National Library of Energy BETA

Sample records for q4 q4 q1

  1. Q2 Q3 Q4 Q4 Q3 Q2 Q1 Q1 Q2 Q3 Q4 Q3 Q2 Q1 Q1 Q2 Q3 Q4 Q4 Q3 Q2 Q1

    E-Print Network [OSTI]

    .00/W Concentrating Solar Power (CSP and CPV) 6 MWac of concentrating solar capacity was installed installations totaled 723 MW in Q1 2013, up 33% over Q1 2012 Cumulative operating PV capacity in the U.S. now, installers, and manufacturers to collect granular data on the U.S. solar market. This data provides

  2. Mathematics 1052 Exam 2, May 3rd, 2014 Q1 Q2 Q3 Q4 Q5 Q6 Total Bonus

    E-Print Network [OSTI]

    Kaygun, Atabey

    Mathematics 1052 Exam 2, May 3rd, 2014 Q1 Q2 Q3 Q4 Q5 Q6 Total Bonus 15pts 20pts 10pts 15pts 30pts) (9 points) n=1 1 n(n+2) #12;Mathematics 1052 Exam 2, May 3rd, 2014 2. Consider the region bounded above about the line y = 1. Page 2 of 5 #12;Mathematics 1052 Exam 2, May 3rd, 2014 3. (10 points) (a

  3. Observations from The EV Project in Q4 2013

    SciTech Connect (OSTI)

    John Smart

    2014-02-01

    This is a summary report for The EV Project 4th quarter 2013 reports. It describes electric vehicle driver driving and charging behavior observed in Q4. It is the same report as the previously approved/published Q3 2013 report, only the numbers have been updated. It is for public release and does not have limited distribution.

  4. Geometry of an elliptic-difference equation related to Q4

    E-Print Network [OSTI]

    James Atkinson; Phil Howes; Nalini Joshi; Nobutaka Nakazono

    2015-06-15

    In this paper, we investigate a nonlinear non-autonomous elliptic difference equation, which was constructed by Ramani, Carstea and Grammaticos by integrable deautonomization of a periodic reduction of the discrete Krichever-Novikov equation, or Q4. We show how to construct it as a birational mapping on a rational surface blown up at eight points in $\\mathbb P^1\\times \\mathbb P^1$, and find its affine Weyl symmetry, placing it in the geometric framework of the Painlev\\'e equations. The initial value space is ell-$A_0^{(1)}$ and its symmetry group is $W(F_4^{(1)})$. We show that the deautonomization is consistent with the lattice-geometry of Q4 by giving an alternative construction, which is a reduction from Q4 in the usual sense. A more symmetric reduction of the same kind provides another example of a second-order integrable elliptic difference equation.

  5. Far-ultraviolet observations of comet C/2001 Q4 (NEAT) with FIMS/SPEAR

    SciTech Connect (OSTI)

    Lim, Y.-M.; Min, K.-W. [Korea Advanced Institute of Science and Technology (KAIST), 291 Daehak-ro, Yuseong-gu, Daejeon 305-701 (Korea, Republic of); Feldman, P. D. [Department of Physics and Astronomy, Johns Hopkins University, 3400 North Charles Street, Baltimore, MD 21218 (United States); Han, W. [Korea Astronomy and Space Science Institute (KASI), 776 Daedeokdae-ro, Yuseong-gu, Daejeon 305-348 (Korea, Republic of); Edelstein, J., E-mail: ymlim@kaist.ac.kr [Space Sciences Laboratory, University of California, Berkeley, 7 Gauss Way, Berkeley, CA 94720 (United States)

    2014-02-01

    We present the results of far-ultraviolet observations of comet C/2001 Q4 (NEAT) that were made with the Far-Ultraviolet Imaging Spectrograph on board the Korean satellite STSAT-1. The observations were conducted in two campaigns during its perihelion approach between 2004 May 8 and 15. Based on the scanning mode observations in the wavelength band of 1400-1700 Å, we have constructed an image of the comet with an angular size of 5°×5°, which corresponds to the central coma region. Several important fluorescence emission lines were detected including S I multiplets at 1429 and 1479 Å, C I multiplets at 1561 and 1657 Å, and the CO A{sup 1}?-X{sup 1}?{sup +} Fourth Positive system; we have estimated the production rates of the corresponding species from the fluxes of these emission lines. The estimated production rate of CO was Q {sub CO} = (2.65 ± 0.63) × 10{sup 28} s{sup –1}, which is 6.2%-7.4% of the water production rate and is consistent with earlier predictions. The average carbon production rate was estimated to be Q{sub C} = ?1.59 × 10{sup 28} s{sup –1}, which is ?60% of the CO production rate. However, the observed carbon profile was steeper than that predicted using the two-component Haser model in the inner coma region, while it was consistent with the model in the outer region. The average sulfur production rate was Q{sub S} = (4.03±1.03) × 10{sup 27} s{sup –1}, which corresponds to ?1% of the water production rate.

  6. Chiral O(Q^4) two-body operators for s-wave pion photoproduction on the NN system

    E-Print Network [OSTI]

    A. Gardestig

    2006-04-16

    The two-body currents for s-wave pion photoproduction on the NN system are derived to O(Q^4) in chiral perturbation theory. For the interesting case of 3S1 1S0 transitions, we show that an axial isovector two-nucleon contact term connects the short-distance physics of pion photoproduction to pion production and several important electroweak reactions. We also find that the standard chiral Lagrangian gives a gamma pi pi N N vertex that have not been explicitly mentioned in previous literature. The corresponding Feynman rule is presented here and some processes where it should be important are briefly discussed.

  7. 2012_Q4

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergyTher i n c i p a l De p u t y A s s i sEnergy It is the intent of the

  8. 2013_Q4.indd

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergyTher i n c i p a l De p u t y A s s i sEnergyEnergy The intent

  9. FORMALDEHYDE IN COMETS C/1995 O1 (HALE-BOPP), C/2002 T7 (LINEAR), AND C/2001 Q4 (NEAT): INVESTIGATING THE COMETARY ORIGIN OF H2CO

    E-Print Network [OSTI]

    FORMALDEHYDE IN COMETS C/1995 O1 (HALE-BOPP), C/2002 T7 (LINEAR), AND C/2001 Q4 (NEAT of formaldehyde (H2CO) have been conducted toward comets C/1995 O1 (Hale-Bopp), C/2001 Q4 (NEAT), and C/2002 T72CO other than the comet nucleus. The extended source of formaldehyde is probably grains composed

  10. U.S. Residential Photovoltaic (PV) System Prices, Q4 2013 Benchmarks: Cash Purchase, Fair Market Value, and Prepaid Lease Transaction Prices

    SciTech Connect (OSTI)

    Davidson, C.; James, T. L.; Margolis, R.; Fu, R.; Feldman, D.

    2014-10-01

    The price of photovoltaic (PV) systems in the United States (i.e., the cost to the system owner) has dropped precipitously in recent years, led by substantial reductions in global PV module prices. This report provides a Q4 2013 update for residential PV systems, based on an objective methodology that closely approximates the book value of a PV system. Several cases are benchmarked to represent common variation in business models, labor rates, and module choice. We estimate a weighted-average cash purchase price of $3.29/W for modeled standard-efficiency, polycrystalline-silicon residential PV systems installed in the United States. This is a 46% decline from the 2013-dollar-adjusted price reported in the Q4 2010 benchmark report. In addition, this report frames the cash purchase price in the context of key price metrics relevant to the continually evolving landscape of third-party-owned PV systems by benchmarking the minimum sustainable lease price and the fair market value of residential PV systems.

  11. FY11 Q4 SHPM Whitepaper DRAFT

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

    Track Paper European Wind Energy Conference (EWEA) Annual Event April 16-19, 2012; Copenhagen, Denmark Prognostic Control to Enhance Offshore Wind Turbine Operations and...

  12. Microchannel Receiver Development- FY12 Q4

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Oregon State University project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  13. FY11 Q4 SHPM Whitepaper DRAFT

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would like submitKansasCommunitiesofExtrans -ORGANIZATION FY 2013MayUncosted of Energyf i c eN

  14. Scattering Solar Thermal Concentrators- FY12 Q4

    Office of Energy Efficiency and Renewable Energy (EERE)

    This document summarizes the progress of this Penn State project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  15. Advanced Manufacture of Reflectors- FY12 Q4

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this University of Arizona project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  16. Next Generation Solar Collectors for CSP- FY12 Q4

    Office of Energy Efficiency and Renewable Energy (EERE)

    This document summarizes the progress of this 3M project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  17. Supercritical Carbon Dioxide Turbo-Expander- FY12 Q4

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this SWRI project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  18. CSP Tower Air Brayton Combustor- FY12 Q4

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this SWRI project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  19. Self-Cleaning CSP Optics with EDS- FY12 Q4

    Office of Energy Efficiency and Renewable Energy (EERE)

    This document summarizes the progress of this Boston University project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  20. On the physics of the $so_q(4)$ hydrogen atom

    E-Print Network [OSTI]

    P. G. Castro; R. Kullock

    2015-03-05

    In this work we investigate the $q$-deformation of the $so(4)$ dynamical symmetry of the hydrogen atom using the theory of the quantum group $su_q(2)$. We derive the energy spectrum in a physically consistent manner and find a degeneracy breaking as well as a smaller Hilbert space. We point out that using the deformed Casimir as was done before leads to inconsistencies in the physical interpretation of the theory.

  1. Baseload CSP Generation Integrated with Sulfur-Based Thermochemical Heat Storage- FY12 Q4

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this General Atomics project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  2. Dish Stirling High Performance Thermal Storage FY14Q4 Quad Chart

    Office of Scientific and Technical Information (OSTI)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield MunicipalTechnical Report:Speeding accessby aLED Street Lighting Host Site: City ofNovelQ3: Charles

  3. Enclosure - FY 2015 Q4 Metrics Report 2015-11-02.xlsx

    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 Data Center Home Page on Delicious Rank EERE:FinancingPetroleum Based|DepartmentStatementofAprilofEnergyEnSys Energy communities

  4. High-Efficiency Receivers for Supercritical Carbon Dioxide Cycles - FY12 Q4

    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 Data Center Home Page on Delicious Rank EERE:FinancingPetroleum12,ExecutiveFinancing ProgramsDepartmentHigh-Efficiency Parking Lighting|

  5. FY 2014 Q4 Metrics Report 2014-11-06.xlsx

    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 Data Center Home Page on Delicious Rank EERE:FinancingPetroleum12, 2015Executive Order14, 20111,FY 2007 FeeFederal Realin

  6. Microsoft PowerPoint - SRS Headcount by County of Residence Q4 FY 2013.pptx

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Outreach Home Room NewsInformationJesse BergkampCentermillionStockpileEqualArraysstructural stabilityInto

  7. Dish Stirling High Performance Thermal Storage FY14Q4 Quad Chart.

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would like submit theCovalentLaboratory | National(Technical Report) | SciTech Connect Dish

  8. SRS Employee Headcount by County of Residence Q4 FY15

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Outreach Home RoomPreservation of Fe(II) byMultidayAlumni > The2/01/12 Page 1NEWS MEDIA16,3 rd Quarter FY 20154

  9. Alcator C-MOD Quarterly Reports

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

    Reports Reports for 1997 Q1 (HTML) Q2 (HTML) Q3 (HTML) Q4 (HTML) Reports for 1998 Q1 (HTML) Q2 (HTML) Q3 (HTML) Q4 (HTML) Reports for 1999 Q1 (HTML) Q2 (HTML) Q3 (HTML) Q4 (HTML)...

  10. Adjustment patterns to commodity terms of trade shocks: the role of exchange rate and international reserves policies

    E-Print Network [OSTI]

    Aizenman, Joshua; Edwards, Sebastian; Riera-Crichton, Daniel

    2012-01-01

    Q3 1997 Q3 2003 Uruguay Q2 2004 Q4 2009 Venezuela, Rep. Bol.Q1 1989 Q1 1989 Venezuela, Rep. Bol. Q4 1990 Q1 1992 End Q4Peru, Uruguay and Venezuela. The data in this table show

  11. 3Q/4Q99 F-Area Hazardous Waste Management Facility Corrective Action Report - Third and Fourth Quarter 1999, Volumes I and II

    SciTech Connect (OSTI)

    Chase, J.

    2000-05-12

    Savannah River Site (SRS) monitors groundwater quality at the F-Area Hazardous Waste management Facility (HWMF) and provides results of this monitoring to the South Carolina Department of Health and Environmental Control (SCDHEC) semiannually as required by the Resource Conservation and Recovery Act (RCRA) permit. SRS also performs monthly sampling of the Wastewater Treatment Unit (WTU) effluent in accordance with Section C of the Underground Injection Control (UIC) application.

  12. Environ. Sci. Technol. 19Q4,28, 1422-1429 Rapid Kinetics of Cu(I I) Adsorption/Desorption on Goethite

    E-Print Network [OSTI]

    Sparks, Donald L.

    /Desorption on Goethite Paul R. Grossl' and Donald L. Sparks Department of Piant and Soil Sciences, University of Delaware, Washington 99352 The kinetics of Cu2+adsorption/desorption on goethite (a-FeOOH) was evaluated using/desorption on goethite. The rate of these relaxations (7)decreased with an increase in pH, alongthe adsorption edge

  13. An Investigation into the Realities of a Quantum Datapath

    E-Print Network [OSTI]

    Isailovic, Nemanja

    2010-01-01

    Q0 being on the longest critical path, Q1 and Q4 on thequbit criticality or critical paths suffer from the drawbackdata. The bulk of the critical path involves independent

  14. High-Efficiency Receivers for Supercritical Carbon Dioxide Cycles...

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

    2012. progressreportsunshotbraytonfy12q4.pdf More Documents & Publications High-Efficiency Low-Cost Solar Receiver for Use in a Supercritical CO2 Recompression Cycle - FY13 Q1...

  15. Domestic Coal Distribution 2009 Q1 by Origin State: Alabama

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming963 1.969 1.979Coal4Cubic43,728 243,242Consumers (Dollars per(Dollars4Q1

  16. Communication and Control for Quantum Circuits

    E-Print Network [OSTI]

    Patel, Yatish

    2010-01-01

    to Output. Classical bits cx and cz are trans- mitted to thePure Quantum h x y z s t cx yes yes yes yes yes yes yes czH q3 q4 zmeasure Correct c3 X cx q1, q0; cx q1, q2; correct

  17. Automatic Point-based Facial Trait Judgments Evaluation Mario Rojas Q.1

    E-Print Network [OSTI]

    Todorov, Alex

    Automatic Point-based Facial Trait Judgments Evaluation Mario Rojas Q.1 , David Masip1 dimensions to automat- ically learn a trait predictor from facial pixel images. We study whether trait evaluations performed by humans can be learned using machine learning classifiers, and used later in automatic

  18. Alcator C-Mod FY2007 Research Totals by Quarter

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

    7 Research Operations as of 83107 Research Days Research Weeks Total FY07 Research Weeks Q1 0.0 0.0 0.0 Q2 1.06 0.27 0.27 Q3 36.20 9.05 9.32 Q4 21.50 5.37 14.69 Detailed run run...

  19. Alcator C-Mod FY2008 Research Totals by Quarter

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

    8 Research Operations as of 52708 Research Days Research Weeks Total FY08 Research Weeks Q1 4.25 1.06 1.06 Q2 34.5 8.6 9.7 Q3 24.2 6.1 15.7 Q4 Detailed run descriptions can be...

  20. Proposed Scope and Schedule for Scenario and

    E-Print Network [OSTI]

    conservation and demand response development. Sensitivity S2 ­ Scenarios 1B and 2C w/Lower Natural Gas Prices on resource development of significantly lower natural gas prices. Sensitivity S3 ­ Scenarios 1B and 2C w and chapters. 2 #12;2014 Q4 Q1 2015 Q2 2015 Demand/Price Forecasts Updated Methodology for Quantification

  1. Quarterly SSP Experiment Summary-FY13-1Q 1

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal GasAdministration Medal of HonorPosterNationalPrograms | National Nuclear1-4Q FINAL3-1Q 1

  2. DOE/EIA-0202|83/2Q)-1 Short-Term Energy Outlook

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.101CompanyProduct:5/4Q)2Q)0/2Q)|83/2Q)-1

  3. Questions & Solutions On Particle Physics Q1. A photon with an energy GeVE 09.2=

    E-Print Network [OSTI]

    Adler, Joan

    Questions & Solutions On Particle Physics Q1. A photon with an energy GeVE 09.2= creates a proton-antiproton pair in which the proton has a kinetic energy of MeV0.95 . What is the kinetic energy of the antiproton particles will have similar kinetic energies . The total energy of each particle is the sum of its rest

  4. Discovery of oscillatory dynamics of city-size distributions in world

    E-Print Network [OSTI]

    White, Douglas R.

    of pdf thru Skype you can ask questions, thru Humberto he will have a chat box to relay questions I test) China leads by 50 years in its Q values ­ up to 1850 PART III: Scaling Examples: Chinese-results are very similar, as reported for the 1- factor test. Q1 Q3 Q5 Q2 Q4 Q6 #12;7 Multiple measures of Q

  5. Frequently Asked Questions about the Math Placement Test (MPT) (last updated on 2015 June 26) (Q1) Where is the Math Placement Test main web page?

    E-Print Network [OSTI]

    Saskatchewan, University of

    ) (Q1) Where is the Math Placement Test main web page? (A1) http://math.usask.ca/placement Information finalized. (Q2) Where is the Sample Math Placement Test main web page? (A2) http

  6. Radial Flow in Non-Extensive Thermodynamics and Study of Particle Spectra at LHC in the Limit of Small $(q-1)$

    E-Print Network [OSTI]

    Trambak Bhattacharyya; Jean Cleymans; Arvind Khuntia; Pooja Pareek; Raghunath Sahoo

    2015-07-30

    We expand the Tsallis distribution in a Taylor series of powers of (q-1), where q is the Tsallis parameter, assuming q is very close to 1. This helps in studying the degree of deviation of transverse momentum spectra and other thermodynamic quantities from a thermalized Boltzmann distribution. After checking thermodynamic consistency, we provide analytical results for the Tsallis distribution in the presence of collective flow up to the first order of (q-1). The formulae are compared with the experimental data.

  7. Chemical Engineering Science, Vol. 45, No. 7, pp. 1719-1731.1990. ooo9-2509/90 53.00 + 0.00 Printed in Grca~ Britain. Q 1wo Pergamon Press plc

    E-Print Network [OSTI]

    Aksay, Ilhan A.

    in Grca~ Britain. Q 1wo Pergamon Press plc SIMULTANEOUS MOMENTUM, HEAT AND MASS TRANSFER WITH CHEMICAL

  8. U.S. Photovoltaic Prices and Cost Breakdowns. Q1 2015 Benchmarks for Residential, Commercial, and Utility-Scale Systems

    SciTech Connect (OSTI)

    Chung, Donald; Davidson, Carolyn; Fu, Ran; Ardani, Kristen; Margolis, Robert

    2015-09-01

    The price of photovoltaic (PV) systems in the United States (i.e., the cost to the system owner) has continued to decline across all major market sectors. This report provides a Q1 2015 update regarding the prices of residential, commercial, and utility scale PV systems, based on an objective methodology that closely approximates the book value of a PV system. Several cases are benchmarked to represent common variations in business models, labor rates, and system architecture choice. We estimate a weighted-average cash purchase price of $3.09/W for residential scale rooftop systems, $2.15/W for commercial scale rooftop systems, $1.77/W for utility scale systems with fixed mounting structures, and $1.91/W for utility scale systems using single-axis trackers. All systems are modeled assuming standard-efficiency, polycrystalline-silicon PV modules, and further assume installation within the United States.

  9. Biochemical Platform Analysis Presentation for BETO 2015 Project...

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

    with NREL Catalytic Conversion of Sugars project - Q4 milestone * 2015 State of Technology assessment for FY15 R&D data - Q4 milestone * FY16 and beyond: TEA support for...

  10. 2014_Q1.indd

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergyTher i n c i p a l De p u t y A s s iof1 of 8 2 of 8 3 ofRuleWe We We el lc lc lc com

  11. Q1 Consider the n = 1 and n = 2 states of an electron in a hydrogen atom. The energy eigenfunctions nlm(r, , ) are

    E-Print Network [OSTI]

    Lee, Tonghun

    Q1 Consider the n = 1 and n = 2 states of an electron in a hydrogen atom. The energy eigenfunctions for the spherical harmonics Y m l (, ) may be found in the formulæ pages at the beginning of the exam. The hydrogen energy due to H is zero. You may do this by either explicit calculation, or by applying selection rules

  12. A Pseudomonas syringae pv. tomato DC3000 mutant lacking the type III effector HopQ1-1 is able to cause disease in the

    E-Print Network [OSTI]

    A Pseudomonas syringae pv. tomato DC3000 mutant lacking the type III effector HopQ1-1 is able-first authors. Summary The model pathogen Pseudomonas syringae pv. tomato DC3000 causes bacterial speck of an avirulence determinant in N. benthamiana: expression in the tobacco wildfire pathogen P. syringae pv. tabaci

  13. CI2525 ESTRUCTURAS DISCRETAS I f-m 2014 P 1/35 P 2/35 Q 1/15 Q 2/15 TOTAL/5

    E-Print Network [OSTI]

    Meza, Oscar J.

    CI2525 ESTRUCTURAS DISCRETAS I f-m 2014 Sección 1 P 1/35 P 2/35 Q 1/15 Q 2/15 TOTAL/5 0740951 Fernandez Luis Ely 1110969 Silva Rodriguez Erick Gabriel 34 35 15 15 1111391 Lupo Loyo Pablo Francisco 6 12 Colmenares Salamanca Bruno 35 11 8 10 1210613 Duque Contreras Lalezka Isabel 28 20 5 15 1210627 Salerno

  14. CI2525 ESTRUCTURAS DISCRETAS I oct-ene 2014 P 1/35 P 2/35 Q 1/15 Q 2/15 Tarea TOTAL

    E-Print Network [OSTI]

    Meza, Oscar J.

    CI2525 ESTRUCTURAS DISCRETAS I oct-ene 2014 P 1/35 P 2/35 Q 1/15 Q 2/15 Tarea TOTAL 0740913 Franco Alejandro 10 27 7 15 3,5 3 1110798 Portillo Rodriguez Ysmar Yoleth 10 2 1 1110883 Rodríguez Fernández Luis 1210848 Alexander Lacour Jean Paul 20 24 15 1 3 3 1210967 Fanghella Valero Alfredo José 35 32 15 15 3,5 5

  15. Fusion Rules of the Lowest Weight Representations of osp_q(1|2) at Roots of Unity: Polynomial Realization and Degeneration at Roots of Unity

    E-Print Network [OSTI]

    D. Karakhanyan; Sh. Khachatryan

    2009-08-27

    The degeneracy of the lowest weight representations of the quantum superalgebra $osp_q(1|2)$ and their tensor products at exceptional values of %when deformation parameter $q$ takes exceptional values is studied. The main features of the structures of the finite dimensional lowest weight representations and their fusion rules are illustrated using realization of group generators as finite-difference operators acting in the space of the polynomials. The complete fusion rules for the decompositions of the tensor products at roots of unity are presented. The appearance of indecomposable representations in the fusions is described using Clebsh-Gordan coefficients derived for general values of $q$ and at roots of unity.

  16. A disease of swine caused by a chromobacterium species 

    E-Print Network [OSTI]

    Sippel, William Lawrence

    1955-01-01

    ?Pa(y.?h.b.PO< TABLE OF CONTENTS x? pPOTa?mrOpaP O9, 1gs,'s, w'us,1 VS r9Q6M6V'w4, Q?uM ?g6?'w,uM 9's 864 V,,8 1,swQgV,1 JQ,?g6us?S g8 sAg8,? p4 A's w68sg1,Q,1 65 su55gwg'84 gM? J6Q4'8w, 56Q ' 1gss,Q4'4g68 JQ6V?,M 56Q 49, 56??6Ag8C Q,'s68s7 ?'? p4 'JJ,'Qs 's '8...M,?? 1gs4g8w4?S 6 5 9S1Q6C,8 wS'8g1, 5xA9gw9 A's JQ61uw,1 g8 Eu'84g4S?xx P6 649,Q Q,5,Q,8w,s 46 49gs J9,86M,868 A,Q, ,8w6u84,Q,1? I 7I <,Q4gw '81 n6u?C'?6? x?? gs6?'4,1 5g? , 1g55,Q,84 sJ,wg,s 65 V 'w4,Qg? 6J9'C, 56Q ?r? ?g6?'w,uM 5Q6M 49, s,A,Q A...

  17. High-p(T) pi(0) production with respect to the reaction plane in Au plus Au collisions at s(NN)=200 GeV 

    E-Print Network [OSTI]

    Afanasiev, S.; Aidala, C.; Ajitanand, N. N.; Akiba, Y.; Alexander, J.; Al-Jamel, A.; Aoki, K.; Aphecetche, L.; Armendariz, R.; Aronson, S. H.; Averbeck, R.; Awes, T. C.; Azmoun, B.; Babintsev, V.; Baldisseri, A.; Barish, K. N.; Barnes, P. D.; Bassalleck, B.; Bathe, S.; Batsouli, S.; Baublis, V.; Bauer, F.; Bazilevsky, A.; Belikov, S.; Bennett, R.; Berdnikov, Y.; Bjorndal, M. T.; Boissevain, J. G.; Borel, H.; Boyle, K.; Brooks, M. L.; Brown, D. S.; Bucher, D.; Buesching, H.; Bumazhnov, V.; Bunce, G.; Burward-Hoy, J. M.; Butsyk, S.; Campbell, S.; Chai, J. -S; Chernichenko, S.; Chiba, J.; Chi, C. Y.; Chiu, M.; Choi, I. J.; Chujo, T.; Cianciolo, V.; Cleven, C. R.; Cobigo, Y.; Cole, B. A.; Comets, M. P.; Constantin, P.; Csanad, M.; Csorgo, T.; Dahms, T.; Das, K.; David, G.; Delagrange, H.; Denisov, A.; d'Enterria, D.; Deshpande, A.; Desmond, E. J.; Dietzsch, O.; Dion, A.; Drachenberg, J. L.; Drapier, O.; Drees, A.; Dubey, A. K.; Durum, A.; Dzhordzhadze, V.; Efremenko, Y. V.; Egdemir, J.; Enokizono, A.; En'yo, H.; Espagnon, B.; Esumi, S.; Fields, D. E.; Fleuret, F.; Fokin, S. L.; Forestier, B.; Fraenkel, Z.; Frantz, J. E.; Franz, A.; Frawley, A. D.; Fukao, Y.; Fung, S. -Y; Gadrat, S.; Gastineau, F.; Germain, M.; Glenn, A.; Gonin, M.; Gosset, J.; Goto, Y.; de Cassagnac, R. Granier; Grau, N.; Greene, S. V.; Perdekamp, M. Grosse; Gunji, T.; Gustafsson, H. A.; Hachiya, T.; Henni, A. Hadj; Haggerty, J. S.; Hagiwara, M. N.; Hamagaki, H.; Harada, H.; Hartouni, E. P.; Haruna, K.; Harvey, M.; Haslum, E.; Hasuko, K.; Hayano, R.; Heffner, M.; Hemmick, T. K.; Heuser, J. M.; He, X.; Hiejima, H.; Hill, J. C.; Hobbs, R.; Holmes, M.; Holzmann, W.; Homma, K.; Hong, B.; Horaguchi, T.; Hur, M. G.; Ichihara, T.; Imai, K.; Inaba, M.; Isenhower, D.; Isenhower, L.; Ishihara, M.; Isobe, T.; Issah, M.; Isupov, A.; Jacak, B. V.; Jia, J.; Jin, J.; Jinnouchi, O.; Johnson, B. M.; Joo, K. S.; Jouan, D.; Kajihara, F.; Kametani, S.; Kamihara, N.; Kaneta, M.; Kang, J. H.; Kawagishi, T.; Kazantsev, A. V.; Kelly, S.; Khanzadeev, A.; Kim, D. J.; Kim, E.; Kim, Y. -S; Kinney, E.; Kiss, A.; Kistenev, E.; Kiyomichi, A.; Klein-Boesing, C.; Kochenda, L.; Kochetkov, V.; Komkov, B.; Konno, M.; Kotchetkov, D.; Kozlov, A.; Kroon, P. J.; Kunde, G. J.; Kurihara, N.; Kurita, K.; Kweon, M. J.; Kwon, Y.; Kyle, G. S.; Lacey, R.; Lajoie, J. G.; Lebedev, A.; Le Bornec, Y.; Leckey, S.; Lee, D. M.; Lee, M. K.; Leitch, M. J.; Leite, M. A. L.; Lim, H.; Litvinenko, A.; Liu, M. X.; Li, X. H.; Maguire, C. F.; Makdisi, Y. I.; Malakhov, A.; Malik, M. D.; Manko, V. I.; Masui, H.; Matathias, F.; McCain, M. C.; McGaughey, P. L.; Miake, Y.; Miller, T. E.; Milov, A.; Mioduszewski, Saskia; Mishra, G. C.; Mitchell, J. T.; Morrison, D. P.; Moss, J. M.; Moukhanova, T. V.; Mukhopadhyay, D.; Murata, J.; Nagamiya, S.; Nagata, Y.; Nagle, J. L.; Naglis, M.; Nakamura, T.; Newby, J.; Nguyen, M.; Norman, B. E.; Nyanin, A. S.; Nystrand, J.; O'Brien, E.; Ogilvie, C. A.; Ohnishi, H.; Ojha, I. D.; Okada, H.; Okada, K.; Omiwade, O. O.; Oskarsson, A.; Otterlund, I.; Ozawa, K.; Pal, D.; Palounek, A. P. T.; Pantuev, V.; Papavassiliou, V.; Park, J.; Park, W. J.; Pate, S. F.; Pei, H.; Peng, J. -C; Pereira, H.; Peresedov, V.; Peressounko, D. Yu; Pinkenburg, C.; Pisani, R. P.; Purschke, M. L.; Purwar, A. K.; Qu, H.; Rak, J.; Ravinovich, I.; Read, K. F.; Reuter, M.; Reygers, K.; Riabov, V.; Riabov, Y.; Roche, G.; Romana, A.; Rosati, M.; Rosendahl, S. S. E.; Rosnet, P.; Rukoyatkin, P.; Rykov, V. L.; Ryu, S. S.; Sahlmueller, B.; Saito, N.; Sakaguchi, T.; Sakai, S.; Samsonov, V.; Sato, H. D.; Sato, S.; Sawada, S.; Semenov, V.; Seto, R.; Sharma, D.; Shea, T. K.; Shein, I.; Shibata, T. -A; Shigaki, K.; Shimomura, M.; Shohjoh, T.; Shoji, K.; Sickles, A.; Silva, C. L.; Silvermyr, D.; Sim, K. S.; Singh, C. P.; Singh, V.; Skutnik, S.; Smith, W. C.; Soldatov, A.; Soltz, R. A.; Sondheim, W. E.; Sorensen, S. P.; Sourikova, I. V.; Staley, F.; Stankus, P. W.; Stenlund, E.; Stepanov, M.; Ster, A.; Stoll, S. P.; Sugitate, T.; Suire, C.; Sullivan, J. P.; Sziklai, J.; Tabaru, T.; Takagi, S.; Takagui, E. M.; Taketani, A.; Tanaka, K. H.; Tanaka, Y.; Tanida, K.; Tannenbaum, M. J.; Taranenko, A.; Tarjan, P.; Thomas, T. L.; Togawa, M.; Tojo, J.; Torii, H.; Towell, R. S.; Tram, V. -N; Tserruya, I.; Tsuchimoto, Y.; Tuli, S. K.; Tydesjo, H.; Tyurin, N.; Vale, C.; Valle, H.; van Hecke, H. W.; Velkovska, J.; Vertesi, R.; Vinogradov, A. A.; Vznuzdaev, E.; Wagner, M.; Wang, X. R.; Watanabe, Y.; Wessels, J.; White, S. N.; Willis, N.; Winter, D.; Woody, C. L.; Wysocki, M.; Xie, W.; Yanovich, A.; Yokkaichi, S.; Young, G. R.; Younus, I.; Yushmanov, I. E.; Zajc, W. A.; Zaudtke, O.; Zhang, C.; Zimanyi, J.; Zolin, L.; PHENIX Collaboration.

