardboard, organics and garbage.

    E-Print Network [OSTI]

    Brownstone, Rob

    , straws, and dvd cases (garbage) Foams & soft # 6 plastics (garbage) Broken glass (garbage) What belongs cans, liquor/beer containers Milk containers Glass bottles and containers Tin, steel, and aluminum sweepings Broken glass (must be boxed & taped) Disposable gloves (latex, vinyl, etc.) Ceramics Packaging

  12. frwebgate.access.gpo.gov/cgi-bin/getdoc.cgi?dbname=2009_register&docid=fr17jy09-36.pdf

    Office of Environmental Management (EM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645 3,625 1,006 492 742 33Frequently20,000 Russian Nuclear Warheads|ofEventsWorkshopY-12a5-34attachment.pdfBPAAUDIT2-14

  13. Mechanism of action of cysteamine in depleting prolactin immunoreactivity

    SciTech Connect (OSTI)

    Sagar, S.M.; Millard, W.J.; Martin, J.B.; Murchison, S.C.

    1985-08-01T23:59:59.000Z

    The thiol reagent cysteamine (CSH) depletes anterior pituitary cells of immunoreactive PRL both in vivo and in vitro. The authors examined the hypothesis that CSH affects either the solubility or immunoreactivity of PRL through a mechanism involving thiol-disulfide exchange. Adult female rats were treated with either CSH (300 mg/kg, sc) or an equimolar dose of ethanolamine as a control. Anterior pituitary glands were extracted in 0.1 M sodium borate buffer, pH 9.0. Treatment of pituitary extracts with beta-mercaptoethanol (BME) destroys the immunoreactivity of PRL. However, extraction in the presence of reduced glutathione or CSH of pituitaries of rats treated with CSH restores immunoreactive PRL to control levels. Extracts were also subjected to polyacrylamide gel electrophoresis (PAGE). On gels of pituitary extracts of CSH-treated rats, the band that comigrates with purified PRL is diminished compared to that in ethanolamine-treated controls. However, extraction of the pituitaries in sodium dodecyl sulfate-containing buffer followed by chemical reduction with BME restores the PRL band. Therefore, CSH acts on PRL through a thiol-related mechanism to yield a product that is poorly soluble in aqueous buffer at pH 9 and is poorly immunoreactive. Dispersed anterior pituitary cells in tissue culture were incubated with L-(TVS)methionine to radiolabel newly synthesized peptides. PAGE followed by autoradiography confirmed the above results obtained in vivo.

  14. Local Power Functions of Tests for Double Unit Roots

    E-Print Network [OSTI]

    Haldrup, Niels Prof.; Lildholdt, Peter

    2000-01-01T23:59:59.000Z

    U! i)|it|t S 2 S  f H S e D fD f fbe fb. ff fbH fbb fff.S f.H fb fHH fb fb. fbe fb. fbb feS fe2 fDH fS2 fS f.SfS fSf fS2 fDe fDf fbS fbS fbe fb fb2 fbf fb fbf fHH fbf

  15. Computer News, Volume 29

    E-Print Network [OSTI]

    MATH DEPT Computer News, Volume 29. How to update your login shell from csh to tcsh. If you, like me, have had an account on the Math network of SUNs ...

  16. A realistic molecular model of cement hydrates

    E-Print Network [OSTI]

    Ulm, Franz-Josef

    Despite decades of studies of calcium-silicate-hydrate (C-S-H), the structurally complex binder phase of concrete, the interplay between chemical composition and density remains essentially unexplored. Together these ...

  17. Multi-Scale Studies of Transport and Adsorption Phenomena of Cement-based Materials in Aqueous and Saline Environment

    E-Print Network [OSTI]

    Yoon, Se Yoon

    2012-01-01T23:59:59.000Z

    and (d) 7days, and (e) Cl XRF map with microscopic image,by X-ray fluorescence (XRF). NaCl-reacted C-S-H samples werean X-ray fluorescence (XRF) map. Using XRD, this chapter

  18. Dynamic behavior of hydration water in calcium-silicate-hydrate gel: A quasielastic neutron scattering spectroscopy investigation

    E-Print Network [OSTI]

    Li, Hua

    The translational dynamics of hydration water confined in calcium-silicate-hydrate (C-S-H) gel was studied by quasielastic neutron scattering spectroscopy in the temperature range from 280 to 230 K. The stretch exponent ...

  19. American Mineralogist, Volume 97, pages 10601069, 2012 0003-004X/12/00071060$05.00/DOI: http://dx.doi.org/10.2138/am.2012.4058 1060

    E-Print Network [OSTI]

    Jacobsen, Steven D.

    -coordination with hydroxyl, VI Si-OH. Thaumasite and ettringite also form in the porous matrix of aging concrete, especially and of carbonation. Because C-S-H in concrete prov

  20. Effects of cysteamine on pituitary, MTTW15 tumor, and serum prolactin levels measured by rat lymphoma cell bioassay and radioimmunoassay

    SciTech Connect (OSTI)

    Parsons, J.A.; Peterson, E.K.; Hartfel, M.A.

    1984-05-01T23:59:59.000Z

    Cysteamine (CSH), a sulfhydryl compound, reduces both serum and anterior pituitary (AP) PRL measured by RIA. We have used the Nb2 lymphoma cell bioassay (BIO) for PRL to evaluate possible CSH-related changes in PRL levels in sera and tissues of male and MtTW15 mammosomatotropic tumor-bearing female rats. Experimental animals received a single sc injection of CSH (300 mg/kg), and samples were collected 0.5-24 h later. Since CSH and serum from CSH rats were toxic in BIO, samples were dialyzed before assay. All samples were evaluated for PRL and GH by RIA as well. A significant decrease (P less than 0.05) in BIO serum PRL was evident in male rats 0.5 h after CSH; levels remained low for 24 h. Serum PRL by RIA was significantly depressed at 4 h but not at 0.5 h or 24 h. PRL in AP extracts was decreased (60-90%) at all times by BIO and RIA. Significant decreases of BIO- and RIA-detectable PRL were recorded in serum and tissues (AP and tumors) at 4 h in tumor rats. Sequentially bled (0.5-4 h) CSH-treated tumor-bearing rats showed 50% and 80% reductions in serum PRL at 1 and 4 h by both BIO and RIA. CSH had no effect on GH levels in sera and tissues of any animal studied at any time interval. Our results substantiate earlier reports on CSH-induced decreases in RIA-detectable PRL. They show that such changes cannot be attributed to assay effects alone, as significant decreases in circulating and stored PRL (both AP and tumor) were evident by BIO. Results with tissue extracts were the most dramatic. They suggest an action of CSH or a metabolic intermediate with stored PRL which reduces both extractable PRL and hormone release. Such an effect of CSH on PRL extraction has been suggested by others. Whatever the mechanism, it appears to be relatively specific, since GH cells were not affected.