    2009-01-01

    library l i b rayy?hyI a? OQItj'Q4'4g68 nS (g??g'M y'AQ,8w, Q'1u'4, Q4g'? 5u?5...g??M ,84 6 5 49, Q,EugQ,M,84s 56Q 49, 1,CQ,, 6 5 ?arOaT a? eopyaQ4'4g68 nS (g??g'M y'AQ,8w,

  18. Semiempirical range and stopping power values for heavy ions 

    E-Print Network [OSTI]

    Schilling, Ralph Franklin, III

    1968-01-01

    and Graphs . . . 21 USE OF THE TABLES AND GRAPHS. . . . . . . 2$ VALIDITY OF SZii1IEviPIRICAL RESULTS. . . . 26 RZFZRZNCES. APPENDIX . . ~ ~ ~ ~, ~ ~ ~ 28 29 LIST OF FIGURES Stopping power curves for 1ons of various atomic numbers 1n Al. The energy... Uj U1 ~ ~ ~ y m I (D r r co ~ ~ ~ a NOND t(1 Q ~ ~ ~ ~ rn a I 4 lf', CJ a Nu ++O (T N 4' 0 In ~ 4 Ill ~ ~ ~ ~ ~ N QNONQ 0 0 nj Q' ~ ~ \\ ((1 Q Q ~ 4 W Gj Q ~l (T ocoa ~ rn a' 4 C' ~ N N N ((I C tn ~ ~ ~ N rh fn nJ 0 Nt 0 0 0 rn...

  19. DOE/EIA-0202(85/1Q) Short-Term Energy Outlook Quarterly Projections

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.101CompanyProduct: Crude7)8)4)1Q)3Q)4Q)1Q)

  20. DOE/EIA-0202(85/2Q) Short-Term Energy Outlook

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.101CompanyProduct: Crude7)8)4)1Q)3Q)4Q)1Q)2Q)

  1. Q1 1998 STEO Docs

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1Markets160Product: TotalCoalbed methaneCrude8

  2. What Does a Scattering Pattern Tell US?

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

    Scattering Space sample light image Image Space lens Angular Space Q 4p sin(q) l Fourier Transform Scattering Pattern Fourier Transform Phase Problem Scattering Pattern...

  3. NNSA Corporate CPEP Process NNSA Honeywell FM&T PER NNSA/NA-00...

    National Nuclear Security Administration (NNSA)

    "meets expectations." Cyber Security - Honeywell's AOP metrics for Q4 and the year were Green, no issues. All AOP milestones were delivered on time. Cyber Security completed...

  4. Energy Efficiency and Conservation Block Grant (EECBG): Better Buildings Neighborhood Program Final Report

    SciTech Connect (OSTI)

    Donnelly, Kat A.

    2014-01-10

    The Neighbor to Neighbor Energy Challenge (N2N) brought together a consortium of 14 leading clean energy rural, suburban, and low income communities throughout Connecticut. N2N was awarded $4.2 million from the U.S. Department of Energy (DOE) competitive BetterBuildings Neighborhood Program on August 10, 2010 to run a two-year pilot program (plus one year of transition and evaluation) (Award No. EMCBC- 00969-10). N2N tested innovative program models and hypotheses for improving Connecticut’s existing residential energy efficiency programs that are overseen by the ratepayer fund board and administered by CT utilities. N2N’s original goal was to engage 10 percent of households in participating communities to reduce their energy usage by 20 percent through energy upgrades and clean energy measures. N2N planned for customers to complete more comprehensive whole-home energy efficiency and clean energy measures and to achieve broader penetration than existing utility-administered regulated programs. Since this was an ARRA award, we report the following figures on job creation in Table 1. Since N2N is not continuing in its current form, we do not provide figures on job retention. Table 1 N2N Job Creation by Quarter Jobs Created 2010 Q4 6.65 2011 Q1 7.13 2011 Q2 4.98 2011 Q3 9.66 2011 Q4 5.43 2012 Q1 11.11 2012 Q2 6.85 2012 Q3 6.29 2012 Q4 6.77 2013 Q1 5.57 2013 Q2 8.35 2013 Q3 6.52 Total 85.31 The N2N team encountered several gaps in the existing efficiency program performance that hindered meeting N2N’s and DOE’s short-term program goals, as well as the State of Connecticut’s long-term energy, efficiency, and carbon reduction goals. However, despite the slow program start, N2N found evidence of increasing upgrade uptake rates over time, due to delayed customer action of one to two years from N2N introduction to completion of deeper household upgrades. Two main social/behavioral principles have contributed to driving deeper upgrades in CT: 1. Word of mouth, where people share their experience with others, which leads to others to take action; and 2. Self-herding, where people follow past behavior, which leads to deeper and deeper actions within individual households.

  5. FOIA Quarterly Reports (Q1-2014)

    Broader source: Energy.gov [DOE]

    Report that captures quarterly FOIA data at the DOE level. Through the use of an Applied Programming Interface (or API), the information will display on www.FOIA.gov.

  6. FOIA Quarterly Reports (Q1 2013)

    Broader source: Energy.gov [DOE]

    The DOE’s mission is to advance the national, economic, and energy security of the United States; to promote scientific and technological innovation in support of that mission; and to ensure the...

  7. What Does a Scattering Pattern Tell US?

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

    amplitude e iwt Phase difference Phase difference S e i (ri Q) A(DK) fi A(Q) Fourier Transform ( ri ) DK Q 4p sin(q) l Lensless Imaging Sample Space Scattering Space...

  8. EERE PowerPoint 97-2004 Template: Green Version

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

    analysis; planned for Q3 to Q4 Calculated for Quaternary faults using stress field from borehole breakouts and fault-kinematic data March '15 & in progress Major Technical...

  9. Optimal Quantum Control Using Randomized Benchmarking R. Barends,1

    E-Print Network [OSTI]

    Martinis, John M.

    on subsequent gates, and identify control crosstalk in superconducting qubits. This method is able to correct). As a testbed, we use a five qubit (Q0-Q4) superconducting system [11] based on the Xmon transmon design [13

  10. Quantified Traveler: Travel Feedback Meets the Cloud to Change Behavior

    E-Print Network [OSTI]

    2013-01-01

    spent traveling (time, cost, CO2, and calories) was able toemissions (kg of CO2), calories burned, cost ($), and traveland cost (Q4) spent traveling did not shift awareness, the information on calories (Q3) and CO2 (

  11. What Does a Scattering Pattern Tell US?

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

    light image Image Space lens Can we create the image without a lens? Angular Space Math Q 4p sin(q) l Lensless Imaging Sample Space Scattering Space sample light image lens...

  12. Fluorescent Pigments for High-Performance Cool Roofing

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

    Identified, End Q2 3. 500g of 2 New Pigments, End Q3 4. ESR Measured on New Cool Roof Coating, End Q4 Budget: Total DOE to date: 474,132 Total future DOE : 0 Key Partners:...

  13. 4 Questions for a Better Buildings Case Competition Judge: Marc...

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

    more than ever, and fresh ideas can be the catalyst for new programs and success in our industry. Q4: Do you plan to participate in the next Better Buildings Case Competition?...

  14. Atmospheric Pressure Deposition for Electrochromic Windows

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

    and Charcaterize Performance FY12-Q4 Milestone: Demonstration Liquid Phase Spray for WO3 at 6" by 6" Current work and future research Work with Sage Electrochromics to Transfer...

  15. Dish Sterling High Performance Thermal Storage- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Sandia National Laboratories/NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

  16. Next Generation Solar Collectors for CSP- FY13 Q1

    Office of Energy Efficiency and Renewable Energy (EERE)

    This document summarizes the progress of this 3M project, funded by SunShot, for the first quarter of fiscal year 2013.

  17. Quarterly SSP Experiment Summary-Q1FY14 1

    National Nuclear Security Administration (NNSA)

    Radiography (pRad) LANL Focused experiments: Materials pRad is a beam line and proton optics capability that uses protons to study fundamental material properties. pRad uses the...

  18. NBB Enclosed Particle Receiver- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

  19. System Advisor Model Enhancements for CSP- FY13 Q1

    Office of Energy Efficiency and Renewable Energy (EERE)

    This document summarizes the progress of this NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

  20. Advanced Manufacture of Reflectors- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this University of Arizona project, funded by SunShot, for the first quarter of fiscal year 2013.

  1. Q1Report for CADWR Project: Desalination Using Carbon NAnotube...

    Office of Scientific and Technical Information (OSTI)

    for CADWR Project: Desalination Using Carbon NAnotube Membranes In this research and development project, LLNL will leverage the process for fabrication of the membranes...

  2. Domestic Coal Distribution 2009 Q1 by Destination State: Alabama

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming963 1.969 1.979Coal4Cubic43,728 243,242Consumers (Dollars per(Dollars4

  3. Microsoft PowerPoint - 2015_Q1Presentation.pptx

    Office of Legacy Management (LM)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouthReport for the t-) S/,,5 'a C O M P R E H E N3 April 20115

  4. Quarterly SSP Experiment Summary-Q1FY14 1

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal GasAdministration Medal of HonorPosterNationalPrograms | National Nuclear1-4Q

  5. Bloo Solar formerly Q1 Nanosystems | 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 on Google Bookmark EERE: Alternative Fuels Data Center Home Page on QA:QA J-E-1 SECTION J APPENDIX ECoop IncIowaWisconsin:Pontiac Biomass Facility JumpII JumpBlackfeetBlock IslandSolar

  6. Mechanism of runaway electron beam formation during plasma disruptions in tokamaks

    E-Print Network [OSTI]

    Abdullaev, S S; Wongrach, K; Tokar, M; Koslowski, H R; Willi, O; Zeng, L

    2015-01-01

    A new physical mechanism of the formation of runaway electron (RE) beams during plasma disruptions in tokamaks is proposed. The plasma disruption is caused by strong stochastic magnetic field formed due to nonlinearly excited low-mode number magnetohydrodynamic (MHD) modes. It is conjectured that the runaway electron beam is formed in the central plasma region confined inside the intact magnetic surface located between $q=1$ and the closest low--order rational magnetic surfaces [$q=3/2$, $q=4/3$, \\dots]. It results in that runaway electron beam current has a helical nature with a predominant $m/n=1/1$ component. The thermal quench and current decay times are estimated using the collisional models for electron diffusion and ambipolar particle transport in a stochastic magnetic field, respectively. Possible mechanisms of the decay of runaway electron current due to an outward drift electron orbits and resonance interaction of high--energy electrons with the $m/n=1/1$ MHD mode are discussed.

  7. Mechanisms of plasma disruption and runaway electron losses in tokamaks

    E-Print Network [OSTI]

    Abdullaev, S S; Wongrach, K; Tokar, M; Koslowski, H R; Willi, O; Zeng, L

    2015-01-01

    Based on the analysis of data from the numerous dedicated experiments on plasma disruptions in the TEXTOR tokamak mechanisms of the formation of runaway electron beams and their losses are proposed. The plasma disruption is caused by strong stochastic magnetic field formed due to nonlinearly excited low-mode number MHD modes. It is hypothesized that the runaway electron beam is formed in the central plasma region confined inside the intact magnetic surface located between $q=1$ and the closest low--order rational [$q=4/3$ or $q=3/2$] magnetic surfaces. The thermal quench time caused by the fast electron transport in a stochastic magnetic field is calculated using the collisional transport model. The current decay stage is due to the ambipolar particle transport in a stochastic magnetic field. The runaway electron beam in the confined plasma region is formed due to their acceleration the inductive toroidal electric field. The runaway electron beam current is modeled as a sum of toroidally symmetric part and a ...

  8. Plano de la Habana 

    E-Print Network [OSTI]

    Garcia, Francisco Rojo

    1963-01-01

    , ", '' XOiQ. t ?T-'1:. ". iiX, ', . @X"lc:. :". iC;3X'661871 f'&)p iQQQ~~Q4MW~XCy w~~~' 8"', ~+~~'~6&, . ". "XCXGSp QD&' GCCQUQ0AB4ay A. QO54pi99 KAXCh XVIAi'-" ~CCG~lCJXC '@16 "QDf3 iC t:$Q&~ 0 3X'3iOB8 '". ""GQM PQPYQt 5Q "M~ 8~' Xg5Ai'lG 4~ pL'354"'C...~ QAC'. PG3, $, GVr* '4"'b% CWLPO84XOXl "'A~~Q &"' fhl~u&PX191 BBVG'XikC? c. ' Q+848~% 'iklf, Cgl WQ'gg~ Qg vpgg~ iV'!=8V@1'"g W9. 2. 1 g3. 'O', "MBA fl&~V@V QC X'CGlig@l. y XD p~@QC!X'Q1 i v Q~tX', V@X'~ CgZR~ M1Q VD3. 'QGtiS, GD 0'"' '&'z1VC;1'u...

  9. Next Generation DHCP Deployments

    E-Print Network [OSTI]

    Hull, Dave; Willard, George F. III

    2005-02-01

    Figure 9 ANSRdhcp request recording logic Figure 10 ANSR device entry Figure 11 DHCP snooping network topology Cisco Catalyst 2950G 48 C2950-I6K2L2Q4-M, Version 12.1(22)EA1 ip dhcp snooping vlan 123 ip dhcp snooping interface FastEthernet0... Figure 9 ANSRdhcp request recording logic Figure 10 ANSR device entry Figure 11 DHCP snooping network topology Cisco Catalyst 2950G 48 C2950-I6K2L2Q4-M, Version 12.1(22)EA1 ip dhcp snooping vlan 123 ip dhcp snooping interface FastEthernet0...

  10. Supplement of "Inversion of and emissions

    E-Print Network [OSTI]

    Meskhidze, Nicholas

    ppbv hydrogen £ ¡¥ : 311 ppbv nitrous oxide ¦§ ©¨ : 0.5 ppbv carbonyl sulfide ozone ¤ ¡¥ ©¡ hydrogen©¦ ¤ ¦ ¤ S ¤ ©¦ ¤ ¡%¦ ¤ Q©¦¢4¦ ¤ %$R¦ ¤ ©$ hydroxy carbonyls from ISOP Long-lived T 5 ¦!IU4¦ ¤ ¡¥QS¦ ¤ ¥¨ ¦ ¤ `$ dimethyl sulfide ¦§¨ ¡ carbon disulfide ¤ ¡¥¨ hydrogen sulfide 7 E $ oxygen atom (excited state

  11. JOURNAL DE PHYSIQUE CoZZoque C8, suppZ6ment au n08, Tome 41, aoGt 1980, page C8-163 STUDY OF LIQUID NICKEL-VANADIUM ALLOYS BY NEUTRON DIFFRACTION AND MODEL SIMULATION

    E-Print Network [OSTI]

    Boyer, Edmond

    , 28 i s the scattering angle, X the neutron wave- length, Q = 4n the modulus of the scattering vector NICKEL-VANADIUM ALLOYS BY NEUTRON DIFFRACTION AND MODEL SIMULATION J.L. Lemarchand, J. Bletry and P with model c a l c u l a t i o ~can lead to a quantitative interpreta- tion. In this paper, neutron

  12. NO. RIY. NO. TRANSMITTER DESIGN ANALYSIS ATM 897

    E-Print Network [OSTI]

    Rathbun, Julie A.

    NO. RIY. NO. TRANSMITTER DESIGN ANALYSIS ATM 897 PAGI 1 84 ( .e-,~·p·oe atam8 Dlvl8lon DATl! 7 - 6 TRANSMITTER DESIGN ANALYSIS PAGI 2 DATE 7-6-70 TABLE OF CONTENTS TRANSMITTER DESIGN ANALYSIS 1. INTRODUCTION AMPLIFIER 7. 4 Q4 OUTPUT NETWORK RE-CALCULATION 011 #12;TRANSMITTER DESIGN ANALYSIS ··-~·pace ltam8 Dlvlelon

  13. file://C:\\Documents%20and%20Settings\\VM3\\My%20Documents\\hc6-7a...

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

    Q 4.2 0.3 0.5 | 15.2 UnknownNo Answer... 7.1 0.7 1.0 0.6 0.2 | 14.0 | Air-Conditioning | | Central Air-Conditioning | Use a Central System... 58.6 1.3...

  14. Detailed Description of Key NIF Milestones for NNSA Description

    E-Print Network [OSTI]

    Operationally qualify ignition diagnostics [Neutron Activation Detector (Cooper), Magnetic Recoil Spectrometer ignition. Q4 FY2011 4073 Demonstrating we can light the "match" ­ alpha heating Conduct first DT implosion experimental campaign to demonstrate limited alpha heating Demonstrate cryogenic layered DT experiments

  15. Decomposing the Impact of Alternative Technology Sets on Future Carbon Emissions Growth1

    E-Print Network [OSTI]

    Wing, Ian Sue

    of carbon capture and storage, nuclear, and hydroelectric generation all lead to upward shifts in the long are the drivers of future global carbon dioxide (CO2) emissions growth and how would the availability of key Classification: D58, Q4, Q54, O1, Keywords: Asia, energy use, carbon emissions, global climate change, computable

  16. A.G.Ramm, Inverse scattering problem with data at fixed energy and fixed incident direction, Nonlinear Analysis: Theory, methods and Applications, 69, N4, (2008), 1478

    E-Print Network [OSTI]

    2008-01-01

    scattering problem with fixed­energy data consists in finding a potential q(x) from the knowledge of A q ([4]), who also gave a method for recovery of q from the exact fixed­energy data, an error estimate of q from noisy fixed­energy data, and an error estimate for this method [5], [6], [7]. Until now

  17. 7-135 A Carnot refrigeration cycle is executed in a closed system with a fixed mass of R-134a. The net work input and the maximum and minimum temperatures are given. The mass fraction of the refrigerant

    E-Print Network [OSTI]

    Bahrami, Majid

    7-61 7-135 A Carnot refrigeration cycle is executed in a closed system with a fixed mass of R-134aJ/kg (Table A-12). Analysis The coefficient of performance of the cycle is T v 20q 4 3 1 2 QH QL -8qC and #12

  18. Pion photo- and electroproduction in relativistic baryon ChPT

    E-Print Network [OSTI]

    Lothar Tiator; Stefan Scherer; Marius Hilt

    2014-02-04

    We present a calculation of pion photo- and electroproduction in manifestly Lorentz-invariant baryon chiral perturbation theory up to and including order q^4. We fix the low-energy constants by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID.

  19. Renewable Energy Finance Tracking Initiative (REFTI): Snapshot of Recent Geothermal Financing Terms, Fourth Quarter 2009 - Second Half 2011

    SciTech Connect (OSTI)

    Lowder, T.; Hubbell, R.; Mendelsohn, M.; Cory, K.

    2012-09-01

    This report is a review of geothermal project financial terms as reported in the National Renewable Energy Laboratory's Renewable Energy Finance Tracking Initiative (REFTI). The data were collected over seven analysis periods from the fourth quarter (Q4) of 2009 to the second half (2H) of 2011.

  20. Secondary constructions on generalized bent functions Brajesh Kumar Singh

    E-Print Network [OSTI]

    International Association for Cryptologic Research (IACR)

    Secondary constructions on generalized bent functions Brajesh Kumar Singh Department of Mathematics of Maiorana-McFarland class of bent functions, for Research supported by CSIR, INDIA. #12;2 B. K. Singh q = 4. Recently, Stanica, Gangopadhyay and Singh [13] studied several proper- ties generalized bent Boolean

  1. TIMES model for the Reunion Island: addressing reliability of electricity supply

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    energy sources. In 2008, the total primary energy consumption was 1295 ktoe, and as most of small islands% on renewable energy sources [1]. In 2008, the total primary energy consumption was 1295 ktoe, and as most. Keywords: Long-term energy planning. Reunion Island. Reliability of electricity supply. JEL: ­ Q4; O21; Q29

  2. Second Quarter 2014 Volume 7, number 2

    E-Print Network [OSTI]

    .5% in Q2, 4.1% in Q3, and 2.6% in Q4. March projections for annual average real GDP provided, the Bureau of Labor Statistics (BLS) reported the Consumer Price Index for All Urban Consumers rose 1.1% year- over-year in February, while core inflation was up 1.6% for the same period. Consumer prices

  3. Fluorescent Pigments for High-Performance Cool Roofing

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

    Q2 and Q6 2. 500g of 2 New Pigments, End Q3 and Q7 3. ESR Measured on New Cool Roof Coating, End Q4 and Q8 4. Potential Manufacturing Partner, Q3 and ongoing 5. Update BTO...

  4. Universality and criticality of a second-order granular solid-liquid-like phase transition

    E-Print Network [OSTI]

    Gustavo Castillo; Nicolás Mujica; Rodrigo Soto

    2015-01-20

    We experimentally study the critical properties of the non-equilibrium solid-liquid-like transition that takes place in vibrated granular matter. The critical dynamics is characterized by the coupling of the density field with the bond-orientational order parameter $Q_4$, which measures the degree of local crystallization. Two setups are compared, which present the transition at different critical accelerations as a a result of modifying the energy dissipation parameters. In both setups five independent critical exponents are measured, associated to different properties of $Q_4$: the correlation length, relaxation time, vanishing wavenumber limit (static susceptibility), the hydrodynamic regime of the pair correlation function, and the amplitude of the order parameter. The respective critical exponents agree in both setups and are given by $\

  5. A study of the middle Dutch poem, Van den vos Reynaerde and its sources in the branches of the old French Roman de Renard

    E-Print Network [OSTI]

    Appelboom, Peter Anton Frederik

    1917-01-01

    col. R. v.1199 Want eer hyt wiste, was hem een strec Omme sinesi bale arde vast.'** 41 R#R# v. BEG Con plus tret, plus eatrcint li las R. v.l£Q4 Rr.de sprang voert; dat strec liep toe R#R« v.860 Qar Martinez li clercono saut 'Or cug> or bug' fet... col. R. v.1199 Want eer hyt wiste, was hem een strec Omme sinesi bale arde vast.'** 41 R#R# v. BEG Con plus tret, plus eatrcint li las R. v.l£Q4 Rr.de sprang voert; dat strec liep toe R#R« v.860 Qar Martinez li clercono saut 'Or cug> or bug' fet...

  6. The influence of temperatures and mechanical treatments on pre- and post-emergence growth of peach and plum seedlings 

    E-Print Network [OSTI]

    Alsalih, Kamil Khidher

    1961-01-01

    , the possibility of variation between speoies SCAPI ICI ~ ~ IA NI A ~ ~ ~ 0 0 0 ~ ~ O IO Ch 33m R R CII CII CII ~ ~ A 4 SI S 0 0 0 '4l Q 4l Q s CII r 0 O ~ ~ as ~8 ~gA ICI IO 0 N Ill OE 0 CIA CIN Ch CO ~ ~ ~ t N ~ ~ 0 CCI ICI 0 0 0...W goeio4 oo ~. f As ooe ~ oero. eheea&eriheIL Q aeero%o areae ia i' piIaoale. Q4e oeaooivagg coal, 4 have hoea oaaee4 Q %he high O~erafeee, '()IIkaeee 4; ea4 0)? . gheee eee4lxlwge 4L4 aos groo ee sapL41p ehoa tirei Osaaeferro4 4e ~ gro hoaa? ?e 4L4...

  7. Power Corrections and Renormalons in Deep Inelastic Structure Functions

    E-Print Network [OSTI]

    M. Dasgupta; B. R. Webber

    1996-04-23

    We study the power corrections (infrared renormalon contributions) to the coefficient functions for non-singlet deep inelastic structure functions due to gluon vacuum polarization insertions in one-loop graphs. Remarkably, for all the structure functions $F_1$, $F_2$, $F_3$ and $g_1$, there are only two such contributions, corresponding to $1/Q^2$ and $1/Q^4$ power corrections. We compute their dependence on Bjorken $x$. The results could be used to model the dominant higher-twist contributions.

  8. Pion Photo- and Electroproduction and the Chiral MAID Interface

    E-Print Network [OSTI]

    Hilt, M; Scherer, S; Tiator, L

    2015-01-01

    We discuss the extended on-mass-shell scheme for manifestly Lorentz-invariant baryon chiral perturbation theory. We present a calculation of pion photo- and electroproduction up to and including order $q^4$. The low-energy constants have been fixed by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID (http://www.kph.uni-mainz.de/MAID/chiralmaid/).

  9. MIE 230-Thermodynamics Professor Rothstein

    E-Print Network [OSTI]

    Rothstein, Jonathan

    below. Steam enters the turbine at p1 = 10MPa and T1=640 C and exits at p2=50kPa. Steam leaves Steam Generator 2 3 1 Turbine Condenser Pump p2 = 50kPa p3 = 50kPa sat. liquid . Q4-1 = 200 MW T1 = 640 the steam power plant shown in the figure below. The cycle requires 150MWinQ of heat to operate as shown

  10. QuaRC Data Acquisition Card Support

    E-Print Network [OSTI]

    Arslan, Gürdal

    Clear HiQ Aero Q3 ControlPaQ-FW Q4 Q8 MultiQ-PCI Gumstix Card Config Buffered I/O Immediate I/O Time Watchdog Watchdog Clear DAQCard-6024e DAQCard-6062e DAQCard-6715 PCI-6023e PCI-6024e PCI-6025e PCI-6032e PCI-6034e PCI-6035e PCI-6036e PCI-6040e PCI-6052e PCI-6220 #12;QuaRC Data Acquisition Card Support

  11. Pion Photo- and Electroproduction and the Chiral MAID Interface

    E-Print Network [OSTI]

    M. Hilt; B. C. Lehnhart; S. Scherer; L. Tiator

    2015-10-15

    We discuss the extended on-mass-shell scheme for manifestly Lorentz-invariant baryon chiral perturbation theory. We present a calculation of pion photo- and electroproduction up to and including order $q^4$. The low-energy constants have been fixed by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID (http://www.kph.uni-mainz.de/MAID/chiralmaid/).

  12. Pion photo- and electroproduction with chiral MAID

    E-Print Network [OSTI]

    M. Hilt; B. C. Lehnhart; S. Scherer; L. Tiator

    2013-09-13

    We present a calculation of pion photo- and electroproduction in manifestly Lorentz-invariant baryon chiral perturbation theory up to and including order $q^4$. We fix the low-energy constants by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID. We explain how our program works and how it can be used for further analysis.

  13. hepph/9512272 ON THE THEORETICAL STATUS OF

    E-Print Network [OSTI]

    (š)N scattering processes are described by six further structure functions W š;\\Sigma 2 , xW š;\\Sigma 3 , F 2Z structure at short distances. Since both charged leptons (e \\Sigma ; ¯ \\Sigma ) and neutrinos (š; š) may ) collects couplings and propagator terms, e.g. P l \\Sigma ;fl (Q 2 ) = 2�ff 2 =Q 4 , P š;W +(Q 2 ) = G 2 F M

  14. Adequacy of milk manufacturing plants in the North Texas marketing area to handle surplus milk, 1953-54 

    E-Print Network [OSTI]

    Humphrey, Mabern David

    1954-01-01

    S St e S lek" Fer Cent de Pe Cent 63 Axe kdgh school Vmaatt + k farsssr lo olcuooo ao Oavlois a cist~- ~ ools & he rayortsso A. vo or vore sLslk corn. lj / e4~a isis ruhr& 5l 4~i' k MLcLX tftu4 4jMZi Q4 ~i 'iisV ~ sX GOiL4l'~~ ~'1'X. % Ftc...

  15. Making a virtue out of virtual communities: working electronically with an advisory panel of library users

    E-Print Network [OSTI]

    Collins, Anne; Kuhn, Isla; Morgan, Peter

    that the Panel's eventual membership provided, as far as possible, a balanced reflection of our actual registered client base.) Launching the Panel The initial invitation (which was reissued after about three weeks) ran for six weeks to the end... we should conduct a comprehensive stock check, proposing some possible options such as closing completely for a week, or a number of less drastic but more complex alternatives. • Q.4 - we listed a range of social networking technologies (FaceBook...

  16. Factors influencing the growth of Sclerotium rolfsii in various soils 

    E-Print Network [OSTI]

    Menon, Sankara Kochukrishna

    1953-01-01

    ~ hssishanh taefossox of hho loyarhasah of Plant Sqrsiahogf ael Pnthologye 'glhRS 4 05ICSN%. XgSSII00%4 4 ~ t ~ 4 g 4 4 4 4+ ~ ~ 0 ~ 4 ~ ~ 1 I t 4* ~ +t gggS4F Q%%4%$$ O. 0 0 ~ 4 0 4 4 ~ ~ f 4 % ~ ~ 1 4'1 0 II 856% 4NP %@IIX@) 's ~ ~ ~ s a e'e ~ i o + t a...

  17. More Than Smart Overview of Discussions Q3 2014 thru Q1 2015

    E-Print Network [OSTI]

    Stoltz, Brian M.

    Resources (DERs) · DERs include distributed renewable generation, energy efficiency, energy storage California's vision for making Distributed Energy Resources (DER) significant contributors to resource Resources Plan Requirements · Identifies optimal locations for the deployment of Distributed Energy

  18. More Than Smart Overview of Discussions Q3 2014 thru Q1 2015

    E-Print Network [OSTI]

    Desbrun, Mathieu

    and energy policy targets regarding renewable and distributed energy resources. · Participants: · Caltech to scale adoption of renewables and distributed energy resources. · Identified key issues that needed and distributed resources in California began at Caltech-Resnick Institute Grid2020 workshop in Fall 2011

  19. Microsoft Word - MDA FINAL FY14 Q1_1_31_14.doc

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

    revenues 304,614 260,757 Materials and supplies, at average cost 115,627 112,019 Prepaid expenses 66,976 40,458 Total current assets 1,837,725 1,841,816 Other assets...

  20. Grupo 10 Control de Xarxes de Computadors 2 Q1: 12-11-2012 Nombre: Apellidos

    E-Print Network [OSTI]

    paquetes que pertenecen al mismo flujo ¨ Tiene un mecanismo de control de error basado en CRC en lugar del tipo vector-distancia ý En terminología OSPF, link significa interfaz de un router ¨ Se usa el

  1. Grupo 10 Control de Xarxes de Computadors 2 Q1: 30-10-2014 Nombre: Apellidos

    E-Print Network [OSTI]

    operadora de telecomunicaciones es un LIR 3. En IPv6, marca las afirmaciones correctas ý Para el tipo loopback es ff02::1 ¨ Una dirección ULA es enrutable en Internet ý Para el tipo anycast se usan direcciones globales 4. En IPv6, marca las afirmaciones correctas ¨ El campo Etiqueta de flujo tiene el mismo

  2. PowerPoint Presentation - FY13 Q1 | Department of Energy

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

    Documents & Publications Low-Cost Self-Cleaning Reflector Coatings for CSP Collectors - FY13 Q2 Low-Cost Self-Cleaning Coatings for CSP Collectors Self-Cleaning CSP Optics with EDS...

  3. IMAGE BY JEN NATALI Q = (1.49/n)*A*(R2/3

    E-Print Network [OSTI]

    woody debris (LWD) input · Inorganic input (coarse sediment) METHODOLGY · Minimum slope for module = 20

  4. IMAGE BY JEN NATALI Q = (1.49/n)*A*(R2/3

    E-Print Network [OSTI]

    gradient alluvial channels TARGETED FUNCTIONS · Bank stabilization · Shading · Large woody debris (LWD

  5. Urea-Induced Denaturation of PreQ1Riboswitch Jeseong Yoon,

    E-Print Network [OSTI]

    Thirumalai, Devarajan

    between solutes in condensed media,13 it is remarkable that the hydrogen-bond network of aqueous water*, School of Computational Sciences, Korea Institute for Advanced Study, Seoul 130-722, Korea of RNA structures is mainly driven by the hydrogen-bonding and stacking interactions of urea

  6. Low-Cost Metal Hydride TES Systems- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress for this Savannah Reiver National Laboratory project, funded by SunShot, for the first quarter of fiscal year 2013.

  7. High Operating Temperature Heat Transfer Fluids for Solar Thermal Power Generation FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this UCLA project, funded by the SunShot CSP Multidisciplinary University Research Initiative, for the first quarter of fiscal year 2013.

  8. Corrosion Studies in High-Temperature Molten Salt Systems for CSP Applications- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Savannah River National Laboratory project, funded by SunShot, for the first quarter of fiscal year 2013.

  9. Quarterly SSP Experiment Summary-FY13-1Q 1

    National Nuclear Security Administration (NNSA)

    Radiography (pRad) LANL Focused experiments: Materials pRad is a beam line and proton optics capability that uses protons to study fundamental material properties. pRad uses the...

  10. Self-Cleaning CSP Optics with EDS- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Boston University project, funded by SunShot, for the first quarter of fiscal year 2013.

  11. U.S. Photovoltaic Prices and Cost Breakdowns: Q1 2015 Benchmarks...

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

    of Energy Office of Energy Efficiency & Renewable Energy Operated by the Alliance for Sustainable Energy, LLC This report is available at no cost from the National Renewable...

  12. FY14-Q1 1.2.1.3.ML.1 INL Biomass Feeding Survey Report

    SciTech Connect (OSTI)

    Tyler L. Westover

    2014-04-01

    Approximately 20 institutions were contacted by telephone and/or electronic mail and requested to provide responses to a survey on feeding biomass feedstock materials. Fourteen individuals responded. Responses from the participants, including information that was offered in addition to answers to the survey questions are summarized in this report, which fully meets the requirements of the milestone.

  13. State","Jan 2014","Feb 2014","Mar 2014","Q1 2014","Apr 2014"...

    U.S. Energy Information Administration (EIA) Indexed Site

    09494,1221339,1152461,3583294,1433421,1482609,1418716,4334746,1354994,1296217,1368933,4020144,16377117 "Alaska",137980,125224,144576,407780,134614,135935,128293,398842,122846,12706...

  14. State","Jan 2014","Feb 2014","Mar 2014","Q1 2014","Apr 2014"...

    U.S. Energy Information Administration (EIA) Indexed Site

    449569,1306162,1543399,4299130,1578949,1604437,1536669,4720055,1634205,1683795,1605354,4923354,1526905,1465505,1533540,4525950,18468489 "Alaska",137267,123685,140775,401727,127429,...

  15. Low-Cost Heliostat for Modular Systems- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

  16. High Efficiency Thermal Energy Storage System for CSP- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress for this Argonne National Laboratory project, funded by SunShot, for the first quarter of fiscal year 2013.

  17. High-Temperature Thermal Array for Next Generation Solar Thermal Power Production- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Los Alamos National Laboratory project, funded by SunShot, for the first quarter of fiscal year 2013.

  18. State","Jan 2015","Feb 2015","Mar 2015","Q1 2015","Apr 2015"...

    U.S. Energy Information Administration (EIA) Indexed Site

    ,"Jul 2015","Aug 2015","Sep 2015","Q3 2015" "Alabama",1382932,1141885,1281975,3806792,1067587,1003155,958490,3029232,1120511,1210360,1145913,3476784 "Alaska",135396,111797,125356,3...

  19. State","Jan 2015","Feb 2015","Mar 2015","Q1 2015","Apr 2015"...

    U.S. Energy Information Administration (EIA) Indexed Site

    "Alabama",1452147,1211568,1366275,4029990,1242782,1163577,1106043,3512402 "Alaska",95607,79773,89960,265340,122070,114301,108638,345009 "Arizona",632217,527479,594832,1754528,6766...

  20. Baseload CSP Generation Integrated with Sulfur-Based Thermochemical Heat Storage- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this General Atomics project, funded by SunShot, for the first quarter of fiscal year 2013.

  1. Warming acceleratesQ:1 decomposition; 2 of decades-old carbon in forest soils

    E-Print Network [OSTI]

    , CA 94720; and d Energy and Resources Group, University of California, Berkeley, CA 94720 AUTHOR to distinguish the contribution of decades-old carbon to CO2 fluxes in a labo- ratory incubation study. The first- sphere, which has declined since the early 1960s when large-scale atmospheric testing of nuclear weapons

  2. state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total...

    U.S. Energy Information Administration (EIA) Indexed Site

    17627215,4881361,5460677,4947015,15289053,5762846,5401692,5104549,16269087,66178091 "Anthracite",138012,121208,146605,405825,116603,127501,125028,369132,124431,140171,115125,379727...

  3. state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total...

    U.S. Energy Information Administration (EIA) Indexed Site

    16264924,5089471,5057952,5110136,15257559,6034905,5163897,5598759,16797561,65454926 "Anthracite",131036,126151,127417,384604,159864,161567,103152,424583,147423,145690,148093,441206...

  4. state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total...

    U.S. Energy Information Administration (EIA) Indexed Site

    16184747,5164431,5730421,5531484,16426336,5787538,6030423,5550719,17368680,67555716 "Anthracite",133480,129360,149128,411968,137000,135432,156673,429105,125414,140118,135144,400676...

  5. State","Jan 2013","Feb 2013","Mar 2013","Q1 2013","Apr 2013"...

    U.S. Energy Information Administration (EIA) Indexed Site

    13063008,4395291,4690749,4309998,13396038,4688289,4686735,4536312,13911336,55160877 "Anthracite (PA)",183278,171924,187404,542606,185555,195811,190531,571897,173912,185610,170546,5...

  6. state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total...

    U.S. Energy Information Administration (EIA) Indexed Site

    16614387,4935905,5546763,4807458,15290126,5422409,5298727,4998875,15720011,65189594 "Anthracite",141165,124979,139183,405327,124628,132527,133537,390692,119571,134819,115911,370301...

  7. Direct s-CO2 Receiver Development- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

  8. The neutron electric form factor to Q² = 1.45 (GeV/c)²

    E-Print Network [OSTI]

    Plaster, Bradley R. (Bradley Robert), 1976-

    2004-01-01

    The nucleon elastic electromagnetic form factors are fundamental quantities needed for an understanding of nucleon and nuclear electromagnetic structure. The evolution of the Sachs electric and magnetic form factors with ...

  9. Underdetermined Anechoic Blind Source Separation -Basis-Pursuit with q < 1

    E-Print Network [OSTI]

    Yilmaz, Ozgur

    a probabilistic interpretation of the proposed algorithm that explains why a choice of 0.1 q 0.4 is appropriate overview of ICA see [8]. ICA extracts n sources from n recorded mixtures under the crucial assumption that the underlying source signals are Rayan Saab is with the Department of Electrical and Computer Engineering

  10. High-Temperature Solar Selective Coating Development for Power Tower Receivers- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Sandia National Laboratories/NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

  11. FY14 Q1 Progress Report for SECA Core Technology Program

    SciTech Connect (OSTI)

    Stevenson, Jeffry W.; Koeppel, Brian J.

    2014-01-31

    This quarterly progress report was prepared under field work proposal (FWP) 40552 and covers technical work performed during the period October 1 through December 31, 2013 (FY14 1st quarter). The report highlights and documents technical progress and milestone status in tasks related to advanced cell and stack component materials development and computational design and simulation. Technical highlights related to cell and stack materials development and characterization include: • Surface modified, Ce-modified MC spinel-coated AISI 441 exhibited improved spallation resistance (compared to coated mill reference 441) after 30,000 hours of oxidation at 800ºC in air. Similar beneficial results from surface modification were observed after 26,000 hours of oxidation at 850ºC. • MnCo spinel coatings prepared from metallic powder precursors exhibited low area-specific resistance after 12,000 hours of testing at 800°C. • Long-term validation tests (6,000 hours of operation followed by 10 deep thermal cycles) of surface-blasted, spinel-coated AISI 441 interconnects were completed using PNNL’s SECA CTP stack test fixture. Results of post-test results will be reported in the next quarterly progress report. • Long-term evaluation of compliant glass seals (SCN-1 glass with YSZ fibers) was in progress using PNNL’s SECA CTP stack test fixture. • Baseline testing of LSCF-based cells from Fuel Cell Materials was performed in PNNL’s SECA CTP stack test fixture. Overall performance was similar to that previously obtained with similar cells from H.C. Starck. • A study on pore coarsening of compliant glass seals with and without inert fillers (ZrO2 short fibers or ZrO2 crushed hollow balls) has reached 2,000 hours of testing; results to date indicate that the addition of the fillers was partially effective in hindering the pore coalescence process. • Cell tests attempting to correlate effects of fuel water content on anode performance with previously observed changes in Ni/YSZ anode microstructure were initiated. Technical highlights in the computational modeling area include: • A method to interface the 3D SOFC-MP modeling tool with commercial FEA codes ABAQUS and ANSYS was developed to facilitate model construction and output of the predicted temperature field for structural stress analyses of stacks. • The error estimation and verification tools of the reduced order modeling (ROM) framework was improved to facilitate error handling for a large number of cases and perform user-specified test cases for error analysis of the generated ROM. • Mechanical behavior and damage characteristics of the compliant glass seal was investigated for a large planar cell design under different realistic electrochemical operating conditions (as predicted using SOFC-MP 3D) and thermal cycling events. • The methodology for lifetime prediction of the interconnect was improved to include the mechanical influence of the spinel protection coating on the prediction of critical scale thickness. 3 • Experimental characterization of the crack healing rate was performed for compliant glass SCN-1 with various amounts of fiber reinforcement. This information is needed for modeling evaluations of compliant seal healing during stack operations.

  12. The Casimir Force in Randall Sundrum Models with q+1 dimensions

    E-Print Network [OSTI]

    Mariana Frank; Nasser Saad; Ismail Turan

    2008-07-02

    We evaluate the Casimir force between two parallel plates in Randall Sundrum (RS) scenarios extended by q compact dimensions. After giving exact expressions for one extra compact dimension (RS 6D model), we generalize to an arbitrary number of compact dimensions. We present the complete calculation for both two brane scenario (RSI model) and one brane scenario (RSII models) using the method of summing over the modes. We investigate the effects of extra dimensions on the magnitude and sign of the force, and comment on limits for the size and number of the extra dimensions.

  13. Microsoft Word - fy09_annualtarget_climatemodeling1_Q1 _2_.doc

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration wouldMass map shines light on77 PAGE OFDetection ofOctober 28,CatastrophictheJuly 2,12,TARGET:

  14. Microsoft Word - MDA FINAL FY14 Q1_1_31_14.doc

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration wouldMass map shines light on77 PAGE OF PAGESpersonal CERTIFIEDPUB-3140September0 3.

  15. Dish Stirling High Performance Thermal Storage FY15Q1 Quad Chart

    Office of Scientific and Technical Information (OSTI)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield MunicipalTechnical Report:Speeding accessby aLED Street Lighting Host Site: City ofNovelQ3: Charles1800

  16. 2012-12-06 Quarterly SSP Experiment Summary-FY12-4Q 1

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouthReporteeo | National Nuclear Securityhr |of energyvision |1G

  17. DRAFT Quarterly SSP Experiment Summary-Q1FY15 1

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouthReporteeo | National/%2A en| National Nuclear SecurityTunnel

  18. Low-Cost, Lightweight Solar Concentrators - FY13 Q1 | Department of Energy

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergyTher i nAand DOE Safety StandardsLaborLignol<ColinandTheRyan

  19. Q1Report for CADWR Project: Desalination Using Carbon NAnotube Membranes

    Office of Scientific and Technical Information (OSTI)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefieldSulfateSciTech ConnectSpeedingConnect Pulse energy measurement at the(Journal Article)

  20. Q1Report for CADWR Project: Desalination Using Carbon NAnotube Membranes

    Office of Scientific and Technical Information (OSTI)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefieldSulfateSciTech ConnectSpeedingConnect Pulse energy measurement at the(Journal Article)(Technical

  1. Annual Employee Survey (AES) Report All Main Questions (Q1-Q71)

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergyTher i n c i p a l De p u t yWaste | DepartmentEnergyEnergy The

  2. FY 2015 Q1 Metrics Supporting Documentation 2015-02-09.xls

    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 Data Center Home Page on Delicious Rank EERE:FinancingPetroleum12, 2015Executive Order14, 20111,FY 2007 FeeFederalFirst Quarter Overall Root

  3. Dish Stirling High Performance Thermal Storage FY15Q1 Quad Chart (Technical

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would like submit theCovalentLaboratory | National(Technical Report) | SciTech Connect

  4. Selected non-holonomic functions in lattice statistical mechanics and enumerative combinatorics

    E-Print Network [OSTI]

    S. Boukraa; J-M. Maillard

    2015-10-15

    We recall that the full susceptibility series of the Ising model, modulo powers of the prime 2, reduce to algebraic functions. We also recall the non-linear polynomial differential equation obtained by Tutte for the generating function of the q-coloured rooted triangulations by vertices, which is known to have algebraic solutions for all the numbers of the form $2 +2 \\cos(j\\pi/n)$, the status of the q= 4 being unclear. We focus on the analysis of the q= 4 case, showing that the corresponding series is quite certainly non-holonomic. Along the line of a previous work on the susceptibility of the Ising model, we consider this q=4 series modulo the first eight primes 2, 3, ... 19, and show that this (probably non-holonomic) function reduces, modulo these primes, to algebraic functions. We conjecture that this probably non-holonomic function reduces to algebraic functions modulo (almost) every prime, or power of prime numbers. This raises the question to see whether such remarkable non-holonomic functions can be seen as ratio of diagonals of rational functions, or even rational, or algebraic, functions of diagonals of rational functions.

  5. Weak-Coupling Model for Pb-212 and Pb-204 

    E-Print Network [OSTI]

    Ko, Che Ming; Kuo, T. T. S.; McGrory, J. B.

    1973-01-01

    g??M ,84 6 5 49, Q,EugQ,M,84s 56Q 49, 1,CQ,, 6 5 ?arOaT a? eopyaQ4'4g68 nS (g??g'M y'AQ,8w, Q4M,84 6Q <4u1,84 l1?gs6Q? b'S x_HH x ? pPOTa?mrOpaP ? ? T.?p.( a? Oo. ypO.TlOmT. ?? PlOmTly arrmTT.Pr.< a? Oo. ?p<.l<. ? ? .?e.Tpb.POly eTa?mrOpaP a? Oo. ?p<.l<. H? op

  6. A Small-Particle Solar Receiver for High-Temperature Brayton Power Cycles- FY13 Q1

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this San Diego State University project, funded by SunShot, for the first quarter of fiscal year 2013.

  7. Roles of poloidal rotation in the q = 1 high-order harmonic tearing modes in a tokamak plasma

    SciTech Connect (OSTI)

    Wei Lai; Wang Zhengxiong [Key Laboratory of Materials Modification by Beams of the Ministry of Education, School of Physics and Optoelectronic Technology, Dalian University of Technology, Dalian 116024 (China)

    2013-01-15

    Roles of poloidal rotation in stabilizing the m/n=1/1 kink-tearing mode and exciting its high-order harmonic tearing modes are numerically investigated by using a reduced magnetohydrodynamic model. It is found that the high-order harmonic tearing modes, such as m/n=2/2, m/n=3/3, or even much higher-m harmonics, can be destabilized so significantly by rotation shear as to be more unstable than or comparable to the m/n=1/1 mode. Moreover, the short wave-length Kelvin- Helmholtz (KH) instabilities can be excited in the large rotation shear regime. The scaling power laws of the linear growth rate for each harmonic mode in different rotation shear regimes are verified by the previous relevant theoretical results based on the non-constant-{psi} and constant-{psi} behavior categories in tearing modes. During the nonlinear evolution, the m/n=2/2 mode dominated phase first appears and then is followed by the m/n=1/1 mode dominated nonlinear phase instead. Afterward, some smaller sub-islands due to the high-order harmonics are produced in the large irregular m=1 crescent-shaped island, and then a coalescence process of turbulent island chains occurs before the decay phase.

  8. /t1AoA-1-i~Q1--Al6A1 VS RegulatoryUS Army Corps

    E-Print Network [OSTI]

    Gray, Matthew

    of the Swazipbuster provisions of the Food Security Act of 1985 (FSA). Both the SCS and the Manual interpret "normal (Section 512.15 of the National Food Security Act Manual, August 1988) as wetlands which were both manipulated (drained or otherwise physically altered to remove excess water from the land) and cropped before

  9. 2 The WU-Minn Human Connectome Project: An overview 3 David C.Q1 Van Essen a,

    E-Print Network [OSTI]

    . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0 46 3 T connectome scanner -- hardware, pulse sequences, and scanning protocols . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0 47 3 T hardware

  10. 1Q1 Esterase-activatable -lapachone prodrug micelles for NQO1-targeted 2 lung cancer therapy

    E-Print Network [OSTI]

    Gao, Jinming

    -targeted 2 lung cancer therapy 3Q2 Xinpeng Ma a,1 , Xiumei Huang b,1 , Zachary Moore b , Gang Huang lung cancer 20 Cancer nanomedicine 21Lung cancer is one of the most lethal forms of cancer and current to be highly efficacious in killing non-small cell lung 23cancer (NSCLC) cells regardless of their p53, cell

  11. 2 Photosystem II and the unique role of bicarbonate: A historical perspective 3 DmitriyQ1 Shevela a,

    E-Print Network [OSTI]

    Govindjee

    fix carbon dioxide (CO2) into carbohydrates; this is necessary to 28support life on Earth. Over 50not include any carbon fixation pathway; Warburg used this discovery to support his idea that O2 at Urbana-Champaign, 265 Morrill Hall, 505 South Goodwin Avenue, Urbana, IL 61801, USA 8 e School of Life

  12. Degradation Mechanisms and Development of Protective Coatings for TES and HTF Containment Materials- F13 Q1

    Office of Energy Efficiency and Renewable Energy (EERE)

    This document summarizes the progress of this NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

  13. Large-$q$ expansion of the specific heat for the two-dimensional $q$-state Potts model

    E-Print Network [OSTI]

    H. Arisue; K. Tabata

    1998-07-03

    We have calculated the large-$q$ expansion for the specific heat at the phase transition point in the two-dimensional $q$-state Potts model to the 23rd order in $1/\\sqrt{q}$ using the finite lattice method. The obtained series allows us to give highly convergent estimates of the specific heat for $q>4$ on the first order transition point. The result confirm us the correctness of the conjecture by Bhattacharya et al. on the asymptotic behavior of the specific heat for $q \\to 4_+$.

  14. Effect of soil temperature on resistance of rice to seedling blight caused by Sclerotium rolfsii Sacc 

    E-Print Network [OSTI]

    Weerapat, Praphas

    1964-01-01

    I":". . -"';-'. , ;::::, RP9?C2 '|GZ - GGt'W "ZR%Zh&'~I'Tgfi *" zo?: 3~Gh'&IPWI|tG! Eh QZ 'BXCAK. - TQ '-, ';: ?' ! ', -':;, i", , ;. :;?-i;'!:G :. BGGZZIIG BBIZGGG, ':G"G", Kl'GZ' h il 'ZZZIIGXIIXGLGZGBZZ;::"BGG. ''::, . :":G ';"', . '?'i... . ". -", "!4&, ";;. . "-TQj:. :. W$4'j@"+hg4ja, " gp, . '. ~@@i"-W? i:RICO, ". "keX5 q -4X'q '. "' ~= ', , '- -', '-' ", . ' ' '-, , . ?' Sxe ?-:. yx4tib&"-Mph'ig. . :t0. :-py$e'gi&Xg' 4hagpk- 'Qg ' . "; P...

  15. The accuracy, stability and convergence characteristics of solution procedures for nonlinear structural analysis 

    E-Print Network [OSTI]

    Malek, Michele

    1974-01-01

    causes a large change in displacement, then the solution is likely to become unstable. However, if the structure stiffens as the load is increased then the solution will be stable. 28 aK NL, O fI q a. Unstabl. e Solution aK . o gq b. Stable... of stability is evident when the fourth-order Milne predictor-corrector equations are used to solve a simple first order linear differential equation. The Milne predictor equation is given by 33 q. =- q. + ?, dP [2g(q. ) ? g(q. , ) + 2g(q. )] 4 (III-30...

  16. Pion photo- and electroproduction and the chiral MAID interface

    E-Print Network [OSTI]

    M. Hilt; B. C. Lehnhart; S. Scherer; L. Tiator

    2015-11-18

    We discuss the extended on-mass-shell scheme for manifestly Lorentz-invariant baryon chiral perturbation theory. We present a calculation of pion photo- and electroproduction up to and including order $q^4$. The low-energy constants have been fixed by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID (http://www.kph.uni-mainz.de/MAID/chiralmaid/). We explain how our program works and how it can be used for further analysis.

  17. Recursion relations for the matrix elements of the two-dimensional harmonic oscillator 

    E-Print Network [OSTI]

    Ferester, Avner Herman

    1970-01-01

    and degree k are given expl1citly (&+~~. '(- ~) (&+R)/ (k-n)/fn+Z)/ n/ $/ J/ p/ L (y= ~~ . + . +~~is. n-0 Two generating functions for the LJ (2) are (10) ~p~ ?, Q t) -Q / (@ 4=o . F, (~ f-, . ~) The ~gQ satisfy the recursion formula ~ i, ~~y= (z... and the Lorentzian (c+z) will also be derived. The recursion relations will be obtained from the generating functions for 0he matrix elements. THE TWO-DIMERSIOVAL RARMO'. JIC OSCILLATOR AVD ITS WAVE- FUWCTIONS A particle of mass m, at the end of . a spr1ng fixed...

  18. Pion photo- and electroproduction and the chiral MAID interface

    E-Print Network [OSTI]

    Hilt, M; Scherer, S; Tiator, L

    2015-01-01

    We discuss the extended on-mass-shell scheme for manifestly Lorentz-invariant baryon chiral perturbation theory. We present a calculation of pion photo- and electroproduction up to and including order $q^4$. The low-energy constants have been fixed by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID (http://www.kph.uni-mainz.de/MAID/chiralmaid/). We explain how our program works and how it can be used for further analysis.

  19. PowerConsumption(mW) Radio in sleeping state/periodic poll

    E-Print Network [OSTI]

    x q 4 Radio on Radio in sleeping state/periodic poll 1 2 3 H ' Gc ( G8 ( P E A c P '@ 8E 'E ' 9 0 P 5 0( A E 9 8 P0 A ( W 0 (A G '@ 8 ( G & b8 ( I A P 3 3 '8E b A A E G0( 8 P A E 2 B P 3 ' 5 8E ' b A ( ( ' b P ' G G8 V P@ P A A I@ P8 b6 '@ 8 ( G P A V A 6A 5 } A '@ (A P c @ ' ' A E 8 V 30 b

  20. Engineering exotic phases for topologically protected quantum computation by emulating quantum dimer models RID B-7826-2008 

    E-Print Network [OSTI]

    Albuquerque, A. Fabricio; Katzgraber, Helmut G.; Troyer, Matthias; Blatter, Gianni.

    2008-01-01

    1934. 5, Osgood, N ~ R "A Theory of Flexure for Beams uith Nonparallel Extreme Fibers. " Journal of ~Alied Eechanics3 Vol. VIS No. 13 (SePtemberp 1939). PP. A 122-126. 6. Saksena~ G. B. "Shear Stress in Tapering Beam. " Aircraft Engineer inE, Vol... derived in mgr tcnct on the theory of elastioity, ox ccrc ~ Y(p-q) ? 4-&x The plus or adnus sign is used depending on the angle 8 and ths shear Sheol groyono/ Figure 13 If 9 is batsmen the shear diagonal and Og, then Oj is aigsbraioa13y ~ than OX...

  1. Grazing activities of cattle on the Jornada Experimental Range during the summer growing season of 1950 

    E-Print Network [OSTI]

    Kilpatrick, Henry Metz

    1955-01-01

    on ~ ? ~ ? ~ ~ ~ ~ ~ ~ ~ ~ ~ 44 ZXST OF FX0USS6 (eOSTZSUS0) 14 ~ 15m 17 ~ 18' Slo Timed aotivit1es of cattle in Al+ K~ 1960 ~ ~ ~ ~ ~ ~ ~ Timed activities of cattle in Angus't 6S 1950 ~ ~ ~ s ~ ~ Timed activities of cattle in August 6s 1950 ~ ~ i ~ ~ ~ Timed... cattle in August Sls 1950 ~ ~ ~ ~ ~ ~ Timed activities of cattle in August Q4S 1960 ~ ~ ~ e ~ ~ Timed activities of cattle in August SVS 1950 s ~ ~ ~ ~ ~ Timed activities of cattle in August Sly 1960 ~ ~ ~ ~ ~ ~ Timed activities of oattle...

  2. SANS (small angle neutron scattering) measurement of deuterium-dislocation correlation in palladium

    SciTech Connect (OSTI)

    Heuser, B.J.; Summerfield, G.C.; King, J.S. ); Epperson, J.E. )

    1989-11-01

    Small angle neutron scattering (SANS) measurements have been made on deformed polycrystal palladium samples with and without deuterium dissolved in the solution phase ({alpha}) at room temperature. Concentrations were held constant during SANS experiments by an equilibrium gas pressure cell. The difference scattering cross section for the same sample with and without deuterium loading has a 1/Q behavior (Q=4{pi}/{lambda} sin{theta}/2) at intermediate values of Q. At very low values of Q the dependence is much stronger than 1/Q. The 1/Q behavior is attributed to deuterium trapping close to long dislocation cores forming rod-like scattering structures.

  3. Coal Distribution Database, 2008

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming963 1.969 1.979Coal4Cubic Feet) Gas Wells (Million7 December3Q4Q 2009

  4. Colorado Associated-Dissolved Natural Gas, Wet After Lease Separation,

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming963 1.969 1.979Coal4Cubic Feet) Gas Wells (Million7 December3Q4Q

  5. DOE/EIA-0202(84/4Q) Short-Term Energy Outlook Quarterly Projections

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.101CompanyProduct: Crude7)8)4)1Q)3Q)4Q)

  6. Milk fat composition of a lactating dairy cow as influenced by abomasal infusion of various long chain fatty acids 

    E-Print Network [OSTI]

    Switzer, Leonard Anderson

    1971-01-01

    Ql 0 tD E IQ CD 4 ID 3 0 0 0 4 Q? 0 ttl CQ 0 0 4 4 LQ 0 Ln CJ 4 tD 3 0 Q- Q? IQ cnl 4 tD 3 Ql 0 CI 0 0 Q- 4 L- ID 0 Gl Lnl o cn 0 4 CQ 3 tD 0 0 0 C Q- 4 Q- IQ 0 Ql cnl cl cn ID 37 IQ V tl In U 4 O cnl 0 CO F ll O... in the same column uith dif'ferent superscripts (a, b, c) differed significantly (P&0. 05). 20 03 C 'I Cll IO LO I CO M OI IO N M IO N IO H C7I 4 LC3 D N M C LO CO D rt W N t N D Ot Cll N N CO LO IO (O CO D D D N \\0 IO LO (8 N N N LO M D f71 CII...

  7. The Fourth Positive System of Carbon Monoxide in the Hubble Space Telescope Spectra of Comets

    E-Print Network [OSTI]

    Roxana E. Lupu; Paul D. Feldman; Harold A. Weaver; Gian-Paolo Tozzi

    2007-08-22

    The rich structure of the Fourth Positive System (A-X) of carbon monoxide accounts for many of the spectral features seen in long slit HST-STIS observations of comets 153P/Ikeya-Zhang, C/2001 Q4 (NEAT), and C/2000 WM1 (LINEAR), as well as in the HST-GHRS spectrum of comet C/1996 B2 Hyakutake. A detailed CO fluorescence model is developed to derive the CO abundances in these comets by simultaneously fitting all of the observed A-X bands. The model includes the latest values for the oscillator strengths and state parameters, and accounts for optical depth effects due to line overlap and self-absorption. The model fits yield radial profiles of CO column density that are consistent with a predominantly native source for all the comets observed by STIS. The derived CO abundances relative to water in these comets span a wide range, from 0.44% for C/2000 WM1 (LINEAR), 7.2% for 153P/Ikeya-Zhang, 8.8% for C/2001 Q4 (NEAT) to 20.9% for C/1996 B2 (Hyakutake). The subtraction of the CO spectral features using this model leads to the first identification of a molecular hydrogen line pumped by solar HI Lyman-beta longward of 1200A in the spectrum of comet 153P/Ikeya-Zhang. (Abridged)

  8. Diophantine properties for q-analogues of Dirichlet's beta function at positive integers

    E-Print Network [OSTI]

    Jouhet, Frederic

    2008-01-01

    small In this paper, we define $q$-analogues of Dirichlet's beta function at positive integers, which can be written as $\\beta_q(s)=\\sum_{k\\geq1}\\sum_{d|k}\\chi(k/d)d^{s-1}q^k$ for $s\\in\\N^*$, where $q$ is a complex number such that $|q|transcendance of the numbers $\\beta_q(2s+1)$ for $q$ algebraic such that $0numbers $\\beta_q(2s)$: we give a lower bound for the dimension of the vector space over $\\Q$ spanned by $1,\\beta_q(2),\\beta_q(4),...,\\beta_q(A)$, where $1/q\\in\\Z\\setminus\\{-1;1\\}$ and $A$ is an even integer. As consequences, for $1/q\\in\\Z\\setminus\\{-1;1\\}$, on the one hand there is an infinity of irrational numbers among $\\beta_q(2),\\beta_q(4),...$, and on the other hand at least one of the numbers $\\beta_q(2),\\...

  9. Canonical factorization and diagonalization of Baxterized braid matrices: Explicit constructions and applications

    E-Print Network [OSTI]

    A. Chakrabarti

    2003-05-07

    Braid matrices $\\hat{R}(\\theta)$, corresponding to vector representations, are spectrally decomposed obtaining a ratio $f_{i}(\\theta)/f_{i}(-\\theta)$ for the coefficient of each projector $P_{i}$ appearing in the decomposition. This directly yields a factorization $(F(-\\theta))^{-1}F(\\theta)$ for the braid matrix, implying also the relation $\\hat{R}(-\\theta)\\hat{R}(\\theta)=I$.This is achieved for $GL_{q}(n),SO_{q}(2n+1),SO_{q}(2n),Sp_{q}(2n)$ for all $n$ and also for various other interesting cases including the 8-vertex matrix.We explain how the limits $\\theta \\to \\pm \\infty$ can be interpreted to provide factorizations of the standard (non-Baxterized) braid matrices. A systematic approach to diagonalization of projectors and hence of braid matrices is presented with explicit constructions for $GL_{q}(2),GL_{q}(3),SO_{q}(3),SO_{q}(4),Sp_{q}(4)$ and various other cases such as the 8-vertex one. For a specific nested sequence of projectors diagonalization is obtained for all dimensions. In each factor $F(\\theta)$ our diagonalization again factors out all dependence on the spectral parameter $\\theta$ as a diagonal matrix. The canonical property implemented in the diagonalizers is mutual orthogonality of the rows. Applications of our formalism to the construction of $L-$operators and transfer matrices are indicated. In an Appendix our type of factorization is compared to another one proposed by other authors.

  10. Final_report_pub1.pdf

    SciTech Connect (OSTI)

    O'Brien, Nicholas

    2014-08-15

    The paper describes Soitecs project to plan,install,qualify and ramp a high volume CPV module manufactruing facility in Southern California. Soitec’s CPV module factory in San Diego was planned with an annual production capacity of 280MWDC. It was scheduled to be operational by the first quarter of 2013, and was expected to create several hundred direct and indirect jobs in the San Diego region. From ground breaking to facility readiness was completed in six months. This enabled the docking of equipment in the Q3’12 time frame. The first 140 MW of capacity was ready for operation in Q4’12. Production of the CX-M500 modules started in Q4 2012. The line yield and factory capacity were ramped in 2013. The annual production capacity demonstration was successfully completed in Q2 2014. The modules manufactured at the plant were used to supply utility scale demand in the US and also world markets.

  11. Contamination in the Kepler field. Identification of 685 KOIs as false positives via ephemeris matching based ON Q1-Q12 data

    SciTech Connect (OSTI)

    Coughlin, Jeffrey L.; Thompson, Susan E.; Burke, Christopher J.; Caldwell, Douglas A.; Jenkins, Jon M.; Mullally, Fergal R.; Rowe, Jason F.; Bryson, Stephen T.; Haas, Michael R.; Howell, Steve B.; Kolodziejczak, Jeffery J.

    2014-05-01

    The Kepler mission has to date found almost 6000 planetary transit-like signals, utilizing three years of data for over 170,000 stars at extremely high photometric precision. Due to its design, contamination from eclipsing binaries, variable stars, and other transiting planets results in a significant number of these signals being false positives (FPs). This directly affects the determination of the occurrence rate of Earth-like planets in our Galaxy, as well as other planet population statistics. In order to detect as many of these FPs as possible, we perform ephemeris matching among all transiting planet, eclipsing binary, and variable star sources. We find that 685 Kepler Objects of Interest (KOIs)—12% of all those analyzed—are FPs as a result of contamination, due to 409 unique parent sources. Of these, 118 have not previously been identified by other methods. We estimate that ?35% of KOIs are FPs due to contamination, when performing a first-order correction for observational bias. Comparing single-planet candidate KOIs to multi-planet candidate KOIs, we find an observed FP fraction due to contamination of 16% and 2.4% respectively, bolstering the existing evidence that multi-planet KOIs are significantly less likely to be FPs. We also analyze the parameter distributions of the ephemeris matches and derive a simple model for the most common type of contamination in the Kepler field. We find that the ephemeris matching technique is able to identify low signal-to-noise FPs that are difficult to identify with other vetting techniques. We expect FP KOIs to become more frequent when analyzing more quarters of Kepler data, and note that many of them will not be able to be identified based on Kepler data alone.

  12. CI2525 ESTRUCTURAS DISCRETAS I d-m 2015 P 1/35 P 2/35 Q 1/15 Q 2/15 TOTAL/5

    E-Print Network [OSTI]

    Meza, Oscar J.

    Edinson 21 17 12 7 3 1110502 Lago Ibañez, Giancarlo Stephan 1 1111274 Di Zio Castillo, Ricardo Andres 5 4,5 3 1110883 Rodriguez Fernandez, Luis Ely 12 13,5 0 2 1111391 Lupo Loyo, Pablo Francisco 13,5 1

  13. 1. (25 pts) Three point charges, q1, q2 and q3 that have the same +2 Coulomb charge are fixed to a circle of radius

    E-Print Network [OSTI]

    Akerib, Daniel S.

    of 6.0 nF and a plate area of 2 2 5.0 10 m- × is connected to a 12 V battery. a. What is the electric A wire and the magnetic field at point O is zero tesla. a. Determine the value of the current, I

  14. The 40m General Purpose Small-Angle Neutron Scattering Instrument at Oak Ridge National Laboratory

    SciTech Connect (OSTI)

    Wignall, George D [ORNL; Bailey, Katherine M [ORNL; Buchanan, Michelle V [ORNL; Butler, Paul D [ORNL; Heller, William T [ORNL; Littrell, Ken [ORNL; Lynn, Gary W [ORNL; Melnichenko, Yuri B [ORNL; Myles, Dean A A [ORNL; Urban, Volker S [ORNL

    2012-01-01

    A high-flux, 40m long small-angle neutron scattering (SANS) instrument has been constructed at Oak Ridge National Laboratory (ORNL). The facility utilizes a mechanical velocity selector, pinhole collimation and a high count-rate (> 105 Hz), large-area (1m2) two-dimensional position-sensitive detector. The incident wavelength ( ), resolution ( / ), incident collimation and sample-detector distance are independently variable under computer control. The detector can translate 45cm off axis to increase the overall Q-range (< 0.001 < Q = 4 -1sin < 1 -1), where 2 is the angle of scatter. The design and characteristics of this instrument are described along with examples of scattering data to illustrate the performance.

  15. Digital Doppler radial velocity data compared objectively with digital reflectivity radar data 

    E-Print Network [OSTI]

    Beaver, Thomas Foster

    1980-01-01

    . , few components toward or away from the radar greater than -1 5 m s . However at 3 km and 4 km a def1n1te area of convergence is noted (Figs. 9 and 10). Although neither the ref lect1vity nor radial veloc1ty analyses at th1s time ind1cate any def1... I N 4 N CLI ILI IL O J ILI 6 0 ) Id CC OE IC + ILI IC I Vl ?T T W 0 0 0 LLI 0 Z 4( W 3 C- 7: LLI ri 4 4 I I N 0' 0 \\L III gQ ~ 4 N NZ WO 8 I 4l zj WN ~4I III W I- g I 0 R 0 O. I 0 0 ~ N 0 0 LI 0 0...

  16. Chebyshev polynomial approximation of the solution to an ordinary differential equation 

    E-Print Network [OSTI]

    Kim, Gil Chang

    1965-01-01

    DQ 50Q 4~( e 15 IF (D(I)+GAD(J)) GQ TO 500 DENQM~D ( I ) D(I)~D(J) D(V)~DENOM CONT INVE CONT I NVE 're ~ a ~ RRINT THE RESULTS osse ~ DQ 666 I~)e )5 C ( I ) ~DEXP ( D ( I li ) 5 ( I ) ~EVAI if O ( I ) ) YX(1)ARABS(C(I ) B(l ) ) CONT IN VE...120)o KEY IIQ FOFXY~YVALPDEXP(T(2e&))-YVALoooe2-YVAL GQ TQ )30 120 FOFXY~DEXP(-T(2oJ)) 2eO~YVAL -IeQ 130 RETURN END DOVBLE PRECI S I GN FVNCTI ON EVAL tl X ) C C THIS ROVTINE EVAl VATES Y(X) AT Xs C DIMENSION TX((5& 15) eXT(15s 15) & VX (15...

  17. Uncertainty Quantification of the Pion-Nucleon Low-Energy Coupling Constants up to Fourth Order in Chiral Perturbation Theory

    E-Print Network [OSTI]

    K. A. Wendt; B. D. Carlsson; A. Ekström

    2014-10-02

    We extract the statistical uncertainties for the pion-nucleon ($\\pi N$) low energy constants (LECs) up to fourth order $\\mathcal{O}(Q^4)$ in the chiral expansion of the nuclear effective Lagrangian. The LECs are optimized with respect to experimental scattering data. For comparison, we also present an uncertainty quantification that is based solely on \\pin{} scattering phase shifts. Statistical errors on the LECs are critical in order to estimate the subsequent uncertainties in \\textit{ab initio} modeling of light and medium mass nuclei which exploit chiral effective field theory. As an example of the this, we present the first complete predictions with uncertainty quantification of peripheral phase shifts of elastic proton-neutron scattering.

  18. An accounting system for a Class I motor common carrier of property 

    E-Print Network [OSTI]

    Packenham, Edward S

    1950-01-01

    QL 'be thoee a?4? to ecsssoetiag lgaoa fee therma Iwstim ef ~ swww ~ J4llkl sw%swl? 1$ %Ash QR OOMMtlaI lllWI leap%&~ S4? 4?ysHag+ f?ea ?see@tel eaah haaliieg ynreo4ese ia ws4? eoeoeasrg 'hy tho ical oat?WLieh?4 ~o of aet oetMomsctct wheseia a aanrsoe...?ahar wiD ba grayer?4g yr?yegg eyg?ci??4 e?4 yeiC. thC? CrrL?a yreei?C?e tha yassihglitf ef fLNlacc? t??a?t ee ahliC?CC??at ~?g. Cll ?f ths ?cyley?es will be yes ee e waahig basis* Vega?CX y?re? ??4 y?y?aaA 4?tes vill bs acCaaCcQ?4 se ee ts yaaac...

  19. Field Notes, Middle America (1956-1968) 

    E-Print Network [OSTI]

    Davis, William B.

    2012-04-09

    &&dLdI f{. L & ? P'3< a3Lc t xLQc32s_? 42...T3{3k VL!e Cat5 j/b) [&vvL,L t e{Q 4Ur te{Qc{3c2YLc p&?2e2&Q X r ?Z t e{ . ! 2Q C }2eL X t e{ . ! 2Q $ &vc...

  20. Bacteriology of cottage cheese: Sources of microorganisms causing spoilage and relative numbers at various stages during processing and storage. 

    E-Print Network [OSTI]

    Maury, James B

    1951-01-01

    ~gi h ~ 4' h I 'I a 8 . 1, ~* tk' gM W . j I 1 " -'; ' '" tsee~jA-~'e", . ig. :+ epeiAe?sr . . ~;"iI?4LiIX. :~r s?I: 4@, .I ~ 4~&rd if. :4s~ 6%54i~'lreeeuse 4t Qii. . ~' @&at, ' tee440% 54 ' of . L0$: ?NAssste! a. . . ' &'e, +?4%4~'4+~~4?I.... 8 (& ' lc )i @~4 8 l l :jjfg, I --4 ~ ~ ~Aj ~u 4 Il A8 C5P 850 gkpg5. A'j q4j, p I ". Ji1 7 ~ , l ~ gK' * . lj I' jp:;. 'i p . l 4 me ~Xj . a'jikkjjb4 'kfi~so, , W iLLl"-, g~W':, . ~. ~ Mes hqt, . 'k wis etc~ &os...

  1. Ebensburg folio, Pennsylvania 

    E-Print Network [OSTI]

    Butts, Charles, 1863-1946.

    1905-01-01

    ~zsisreet. diMrI'F44 BQ EMicer kcteet3 4ccQi, ~&? Eel'1$er rt GRtch ?t 'iezks 484 Vakvera~ wttb lkLreeJI, b-g5 bad ~teated tbet it bshe eb AatidL~'rr~ . t '0 ectido ixh t~ ~-'. ~ ~ a4 cQkvee& PeLleted . ~lg cr ' ~ 'r ead ?Bek:~ Rgb vere giveKL ee a feme ciao... MS' L~t~ @beg M. '' calves vere I. . ~i%'~ to eet et eve Qs~. + c4; age ~ ~~-'& ~t11 tbsp ead yf t:- -""-. . :rimeeti Thy j@r~ ~. . ';alf QCa~'~~ ~ ea ho P~p~74 ~+'QQ pQLQIQo H0 ~L ~&~ Q H 4@h eg pQ 4~a eZ eku 4~~~~ w& eR C&m @ALL~~. "~~ egml~a 'E...

  2. Measurement of B(d) mixing using opposite-side flavor tagging

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Coppage, Don; Hensel, Carsten; Moulik, Tania; Wilson, Graham Wallace

    2006-12-15

    identification algorithm can be found in Ref. [9]. DØ 0 1000 -1 -0.5 0 0.5 1 Muon jet charge N um be r o f e ve nt s (a) q(brec) 0 0 500 -1 -0.5 0 0.5 1 Muon jet charge N um be r o f e ve nt s (b) 0 250 -1 -0.5 0 0.5 1 Electron jet charge N um... for electrons QeJ. Here q#4;brec#7; is the charge of the muon from the reconstruction side. DØ 0 200 -1 -0.5 0 0.5 1 SV charge N um be r o f e ve nt s (a) q(brec) 0 0 1000 -1 -0.5 0 0.5 1 SV charge N um be r o f e ve nt s (b) 0 2000 -1 -0.5 0 0.5...

  3. Low voltage vertical recording preamplifier for hard disk drives 

    E-Print Network [OSTI]

    Mellachervu, Ramachandra Murthy

    2004-11-15

    CA1G mL + s2[CCgs+Cpi(C+Cgs)]g mNGmL 1 + s bracketleftBig 2C GmLAo + Cgs gmN + gpi(C+Cgs) gmNGmLAo bracketrightBig + s2 [2CCgs+Cpi(C+Cgs)]Aog mNGmL (6.22) The terms used have been shown in Fig.29. A1 = GmLRGmL where RGmL is the output resistance... Q2 Q4 Vout/2 Q3 RL Cpi Cpi GmL LR Cgs Ib 3Ib/8 3Ib/8 Vbias VCC VEE C Fig. 29. Schematic to understand signal feedthrough due to parasitic base-emitter ca- pacitor The equation can be simplified if we assume gmN >> GmLAo6 and can be written as, Vo Vin...

  4. An investigation of relationships between meso- and synoptic-scale phenomena 

    E-Print Network [OSTI]

    Wood, James Eugene

    1971-01-01

    . The figure shows the trough sloping westward from '04i . 0, &47' . ' / 'I I la 2:-, f WQQ. ' gf' , I g I. . I . ?, i&9 I +3~o . . --'; (a) 850 mb 34 ) 1- K . g(7!- . I , p6. (c) 500 mb 'r 'I 9" . 3O8 303 , . 3l 2 1 332 (b) 700 mb Fig. 6...'. '. '" "147 ~; C . r, t I' l. , 4 I -s 430 , 1I 1/0 3- 156 147 I 44, , $4 (a) 850 mb '652 6 fy, '". 534~53'4 &0 1540% P q'', -4 65$ 'g' )( C' ~i5~7 (c) 500 mb 0910 ' 88 I, ' ' 8196gp ', 70 -" - . - : . , '- ' ' ' ' ' ' . 'F4 0 . 97p 000...

  5. Waterfowl utilization characteristics of floodwater retarding structures in north-central Texas 

    E-Print Network [OSTI]

    Hobaugh, William Carl

    1977-01-01

    of the physical and limnological characteristics of 55 flood prevention lakes. Parameters +I IU Ql 0 E 0. 0 Ql Ql 0 QI Ql O IQ 4 lQ L Ql 5- I/I cL Ql IQ K L. LI QI QI CL Ol ) CU cC cC CU 0 O LI IU I IQ I- Ql 5- Ql Cll IU IV O lQ 4 IU I...- CO M IQ O 3 ~ 0 GL 0 E/) LL III z 0. cC Ql 0 lU CL Ql OI Ul QI OI IQ CL Ul O C O IQ Ql L 0 0 0 L 0 Ql IU CL Ql Lll CQ Shoreline development Surface area ++ ++ ++ Age Average depth Drainage area to surface area...

  6. An economic evaluation of fertilizer application to Coastal Bermudagrass under irrigation on Lufkin fine sandy loam 

    E-Print Network [OSTI]

    Prochaska, Frank Charles

    1958-01-01

    AZ:-V@~'. W. . ; j)~303;. ~t42@~6 W. 't5e':, X eqv Ny@ee4. . - gW':. Mi': 6e~m. qZ k '. 5g:~~ "'~M~'. 4pggiRCS; , . 'A~t?'. "Xgg8, . ' ?- ~qi ''Sijb] johns' A~S~i@tmeX'%e~~m = ', 1 il l:, . "i 'i":. ", , i:;:, :, . 'ilia. ;:;::. ::." ' Ag ggMSI iC!L V... ''. '. . . =, . '=;;;-"i-"' A&~Mf@$. C@';40 'g5$XS. ; @4i6"-Cli'PS~4. , 6$$ '0 . (@Bi?' ' 'Q~' Qm'MM') 1 (kg', K4'. X. 4AQCi~wWQw ) A~mC'. 3@~8 1 J +; r ! ~BV~~RVS - - SyeeQ4:. -jp~t44vide La;~assai-to. . ~-. 8? -4+-. '-NLlMqth? -: -. kaa~~ie& MM...

  7. FY12 Quarter 3 Computing Utilization Report – LANL

    SciTech Connect (OSTI)

    Wampler, Cheryl L. [Los Alamos National Laboratory; McClellan, Laura Ann [Los Alamos National Laboratory

    2012-07-25

    DSW continues to dominate the capacity workload, with a focus in Q3 on common model baselining runs in preparation for the Annual Assessment Review (AAR) of the weapon systems. There remains unmet demand for higher fidelity simulations, and for increased throughput of simulations. Common model baselining activities would benefit from doubling the resolution of the models and running twice as many simulations. Capacity systems were also utilized during the quarter to prepare for upcoming Level 2 milestones. Other notable DSW activities include validation of new physics models and safety studies. The safety team used the capacity resources extensively for projects involving 3D computer simulations for the Furrow series of experiments at DARHT (a Level 2 milestone), fragment impact, surety theme, PANTEX assessments, and the 120-day study. With the more than tripling of classified capacity computing resources with the addition of the Luna system and the safety team's imminent access to the Cielo system, demand has been met for current needs. The safety team has performed successful scaling studies on Luna up to 16K PE size-jobs with linear scaling, running the large 3D simulations required for the analysis of Furrow. They will be investigating scaling studies on the Cielo system with the Lustre file system in Q4. Overall average capacity utilization was impacted by negative effects of the LANL Voluntary Separation Program (VSP) at the beginning of Q3, in which programmatic staffing was reduced by 6%, with further losses due to management backfills and attrition, resulting in about 10% fewer users. All classified systems were impacted in April by a planned 2 day red network outage. ASC capacity workload continues to focus on code development, regression testing, and verification and validation (V&V) studies. Significant capacity cycles were used in preparation for a JOWOG in May and several upcoming L2 milestones due in Q4. A network transition has been underway on the unclassified networks to increase access of all ASC users to the unclassified systems through the Yellow Turquoise Integration (YeTI) project. This will help to alleviate the longstanding shortage of resources for ASC unclassified code development and regression testing, and also make a broader palette of machines available to unclassified ASC users, including PSAAP Alliance users. The Moonlight system will be the first capacity resource to be made available through the YETI project, and will make available a significant increase in cycles, as well as GPGPU accelerator technology. The Turing and Lobo machines will be decommissioned in the next quarter. ASC projects running on Cielo as part of the CCC-3 include turbulence, hydrodynamics, burn, asteroids, polycrystals, capability and runtime performance improvements, and materials including carbon and silicone.

  8. Tax decisions involving the cost method of inventory valuation 

    E-Print Network [OSTI]

    McMenamy, Bobby Benton

    1950-01-01

    '. ?1'pQ@lg'QP ig, ". t O'Q@ ". 'Q J. '~" @~i 8 GXG C4 S6 7) PQ. &3. C'5'c' 'P~$. C" 'v'1&~ PIC&/'~%CD%'b ". QCO~1"10@7'8 ZRGQ4 3;4-'i;", ZCQQgpy P&C. $~tQ jf&53 ~~'1 $1 lg ~CXXQi1 d') + s. 2 ( C ) c XZ 3iQC9 'Nl& ACt Gf 1~1'3 y v~l8 BO&~il-"". 'XC...~15QXCX 8 pPQVXSXGlh 'KVQ~ 'K'lg OGB'5 9" Q2g p~5Q~B l&PQBQCGG. 8211CC @18 DC'. i', $Q~NDg Qf 4-. !'w QQQX' Bit&11 LAC3M8 ROC & GZ'WZl66 Q. MXQGA~ 49 M16'- BCC&QQG~g f, Q?" 4V pX'GQU4510'1 Qa iI-'Q "36~'43%43. ~~ 81 t9. @18 ' gX153TXc?:XHg ig, g. '?XO...

  9. Depression among abused or neglected children in substitute care 

    E-Print Network [OSTI]

    Woodward, Gail Cohn

    1985-01-01

    CJ I OI CJ CO COCh 0?0?Q Q HIO 0 4J V t0 00 0 N t0 0 Cl 4J 0 Cl nl~ JO g 0 ttt 0 ?0 R M mW ?II M&?CI CJQYI NQN0?I 0 V t0 0 0 4J CJ I/I Q A ?a IOI 0?CO MCJ COI 0?mQ~ OC Cl 44 CI 4J 44 m04~ CO 4J 4J 44 5 A CI 0 Q... Ch CJ CO t?t U1 Cl '0 Q 00 0 44 IJ 0, 44 44 0 84?04 84A' 4J 44 0 IH 6 A t0 44 0 Q CO Q 4J JJ 0 8)8 ttl 44 CI Q 0 0 4J 0 al Cl 0 ?0 0 CI 44 04 M t0 A I A V ?n Cl o 0 0 C4 [00 A 26 the clinical group scores. Each...

  10. Minimally non-local nucleon-nucleon potentials with chiral two-pion exchange including Delta resonances

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

    Piarulli, M; Girlanda, L; Schiavilla, R; Perez, R Navarro; Amaro, J E; Arriola, E Ruiz

    2015-02-01

    We construct a coordinate-space chiral potential, including ?-isobar intermediate states in its two-pion-exchange component up to order Q3 (Q denotes generically the low momentum scale).The contact interactions entering at next-to-leading and next-to-next-to-next-to-leading orders (Q2 and Q4, respectively) are rearranged by Fierz transformations to yield terms at most quadratic in the relative momentum operator of the two nucleons. The low-energy constant multiplying these contact interactions are fitted to the 2013 Granada database, consisting of 2309 pp and 2982 np data (including, respectively, 148 and 218 normalizations) in the laboratory-energy range 0--300 MeV. For the total 5291 $pp$ and $np$ data inmore »this range, we obtain a ?2 /datum of roughly 1.3 for a set of three models characterized by long- and short-range cutoffs, RL and RS respectively, ranging from (RL,RS)=(1.2,0.8) fm down to (0.8,0.6) fm. The long-range (short-range) cutoff regularizes the one- and two-pion exchange (contact) part of the potential.« less

  11. Liouville Brownian motion at criticality

    E-Print Network [OSTI]

    Rémi Rhodes; Vincent Vargas

    2015-02-15

    In this paper, we construct the Brownian motion of Liouville Quantum Gravity with central charge $c=1$ (more precisely we restrict to the corresponding free field theory). Liouville quantum gravity with $c=1$ corresponds to two-dimensional string theory and is the conjectural scaling limit of large planar maps weighted with a $O(n=2)$ loop model or a $Q=4$-state Potts model embedded in a two dimensional surface in a conformal manner. Following \\cite{GRV1}, we start by constructing the critical LBM from one fixed point $x\\in\\mathbb{R}^2$ (or $x\\in\\S^2$), which amounts to changing the speed of a standard planar Brownian motion depending on the local behaviour of the critical Liouville measure $M'(dx)=-X(x)e^{2X(x)}\\,dx$ (where $X$ is a Gaussian Free Field, say on $\\mathbb{S}^2$). Extending this construction simultaneously to all points in $\\mathbb{R}^2$ requires a fine analysis of the potential properties of the measure $M'$. This allows us to construct a strong Markov process with continuous sample paths living on the support of $M'$, namely a dense set of Hausdorff dimension $0$. We finally construct the associated Liouville semigroup, resolvent, Green function, heat kernel and Dirichlet form. In passing, we extend to quite a general setting the construction of the critical Gaussian multiplicative chaos that was initiated in \\cite{Rnew7,Rnew12} and also establish new capacity estimates for the critical Gaussian multiplicative chaos.

  12. New method to measure proper motions of microlensed sources: Application to candidate free-floating-planet event MOA-2011-BLG-262

    SciTech Connect (OSTI)

    Skowron, Jan [Warsaw University Observatory, Al. Ujazdowskie 4, 00-478 Warszawa (Poland); Department of Astronomy, Ohio State University, 140 W. 18th Ave., Columbus, OH 43210 (United States); Udalski, Andrzej; Szyma?ski, Micha? K., E-mail: jskowron@astrouw.edu.pl, E-mail: udalski@astrouw.edu.pl, E-mail: msz@astrouw.edu.plm [Warsaw University Observatory, Al. Ujazdowskie 4, 00-478 Warszawa (Poland); and others

    2014-04-20

    We develop a new method to measure source proper motions in microlensing events, which can partially overcome problems due to blending. It takes advantage of the fact that the source position is known precisely from the microlensing event itself. We apply this method to the event MOA-2011-BLG-262, which has a short timescale t {sub E} = 3.8 day, a companion mass ratio q = 4.7 × 10{sup –3}, and a very high or high lens-source relative proper motion ?{sub rel} = 20 mas yr{sup –1} or 12 mas yr{sup –1} (for two possible models). These three characteristics imply that the lens could be a brown dwarf or a massive planet with a roughly Earth-mass 'moon'. The probability of such an interpretation would be greatly increased if it could be shown that the high lens-source relative proper motion was primarily due to the lens rather than the source. Based on the long-term monitoring data of the Galactic bulge from the Optical Gravitational Lensing Experiment, we measure the source proper motion that is small, ?{sub s}=(?2.3,?0.9)±(2.8,2.6) mas yr{sup ?1} in a (north, east) Galactic coordinate frame. These values are then important input into a Bayesian analysis of the event presented in a companion paper by Bennett et al.

  13. Physics in Ultra-strong Magnetic Fields

    E-Print Network [OSTI]

    Duncan, R C

    2000-01-01

    In magnetic fields stronger than B_Q = 4.4 X 10^13 Gauss, an electron'sLandau excitation energy exceeds its rest energy. I review the physics of thisstrange regime and some of its implications for the crusts and magneto- spheresof neutron stars. In particular, I describe how ultra-strong fields >> render the vacuum birefringent and capable of distorting and magnifying images ("magnetic lensing"); >> change the self-energy of electrons: as B increases they are first slightly lighter than $m_e$, then slightly heavier; >> cause photons to rapidly split and merge with each other; >> distort atoms into long, thin cylinders and molecules into strong, polymer-like chains; >> enhance the pair density in thermal pair-photon gases; >> stronglysuppress photon-electron scattering, and >> drive the vacuum itself unstable,at extremely large B. In a concluding section, I discuss recent observations of the spindownhistories of soft gamma repeaters and anomalous X-ray pulsars. The magnetarmodel gives a promising framework for...

  14. Physics in Ultra-strong Magnetic Fields

    E-Print Network [OSTI]

    Robert C. Duncan

    2000-02-23

    In magnetic fields stronger than B_Q = 4.4 X 10^13 Gauss, an electron's Landau excitation energy exceeds its rest energy. I review the physics of this strange regime and some of its implications for the crusts and magneto- spheres of neutron stars. In particular, I describe how ultra-strong fields >> render the vacuum birefringent and capable of distorting and magnifying images ("magnetic lensing"); >> change the self-energy of electrons: as B increases they are first slightly lighter than $m_e$, then slightly heavier; >> cause photons to rapidly split and merge with each other; >> distort atoms into long, thin cylinders and molecules into strong, polymer-like chains; >> enhance the pair density in thermal pair-photon gases; >> strongly suppress photon-electron scattering, and >> drive the vacuum itself unstable, at extremely large B. In a concluding section, I discuss recent observations of the spindown histories of soft gamma repeaters and anomalous X-ray pulsars. The magnetar model gives a promising framework for understanding these data.

  15. Minimally non-local nucleon-nucleon potentials with chiral two-pion exchange including $?$'s

    E-Print Network [OSTI]

    M. Piarulli; L. Girlanda; R. Schiavilla; R. Navarro Pérez; J. E. Amaro; E. Ruiz Arriola

    2015-02-16

    We construct a coordinate-space chiral potential, including $\\Delta$-isobar intermediate states in its two-pion-exchange component. The contact interactions entering at next-to-leading and next-to-next-to-next-to-leading orders ($Q^2$ and $Q^4$, respectively, $Q$ denoting generically the low momentum scale) are rearranged by Fierz transformations to yield terms at most quadratic in the relative momentum operator of the two nucleons. The low-energy constants multiplying these contact interactions are fitted to the 2013 Granada database, consisting of 2309 $pp$ and 2982 $np$ data (including, respectively, 148 and 218 normalizations) in the laboratory-energy range 0--300 MeV. For the total 5291 $pp$ and $np$ data in this range, we obtain a $\\chi^2$/datum of roughly 1.3 for a set of three models characterized by long- and short-range cutoffs, $R_{\\rm L}$ and $R_{\\rm S}$ respectively, ranging from $(R_{\\rm L},R_{\\rm S})=(1.2,0.8)$ fm down to $(0.8,0.6)$ fm. The long-range (short-range) cutoff regularizes the one- and two-pion exchange (contact) part of the potential.

  16. Latest Results of ILC High-Gradient R&D 9-cell Cavities at JLAB

    SciTech Connect (OSTI)

    Rongli Geng

    2008-02-11

    It has been over a year since JLAB started processing and testing ILC 9-cell cavities in the frame work of ILC high-gradient cavity R&D, aiming at the goal of a 35 MV/m gradient at a Q #4; of 1E10 with a yield of 90%. The necessary cavity processing steps include field flatness tuning, electropolishing (EP), hydrogen out-gassing under vacuum, high-pressure water rinsing, clean room assembly, and low temperature bake. These are followed by RF test at 2 Kelvin. Ultrasonic cleaning with Micro-90, an effective post-EP rinsing recipe discovered at JLAB, is routinely used. Seven industry manufactured 9-cell TESLAshape cavities are processed and tested repeatedly. So far, 33 EP cycles are accumulated, corresponding to more than 65 hours of active EP time. An emphasis put on RF testing is to discern cavity quench characteristics, including its nature and its location. Often times, the cavity performance is limited by thermal-magnetic quench instead of field emission. The quench field in some cavities is lower than 20 MV/m and remains unchanged despite repeated EP, implying material and/or fabrication defects. The quench field in some other cavities is high but changes unpredictably after repeated EP, suggesting processing induced defects. Based on our experience and results, several areas are identified where improvement is needed to improve cavity performance as well as yield.

  17. Minimally nonlocal nucleon-nucleon potentials with chiral two-pion exchange including ? resonances

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

    Piarulli, M.; Girlanda, L.; Schiavilla, R.; Pérez, R. Navarro; Amaro, J. E.; Arriola, E. Ruiz

    2015-02-26

    In this study, we construct a coordinate-space chiral potential, including ?-isobar intermediate states in its two-pion-exchange component up to order Q3 (Q denotes generically the low momentum scale). The contact interactions entering at next-to-leading and next-to-next-to-next-to-leading orders (Q2 and Q4, respectively) are rearranged by Fierz transformations to yield terms at most quadratic in the relative momentum operator of the two nucleons. The low-energy constant multiplying these contact interactions are fitted to the 2013 Granada database, consisting of 2309 pp and 2982 np data (including, respectively, 148 and 218 normalizations) in the laboratory-energy range 0–300 MeV. For the total 5291 $pp$more »and $np$ data in this range, we obtain a ?2 /datum of roughly 1.3 for a set of three models characterized by long- and short-range cutoffs, RL and RS respectively, ranging from (RL,RS)=(1.2,0.8) fm down to (0.8,0.6) fm. The long-range (short-range) cutoff regularizes the one- and two-pion exchange (contact) part of the potential.« less

  18. Elements of Greek tragedy in three Eugene O'Neill plays 

    E-Print Network [OSTI]

    Koinm, Albert Julius

    1963-01-01

    '-&o &%3 A eel ~Re~ AG"" VV'"L"XVZ K ~' ' 0 X f&Qkh M R~ SPY 8o Pe 6'bhWCC ~ =-'g* K@ Ey ZQk~~ SQP CAW'~ GR~~~BC ERA 5". '499~ 48VXCC QD 86VQi, CL~. ~G~K~ %~CD ~QQ I'LL tJ::N tNl5~ Qf &98 MQS So ~ 638v e. "~8'~ M mains g ~~ vre~M e Mxm'8... ~ -'Pe Se Se f'~ ZQZ' ll& ~q& ~WC~ QZ ~X Q~& ~%~%I XQ Q% FG~~' Q~ ~~Q Q4RG TJCQ'L 9. B'GQ 5F~@ ~ pPI?3QCC o l j AU~ ~ ~ . a. e :*' e i s s a 0 o s 0 e e e e o e o e s s XVe C JJKU3SXGii e s y s o e o e s o e o e @ o e LXST GF 56K'=3 CGPiSVL~M e a...

  19. The unexpected role of D waves in low-energy neutral pion photoproduction

    E-Print Network [OSTI]

    C. Fernandez-Ramirez

    2009-12-21

    It has been commonly assumed that low-energy neutral pion photoproduction from the proton can be described accounting only for S and P waves, and that higher partial waves are irrelevant. We have found that this assumption is not correct and that the inclusion of D waves is necessary to obtain a reliable extraction of the $E_{0+}$ multipole from experimental data. This is due in large measure to the spontaneous breaking of chiral symmetry in QCD which leads to very small S-wave contributions. This makes the usual partial wave expansion less accurate and although D waves are small, their contribution is enhanced through the interference with P waves, which compromises the S-wave extraction from data if D waves are not taken into account. In our work we have used Heavy Baryon Chiral Perturbation Theory to one loop, and up to ${\\cal O}(q^4)$, to account for the S and P waves, while D waves are added in an almost model-independent way using standard Born terms and vector mesons. We also show that higher partial waves do not play an important role.

  20. SELF-CONSISTENT SIZE AND VELOCITY DISTRIBUTIONS OF COLLISIONAL CASCADES

    SciTech Connect (OSTI)

    Pan, Margaret [Department of Astronomy, University of California, Berkeley, CA 94720 (United States); Schlichting, Hilke E., E-mail: mpan@astro.berkeley.edu, E-mail: hilke@ucla.edu [Department of Earth and Space Sciences, University of California, Los Angeles, CA 90095 (United States)

    2012-03-10

    The standard theoretical treatment of collisional cascades derives a steady-state size distribution assuming a single constant velocity dispersion for all bodies regardless of size. Here we relax this assumption and solve self-consistently for the bodies' steady-state size and size-dependent velocity distributions. Specifically, we account for viscous stirring, dynamical friction, and collisional damping of the bodies' random velocities in addition to the mass conservation requirement typically applied to find the size distribution in a steady-state cascade. The resulting size distributions are significantly steeper than those derived without velocity evolution. For example, accounting self-consistently for the velocities can change the standard q = 3.5 power-law index of the Dohnanyi differential size spectrum to an index as large as q = 4. Similarly, for bodies held together by their own gravity, the corresponding power-law index range 2.88 < q < 3.14 of Pan and Sari can steepen to values as large as q = 3.26. Our velocity results allow quantitative predictions of the bodies' scale heights as a function of size. Together with our predictions, observations of the scale heights for different-sized bodies for the Kuiper belt, the asteroid belt, and extrasolar debris disks may constrain the mass and number of large bodies stirring the cascade as well as the colliding bodies' internal strengths.

  1. 8D likelihood effective Higgs couplings extraction framework in h ? 4?

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

    Chen, Yi; Di Marco, Emanuele; Lykken, Joe; Spiropulu, Maria; Vega-Morales, Roberto; Univ. Paris-Sud, Orsay Cedex; Northwestern Univ., Evanston, IL; Xie, Si

    2015-01-23

    We present an overview of a comprehensive analysis framework aimed at performing direct extraction of all possible effective Higgs couplings to neutral electroweak gauge bosons in the decay to electrons and muons, the so called ‘golden channel’. Our framework is based primarily on a maximum likelihood method constructed from analytic expressions of the fully differential cross sections for h ? 4l and for the dominant irreducible $ q\\overline{q} $ ? 4l background, where 4l = 2e2?, 4e, 4?. Detector effects are included by an explicit convolution of these analytic expressions with the appropriate transfer function over all center of massmore »variables. Utilizing the full set of observables, we construct an unbinned detector-level likelihood which is continuous in the effective couplings. We consider possible ZZ, Z?, and ?? couplings simultaneously, allowing for general CP odd/even admixtures. A broad overview is given of how the convolution is performed and we discuss the principles and theoretical basis of the framework. This framework can be used in a variety of ways to study Higgs couplings in the golden channel using data obtained at the LHC and other future colliders.« less

  2. --No Title--

    U.S. Energy Information Administration (EIA) Indexed Site

    ... 5,908 Q 1,248 1,126 Q 1,123 Q Q Q 766 Principal Building Activity Education ... 9,874 Q 1,384 1,990 552 2,445 341 1,198...

  3. --No Title--

    Gasoline and Diesel Fuel Update (EIA)

    500,000 ... 7 Q 1 1 Q 1 Q Q Q 1 Principal Building Activity Education ... 386 Q 21 34 29 87 Q 56 39 97 Food Sales...

  4. Phonon-roton modes of liquid 4He beyond the roton in MCM-41

    SciTech Connect (OSTI)

    Azuah, Richard T NIST Center for Neutron Research , Gaithersburg, MD; Omar Diallo, Souleymane ORNL; Adams, Mark A. ISIS Facility, Rutherford Appleton Laboratory; Kirichek, Oleg ISIS Facility, Rutherford Appleton Laboratory; Glyde, Henry R University of Delaware

    2013-01-01

    We present neutron scattering measurements of the phonon-roton (P-R) mode of superfluid 4He confined in 47 A MCM-41 at T = 0.5 K at wave vectors, Q, beyond the roton wave vector (QR = 1.92 A-1). Measurements beyond the roton require access to high wave vectors (up to Q = 4 A-1) with excellent energy resolution and high statistical precision. The present results show for the first time that at T = 0.5 K the P-R mode in MCM-41 extends out to wave-vector Q 3.6 A-1 with the same energy and zero width (within precision) as observed in bulk superfluid 4He. Layer modes in the roton region are also observed. Specifically, the P-R mode energy, !Q, increases with Q for Q > QR and reaches a plateau at a maximum energy !Q = 2 where is the roton energy, = 0.74 0.01 meV in MCM-41. This upper limit means the P-R mode decays to two rotons when its energy exceeds 2 . It also means that the P-R mode does not decay to two layers modes. If the P-R could decay to two layer modes, !Q would plateau at a lower energy, !Q = 2 L where L = 0.60 meV is the energy of the roton like minimum of the layer mode. The observation of the P-R mode with energy up to 2 shows that the P-R mode and the layer modes are independent modes with apparently little interaction between them.

  5. Heavy Truck Engine Program

    SciTech Connect (OSTI)

    Nelson, Christopher

    2009-01-08

    The Heavy Duty Truck Engine Program at Cummins embodied three significant development phases. All phases of work strove to demonstrate a high level of diesel engine efficiency in the face of increasingly stringent emission requirements. Concurrently, aftertreatment system development and refinement was pursued in support of these efficiency demonstrations. The program's first phase focused on the demonstration in-vehicle of a high level of heavy duty diesel engine efficiency (45% Brake Thermal Efficiency) at a typical cruise condition while achieving composite emissions results which met the 2004 U.S. EPA legislated standards. With a combination of engine combustion calibration tuning and the development and application of Urea-based SCR and particulate aftertreatment, these demonstrations were successfully performed by Q4 of 2002. The second phase of the program directed efforts towards an in-vehicle demonstration of an engine system capable of meeting 2007 U.S. EPA legislated emissions requirements while achieving 45% Brake Thermal Efficiency at cruise conditions. Through further combustion optimization, the refinement of Cummins Cooled EGR architecture, the application of a high pressure common rail fuel system and the incorporation of optimized engine parasitics, Cummins Inc. successfully demonstrated these deliverables in Q2 of 2004. The program's final phase set a stretch goal of demonstrating 50% Brake Thermal Efficiency from a heavy duty diesel engine system capable of meeting 2010 U.S. EPA legislated emissions requirements. Cummins chose to pursue this goal through further combustion development and refinement of the Cooled EGR system architecture and also applied a Rankine cycle Waste Heat Recovery technique to convert otherwise wasted thermal energy to useful power. The engine and heat recovery system was demonstrated to achieve 50% Brake Thermal Efficiency while operating at a torque peak condition in second quarter, 2006. The 50% efficient engine system was capable of meeting 2010 emissions requirements through the application of NOx and particulate matter reduction techniques proven earlier in the program.

  6. High performance charge breeder for HIE-ISOLDE and TSR@ISOLDE applications

    SciTech Connect (OSTI)

    Shornikov, Andrey Mertzig, Robert C.; Wenander, Fredrik J. C.; Beebe, Edward N.; Pikin, Alexander

    2015-01-09

    We report on the development of the HEC{sup 2} (High Energy Compression and Current) charge breeder, a possible high performance successor to REXEBIS at ISOLDE. The new breeder would match the performance of the HIE-ISOLDE linac upgrade and make full use of the possible installation of a storage ring at ISOLDE (the TSR@ISOLDE initiative [1]). Dictated by ion beam acceptance and capacity requirements, the breeder features a 2–3.5 A electron beam. In many cases very high charge states, including bare ions up to Z=70 and Li/Na-like up to Z=92 could be requested for experiments in the storage ring, therefore, electron beam energies up to 150 keV are required. The electron-beam current density needed for producing ions with such high charge states at an injection rate into TSR of 0.5–1 Hz is between 10 and 20 kA/cm{sup 2}, which agrees with the current density needed to produce A/q<4.5 ions for the HIE-ISOLDE linac with a maximum repetition rate of 100 Hz. The first operation of a prototype electron gun with a pulsed electron beam of 1.5 A and 30 keV was demonstrated in a joint experiment with BNL [2]. In addition, we report on further development aiming to achieve CW operation of an electron beam having a geometrical transverse ion-acceptance matching the injection of 1{sup +} ions (11.5 ?m), and an emittance/energy spread of the extracted ion beam matching the downstream mass separator and RFQ (0.08 ?m normalized / ± 1%)

  7. Measurements on the 3He+?System at ANKE

    E-Print Network [OSTI]

    A. Khoukaz

    2010-11-03

    The differential and total cross-sections for the dp \\to 3He \\eta reaction have been measured in a high precision high statistics COSY-ANKE experiment near threshold using a continuous beam energy ramp up to an excess energy Q of 11.3 MeV with essentially 100% acceptance. The kinematics allowed the mean value of Q to be determined to about 9 keV. Evidence is found for the effects of higher partial waves for Q > 4 MeV. The very rapid rise of the total cross-section to its maximum value within 0.5 MeV of threshold implies a very large \\eta 3He scattering length and hence the presence of a quasi-bound state extremely close to threshold. In addition, differential and total cross-sections have been measured at excess energies of 19.5, 39.4, and 59.4 MeV over the full angular range. While at 19.5 MeV the results can be described in terms of s- and p-wave production, by 59.4 MeV higher partial waves are required. Including the 19.5 MeV point together with the near-threshold data in a global s- and p-wave fit gives a poorer overall description of the data though the position of the pole in the \\eta 3He scattering amplitude, corresponding to the quasi-bound or virtual state, is hardly changed.

  8. Catalytic fast pyrolysis of lignocellulosic biomass

    SciTech Connect (OSTI)

    Liu, Changjun; Wang, Huamin; Karim, Ayman M.; Sun, Junming; Wang, Yong

    2014-11-21

    Increasing energy demand, especially in the transportation sector, and soaring CO2 emissions necessitate the exploitation of renewable sources of energy. Despite the large variety of new energy Q3 carriers, liquid hydrocarbon still appears to be the most attractive and feasible form of transportation fuel taking into account the energy density, stability and existing infrastructure. Biomass is an abundant, renewable source of energy; however, utilizing it in a cost-effective way is still a substantial challenge. Lignocellulose is composed of three major biopolymers, namely cellulose, hemicellulose and lignin. Fast pyrolysis of biomass is recognized as an efficient and feasible process to selectively convert lignocellulose into a liquid fuel—bio-oil. However bio-oil from fast pyrolysis contains a large amount of oxygen, distributed in hundreds of oxygenates. These oxygenates are the cause of many negative properties, such as low heating values, high corrosiveness, high viscosity, and instability; they also greatly Q4 limit the application of bio-oil particularly as transportation fuel. Hydrocarbons derived from biomass are most attractive because of their high energy density and compatibility with the existing infrastructure. Thus, converting lignocellulose into transportation fuels via catalytic fast pyrolysis has attracted much attention. Many studies related to catalytic fast pyrolysis of biomass have been published. The main challenge of this process is the development of active and stable catalysts that can deal with a large variety of decomposition intermediates from lignocellulose. This review starts with the current understanding of the chemistry in fast pyrolysis of lignocellulose and focuses on the development of catalysts in catalytic fast pyrolysis. Recent progress in the experimental studies on catalytic fast pyrolysis of biomass is also summarized with the emphasis on bio-oil yields and quality.

  9. Chromosome abnormalities in primary ovarian cancer

    SciTech Connect (OSTI)

    Yonescu, R.; Currie, J.; Griffin, C.A.

    1994-09-01

    Chromosome abnormalities that are specific and recurrent may occur in regions of the genome that are involved in the conversion of normal cells to those with tumorigenic potential. Ovarian cancer is the primary cause of death among patients with gynecological malignancies. We have performed cytogenetic analysis of 16 ovarian tumors from women age 28-82. Three tumors of low malignant potential and three granulosa cell tumors had normal karyotypes. To look for the presence of trisomy 12, which has been suggested to be a common aberration in this group of tumors, interphase fluorescence in situ hybridization was performed on direct preparations from three of these tumors using a probe for alpha satellite sequences of chromosome 12. In the 3 preparations, 92-98 percent of the cells contained two copies of chromosome 12, indicating that trisomy 12 is not a universal finding in low grade ovarian tumors. Endometrioid carcinoma of the ovary is histologically indistinguishable from endometial carcinoma of the uterus. We studied 10 endometrioid tumors to determine the degree of genetic similarity between these two carcinomas. Six out of ten endometrioid tumors showed a near-triploid modal number, and one presented with a tetraploid modal number. Eight of the ten contained structural chromosome abnormalities, of which the most frequent were 1p- (5 tumors), 19q+ (3 tumors), 6q- or ins(6) (4 tumors), 3q- or 3q+ (4 tumors). These cytogenetic results resemble those reported for papillary ovarian tumors and differ from those of endometrial carcinoma of the uterus. We conclude that despite the histologic similarities between the endometrioid and endometrial carcinomas, the genetic abnormalities in the genesis of these tumors differ significantly.

  10. The equitable presentation for the quantum group $U_q(g)$ associated with a symmetrizable Kac-Moody algebra $g$

    E-Print Network [OSTI]

    Paul Terwilliger

    2005-07-22

    We consider the quantum group $U_q(g)$ associated with a symmetrizable Kac-Moody algebra $g$. We display a presentation for $U_q(g)$ that we find attractive; we call this the equitable presentation. For $g=sl_2$ the equitable presentation has generators $X,X^{-1},Y,Z$ and relations $X X^{-1} =1$, $X^{-1} X=1$, $\\frac{qXY-q^{-1}YX}{q-q^{-1}}=1$, $\\frac{qYZ-q^{-1}ZY}{q-q^{-1}}=1$, $\\frac{qZX-q^{-1}XZ}{q-q^{-1}}=1$.

  11. The quantum algebra $U_q(sl_2)$ and its equitable presentation

    E-Print Network [OSTI]

    Tatsuro Ito; Paul Terwilliger; Chih-wen Weng

    2005-07-22

    We show that the quantum algebra $U_q(sl_2)$ has a presentation with generators $x,x^{-1},y,z$ and relations $x x^{-1}=1$, $x^{-1} x=1$, $\\frac{qxy-q^{-1}yx}{q-q^{-1}}=1$, $\\frac{qyz-q^{-1}zy}{q-q^{-1}}=1$, $\\frac{qzx-q^{-1}xz}{q-q^{-1}}=1$. We call this the equitable presentation. We investigate the action of $x,x^{-1},y,z$ on finite-dimensional $U_q(sl_2)$-modules.

  12. SOUTHEAST REGIONAL CARBON SEQUESTRATION PARTNERSHIP (SECARB)

    SciTech Connect (OSTI)

    Kenneth J. Nemeth

    2004-09-01

    The Southeast Regional Carbon Sequestration Partnership (SECARB) is on schedule and within budget projections for the work completed during the first year of its two year program. Work during the semiannual period (third and fourth quarter) of the project (April 1--September 30, 2004) was conducted within a ''Task Responsibility Matrix.'' Under Task 1.0 Define Geographic Boundaries of the Region, Texas and Virginia were added during the second quarter of the project and no geographical changes occurred during the third or fourth quarter of the project. Under Task 2.0 Characterize the Region, general mapping and screening of sources and sinks has been completed, with integration and Geographical Information System (GIS) mapping ongoing. The first step focused on the macro level characterization of the region. Subsequent characterization will focus on smaller areas having high sequestration potential. Under Task 3.0 Identify and Address Issues for Technology Deployment, SECARB has completed a preliminary assessment of safety, regulatory, permitting, and accounting frameworks within the region to allow for wide-scale deployment of promising terrestrial and geologic sequestration approaches. Under Task 4.0 Develop Public Involvement and Education Mechanisms, SECARB has conducted a survey and focus group meeting to gain insight into approaches that will be taken to educate and involve the public. Task 5.0 and 6.0 will be implemented beginning October 1, 2004. Under Task 5.0 Identify the Most Promising Capture, Sequestration, and Transport Options, SECARB will evaluate findings from work performed during the first year and shift the focus of the project team from region-wide mapping and characterization to a more detailed screening approach designed to identify the most promising opportunities. Under Task 6.0 Prepare Action Plans for Implementation and Technology Validation Activity, the SECARB team will develop an integrated approach to implementing and setting up measurement, monitoring and verification (MMV) programs for the most promising opportunities. During this semiannual period special attention was provided to Texas and Virginia, which were added to the SECARB region, to ensure a smooth integration of activities with the other 9 states. Milestones completed and submitted during the third and fourth quarter included: Q3-FY04--Complete initial development of plans for GIS; and Q4-FYO4--Complete preliminary action plan and assessment for overcoming public perception issues.

  13. XCOM intrinsic dimensionality for low-Z elements at diagnostic energies

    SciTech Connect (OSTI)

    Bornefalk, Hans [Department of Physics, Royal Institute of Technology, SE-106 91 Stockholm (Sweden)

    2012-02-15

    Purpose: To determine the intrinsic dimensionality of linear attenuation coefficients (LACs) from XCOM for elements with low atomic number (Z = 1-20) at diagnostic x-ray energies (25-120 keV). H{sub 0}{sup q}, the hypothesis that the space of LACs is spanned by q bases, is tested for various q-values. Methods: Principal component analysis is first applied and the LACs are projected onto the first q principal component bases. The residuals of the model values vs XCOM data are determined for all energies and atomic numbers. Heteroscedasticity invalidates the prerequisite of i.i.d. errors necessary for bootstrapping residuals. Instead wild bootstrap is applied, which, by not mixing residuals, allows the effect of the non-i.i.d residuals to be reflected in the result. Credible regions for the eigenvalues of the correlation matrix for the bootstrapped LAC data are determined. If subsequent credible regions for the eigenvalues overlap, the corresponding principal component is not considered to represent true data structure but noise. If this happens for eigenvalues l and l + 1, for any l{<=}q, H{sub 0}{sup q} is rejected. Results: The largest value of q for which H{sub 0}{sup q} is nonrejectable at the 5%-level is q = 4. This indicates that the statistically significant intrinsic dimensionality of low-Z XCOM data at diagnostic energies is four. Conclusions: The method presented allows determination of the statistically significant dimensionality of any noisy linear subspace. Knowledge of such significant dimensionality is of interest for any method making assumptions on intrinsic dimensionality and evaluating results on noisy reference data. For LACs, knowledge of the low-Z dimensionality might be relevant when parametrization schemes are tuned to XCOM data. For x-ray imaging techniques based on the basis decomposition method (Alvarez and Macovski, Phys. Med. Biol. 21, 733-744, 1976), an underlying dimensionality of two is commonly assigned to the LAC of human tissue at diagnostic energies. The finding of a higher statistically significant dimensionality thus raises the question whether a higher assumed model dimensionality (now feasible with the advent of multibin x-ray systems) might also be practically relevant, i.e., if better tissue characterization results can be obtained.

  14. After runaway: The trans-Hill stage of planetesimal growth

    SciTech Connect (OSTI)

    Lithwick, Yoram [Department of Physics and Astronomy, Northwestern University, Evanston, IL 60208, USA and Center for Interdisciplinary Exploration and Research in Astrophysics (CIERA), Evanston, IL 60208 (United States)

    2014-01-01

    When planetesimals begin to grow by coagulation, they first enter an epoch of runaway, during which the biggest bodies grow faster than all the others. The questions of how runaway ends and what comes next have not been answered satisfactorily. We show that runaway is followed by a new stage—the 'trans-Hill stage'—that commences when the bodies that dominate viscous stirring ('big bodies') become trans-Hill, i.e., when their Hill velocity matches the random speed of the small bodies they accrete. Subsequently, the small bodies' random speed grows in lockstep with the big bodies' sizes, such that the system remains in the trans-Hill state. Trans-Hill growth is crucial for determining the efficiency of growing big bodies, as well as their growth timescale and size spectrum. Trans-Hill growth has two sub-stages. In the earlier one, which occurs while the stirring bodies remain sufficiently small, the evolution is collisionless, i.e., collisional cooling among all bodies is irrelevant. The efficiency of forming big bodies in this collisionless sub-stage is very low, ?10? << 1, where ? ? 0.005(a/AU){sup –1} is the ratio between the physical size of a body and its Hill radius. Furthermore, the size spectrum is flat (equal mass per size decade, i.e., q = 4). This collisionless trans-Hill solution explains results from previous coagulation simulations for both the Kuiper Belt and the asteroid belt. The second trans-Hill sub-stage commences once the stirring bodies grow big enough (>?{sup –1} × the size of the accreted small bodies). After that time, collisional cooling among small bodies controls the evolution. The efficiency of forming big bodies rises and the size spectrum becomes more top heavy. Trans-Hill growth can terminate in one of two ways, depending on the sizes of the small bodies. First, mutual accretion of big bodies can become significant and conglomeration proceeds until half of the total mass is converted into big bodies. This mode of growth may explain the observed size distributions of small bodies in the solar system and is explored in our subsequent work. Second, if the big bodies' orbits become separated by their Hill radius, oligarchy commences. This mode likely precedes the formation of fully fledged planets.

  15. c17a.xls

    Annual Energy Outlook [U.S. Energy Information Administration (EIA)]

    ... Q 26 19 Q 1,451 1,192 Q 17.9 16.3 Principal Building Activity Education ... Q 12 16 Q 1,384 1,990 Q 8.4 7.9 Food...

  16. --No Title--

    U.S. Energy Information Administration (EIA) Indexed Site

    ... 7 Q Q 2 4 5,908 Q Q 1,418 3,688 Principal Building Activity Education ... 386 Q Q 27 340 9,874 Q Q 1,017 8,586...

  17. Energy Information Administration - Commercial Energy Consumption...

    Gasoline and Diesel Fuel Update (EIA)

    ... Q Q Q Q 1,248 1,126 Q Q Q Principal Building Activity Education ... Q 143 175 Q 1,384 1,990 Q 103.1 87.7...

  18. The SM8 Universal Solvation Model Christopher J. Cramer and Donald G. Truhlar, University of Minnesota

    E-Print Network [OSTI]

    Truhlar, Donald G

    constants, redox potentials, solubilities, temperature-dependent absolute free energies of solvation pollutants, and the thermodynamics of processes taking place in electrochemical fuel cells. q1 q2 q3 q2 q1 q

  19. The impact of uncertainty and risk measures

    E-Print Network [OSTI]

    Jo, Soojin; Jo, Soojin

    2012-01-01

    papers indicating crude oil price shocks as a contributingdifferent measures of the crude oil price volatility series.of real average crude oil prices from 1957Q1 to 2010Q1

  20. Purchase Obligations, Earnings Persistence and Stock Returns

    E-Print Network [OSTI]

    Lee, Kwang June

    2010-01-01

    inventory and raw materials Shipbuilding, Railroad EquipmentMean Median Q1 Q3 Min Max Shipbuilding, Railroad Equipment

  1. Refined bounds on the number of connected compo- nents of sign ...

    E-Print Network [OSTI]

    2013-03-11

    Purdue University, West Lafayette, IN 47907 .... into account the dimensions of the intermediate varieties V1 = Zer(Q1, Rk), V2 = Zer({Q1, Q2}, Rk) etc. ...... we can assume that the tangent space Tx Vj is transversal to ?[1,q]. ?1 (z ) (recall.

  2. Approximation Techniques for Incompressible Flows with Heterogeneous Properties 

    E-Print Network [OSTI]

    Salgado Gonzalez, Abner Jonatan

    2011-10-21

    {velocity, P2{pressure. : 62 III 3D Iterative Algorithm. Exponential Porosity. Q1dc{velocity, Q1{ pressure. : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 63 IV 3D Splitting Algorithm. (Q1dc;Q1;Q1) discretization. : : : : : : : : : 64 V...: Reprinted with permission from: Finite Element Discretization of Darcy?s Equations with Pressure Dependent Poros- ity by V. Girault, F. Murat and A. Salgado. M2AN Math. Model. Nu- mer. Anal. DOI: 10.1051/m2an/2010019. Copyright 2010 by EDP Sciences. http...

  3. INFS 767 Fall 2000 Administrative RBAC

    E-Print Network [OSTI]

    Sandhu, Ravi

    ) Department Security Officer (DSO) Project Security Officer 1 (PSO1) Project Security Officer 2 (PSO2) 8© Ravi Sandhu 2000 URA97 GRANT MODEL: can-assign ARole Prereq Role Role Range PSO1 ED [E1,PL1) PSO2 ED [E2,PL2-assign ARole Prereq Cond Role Range PSO1 ED [E1,E1] PSO1 ED & ¬ P1 [Q1,Q1] PSO1 ED & ¬ Q1 [P1,P1] PSO2 ED [E2,E

  4. Sistemas No-Integrveis 6.1 O Mtodo WKB Dependente do Tempo

    E-Print Network [OSTI]

    de Aguiar, Marcus A. M.

    explicitamente as derivadas que entram na equação de Schroedinger obtemos q2 q1 #12;6 O Caso não-Integrável 68

  5. EXCITING OPPORTUNITIES TO ADVANCE FUSION ENERGY

    E-Print Network [OSTI]

    Control FRC (q > 1) (q Roadmap for MFE 99 by Taylor 9 MHD Stability in the MFE Roadmap Steady-State Integration Burning Plasma MHD Transport

  6. Photovoltaic System Pricing Trends: Historical, Recent, and Near...

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

    Laboratory. * Chung, D.; Davidson, C.; Fu, R.; Ardani, K. Margolis, R. (2015). U.S. Photovoltaic (PV) Prices and Cost Breakdowns: Q1 2015 Benchmarks for Residential, Commercial,...

  7. Teoria de la Computacion 1. Encuentre una gramatica libre del contexto para los siguientes lenguajes

    E-Print Network [OSTI]

    Merino, Criel

    ´atica libre del contexto que genere el lenguaje acep- tado por pila vac´ia del aut´omata de pila M = ({q0, q1

  8. --No Title--

    Gasoline and Diesel Fuel Update (EIA)

    500,000 ... 7 Q 1 1 0 1 2 1 Q Principal Building Activity Education ... 386 12 26 78 60 58 44 75 32 Food Sales...

  9. Photovoltaic (PV) Pricing Trends: Historical, Recent, and Near-Term Projections

    E-Print Network [OSTI]

    Feldman, David

    2014-01-01

    all. Super monocrystalline PV modules are currently the mostBloomberg New Energy Finance. PV Market Outlook, Q1 2012 (Solar Photovoltaic Industry: Solar PV industry outlook and

  10. Getting Ready for the Technical Assessment at Snowmass "Go ahead, make my FIRE"

    E-Print Network [OSTI]

    Plasma Conditions (Alpha Dominated) Q ~ 1 Q ~ 0.01 Q ~ 0.00001 Q ~ 0.001 Q ~ 0.01 NIF LMJ NIF LMJ T-3

  11. Inverse Stochastic Linear Programming

    E-Print Network [OSTI]

    2007-01-05

    Keywords: Inverse Optimization, Stochastic Programming, Decomposition ..... i ) i = q + 1,··· , r. (29) .... Royal Statistical Society, Series B, 17 (1955) 173–184.

  12. High Operating Temperature Heat Transfer Fluids for Solar Thermal...

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

    High Operating Temperature Heat Transfer Fluids for Solar Thermal Power Generation FY13 Q1 High Operating Temperature Heat Transfer Fluids for Solar Thermal Power Generation FY13...

  13. --No Title--

    Gasoline and Diesel Fuel Update (EIA)

    226 188 94 68 Q N Food Service ... 297 282 94 149 Q Q Health Care ... 129 124 49 65 Q 1 Inpatient...

  14. Direct s-CO2 Reciever Development | Department of Energy

    Office of Environmental Management (EM)

    Solar Receiver for Use in a Supercritical CO2 Recompression Cycle - FY13 Q1 High-Temperature Solar Thermoelectric Generators (STEG) Near-Blackbody Enclosed Particle Receiver...

  15. c22.pdf

    U.S. Energy Information Administration (EIA) Indexed Site

    0.82 Pacific ... Q Q Q 1.8 Q 0.79 Fuel Oil Consumption Fuel Oil Expenditures Table C22. Fuel Oil Consumption and Expenditure...

  16. MEASURING THE ABUNDANCE OF SUB-KILOMETER-SIZED KUIPER BELT OBJECTS USING STELLAR OCCULTATIONS

    SciTech Connect (OSTI)

    Schlichting, Hilke E. [Department of Earth and Space Science, UCLA, 595 Charles East Young Drive East, Los Angeles, CA 90095 (United States); Ofek, Eran O.; Gal-Yam, Avishay [Faculty of Physics, Weizmann Institute of Science, P.O. Box 26, Rehovot 76100 (Israel); Sari, Re'em [Racah Institute of Physics, Hebrew University, Jerusalem 91904 (Israel); Nelan, Edmund P.; Livio, Mario [Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218 (United States); Wenz, Michael [Goddard Space Flight Center, 8800 Greenbelt Road, Greenbelt, MD 20771 (United States); Muirhead, Philip [Department of Astronomy, California Institute of Technology, MC 130-33, Pasadena, CA 91125 (United States); Javanfar, Nikta, E-mail: hilke@ucla.edu [Department of Physics, Physics Engineering and Astronomy, Queen's University, 99 University Avenue, Kingston, Ontario K7L 3N6 (Canada)

    2012-12-20

    We present here the analysis of about 19,500 new star hours of low ecliptic latitude observations (|b| {<=} 20 Degree-Sign ) obtained by the Hubble Space Telescope's Fine Guidance Sensors over a time span of more than nine years, which is in addition to the {approx}12, 000 star hours previously analyzed by Schlichting et al. Our search for stellar occultations by small Kuiper Belt Objects (KBOs) yielded one new candidate event corresponding to a body with a 530 {+-} 70 m radius at a distance of about 40 AU. Using bootstrap simulations, we estimate a probability of Almost-Equal-To 5% that this event is due to random statistical fluctuations within the new data set. Combining this new event with the single KBO occultation reported by Schlichting et al. we arrive at the following results: (1) the ecliptic latitudes of 6. Degree-Sign 6 and 14. Degree-Sign 4 of the two events are consistent with the observed inclination distribution of larger, 100-km-sized KBOs. (2) Assuming that small, sub-kilometer-sized KBOs have the same ecliptic latitude distribution as their larger counterparts, we find an ecliptic surface density of KBOs with radii larger than 250 m of N(r > 250 m) = 1.1{sup +1.5}{sub -0.7} Multiplication-Sign 10{sup 7} deg{sup -2}; if sub-kilometer-sized KBOs have instead a uniform ecliptic latitude distribution for -20 Degree-Sign < b < 20 Degree-Sign then N(r > 250 m) = 4.4{sup +5.8}{sub -2.8} Multiplication-Sign 10{sup 6} deg{sup -2}. This is the best measurement of the surface density of sub-kilometer-sized KBOs to date. (3) Assuming the KBO size distribution can be well described by a single power law given by N(> r){proportional_to}r{sup 1-q}, where N(> r) is the number of KBOs with radii greater than r, and q is the power-law index, we find q = 3.8 {+-} 0.2 and q = 3.6 {+-} 0.2 for a KBO ecliptic latitude distribution that follows the observed distribution for larger, 100-km-sized KBOs and a uniform KBO ecliptic latitude distribution for -20 Degree-Sign < b < 20 Degree-Sign , respectively. (4) Regardless of the exact power law, our results suggest that small KBOs are numerous enough to satisfy the required supply rate for the Jupiter family comets. (5) We can rule out a single power law below the break with q > 4.0 at 2{sigma}, confirming a strong deficit of sub-kilometer-sized KBOs compared to a population extrapolated from objects with r > 45 km. This suggests that small KBOs are undergoing collisional erosion and that the Kuiper Belt is a true analog to the dust producing debris disks observed around other stars.

  17. Materials for Advanced Ultrasupercritical Steam Turbines Task 4: Cast Superalloy Development

    SciTech Connect (OSTI)

    Thangirala, Mani

    2015-09-30

    The Steam Turbine critical stationary structural components are high integrity Large Shell and Valve Casing heavy section Castings, containing high temperature steam under high pressures. Hence to support the development of advanced materials technology for use in an AUSC steam turbine capable of operating with steam conditions of 760°C (1400°F) and 35 Mpa (5000 psia), Casting alloy selection and evaluation of mechanical, metallurgical properties and castability with robust manufacturing methods are mandated. Alloy down select from Phase 1 based on producability criteria and creep rupture properties tested by NETL-Albany and ORNL directed the consortium to investigate cast properties of Haynes 282 and Haynes 263. The goals of Task 4 in Phase 2 are to understand a broader range of mechanical properties, the impact of manufacturing variables on those properties. Scale up the size of heats to production levels to facilitate the understanding of the impact of heat and component weight, on metallurgical and mechanical behavior. GE Power & Water Materials and Processes Engineering for the Phase 2, Task 4.0 Castings work, systematically designed and executed casting material property evaluation, multiple test programs. Starting from 15 lbs. cylinder castings to world’s first 17,000 lbs. poured weight, heavy section large steam turbine partial valve Haynes 282 super alloy casting. This has demonstrated scalability of the material for steam Turbine applications. Activities under Task 4.0, Investigated and characterized various mechanical properties of Cast Haynes 282 and Cast Nimonic 263. The development stages involved were: 1) Small Cast Evaluation: 4 inch diam. Haynes 282 and Nimonic 263 Cylinders. This provided effects of liquidus super heat range and first baseline mechanical data on cast versions of conventional vacuum re-melted and forged Ni based super alloys. 2) Step block castings of 300 lbs. and 600 lbs. Haynes 282 from 2 foundry heats were evaluated which demonstrated the importance of proper heat treat cycles for Homogenization, and Solutionizing parameters selection and implementation. 3) Step blocks casting of Nimonic 263: Carried out casting solidification simulation analysis, NDT inspection methods evaluation, detailed test matrix for Chemical, Tensile, LCF, stress rupture, CVN impact, hardness and J1C Fracture toughness section sensitivity data and were reported. 4) Centrifugal Casting of Haynes 282, weighing 1400 lbs. with hybrid mold (half Graphite and half Chromite sand) mold assembly was cast using compressor casing production tooling. This test provided Mold cooling rates influence on centrifugally cast microstructure and mechanical properties. Graphite mold section out performs sand mold across all temperatures for 0.2% YS; %Elongation, %RA, UTS at 1400°F. Both Stress-LMP and conditional Fracture toughness plots data were in the scatter band of the wrought alloy. 5) Fundamental Studies on Cooling rates and SDAS test program. Evaluated the influence of 6 mold materials Silica, Chromite, Alumina, Silica with Indirect Chills, Zircon and Graphite on casting solidification cooling rates. Actual Casting cooling rates through Liquidus to Solidus phase transition were measured with 3 different locations based thermocouples placed in each mold. Compared with solidification simulation cooling rates and measurement of SDAS, microstructure features were reported. The test results provided engineered casting potential methods, applicable for heavy section Haynes 282 castings for optimal properties, with foundry process methods and tools. 6) Large casting of Haynes 282 Drawings and Engineering FEM models and supplemental requirements with applicable specifications were provided to suppliers for the steam turbine proto type feature valve casing casting. Molding, melting and casting pouring completed per approved Manufacturing Process Plan during 2014 Q4. The partial valve casing was successfully cast after casting methods were validated with solidification simulation analysis and the casting met NDT inspection and a

  18. Annual Hanford Seismic Report for Fiscal Year 2010

    SciTech Connect (OSTI)

    Rohay, Alan C.; Clayton, Ray E.; Sweeney, Mark D.; Devary, Joseph L.; Hartshorn, Donald C.

    2010-12-27

    The Hanford Seismic Assessment Program (HSAP) provides an uninterrupted collection of high-quality raw and processed seismic data from the Hanford Seismic Network for the U.S. Department of Energy and its contractors. The HSAP is responsible for locating and identifying sources of seismic activity and monitoring changes in the historical pattern of seismic activity at the Hanford Site. The data are compiled, archived, and published for use by the Hanford Site for waste management, natural phenomena hazards assessments, and engineering design and construction. In addition, the HSAP works with the Hanford Site Emergency Services Organization to provide assistance in the event of a significant earthquake on the Hanford Site. The Hanford Seismic Network and the Eastern Washington Regional Network consist of 44 individual sensor sites and 15 radio relay sites maintained by the Hanford Seismic Assessment Team. During FY 2010, the Hanford Seismic Network recorded 873 triggers on the seismometer system, which included 259 seismic events in the southeast Washington area and an additional 324 regional and teleseismic events. There were 210 events determined to be local earthquakes relevant to the Hanford Site. One hundred and fifty-five earthquakes were detected in the vicinity of Wooded Island, located about eight miles north of Richland just west of the Columbia River. The Wooded Island events recorded this fiscal year were a continuation of the swarm events observed during fiscal year 2009 and reported in previous quarterly and annual reports (Rohay et al. 2009a, 2009b, 2009c, 2010a, 2010b, and 2010c). Most events were considered minor (coda-length magnitude [Mc] less than 1.0) with the largest event recorded on February 4, 2010 (3.0Mc). The estimated depths of the Wooded Island events are shallow (averaging approximately 1.5 km deep) placing the swarm within the Columbia River Basalt Group. Based upon the last two quarters (Q3 and Q4) data, activity at the Wooded Island area swarm has largely subsided. Pacific Northwest National Laboratory will continue to monitor for activity at this location. The highest-magnitude events (3.0Mc) were recorded on February 4, 2010 within the Wooded Island swarm (depth 2.4 km) and May 8, 2010 on or near the Saddle Mountain anticline (depth 3.0 km). This latter event is not considered unusual in that earthquakes have been previously recorded at this location, for example, in October 2006 (Rohay et al. 2007). With regard to the depth distribution, 173 earthquakes were located at shallow depths (less than 4 km, most likely in the Columbia River basalts), 18 earthquakes were located at intermediate depths (between 4 and 9 km, most likely in the pre-basalt sediments), and 19 earthquakes were located at depths greater than 9 km, within the crystalline basement. Geographically, 178 earthquakes were located in known swarm areas, 4 earthquakes occurred on or near a geologic structure (Saddle Mountain anticline), and 28 earthquakes were classified as random events. The Hanford Strong Motion Accelerometer (SMA) network was triggered several times by the Wooded Island swarm events and the events located on or near the Saddle Mountain anticline. The maximum acceleration value recorded by the SMA network during fiscal year 2010 occurred February 4, 2010 (Wooded Island swarm event), approximately 2 times lower than the reportable action level for Hanford facilities (2% g) with no action required.

  19. Impediments to Predicting Site Response: Seismic Property Estimation and Modeling Simplifications

    E-Print Network [OSTI]

    Guzina, Bojan

    energy to heat through friction, viscosity, permanent deformations, and thermal relaxation. On the other site response. Seismic waves are attenuated by scattering (Sc Q-1 ) and from anelastic processes by heterogeneities within the medium. i Q-1 includes multiple physical processes, such as the conver- sion of seismic

  20. Further Discussion on Proposed Approach for Assessing Balancing

    E-Print Network [OSTI]

    requirements for each BA can be met by resources within each BA (with exception of long term Mid-C hydro Power Capable Resources: In Region BA Hydro Q1 Non-Hydro Q1 Avista Corporation 71% 29% Idaho Power Company 70 Characteristics of the Power System · Ability of the system to respond to changes in supply and demand of power

  1. Z .Thin Solid Films 372 2000 212 217 Z .Na in selenized Cu In,Ga Se on Na-containing and Na-free2

    E-Print Network [OSTI]

    Rockett, Angus

    of the substrate glass on standard Z . Z .production Cu In Ga Se CIGS -based solar cells fabricated by selenization; Selenides2 1. Introduction Z .Production of large quantities of Cu In Ga Se1yx x 2 Z . Z .CIGS -based solar solar cell performance. Impurities, both U Corresponding author. Tel.: q1-217-333-0417; fax: q1

  2. Planetary Nebulae as astronomical tools, Gdansk, POLAND, June 28 -July 2, 2005 c M. Steffen et al., AIP, 2005 Modeling X-ray Emission from

    E-Print Network [OSTI]

    update steps (operator splitting): (a) Q(t) advection Q1(t +t) (b) Q1(t +t) diffusion Q2(t +t) energy update at constant (c) Q2(t +t) radiation Q (t +t) energy update at constant For step (b), we solve flux to the saturation value given by Eq.(5). Ionization is frozen during step (b), being updated

  3. Z .Sensors and Actuators 78 1999 138142 www.elsevier.nlrlocatersna

    E-Print Network [OSTI]

    Bashir, Rashid

    the backside of double-sided polished wafers to release the thin silicon membranes. The zero-bias capacitance. Tel.: q1-765-496-6229; fax: q1-765-494- 6441 The condenser type capacitive microphones sense . Pedersen et al. have reported condenser microphones fabricated by micro-machining of polyimide on silicon

  4. Fields Institute University of Ottawa, Ontario Canada June 30 July 4, 2008 http://www.fields.utoronto.ca/programs/scientific/07-08/analytic/

    E-Print Network [OSTI]

    Waldschmidt, Michel

    Approximation An Introduction to Irrationality and Transcendence Methods. Michel Waldschmidt 3 Auxiliary/q = a/b, the inequality a b - p q 1 bq holds. For an irrational real number x, on the contrary, for any > 0 there exists a rational number p/q such that x - p q 1 q2 · This yields an irrationality

  5. MATHEMATICS OF COMPUTATION Volume 00, Number 0, Xxxx XXXX, Pages 000 000

    E-Print Network [OSTI]

    Luskin, Mitchell

    , the elastic energy density attains its minimum value below the transformation temperature on a set SO3U1 SO3UN;1.1 where SO3 is the group of proper rotations de ned by SO3 = Q 2 R33 : QT = Q,1 and detQ = 1

  6. In SIAM J. Numer. Anal., 35 : 1998, 376-392. FINITE ELEMENT ANALYSIS OF MICROSTRUCTURE FOR THE

    E-Print Network [OSTI]

    Luskin, Mitchell

    -convex and is minimized on a set of deformation gradients SO3U1 ::: SO3UM for M 1; where SO3 is the set of proper rotations, that is, SO3 = Q 2 R33 : QT = Q,1 and detQ = 1 ; where R33 is the set of all 3 3 real matrices

  7. ON A REAL ANALOGUE OF BEZOUT INEQUALITY AND THE ...

    E-Print Network [OSTI]

    2014-07-12

    Jul 12, 2014 ... into account the dimensions of the intermediate varieties V1 = Zer(Q1, Rk), V2 = Zer({Q1 ...... that the tangent space Tx Vj is transversal to ??1. [1,q] ..... Department of Mathematics, Purdue University, West Lafayette, IN 47907.

  8. c36.xls

    Annual Energy Outlook [U.S. Energy Information Administration (EIA)]

    Education ... 293 Q Q Q 1.04 Q Q Q 0.31 Q Q Q Health Care... Q Q 19 8 Q 1.06 1.08 1.16 Q Q 0.02 0.03...

  9. c36a.xls

    Gasoline and Diesel Fuel Update (EIA)

    Education ... 293 Q Q Q 1.04 Q Q Q 0.31 Q Q Q Health Care... Q Q 19 8 Q 1.06 1.08 1.16 Q Q 0.02 0.03...

  10. Energy Information Administration - Commercial Energy Consumption...

    Annual Energy Outlook [U.S. Energy Information Administration (EIA)]

    Education ... 293 Q Q Q 1.04 Q Q Q 0.31 Q Q Q Health Care... Q Q 19 8 Q 1.06 1.08 1.16 Q Q 0.02 0.03...

  11. INFS 767 Fall 2001 Administrative RBAC

    E-Print Network [OSTI]

    Sandhu, Ravi

    Security Officer (DSO) Project Security Officer 1 (PSO1) Project Security Officer 2 (PSO2) 8© Ravi Sandhu 2001 URA97 GRANT MODEL: can-assign ARole Prereq Role Role Range PSO1 ED [E1,PL1) PSO2 ED [E2,PL2) DSO-assign ARole Prereq Cond Role Range PSO1 ED [E1,E1] PSO1 ED & ¬ P1 [Q1,Q1] PSO1 ED & ¬ Q1 [P1,P1] PSO2 ED [E2,E

  12. Oddification of the cohomology of type A Springer varieties

    E-Print Network [OSTI]

    Lauda, Aaron D

    2012-01-01

    We identify the ring of odd symmetric functions introduced by Ellis and Khovanov as the space of skew polynomials fixed by a natural action of the Hecke algebra at q=-1. This allows us to define graded modules over the Hecke algebra at q=-1 that are `odd' analogs of the cohomology of type A Springer varieties. The graded module associated to the full flag variety corresponds to the quotient of the skew polynomial ring by the left ideal of nonconstant odd symmetric functions. The top degree component of the odd cohomology of Springer varieties is identified with the corresponding Specht module of the Hecke algebra at q=-1.

  13. From Decay to Complete Breaking: Pulling the Strings in SU(2) Yang-Mills Theory

    SciTech Connect (OSTI)

    Pepe, M.; Wiese, U.-J.

    2009-05-15

    We study (2Q+1) strings connecting two static charges Q in (2+1)D SU(2) Yang-Mills theory. While the fundamental (2) string between two charges Q=(1/2) is unbreakable, the adjoint (3) string connecting two charges Q=1 can break. When a (4) string is stretched beyond a critical length, it decays into a (2) string by gluon pair creation. When a (5) string is stretched, it first decays into a (3) string, which eventually breaks completely. The energy of the screened charges at the ends of a string is well described by a phenomenological constituent gluon model.

  14. Higher Order Discontinuous Finite Element Methods for Discrete Ordinates Thermal Radiative Transfer 

    E-Print Network [OSTI]

    Maginot, Peter G

    2015-07-28

    The linear discontinuous finite element method (LDFEM) is the current work horse of the radiation transport community. The popularity of LDFEM is a result of LDFEM (and its Q1 multi-dimensional extensions) being both ...

  15. c18a.xls

    Gasoline and Diesel Fuel Update (EIA)

    ... Q 38 Q Q 1,572 Q Q 24.3 Q Principal Building Activity Education ... 5 39 Q 549 2,445 Q 8.8 16.0 Q Food...

  16. c19a.xls

    Gasoline and Diesel Fuel Update (EIA)

    ... 21 Q 16 Q Q 1,119 21.2 Q 14.5 Principal Building Activity Education ... 15 6 11 1,198 640 1,027 12.8 9.4 10.7...

  17. --No Title--

    Annual Energy Outlook [U.S. Energy Information Administration (EIA)]

    Concrete (Block or Poured) ... 10,832 1,216 629 247 332 1,033 1,742 Concrete Panels ... 6,559 1,815 Q Q Q Q 1,963 Siding or Shingles...

  18. Energy Information Administration - Commercial Energy Consumption...

    Annual Energy Outlook [U.S. Energy Information Administration (EIA)]

    ... Q 137 Q Q 1,123 Q Q 122.1 Q Principal Building Activity Education ... 45 198 Q 552 2,445 341 81.0 80.9 Q Food...

  19. --No Title--

    Gasoline and Diesel Fuel Update (EIA)

    ... 7 Q Q 2 4 5,908 Q Q 1,748 3,448 Principal Building Activity Education ... 386 Q 28 107 248 9,874 Q 332 4,202 5,299...

  20. --No Title--

    U.S. Energy Information Administration (EIA) Indexed Site

    ... 7 Q Q Q 2 3 5,908 Q Q Q 1,516 3,036 Principal Building Activity Education ... 386 281 60 31 14 Q 9,874 3,696 2,911...

  1. 2008 WIND TECHNOLOGIES MARKET REPORT

    E-Print Network [OSTI]

    Bolinger, Mark

    2010-01-01

    December 17, 2008. New Energy Finance (NEF). 2009. Q1 WindLondon, UK: New Energy Finance. North American ElectricMW (Hays 2009) and New Energy Finance (NEF) predicts 4,900 –

  2. Preliminary Evaluation of the Impact of the Section 1603 Treasury Grant Program on Renewable Energy Deployment in 2009

    E-Print Network [OSTI]

    Bolinger, Mark

    2010-01-01

    s/News.asp New Energy Finance (NEF). 2009a. USQ4 WindLondon, UK: New Energy Finance. _________. 2009b. Q1 WindLondon, UK: New Energy Finance. _________. 2008. US Wind

  3. Preliminary Evaluation of the Section 1603 Treasury Grant Program for Renewable Power Projects in the United States

    E-Print Network [OSTI]

    Bolinger, Mark

    2012-01-01

    s/News.asp New Energy Finance (NEF). 2009a. USQ4 WindLondon, UK: New Energy Finance. _________. 2009b. Q1 WindLondon, UK: New Energy Finance. _________. 2008. US Wind

  4. 2009 Wind Technologies Market Report

    E-Print Network [OSTI]

    Wiser, Ryan

    2010-01-01

    Monthly. Bloomberg New Energy Finance. 2010a. Q1 Wind MarketOutlook. February 2010. Bloomberg New Energy Finance.Bloomberg New Energy Finance. 2010b. Q2 Wind Market Outlook.

  5. High-Efficiency Low-Cost Solar Receiver for Use in a Supercritical...

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

    Low-Cost Solar Receiver for Use in a Supercritical CO2 Recompression Cycle - FY13 Q1 High-Efficiency Low-Cost Solar Receiver for Use in a Supercritical CO2 Recompression Cycle -...

  6. Europaisches Patentamt European Patent Office

    E-Print Network [OSTI]

    Church, George M.

    Europaisches Patentamt European Patent Office Office europeen des brevets ® Publication number: o 303 459 A2 @ EUROPEAN PATENT APPLICATION ® Application number: 88307391.8 @ Int. C1.4: C 12 Q 1

  7. Analisi Matematica 2 per Matematica Esercizi 17 maggio 2012

    E-Print Network [OSTI]

    Marconi, Umberto

    (x, z): x p + z q = 1 in una rotazione completa attorno all'asse z. 2. Esercizio. Determinare il rotazione si chiama sferoide schiacciato nel caso in cui la rotazione avvenga intorno all'asse minore, si

  8. What is visual structure? That which allows you to identify a object?

    E-Print Network [OSTI]

    Lewicki, Michael S.

    #12;Surface normals The unit surface normal is ^n = n |n| = (-p, -q, 1)T 1 + p2 + q2 Now we can (edges, blobs, junctions, etc) · feature classes (e.g. orientation, depth, illumination, and reflectance

  9. Laboratories to Explore the Frontiers of Plasma Science VLBACHANDRA

    E-Print Network [OSTI]

    Dominated) Q ~ 1 Q ~ 0.01 Q ~ 0.00001 Q ~ 0.001 Q ~ 0.01 NIF LMJ NIF LMJ T-3 1965 T-3 1968 Laser 1996 Direct

  10. Status of Next Step Option Study on Fusion Ignition Research Experiment

    E-Print Network [OSTI]

    Conditions (Alpha Dominated) Q ~ 1 Q ~ 0.01 Q ~ 0.00001 Q ~ 0.001 Q ~ 0.01 NIF LMJ NIF LMJ T-3 1965 T-3 1968

  11. Burning Plasma Science: The Challenge and Opportunity

    E-Print Network [OSTI]

    Dominated) Q ~ 1 Q ~ 0.01 Q ~ 0.00001 Q ~ 0.001 Q ~ 0.01 NIF LMJ NIF LMJ T-3 1965 T-3 1968 Laser 1996 Direct

  12. Physics Analysis of FIRE UFA 2nd Burning PlasmaWorkshop

    E-Print Network [OSTI]

    trajectories. Everything else is predictive · Supported the correlation between the q=1 surface and termination ­ 150 MHz for 2D T , H or He3 minority · High Frequency Fast Wave · Optional /Partial replacement

  13. High-Efficiency Receivers for Supercritical Carbon Dioxide Cycles...

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

    More Documents & Publications High-Efficiency Low-Cost Solar Receiver for Use in a Supercritical CO2 Recompression Cycle - FY13 Q1 High-Efficiency Receivers for...

  14. Technology Performance Exchange

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

    Q3 Deliverable: Develop Site Workflows and Design Website Layout Q3 GoNo-Go DOE Decision Point: Passed Q1 Milestone: Develop Data Entry Forms Q2 Milestone: Release Technology...

  15. Mechanical behavior and magnetic separation of quasi-one-dimensional SnO2 nanostructures: A technique for achieving monosize

    E-Print Network [OSTI]

    Wang, Zhong L.

    thermal annealing was able to prepare Q1D nanostructures.20­23 The ball mill- ing method has also been collision among steel balls. During the milling process, the impurities originated from the milling jar

  16. (1, 0, 2) and (1, 2, 1

    E-Print Network [OSTI]

    2014-09-08

    Quiz 1 solutions, Section ALL. (10 pts.) Find a vector v perpendicular to the plane containing (0, 0, 2), (1, 0, 2) and (1, 2, 1). Solution. Let P = (0, 0, 2), Q = (1, 0, ...

  17. Decentralized Wastewater Management Solutions for Improved Public Health Protection and Reclamation: Optimization and Application

    E-Print Network [OSTI]

    Naik, Kartiki Shirish

    2014-01-01

    C=(9.89 x 10 4 )Q 1.35 Sludge incineration C=(8.77 x 10 4 )Qdollars/100,000 capita incineration of sludge 7 Bibliography

  18. Tobacco Control in North Dakota, 2004-2012: Reaching for Higher Ground

    E-Print Network [OSTI]

    Rosenbaum, Daniel J.; Barnes, Richard L.; Glantz, Stanton A.

    2012-01-01

    posted to Local Coordinators grantees only site. All schoolboards of health support Q1 Grantees encouraging all schools4. Develop a list of steps grantees Q2 Center should take to

  19. Dr. Heinzer Exam 2 Review

    E-Print Network [OSTI]

    firé' Q1/ . Let V be an abelian group with generators (111,112, '03) that has ... by de?ning :w = T(v) for each 1) E V. Assume that Mr) = ccz(93 - 1)} is the minimal.

  20. --No Title--

    Annual Energy Outlook [U.S. Energy Information Administration (EIA)]

    226 Q N 1,255 Q N Food Service ... 297 27 Q 1,654 264 Q Health Care ... 129 26 4 3,163 1,899 733 Inpatient...

  1. c6.xls

    Gasoline and Diesel Fuel Update (EIA)

    ... 3,482 3,611 5,714 3,208 18.67 12.52 16.68 20.50 1.59 1.25 1.43 1.81 Concrete Panels ... Q 1,877 4,661 2,967 Q 12.55 16.16 19.37 Q 1.53 1.69...

  2. PTG exam 2322011 short answers 75. For this cyclic process: 0dUQW

    E-Print Network [OSTI]

    Zevenhoven, Ron

    PTG exam 2322011 ­ short answers 75. For this cyclic process: 0dUQW a. Q1 + W2 + Q2 + W3 = 0 W3 = ( Q1 + W2 + Q2) = (180 + 50 200) = 30 J; Given off ­W3 = 30 J. Or, if also taking into consideration input W2, then total given off W3 ­ W2 = 20 J (system gain + 20 J) b

  3. The Second Law of Thermodynamics Chemistry CHEM 213W

    E-Print Network [OSTI]

    Ronis, David M.

    ) It is impossi- ble to devise an engine operating in a cycle which does work by taking heat from a single heat is a Carnot refrigerator. If we adjust the sizes of E and R such that all the work is used to run the Carnot Q1 Q1 1 2 W= Q2 C H C where C is a Carnot engine and where the sizes of the Carnot engine and our

  4. A complete characterization of termination of Hans ZANTEMA

    E-Print Network [OSTI]

    Utrecht, Universiteit

    A complete characterization of termination of 0 p 1 q ! 1 r 0 s Hans ZANTEMA Universiteit Utrecht@fmi.uni­passau.de Abstract We completely characterize termination of one­rule string rewriting systems of the form 0 p 1 q ! 1 r 0 s for every choice of positive integers p, q, r, and s. For the simply terminating cases, we

  5. A new computational approach to the synthesis of fixed order controllers 

    E-Print Network [OSTI]

    Malik, Waqar Ahmad

    2008-10-10

    ) is the same as the number of variations of ak+1(s+1) ^Pk(ak+1s). Suppose ^Pk(ak+1s) = q0 +q1s+:::+qn+k rsn+k r. Then, (s+ 1) ^Pk(ak+1s) = q0 + (q1 +q0)s+ (q2 +q1)s2 +:::+ (qn+k r +qn+k r 1)sn+k r +qn+k rsn+k r. Since qi +qi 1 is of the same sign as either qi..., then the characteristic polynomial for the closed loop system given below must be Hurwitz: (s) = (s;n0; ;nm;d0;:::;dm 1) = smDp(s)| {z } P0(s) +n0Np(s)|{z} P1(s) + +nmsmNp(s)| {z } Pm+1(s) +d0 Dp(s)|{z} Pm+2(s) + +dm 1sm 1Dp(s)| {z } P2m(s) : The problem...

  6. Three body kinematic endpoints in SUSY models with non-universal Higgs masses.

    E-Print Network [OSTI]

    Lester, Christopher G; Parker, Michael A; White, Martin J

    ˜L, c˜L) ? g˜q 1.5% (u˜R, c˜R) ? g˜q 2.3% g˜ ? ?˜±1 qq¯ 6.8% (u˜L, c˜L) ? ?˜+1 q 63% g˜ ? ?˜01qq¯ 2.2% (u˜L, c˜L) ? ?˜+2 q 2.5% g˜ ? ?˜02qq¯ 3.4% (d˜L, s˜L) ? ?˜01q 2.1% (d˜R, s˜R) ? ?˜01q 98% (d˜L, s˜L) ? ?˜02q 30% (d˜R, s˜R) ? ?˜02q 1% (d˜L, s˜L) ? ?...

  7. Anisotropic Mesh Adaptation for the Finite Element Solution of Anisotropic Diffusion Problems

    E-Print Network [OSTI]

    Li, Xianping

    2011-12-31

    the definition of the heat flux q (1.5), the problem (1.4) is an anisotropic diffusion problem with significant anisotropy due to the large ratio ??/??. One goal in the plasma physics research is to control the thermonuclear fusion power by magnetic confinement... the definition of the heat flux q (1.5), the problem (1.4) is an anisotropic diffusion problem with significant anisotropy due to the large ratio ??/??. One goal in the plasma physics research is to control the thermonuclear fusion power by magnetic confinement...

  8. Heating of semiconductor devices in electric Markus Brunk and Ansgar Jungel

    E-Print Network [OSTI]

    Jüngel, Ansgar

    -consistent electric potential V read as tn-q-1 divJn = -R(n, p), t p+q-1 divJp = -R(n, p), (1) t(3 2 kBnTn)-divJw +Jn ·V = W(n,Tn)- 3 2 kBTnR(n, p), (2) sV = q(n- p-C(x)), (3) where q is the elementary cha (mixed) finite elements. Heating effects from numerical simulations in a pn-junction diode and a clipper

  9. Approximate String Joins in a Database (Almost) for Free Luis Gravano Panagiotis G. Ipeirotis H. V. Jagadish

    E-Print Network [OSTI]

    Gravano, Luis

    1AiQ.Pos - R2AjQ.Pos k AND R2AjQ.Pos - R1AiQ.Pos k AND LEN(R1.Ai) - LEN(R2.Aj) k AND LEN(R2.Aj) - LEN(R1.Ai) k GROUP BY R1.A0, R2.A0, R1.Ai, R2.Aj HAVING COUNT(*) LEN(R1.Ai)+q-1 - k*q AND COUNT(*) LEN(R2.Aj)+q-1 - k*q AND edit distance(R1.A

  10. Vector Norms and Matrix Norms 6.1 Normed Vector Spaces

    E-Print Network [OSTI]

    Gallier, Jean

    R, if , 0, then p p + q q . () (2) For any two vectors u, v 2 E, we have nX i=1 |uivi| kukp kvkq . () #12;6.1. NORMED VECTOR SPACES 377 For p > 1 and 1/p + 1/q = 1, the inequality nX i=1 |uivi| nX i=1 |ui|p 1/p nX i=1 |vi|q 1/q is known as H¨older's inequality. For p = 2, it is the Cauchy

  11. Varit de Nakajima associe un Carquois.

    E-Print Network [OSTI]

    Sabourin, Hervé

    . On associe à Q une matrice de Cartan C = (C ij ), dé#28;nie par : i 6= j; c ij = c ji = nombre de #29;èches#28;nit de même : RQ (v) = M a2Q 1 Hom(V s(a) ; V t(a) ) = M a2Q 1 Hom(C s(a) ; C t(a) ) RQ (v) = RQ = t v(2d + (2I C)v) On va dé#28;nir maintenant un produit dans RQ (v), de la manière suivante : Soit V

  12. HAZARDOUS MATERIALS EMERGENCY RESPONSE

    E-Print Network [OSTI]

    ANNEX Q HAZARDOUS MATERIALS EMERGENCY RESPONSE #12;ANNEX Q - HAZARDOUS MATERIALS EMERGENCY RESPONSE 03/10/2014 v.2.0 Page Q-1 PROMULGATION STATEMENT Annex Q: Hazardous Materials Emergency Response, and contents within, is a guide to how the University conducts a response specific to a hazardous materials

  13. Interval methods for computing various refinements of Nash equilibria

    E-Print Network [OSTI]

    Sainudiin, Raazesh

    Interval methods for computing various refinements of Nash equilibria Bartlomiej Jacek Kubica, assumptions on their knowledge, ... Concepts: Dominant strategy equilibrium. The Nash equilibrium. The core of a game (for cooperative games). ... #12;Nash equilibrium Let the game (X1 ,...,Xn ;q1 ,...,qn

  14. Biochemistry 118Q Parental Selection and Genetic Enhancements: Problems or Potential?

    E-Print Network [OSTI]

    Brutlag, Doug

    Iris Jovel Biochemistry 118Q 1 Parental Selection and Genetic Enhancements: Problems-medical uses--such as genetic enhancement and engineering--are concurrently discovered. With such high demand of the autonomy of the child. Should parents select for their child to be very fit to #12;Iris Jovel Biochemistry

  15. Design-Space Exploration for CMOS Photonic Processor Vladimir Stojanovi!a

    E-Print Network [OSTI]

    Batten, Christopher

    advances Q1,ER in building high-throughput, energy-efficient photonic net4or5s for core-to-core and core a re^uired optical po4er envelope, [ig. 3a, the physical layout of the net4or5 follo4s a `- shape

  16. A stability theorem for concordance embeddings Guo-Wu Meng, Hong Kong

    E-Print Network [OSTI]

    (N`+)) In the diagram Q = 1 S1 , X+ is X together with a disjoint point, and S is the* * unit circle viewed both+fi+fi21+fl) ss2n-5(FOE) ~=Coker(Z[ss x ss] Z[ss x ss] -! Z[ss x ss

  17. An Experimental Comparison of Human and Automatic Music Segmentation Justin de Nooijer,*1

    E-Print Network [OSTI]

    Veltkamp, Remco

    , the experiments were designed to answer the following questions: Q1. Is there enough agreement in human melodyAn Experimental Comparison of Human and Automatic Music Segmentation Justin de Nooijer,*1 Frans works need to be decomposed into segments and voices. One would expect that methods that model human

  18. "Table HC14.1 Housing Unit Characteristics by West Census Region...

    U.S. Energy Information Administration (EIA) Indexed Site

    in 5 or More Unit Buildings",14.4,3,0.6,2.4 "Mobile Homes",1.2,0.3,"Q",0.2 "Year of Construction" "1939 or Before",14.7,2.2,0.5,1.7 "1940 to 1949",7.4,1.6,"Q",1.4 "1950 to...

  19. For discussion only Email & Calendaring

    E-Print Network [OSTI]

    Turner, Monica G.

    -its for data center aggregation with all responses as positive or neutral, no responses were negative. ·Three diminution of service Email & Calendaring Data Center Aggregation Computer Bundles Demand Management Space Q1 and calendaring with all responses as positive or neutral, no responses were negative. ·"No brainer

  20. Auxiliary materials for Paper Amazon forests did not green-up during the 2005 drought

    E-Print Network [OSTI]

    Myneni, Ranga B.

    of methods to calculate standardized anomalies of EVI, precipitation and radiation not given in the main text) Landcover: A vegetation map at 1x1 km2 spatial resolution (MOD12Q1) is used to identify forest pixels contains the AOT at 550 nm at daily frequency. 1.4 Radiation Data Monthly solar radiation data at 1o x1o

  1. 1 An automated tool for detection of FLAIR-hyperintense white-matter lesions in 2 Multiple Sclerosis

    E-Print Network [OSTI]

    Gaser, Christian

    -matter lesions in 2 Multiple Sclerosis 3 PaulQ1 Schmidt a,b,1 , Christian Gaser c,d,1 , Milan Arsic a , Dorothea segmentation 22 FLAIR 23 Multiple Sclerosis 24 Voxel-based morphometry 25In Multiple Sclerosis (MS), detection. 43© 2011 Published by Elsevier Inc. 4445 46 47 48 Introduction 49 Multiple Sclerosis (MS

  2. ITC-12/APFA'01 December 10-14, 2001

    E-Print Network [OSTI]

    ) Electricity Generation Equivalent Q > 1 ~ Advanced Tokamak Study Reactor Technologies Core Program EffortsEnergy Emphasized Efforts LongLong--Term R & D IssuesTerm R & D Issues Basic/Fundamental ResearchBasic/FundamentalMagneto-- electric/Magnetelectric/Magnet System/SafetySystem/Safety ICFICF Structural MaterialsStructural Materials

  3. c25.xls

    Gasoline and Diesel Fuel Update (EIA)

    ... 17 28 25 13 510 684 534 269 32.8 40.9 46.2 49.8 Metal Panels ... Q 30 43 34 Q 1,050 1,541 986 Q 28.7 27.8 34.8...

  4. c10.xls

    Annual Energy Outlook [U.S. Energy Information Administration (EIA)]

    ... 83 81 22 72 Q 1,294 1,319 443 849 214 64.3 61.6 49.0 84.3 Q Metal Panels ... 102 112 84 134 32 1,665 1,492 1,287 2,394 1,074...

  5. Photonic polarization gears for ultra-sensitive angular measurements -Supplementary Information

    E-Print Network [OSTI]

    Marrucci, Lorenzo

    Photonic polarization gears for ultra-sensitive angular measurements - Supplementary Information with the single-photon photonic gear (q = 10 and m = 2q +1 = 21) for different values of initial state phase i: {0 photonic gears. The photonic gear concept based on hybrid polarization- OAM states can be adopted also

  6. Holstein model and Peierls instability in one-dimensional boson-fermion lattice gases E. Pazy and A. Vardi

    E-Print Network [OSTI]

    Vardi, Amichay

    to fermion superfluidity. Furthermore, novel phenomena are predicted, such as the formation of composite in a Q1D configuration without ex- plicit periodic confinement, here we study a system subject also band needs to be considered and one can expand boson- and fermion-field operators in terms of the one-mode

  7. Zero-error capacities and very different sequences (Preliminary version)

    E-Print Network [OSTI]

    Simonyi, Gábor

    of a set DC Q1 any two sequences of which IU'e well-separated. Once again, what is limsup .!:.log are indexed by the different elements of X. Shannon's basic model of information transmission described one transmission would mean X= Y and W(yix) = 1- 6.,11 where 6.,11 is Kronecker's delta. To counterbalance random

  8. October 1986 R. H. Johnson 721 Lower-Tropospheric Warming and Drying in Tropical Mesoscale Convective Systems

    E-Print Network [OSTI]

    Johnson, Richard H.

    October 1986 R. H. Johnson 721 Lower-Tropospheric Warming and Drying in Tropical Mesoscale components of tropical mesoscale convective systems. It is found that while the apparent heat source Q1 of mesoscale downdrafts within the mesoscale convective systems. The warming and drying at low levels

  9. Energy Information Administration - Commercial Energy Consumption...

    Annual Energy Outlook [U.S. Energy Information Administration (EIA)]

    176 421 Q 1,566 2,986 1,357 112.1 141.2 Q Principal Building Activity Education ... 248 385 187 3,191 4,359 2,324 77.6 88.4...

  10. --No Title--

    Gasoline and Diesel Fuel Update (EIA)

    ... 5,908 4,613 2,396 2,217 N 1,295 606 Q Q Principal Building Activity Education ... 9,874 2,070 1,232 839 N 7,804 Q 1,671...

  11. The topology of terminal quartic 3-folds

    E-Print Network [OSTI]

    Kaloghiros, Anne-Sophie

    2007-06-20

    complexK = ((KQ,W ), (KC,W, F )) on E and, in particular, the following resolution of QE: 0? QE ? a0?QE0 ? a1?QE1 ? a2?QE2 ? 0. I omit results related to the Hodge filtration. The weight spectral sequence reads: wE p,q 1 = H q(Ep,C). The spectral sequence...

  12. A SIMPLE METHOD FOR ESTIMATING THE FOOD CONSUMPTION OF FISH POPULATIONS FROM GROWTH DATA AND

    E-Print Network [OSTI]

    CONVERSION EXPERIMENTS} DANIEL PAULy2 ABSTRACf Experimental data on the gross food conversion efficiency model can be used to compute the food consumption per unit biomass of an age-structured fish population difficult to obtain is the average food conswnption per unit biomass (Q1B) of each group. The present study

  13. Passive torque regulation in an underactuated flapping wing robotic insect

    E-Print Network [OSTI]

    Wood, Robert

    , the Berkeley Micromechanical Flying Insect (MFI) is a FWMAV platform with the ability to execute a range angles of attack [1]. The associated reduction in complexity has allowed this aeromechanical platform. 1: A car differential balances output torques using an underactuated mechanism. Degree of freedom q1

  14. Contents lists available at ScienceDirect journal homepage: www.elsevier.com/locate/enpol

    E-Print Network [OSTI]

    Firestone, Jeremy

    2011 Keywords: Wind power Offshore wind power Levelized cost of energy Breakeven priceQ1 a b s t r a c in CO2 and other harmful pollutants. The private cost of offshore wind power is lower than that of most other new renewable energy technologies, though it is more costly than land-based wind power and most

  15. 4000 cm D2 MAGNET D3 MAGNET

    E-Print Network [OSTI]

    Tokyo, University of

    MONITOR D2 MAGNET S2 STEERING HORIZONTAL BEAM PIPE SUPER-KAMIOKANDE TANK 1350mm LEAD SHIELD LEAD SHIELD SUPER-KAMIOKANDE TANK C4 COLLIMATOR Q1 QUADROPOLE M2 BEAM MONITOR D3 BENDING MAGNET Q2 QUADRO- POLE

  16. The water entry of decelerating spheres Jeffrey M. Aristoff,1

    E-Print Network [OSTI]

    Bush, John W.M.

    negligible decelera- tion over the time scale of cavity collapse. In general, how- ever, hydrodynamic forces angle a, and the cavitation number Q= p-pv / 1/2 U0 2 , where p is the local water pressure and pv is the water vapor pressure. In our study, Q 1, so the creation of cavitation bubbles in the liquid need

  17. Absolute cross sections for photoionization of Xe$^{q+}$ ions (1 $\\le$ q $\\le$ 5) at the 3d ionization threshold

    E-Print Network [OSTI]

    Schippers, S; Buhr, T; Borovik, A; Hellhund, J; Holste, K; Huber, K; Schäfer, H -J; Schury, D; Klumpp, S; Mertens, K; Martins, M; Flesch, R; Ulrich, G; Rühl, E; Jahnke, T; Lower, J; Metz, D; Schmidt, L P H; Schöffler, M; Williams, J B; Glaser, L; Scholz, F; Seltmann, J; Viefhaus, J; Dorn, A; Wolf, A; Ullrich, J; Müller, A

    2014-01-01

    The photon-ion merged-beams technique has been employed at the new Photon-Ion spectrometer at PETRA III (PIPE) for measuring multiple photoionization of Xe$^{q+}$ (q=1-5) ions. Total ionization cross sections have been obtained on an absolute scale for the dominant ionization reactions of the type h\

  18. Million U.S. Housing Units Total U.S...........................

    Annual Energy Outlook [U.S. Energy Information Administration (EIA)]

    PropaneLPG... 5.6 4.9 3.8 N N Q 1.1 Built-inStove-top Grills Use a Built-inStove-top Grill... 4.9 4.0 3.4 Q Q Q Q Do Not...

  19. TableHC2.9.xls

    Gasoline and Diesel Fuel Update (EIA)

    PropaneLPG... 5.6 4.2 Q Q Q 1.3 Built-inStove-top Grills Use a Built-inStove-top Grill... 4.9 3.5 0.3 Q 0.6 Q Do...

  20. "Table HC3.9 Home Appliances Characteristics by Owner-Occupied...

    U.S. Energy Information Administration (EIA) Indexed Site

    ",39,26.5,21.3,1.7,1.1,0.8,1.5 "PropaneLPG",5.6,4.9,3.8,"N","N","Q",1.1 "Built-inStove-top Grills" "Use a Built-inStove-top Grill",4.9,4,3.4,"Q","Q","Q","Q" "Do Not Use a...

  1. " Million U.S. Housing Units"

    U.S. Energy Information Administration (EIA) Indexed Site

    Gas",39,24.4,3.1,3.9,5.7,1.8 "PropaneLPG",5.6,4.2,"Q","Q","Q",1.3 "Built-inStove-top Grills" "Use a Built-inStove-top Grill",4.9,3.5,0.3,"Q",0.6,"Q" "Do Not Use a...

  2. Table HC2.9 Home Appliances Characteristics by Type of Housing...

    Gasoline and Diesel Fuel Update (EIA)

    PropaneLPG... 5.6 4.2 Q Q Q 1.3 Built-inStove-top Grills Use a Built-inStove-top Grill... 4.9 3.5 0.3 Q 0.6 Q Do...

  3. Safe Prime Generation with a Combined Sieve Michael J. Wiener

    E-Print Network [OSTI]

    International Association for Cryptologic Research (IACR)

    Safe Prime Generation with a Combined Sieve Michael J. Wiener Cryptographic Clarity, 20 Hennepin St p and (p - 1)/2 are prime. This note describes a method of generating safe primes that is considerably faster than repeatedly generating random primes q until p = 2q + 1 is also prime. Key words. Safe

  4. Safe Prime Generation with a Combined Sieve Michael J. Wiener

    E-Print Network [OSTI]

    International Association for Cryptologic Research (IACR)

    Safe Prime Generation with a Combined Sieve Michael J. Wiener Cryptographic Clarity, 20 Hennepin St p and (p 1)=2 are prime. This note describes a method of generating safe primes that is considerably faster than repeatedly generating random primes q until p = 2q + 1 is also prime. Key words. Safe primes

  5. C Gormezano OV FTU 2004 OVERVIEW OF THE FTU RESULTS by C. Gormezano

    E-Print Network [OSTI]

    and the ECRH teams EURATOM/ENEA Frascati, Italy Compact all metallic device (circular) R=0.93m, a=0.3m, Bt 8T plasmas: reaching q=1 sufficient to fuel plasma center ? #12;8 C Gormezano OV FTU 2004 Steady e

  6. FY11 Joint Research Target: Status and Planning on

    E-Print Network [OSTI]

    Princeton Plasma Physics Laboratory

    FY11 Joint Research Target: Status and Planning on Alcator C-Mod Jerry Hughes Including slides from C-Mod Activity Q1 Develop a preliminary research plan coordinated among the three facilities, delineating the planned experiments aimed at developing understanding of the physics mechanisms responsible

  7. ~ioikerfacialStrategies, Tissue Engineering, Angela K. Dillow

    E-Print Network [OSTI]

    Barron, Annelise E.

    tension at the air--liquid interface of the alveoli (the network of air sacs that perhrm gas exchange Norlhwestern Unive~it%/,Evansfon, iirlinois Pulmonary surfactnnt, or lung surhctanr ILS), is a natural.syricfed into twcs different. classes: "'natural" and ""snnQ1eticn LS replaccaaaents, So-called r~atural LS

  8. CONTROL ISSUES IN THE DESIGN OF A GAS TURBINE CYCLE FOR CO2 CAPTURE

    E-Print Network [OSTI]

    Foss, Bjarne A.

    CONTROL ISSUES IN THE DESIGN OF A GAS TURBINE CYCLE FOR CO2 CAPTURE Query Sheet Q1: AU: short title OF A GAS TURBINE CYCLE FOR CO2 CAPTURE Lars Imsland, Dagfinn Snarheim, and Bjarne A. Foss Department-closed / gas turbine cycle for capture. Some control strategies and their interaction with the process design

  9. On the Static Diffie-Hellman Problem on Elliptic Curves over Extension Fields

    E-Print Network [OSTI]

    International Association for Cryptologic Research (IACR)

    On the Static Diffie-Hellman Problem on Elliptic Curves over Extension Fields Robert Granger Claude@computing.dcu.ie Abstract. We show that for any elliptic curve E(Fqn ), if an adversary has access to a Static Diffie-Hellman Problem (Static DHP) oracle, then by making O(q1- 1 n+1 ) Static DHP oracle queries during an initial

  10. The Euler equations in fluid mechanics relative to a rotating-translating reference frame

    E-Print Network [OSTI]

    Bridges, Tom

    velocity and space velocity is X = Q(x + d) + Q x + q . (1.1) Define the body angular velocity by = QT Q is such that r = × r , for any r R3 , := 1 2 3 . The body angular velocity is to be contrasted with the spatial angular velocity ­ the angular velocity viewed from the spatial frame ­ which is spatial := QQT

  11. Z .Journal of Contaminant Hydrology 51 2001 112 www.elsevier.comrlocaterjconhyd

    E-Print Network [OSTI]

    Hu, Qinhong "Max"

    in the unsaturated, fractured welded tuff Z .within the Exploratory Studies Facility ESF at Yucca Mountain, NV repository at Yucca Mountain. While fast and localized fracture flow has ) Corresponding author. Fax: q1 continuum model for simulating transient flow and transport at Yucca Mountain. An extensive set

  12. Electromechanical instability on dielectric polymer surface: Modeling and experiment

    E-Print Network [OSTI]

    Park, Harold S.

    Electromechanical instability on dielectric polymer surface: Modeling and experiment Harold S. Park this by modifying the Q1P0 formulation of Simo et al. [1], and adapting it to the electromechanical coupling on the critical electric fields that are necessary to induce electromechanical instabilities such as creasing

  13. "Table HC12.11 Home Electronics Characteristics by Midwest Census...

    U.S. Energy Information Administration (EIA) Indexed Site

    "1.",26.3,5.8,4.3,1.5 "2.",3.6,0.9,0.6,"Q" "3 or More",0.6,"Q","Q","Q" "Plasma Television Sets",3.6,0.7,0.6,"Q" "1.",2.7,0.6,0.5,"Q" "2 or More",0.9,"Q","Q","Q"...

  14. " Million U.S. Housing Units"

    U.S. Energy Information Administration (EIA) Indexed Site

    "2.",3.6,2.9,0.2,"Q",0.2,"Q" "3 or More",0.6,0.4,"Q","N","Q","N" "Plasma Television Sets",3.6,2.6,0.3,"Q",0.4,"Q" "1.",2.7,2.1,0.2,"Q","Q","Q" "2 or...

  15. "Table HC3.11 Home Electronics Characteristics by Owner-Occupied...

    U.S. Energy Information Administration (EIA) Indexed Site

    "2.",3.6,3,2.6,"Q","Q","Q","Q" "3 or More",0.6,0.5,0.4,"Q","N","Q","N" "Plasma Television Sets",3.6,2.8,2.2,"Q","Q","Q","Q" "1.",2.7,2.1,1.8,"Q","Q","Q","N" "2 or...

  16. "Table HC4.11 Home Electronics Characteristics by Renter-Occupied...

    U.S. Energy Information Administration (EIA) Indexed Site

    "2.",3.6,0.7,0.3,"Q","Q",0.2,"Q" "3 or More",0.6,"Q","N","N","N","Q","N" "Plasma Television Sets",3.6,0.8,0.4,"Q","Q",0.3,"Q" "1.",2.7,0.6,0.2,"Q","Q","Q","Q" "2 or...

  17. Click to edit Master subtitle style Internship Development Program

    E-Print Network [OSTI]

    Heller, Barbara

    Click to edit Master subtitle style 12 3 2 NCARB Internship Development Program Basic information (Q&A) ARC Workshop for Architecture By: Hyesun Jeong #12;Click to edit Master subtitle style 12 3 2 Q1. What's IDP? : The Intern Development Program is an essential step in the path to become

  18. Bio-Char Soil Management on Highly Weathered Soils in the Humid Tropics

    E-Print Network [OSTI]

    Lehmann, Johannes

    36 Bio-Char Soil Management on Highly Weathered Soils in the Humid Tropics Johannes Lehmann1), ColombiaQ1 CONTENTS 36.1 Bio-Char Management and Soil Nutrient Availability ............................................. 518 36.2 Microbial Cycling of Nutrients in Soils with Bio-Char

  19. The Suspension of the Habeas Corpus Act in England

    E-Print Network [OSTI]

    Crawford, Clarence Cory

    1903-01-01

    York. 1901. History for Handy inference and Topical Reading by J.B. larned. Springfield, Mass*, 1095. (Sse under topic, "aaglaad.") Sa^ sfiBASJQE ffifflirsJIl ajs\\ q»*- > 1 |'* < | .orka. Adams, Hsnry. Sssays on £nglo-3axon Law. Louisa 1876. J^ A...

  20. A 400 to 500-MHz CMOS Power Amplifier with Multi-Watt Output

    E-Print Network [OSTI]

    Kuhn, William B.

    PA cells are power-combined to generate approximately 5-Watt output. The same PA chip is used, the authors demonstrated a fully integrated CMOS 1-Watt PA with high-Q 1:3 turns- ratio output balun [8A 400 to 500-MHz CMOS Power Amplifier with Multi-Watt Output Jeongmin Jeon, Student Member, IEEE

  1. Analysis of Conforming and Nonconforming Quadrilateral Finite Element Methods for the

    E-Print Network [OSTI]

    Sheen, Dongwoo

    Analysis of Conforming and Nonconforming Quadrilateral Finite Element Methods for the Helmholtz in this analysis are the standard Q1 conforming finite element, the DSSY nonconforming element [5] and the P1-Santos-Sheen-Bennethum in [4]; also in the same paper a first rigorous finite element error analysis was carried out

  2. Assignment 3 Objective: Signal processing through simple time domain operations.

    E-Print Network [OSTI]

    Naik, Naren

    Assignment 3 Objective: Signal processing through simple time domain operations. Part 1 : Q1. Play millisecond and alpha = 0.2 . Compare your output with signal generated by an audio processing software. Audacity Software: It is a open source software to do basic signal processing operations over audio

  3. Exotic fusion systems over 2-groups

    E-Print Network [OSTI]

    Thévenaz, Jacques

    Exotic fusion systems over 2-groups Bob Oliver joint with Kasper Andersen and Joana Ventura The fusion category of a finite group G encodes the conjugacy relations within a Sylow p-subgroup S of GFS(G)(P, Q) = HomG(P, Q). 1 #12;The notion of an abstract fusion system is due to Puig. The definitions we

  4. A General Framework for Nonlinear Multigrid Inversion

    E-Print Network [OSTI]

    cost. . . . . . . . . 9 2 Pseudo­code specification of a two­grid inversion algorithm. The notation c) and r (q+1) explicit. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10 3 Pseudo­code 4 Pseudo­code specification of fixed grid and multigrid inversion methods for ODT problem showing (a

  5. Ris Report No. 352 Physics Department

    E-Print Network [OSTI]

    earth metals 11 1.3 Field dependence of the magnetic excitations in Pr ....... 12 1.4 Theory of rare.7 Calculations of J in Gd from energy bands 17 q 1.8 Theory of the magnetic properties of rare-earth transition transform method for treating strongly anisotropic magnets 10 1.2 Theory of spin waves in the heavy rare

  6. ECE 103 Solid State Electronics Master Exam 2012 Assume silicon, room temperature, complete ionization.

    E-Print Network [OSTI]

    Wang, Deli

    ECE 103 Solid State Electronics Master Exam 2012 Assume silicon, room temperature, complete ionization. (q=1.6×10-19 C, ox=3.9×8.85×10-14 F/cm, si=11.7×8.85×10-14 F/cm, kT/q=0.0259 V, Eg=1.12 e

  7. Boost Converter Provides Temperature-Controlled Operation of 12V Fan from +5V Supply

    E-Print Network [OSTI]

    McNeill, John A.

    . As shown in the timing diagram in Fig. 1, the duty cycle of the switch drive signal is determined by on. This changes the duty cycle of the comparator output and MOSFET gate drive such that the amount of time when Q1 reference, error amplifier, comparator, MOSFET gate drive, and oscillator) for closed loop PWM power supply

  8. Potential Energy Total electric potential energy, U, of a system of

    E-Print Network [OSTI]

    Bertulani, Carlos A. - Department of Physics and Astronomy, Texas A&M University

    Potential Energy Total electric potential energy, U, of a system of charges is obtained from of work done by the field, W*= -W. Bring q1 from , W *= 0 since no electric F yet #12;Potential Energy Total electric potential energy, U, of a system of charges is obtained from the work done by an external

  9. Contrib. Plasma Phys. 41 (2001) 2-3, 155-158 Dielectric Properties of Correlated Quantum Plasmas

    E-Print Network [OSTI]

    Bonitz, Michael

    2001-01-01

    Contrib. Plasma Phys. 41 (2001) 2-3, 155-158 Dielectric Properties of Correlated Quantum Plasmas M and the Fourier transform of which yields the dynamic structure factor, C(q, ) ^q()^-q(0) , S(, q) = 1 2 - d ei

  10. Integration of renewable energy into the transport and electricity sectors through V2G

    E-Print Network [OSTI]

    Firestone, Jeremy

    Integration of renewable energy into the transport and electricity sectors through V2G Henrik Lund Renewable energy Wind powerQ1 a b s t r a c t Large-scale sustainable energy systems will be necessary replace oil in the transportation sector, and (2) since today's inexpensive and abundant renewable energy

  11. GENDER AND CULTURE HER_10.indd 231HER_10.indd 231 11/29/2006 5:55:43 PM11/29/2006 5:55:43 PM

    E-Print Network [OSTI]

    Herring, Susan

    flirtatious conversations with females than vice versa (Bruckman, 1993). We find that females participate more with how appropriate it is for women to speak and be heard in public, as well as attitudes toward AND CULTURE Q1 dominance reproduced from offline Thai culture--in which women are socialized to be docile

  12. Additional Questions, Answers, and Clarifications start on page 11. Original Questions, Answers, and Clarifications

    E-Print Network [OSTI]

    and demonstration (excluding vehicle demonstration). However, costs for vehicle technology development, and Clarifications Centers for Alternative Fuels and Advanced Vehicle Technology PON-13-605 Alternative and Renewable Fuel and Vehicle Technology Program California Energy Commission October 4, 2013 Available Funding Q.1

  13. Nuclear Structure Thomas Neff

    E-Print Network [OSTI]

    Neff, Thomas

    Nuclear Structure in FMD Thomas Neff #12;FMD attributes Fermionic ^Q = C A q1 ··· qA Unitary = ^Q H ^Q ^Q ^Q Nuclear Structure in FMD Thomas Neff­ September 2, 1998 #12;Nuclear Interactions-interactions Nuclear Structure in FMD Thomas Neff­ September 2, 1998 #12;Unitary Correlator How to address the hard

  14. Examining activism in practice: A qualitative study of archival activism

    E-Print Network [OSTI]

    Novak, Joy Rainbow

    2013-01-01

    MA – Public History (2001); MLIS (2006) BA – History andBA/BS/BFA MA/MS/MFA MLS/MLIS MBA PhD JD Other (PleaseBFA Q8d. MA/MS/MFA Q8e. MLS/MLIS Q8f. PhD Q1. What is your

  15. Chemistry 593: Problem Set 1 David Ronis

    E-Print Network [OSTI]

    Ronis, David M.

    Chemistry 593: Problem Set 1 © David Ronis McGill University DUE: Friday, January 23, 2015 1). What does = 1 signify? In Eq. (1.1), the first 4 terms were evaluated analytically, while in class. 4. Near a critical point, experiment shows that S(q) 1 + (q)2 , Winter, 2015 #12;Chemistry 593

  16. NAME GVacitl/xjl K€/y .

    E-Print Network [OSTI]

    51.? a(£)=1'.1t —-IQ_, IQt+IQ =0 => t—f-l. NU): “11 5L T5 velocity = - Q .1. gig— = X + ilk/QM K ... Q'Qv) 1 J7} 42'“) z 9"“? HR. A l _ T§ (CowQc'l' €VVMV\\cL). [3?

  17. ???????? § © ¦ ?? § ?? "! $#??%©"??&' £( ¦)' $#??1 0 23£ $¡ ?? " 4

    E-Print Network [OSTI]

    ????q? ? ??d1?SqT?y??g%qTx w??g ?y?r d1??q wd1? ?9?? qQ????qi?!?? d0o? t¹ ?Ct0??q? ????qTdF??v¬ t???q1? ·?yx??w?f ????t??d ...

  18. Sourabh Saha & Martin Culpepper, All rights reserved 1 2.72: Elements of Mechanical Design, Spring 2014

    E-Print Network [OSTI]

    Culpepper, Martin L.

    © Sourabh Saha & Martin Culpepper, All rights reserved 1 2.72: Elements of Mechanical Design z P q1 y x L'2 B B' L'1 1 2 y O #12;© Sourabh Saha & Martin Culpepper, All rights reserved 2 Step 3 q q q #12;© Sourabh Saha & Martin Culpepper, All rights reserved 3 Result in parametric form: Error

  19. Towards an improved understanding of eta --> gamma^* gamma^*

    E-Print Network [OSTI]

    Xiao, C W; Hanhart, C; Kubis, B; Meißner, U -G; Wirzba, A

    2015-01-01

    We argue that high-quality data on the reaction $e^+e^-\\to \\pi^+\\pi^-\\eta$ will allow one to determine the double off-shell form factor $\\eta \\to \\gamma^*\\gamma^*$ in a model-independent way with controlled accuracy. This is an important step towards a reliable evaluation of the hadronic light-by-light scattering contribution to the anomalous magnetic moment of the muon. When analyzing the existing data for $e^+e^- \\to \\pi^+\\pi^-\\eta$ in the range of total energies $1\\text{GeV}^2off-shell form factor $F_{\\eta\\gamma^*\\gamma^*}(Q_1^2,Q_2^2)$ is consistent with the commonly employed factorization ansatz at least for $Q_1^2<1\\text{GeV}^2$, if the effect of the $a_2$ meson is taken into account. However, better data are needed to draw firm conclusions.

  20. A New Blackbody Radiation Law Based on Fractional Calculus and its Application to NASA COBE Data

    E-Print Network [OSTI]

    Minoru Biyajima; Takuya Mizoguchi; Naomichi Suzuki

    2015-08-20

    By applying fractional calculus to the equation proposed by M. Planck in 1900, we obtain a new blackbody radiation law described by a Mittag-Leffler (ML) function. We have analyzed NASA COBE data by means of a non-extensive formula with a parameter $(q-1)$, a formula proposed by Ertik et al. with a fractional parameter $(\\alpha-1)$, and our new formula including a parameter $(p-1)$, as well as the Bose-Einstein distribution with a dimensionless chemical potential $\\mu$. It can be said that one role of the fractional parameter $(p-1)$ is almost the same as that of chemical potential $(\\mu)$ as well as that of the parameter $(q-1)$ in the non-extensive approach.

  1. Constant power speed range extension of surface mounted PM motors

    DOE Patents [OSTI]

    Lawler, Jack Steward (Knoxville, TN); Bailey, John Milton (Knoxville, TN)

    2001-01-01

    A circuit and method for controlling a rotating machine (11) in the constant horsepower range above base speed uses an inverter (15) having SCR's (T1-T6) connected in series with the primary commutation switches (Q1-Q6) to control turn off of the primary commutation switches and to protect the primary commutation switches from faults. The primary commutation switches (Q1-Q6) are controlled by a controller (14), to fire in advance or after a time when the back emf equals the applied voltage, and then to turn off after a precise dwell time, such that suitable power is developed at speeds up to at least six times base speed.

  2. Understanding the bursty electron cyclotron emission during a sawtooth crash in the HT-7 tokamak

    SciTech Connect (OSTI)

    Li, Erzhong, E-mail: rzhonglee@ipp.ac.cn; Hu, Liqun; Chen, Kaiyun [Institute of Plasma Physics, Chinese Academy of Science, Hefei 230031 (China)] [Institute of Plasma Physics, Chinese Academy of Science, Hefei 230031 (China)

    2014-01-15

    Bursts in electron cyclotron emission (ECE) were observed during sawtooth crashes in HT-7 in discharges with ion cyclotron resonance heating injected near the q?=?1 rational surface (q is the safety factor). The local ECE measurement indicated that the bursty radiation is only observed on channels near but a little away outward from the q?=?1 magnetic surface. In conjunction with the soft x-ray tomography analysis, it was determined that, for the first time, only a compression process survives in the later stage of fast magnetic reconnection but before prompt heat transport. The compression enhanced the electron radiation temperature, the increased amplitude of which agreed well with the estimation according to a kinetic compression theory model [R. J. Hastie and T. C. Hender, Nucl. Fusion 28, 585 (1988)]. This paper presents the experimental evidence that there indeed exists a transient compression phase which results in the bursty ECE radiation during a sawtooth crash.

  3. Discrimination of particle masses in multivariant space-time geometry

    E-Print Network [OSTI]

    Yuri A. Rylov

    2007-12-11

    Multivariance of geometry means that at the point $P_{0}$ there exist many vectors $P_{0}P_{1}$, $\\P_{0}P_{2}$,... which are equivalent (equal) to the vector $\\Q_{0}Q_{1}$ at the point $Q_{0}$, but they are not equivalent between themselves. The discrimination capacity (zero-variance) of geometry appears, when at the point $P_{0}$ there are no vectors, which are equivalent to the vector $Q_{0}Q_{1}$ at the point $Q_{0}$. It is shown, that in some multivariant space-time geometries some particles of small mass may be discriminated (i.e. either they do not exist, or their evolution is impossible). The possibility of some particle discrimination may appear to be important for explanation of the discrete character of mass spectrum of elementary particles.

  4. Subspaces of R. H. Bing's example G 

    E-Print Network [OSTI]

    Lewis, Ira Wayne

    1974-01-01

    no limit points. Thus the definition for preparacompactness is always vacuously satisfied by G. 2. K jHodel, [13] and f8]3 Let K = F U ( p Every open cover of fU(p, r )g where gp j er for metalindelof. f ) f(q) = 1 for at most countably many qadi...]q), and p p p P A = A 'QA ". Then there exists an uncountable subset P" of P' p p p such that g' g A , " = p for all p, p' in P". Let f be defined by f(q) = 1 iff qeA ' for some pep". Then f is in X C'X and fsU(p, r )Q X for each peP". Thus U is not m...

  5. Quasi-power law ensembles

    E-Print Network [OSTI]

    Wilk, Grzegorz

    2015-01-01

    Quasi-power law ensembles are discussed from the perspective of nonextensive Tsallis distributions characterized by a nonextensive parameter $q$. A number of possible sources of such distributions are presented in more detail. It is further demonstrated that data suggest that nonextensive parameters deduced from Tsallis distributions functions $f\\left(p_T\\right)$, $q_1$, and from multiplicity distributions (connected with Tsallis entropy), $q_2$, are not identical and that they are connected via $q_1 + q_2 = 2$. It is also shown that Tsallis distributions can be obtained directly from Shannon information entropy, provided some special constraints are imposed. They are connected with the type of dynamical processes under consideration (additive or multiplicative). Finally, it is shown how a Tsallis distribution can accommodate the log-oscillating behavior apparently seen in some multiparticle data.

  6. Quasi-power law ensembles

    E-Print Network [OSTI]

    Grzegorz Wilk; Zbigniew W?odarczyk

    2014-12-12

    Quasi-power law ensembles are discussed from the perspective of nonextensive Tsallis distributions characterized by a nonextensive parameter $q$. A number of possible sources of such distributions are presented in more detail. It is further demonstrated that data suggest that nonextensive parameters deduced from Tsallis distributions functions $f\\left(p_T\\right)$, $q_1$, and from multiplicity distributions (connected with Tsallis entropy), $q_2$, are not identical and that they are connected via $q_1 + q_2 = 2$. It is also shown that Tsallis distributions can be obtained directly from Shannon information entropy, provided some special constraints are imposed. They are connected with the type of dynamical processes under consideration (additive or multiplicative). Finally, it is shown how a Tsallis distribution can accommodate the log-oscillating behavior apparently seen in some multiparticle data.

  7. Power corrections and renormalons in Drell-Yan production

    E-Print Network [OSTI]

    M. Beneke; V. M Braun

    1995-06-30

    The resummed Drell-Yan cross section in the double-logarithmic approximation suffers from infrared renormalons. Their presence was interpreted as an indication for non-perturbative corrections of order $\\lqcd/(Q(1-z))$. We find that, once soft gluon emission is accurately taken into account, the leading renormalon divergence in the resummed cross section is cancelled by higher-order perturbative contributions in the exponent of the resummed cross section. From this evidence, `higher twist' corrections to the hard cross section in Drell-Yan production should therefore intervene only at order $\\lqcd^2/((Q^2 (1-z)^2)$ in the entire perturbative domain $Q (1-z) > \\lqcd$. We compare this result with hadronic event shape variables, comment on the potential universality of non-perturbative corrections to resummed cross sections, and on possible implications for phenomenology.

  8. BIG BANG NUCLEOSYNTHESIS WITH A NON-MAXWELLIAN DISTRIBUTION

    SciTech Connect (OSTI)

    Bertulani, C. A. [GSI Helmholtzzentrum fuer Schwerionenforschung, D-64291 Darmstadt (Germany)] [GSI Helmholtzzentrum fuer Schwerionenforschung, D-64291 Darmstadt (Germany); Fuqua, J. [Texas A and M University-Commerce, Commerce, TX 75429-3011 (United States)] [Texas A and M University-Commerce, Commerce, TX 75429-3011 (United States); Hussein, M. S. [Instituto de Estudos Avancados, Universidade de Sao Paulo, C.P. 72.012, 05508-970 Sao Paulo (Brazil)] [Instituto de Estudos Avancados, Universidade de Sao Paulo, C.P. 72.012, 05508-970 Sao Paulo (Brazil)

    2013-04-10

    The abundances of light elements based on the big bang nucleosynthesis model are calculated using the Tsallis non-extensive statistics. The impact of the variation of the non-extensive parameter q from the unity value is compared to observations and to the abundance yields from the standard big bang model. We find large differences between the reaction rates and the abundance of light elements calculated with the extensive and the non-extensive statistics. We found that the observations are consistent with a non-extensive parameter q = 1{sub -} {sub 0.12}{sup +0.05}, indicating that a large deviation from the Boltzmann-Gibbs statistics (q = 1) is highly unlikely.

  9. Surjectivity of cycle maps Hel`ene Esnault and Marc Levine

    E-Print Network [OSTI]

    Levine, Marc

    for which the rational topological cycle maps CHp (X) Q H2p B (X, Q) #12;Surjectivity of cycle maps i cycle, and d = dim(X). One consequence of this decomposition is that the total cycle map d p=0 CHp) the Hodge numbers hp,q (X) all vanish for |p - q| > 1. (4) the maps CHp (X) C× Hp (X, Kp+1) are all

  10. 2 May 2000 1 Burning Plasmas Physics Issues

    E-Print Network [OSTI]

    2 May 2000 1 Burning Plasmas Physics Issues Illustrated by FIRE Simulations W.A. Houlberg ORNL Workshop on Physics Issues for FIRE 1-3 May 2000 Princeton, NJ #12;2 May 2000 2 Outline q WHIST simulations-mode q Conclusions #12;2 May 2000 3 1-1/2-D Time-Dependent Transport Modeling q 1-1/2-D time

  11. Frequencies of the geodesic acoustic mode and Alfvén gap modes in high-q{sup 2}? plasmas with non-circular cross section

    SciTech Connect (OSTI)

    Fesenyuk, O. P.; Kolesnichenko, Ya. I.; Yakovenko, Yu. V.; National University of Kyiv Mohyla Academy, Vul. Skovorody 2, Kyiv 04070

    2013-12-15

    This work generalizes recent results [O. P. Fesenyuk et al., Plasma Phys. Controlled Fusion 54, 085014 (2012)] to plasmas with elongated cross section. It suggests new expressions for the frequencies of the geodesic acoustic mode and Alfvén gap modes in tokamaks, with a large ratio of the plasma pressure to the magnetic field pressure and a large safety factor (q?1, which takes place in discharges with reversed-shear configuration and, especially, in hollow-current discharges)

  12. Total Space Heat-

    Annual Energy Outlook [U.S. Energy Information Administration (EIA)]

    Concrete (Block or Poured) ... 89.9 31.3 7.2 5.8 7.5 18.6 2.4 6.7 Q 1.7 7.7 Concrete Panels ... 101.7 33.3 8.0 7.1 5.5 28.3 1.5 3.3 1.6 4.3 8.8 Siding or...

  13. Strategy for Chinese MFE J.Li, Y.X.Wan, B.N.Wan, Y.C.Wu

    E-Print Network [OSTI]

    -type compact device Option 2: Fusion ­Fission hybrid Fusion: Q=1-3, Pth=100-200MW Fission: M= 20-30, Pth = 2 with a changeable core. #12;Competitions to Fusion in China G-IV Reactor: Fast Breeder 65MW (now) 800MW(2015) HTGR reactor configurations also proposed #12;China Fusion Engineering Testing Reactor Step 2: AT H-mode R=4

  14. Hagedorn's temperature from nonextensive thermodynamics for pp collisions

    SciTech Connect (OSTI)

    Marques, L.; Andrade II, E.; Deppman, A.

    2014-11-11

    In this work some aspects of the nonextensive thermodynamics of hadronic matter are investigated. In particular, an extense analysis of the fitting procedure of the nonextensive distributions of transverse momentum of several particles is performed focusing on the correlation between the entropic index and the effective temperature. The linear relation between ? and (q ? 1) is determined and it is shown that the Hagedorn's temperature can be obtained.

  15. Coulomb Interaction Symmetries and the Mayer Series in the Two-Dimensional Dipole Gas

    E-Print Network [OSTI]

    Procacci, Aldo

    ´atica-ICEx, UFMG, CP 702, Belo Horizonte MG 30.161-970, Brazil 2 Dep. F´isica-ICEx, UFMG, CP 702, Belo Horizonte MG 30.161-970, Brazil 3 Instituto de F´isica, Universidade de S~ao Paulo 01452 S~ao Paulo, SP, Brazil carrying vectorial moments q of unit length (q R2 , q2 = 1), interacting via the potential V (1, 2) = (q1

  16. Thermal distributions in stellar plasmas, nuclear reactions and solar neutrinos

    E-Print Network [OSTI]

    M. Coraddu; G. Kaniadakis; A. Lavagno; M. Lissia; G. Mezzorani; P. Quarati

    1998-11-24

    The physics of nuclear reactions in stellar plasma is reviewed with special emphasis on the importance of the velocity distribution of ions. Then the properties (density and temperature) of the weak-coupled solar plasma are analysed, showing that the ion velocities should deviate from the Maxwellian distribution and could be better described by a weakly-nonexstensive (|q-1|solar neutrino fluxes, and on the pp neutrino energy spectrum, and analyse the consequences for the solar neutrino problem.

  17. Demonstration of sawtooth period control with EC waves in KSTAR plasma

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

    Jeong, J. H.; Bae, Y. S.; Joung, M.; Kim, D.; Goodman, T. P.; Sauter, O.; Sakamoto, K.; Kajiwara, K.; Oda, Y.; Kwak, J. G.; et al

    2015-03-12

    The sawtooth period control in tokamak is important issue in recent years because the sawtooth crash can trigger TM/NTM instabilities and drive plasmas unstable. The control of sawtooth period by the modification of local current profile near the q=1 surface using ECCD has been demonstrated in a number of tokamaks [1, 2] including KSTAR. As a result, developing techniques to control the sawtooth period as a way of controlling the onset of NTM has been an important area of research in recent years [3]. In 2012 KSTAR plasma campaign, the sawtooth period control is carried out by the different depositionmore »position of EC waves across the q=1 surface. The sawtooth period is shortened by on-axis co-ECCD (destabilization), and the stabilization of the sawtooth is also observed by off-axis co-ECCD at outside q=1 surface. In 2013 KSTAR plasma campaign, the sawtooth locking experiment with periodic forcing of 170 GHz EC wave is carried out to control the sawtooth period. The optimal target position which lengthens the sawtooth period is investigated by performing a scan of EC beam deposition position nearby q=1 surface at the toroidal magnetic field of 2.9 T and plasma current of 0.7 MA. The sawtooth locking by the modulated EC beam is successfully demonstrated as in [3-5] with the scan of modulation-frequency and duty-ratio at the low beta (?N~0.5) plasma. In this paper, the sawteeth behavior by the location of EC beam and the preliminary result of the sawtooth locking experiments in KSTAR will be presented.« less

  18. ( ; ')u x x 1) Overview!

    E-Print Network [OSTI]

    the MAP cost. Result: An MRF prior which adapts to local image structure. MRFs can be expressed as Gibbs GGMRF (p=1.2) qGGMRF (p=2, q=1, c=1.5) 5) Computing the Surrogate Energy Function! We introduced a new,r entry References! [1] C. B. Atkins, C. A. Bouman and J. P. Allebach, "Optimal image scaling using pixel

  19. ?W H A T I S . . . an Automatic

    E-Print Network [OSTI]

    Rowland, Eric

    ?W H A T I S . . . an Automatic Sequence? Eric Rowland A sequence s(n)n0 is called k-automatic if s, hence the name "automatic sequence." For example, consider an automaton with only two states, q1 and q2, b, a, b, b, a, . . . is known as the Thue­Morse sequence. It is 2- automatic, since we are reading

  20. ROOT LOCUS TECHNIQUE 323 7.6.1 Hydro Power Plant Experiment

    E-Print Network [OSTI]

    Gajic, Zoran

    ROOT LOCUS TECHNIQUE 323 7.6.1 Hydro Power Plant Experiment The design of a static controller for a real hydro power plant is considered in Skatariâ?? c and Gajiâ?? c (1992). The hydro power plant is treated variables of this hydro power plant are represented by x T = [1` 1! 1u f 1/ d 1/ q 1/ f 1/D 1/Q ] where 1

  1. Eltron Research & Development

    SciTech Connect (OSTI)

    Evenson, Carl; Mackay, Richard; Faull, John

    2014-03-01

    This topical report covers technical work conducted under contract DE-FC26-05NT42469 between FY06 Q1 through FY14 Q2. The project evolved through several budget periods, budget revisions and continuation applications. This report covers work performed under the “base” program. In 2010 ARRA funding was added to the project. A separate report covering the ARRA portion of the project was submitted to DOE. The original project was focused on research and development for scale-up of hydrogen separation membrane for a FutureGen type power plant. The work included membrane testing and evaluation of metal alloy flat plates vs. tubes and metal membranes vs. cermet membranes. In addition, economic analysis and process modeling was performed. The original project team included CoorsTek, NORAM, and Praxair. In FY10Q2 a continuation application was filed for conducting a scale-up test at Eastman Chemical. In this part of the project a Subscale Engineering Prototype (SEP) membrane skid was designed, fabricated, and operated on a gasified coal slip-stream on Eastman’s site in Kingsport, TN. Following operation, the project was reorganized and a second continuation application with a new statement of work was initiated in FY12Q1. Finally, based on DOE’s decision not to proceed with a Process Development Unit (PDU) field test, a third continuation application and statement of work was initiated in FY13Q1 to close out the project.

  2. University Downtown Center 67 Washington St., Binghamton

    E-Print Network [OSTI]

    Cho, Junghyun

    METERED PARKING Lot M2 Lot F3 LotH LotH LotI Lot F Lot G LotC Lot F1 Lot J LotJ1 LotJ2 LotJ3 Lot E1 Lot E Lot T LotO1 LotV Lot Q2 Lot 02 Lot Q1 Lot W Lot Y1 Lot R METERED PARKING METERED PARKING METERED PARKING METEREDPARKING Lot A Lot F2 LotY4 LotY5 Visitors Parking Lot K Lot B LotG Lot03 Lot04 Lot

  3. DOE/EIS-0222-SA-02

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would like submit theCovalent Bonding Low-Cost2 DOE HQSiteo n n e v i l l e2Q)1 ergy02 Revision

  4. DOE/EIS-0222-SA-O1 Supplement Analysis Hanford Comprehensive Land-Use Plan Environmental Impact

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would like submit theCovalent Bonding Low-Cost2 DOE HQSiteo n n e v i l l e2Q)1 ergy02

  5. DOE/EIS-0391-SA-01

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would like submit theCovalent Bonding Low-Cost2 DOE HQSiteo n n e v i l l e2Q)1 ergy0291D-SA-01

  6. Downward Muon Intensity at Surface dI 0 (E 0 ; cos )

    E-Print Network [OSTI]

    Learned, John

    Downward Muon Intensity at Surface dI #22;0 (E #22;0 ; cos #18;) dE #22;0 = 0:14 #1; E #22;0 #1; 0 B @ 1 1 + 1:1E #22;0 cos #18; #3; 115 GeV + 0:054 1 + 1:1E #22;0 cos #18; ? 850 GeV + R c 1 C A Ref Approx. Isotropic H.E. Primary C.R. Flux Depth of Atmosphere a( ) q -1 -0.5 0 0.5 1 cos q 10 100 1000

  7. The Theory of the Kink Mode during the Vertical Disruption Events in Tokamaks

    SciTech Connect (OSTI)

    Leonid E. Zakharov

    2008-01-14

    This paper explains the locked m/n = 1/1 kink mode during the vertical disruption event when the plasma has an electrical contact with the plasma facing conducting surfaces. It is shown that the kink perturbation can be in equilibrium state even with a stable safety factor q > 1, if the halo currents, excited by the kink mode, can flow through the conducting structure. This suggests a new explanation of the so-called sideway forces on the tokamak in-vessel components during the disruption event. __________________________________________________

  8. ou)..u, I\\J. \\-\\cu..D\\<.. ffio..\\Y\\ r'Y\\oJ.ce~ 10\\L.

    E-Print Network [OSTI]

    .f"I G~eo(iO ~eS~\\' 8 ~'oe.,~~) \\.o.X/lor'tf~-O\\.~os' )- \\O~o5D,{79'~ e.l.v. 2.1Q1.M 0'" \\-\\ CX)~ ~(c°D\\,:lOS' I - I()CoO 50.llq ') 6.Q.v ' ~l'\\ ~ fY'\\ ~N\\-\\ CX)3 ~ (CSN) Nec\\-()..(\\o.. C.i aRCQ Q. 31Y'o.mmol()9~ claSS btOl.l Q7 Q}obe, .aD\\'2 Wt~~ 33.6~c>~'660o)- \\O,,4CX d

  9. Bunch Length and Impedance Measurements at SPEAR3

    SciTech Connect (OSTI)

    Corbett, W.J.; Cheng, W.X.; Fisher, A.S.; Huang, X.; /SLAC

    2011-11-02

    Streak camera measurements were made at SPEAR3 to characterize longitudinal coupling impedance. For the nominal optics, data was taken at three rf voltages and a single-bunch current range of 0-20mA. Both bunchcentroid phase shift and bunch lengthening were recorded to extract values for resistive and reactive impedance. An (R+L) and a Q=1 model were then back-substituted into the Haissinski equation and compared with raw profile data. In the short bunch (low-{alpha}) mode, distribution 'bursting' was observed.

  10. Load Sharing and Spacer Flexibility in Double Pane and Triple Pane Insulating Glass Units 

    E-Print Network [OSTI]

    Mertens, Karl Phillip

    2015-03-25

    , is the initial gas space temper- ature measured in degrees Kelvin. To then find the current gas space pressure Pgs, insert the constant C into: Pgs = C ? Tgs/Vgs (5) where Tgs, is the current gas space temperature and Vgs, is the current gas space volume... the net loads that act on the outer plate by combining equations (1) and (5) to get: q1 = q0 + Pa ? C ? Tgs/Vgs (11) This equation can then be inserted into equation (9) and rearranged to find the load distribution factor n? for each iteration: n...

  11. Colorful plane vortices and Chiral Symmetry Breaking in $SU(2)$ Lattice Gauge Theory

    E-Print Network [OSTI]

    Seyed Mohsen Hosseini Nejad; Manfried Faber; Roman Höllwieser

    2015-08-11

    We investigate plane vortices with color structure. The topological charge and gauge action of such colorful plane vortices are studied in the continuum and on the lattice. These configurations are vacuum to vacuum transitions changing the winding number between the two vacua, leading to a topological charge $Q=-1$ in the continuum. After growing temporal extent of these vortices, the lattice topological charge approaches $-1$ and the index theorem is fulfilled. We analyze the low lying modes of the overlap Dirac operator in the background of these colorful plane vortices and compare them with those of spherical vortices. They show characteristic properties for spontaneous chiral symmetry breaking.

  12. Colorful plane vortices and Chiral Symmetry Breaking in $SU(2)$ Lattice Gauge Theory

    E-Print Network [OSTI]

    Seyed Mohsen Hosseini Nejad; Manfried Faber; Roman Höllwieser

    2015-08-05

    We investigate plane vortices with color structure. The topological charge and gauge action of such colorful plane vortices are studied in the continuum and on the lattice. These configurations are vacuum to vacuum transitions changing the winding number between the two vacua, leading to a topological charge $Q=-1$ in the continuum. After growing temporal extent of these vortices, the lattice topological charge approaches $-1$ and the index theorem is fulfilled. We analyze the low lying modes of the overlap Dirac operator in the background of these colorful plane vortices and compare them with those of spherical vortices. They show characteristic properties for spontaneous chiral symmetry breaking.

  13. Crimea as Kosovo and Sudetenland: The Peril of Historical Narratives in the 2014 Russo-Ukrainian Crisis.

    E-Print Network [OSTI]

    Jameson, Robert

    2014-08-25

    March 2014]. Andrew Osborn and Alastair Macdonald. “Ukraine appeals to West as Crimea turns to Russia.” Reuters. http://www.reuters.com/article/2014/03/11/us-ukraine-crisis- idUSBREA1Q1E820140311. [Accessed 20 March 2014]. Vladimir Putin. “Address... of crisis participants’ behavior – and their next moves. Everyone thinks the past is prologue; disagreement abounds as to which past. Two opposing narratives have emerged that, at the risk of simplification, I associate with Russia and ‘the West...

  14. NGC2613, 3198, 6503, 7184: Case studies against `maximum' disks

    E-Print Network [OSTI]

    B. Fuchs

    1998-12-02

    Decompositions of the rotation curves of NGC2613, 3198, 6505, and 7184 are analysed. For these galaxies the radial velocity dispersions of the stars have been measured and their morphology is clearly discernible. If the parameters of the decompositions are chosen according to the `maximum' disk hypothesis, the Toomre Q stability parameter is systematically less than one and the multiplicities of the spiral arms as expected from density wave theory are inconsitent with the observed morphologies of the galaxies. The apparent Q<1 instability, in particular, is a strong argument against the `maximum' disk hypothesis.

  15. Double vector meson production in the International Linear Collider

    E-Print Network [OSTI]

    F. Carvalho; V. P. Goncalves; B. D. Moreira; F. S. Navarra

    2015-04-17

    In this paper we study double vector meson production in $\\gamma \\gamma$ interactions at high energies and, using the color dipole picture, estimate the main observables which can be probed at the International Linear Collider (ILC). The total $\\gamma (Q_1^2) + \\gamma (Q_2^2) \\rightarrow V_1 + V_2$ cross-sections for $V_i = \\rho$, $\\phi$, $J/\\psi$ and $\\Upsilon$ are computed and the energy and virtuality dependencies are studied in detail. Our results demonstrate that the experimental analysis of this process is feasible at the ILC and it can be useful to constrain the QCD dynamics at high energies.

  16. Real-Time Kadanoff-Baym Approach to Nuclear Response Functions

    E-Print Network [OSTI]

    H. S. Kohler; N. H. Kwong

    2013-11-19

    Linear response functions are calculated for symmetric nuclear matter of normal density by time-evolving two-time Green's functions with conserving self-energy insertions, thereby satisfying the energy-sum rule. Nucleons are regarded as moving in a mean field defined by an effective mass. A two-body effective (or residual) interaction, represented by a gaussian local interaction, is used to find the effect of correlations in a second order as well as a ring approximation. The response function S(e,q) is calculated for 0.2<q<1.2 fm^{-1}. Comparison is made with the nucleons being un-correlated, "RPA+HF" only.

  17. Colorful plane vortices and Chiral Symmetry Breaking in $SU(2)$ Lattice Gauge Theory

    E-Print Network [OSTI]

    Seyed Mohsen Hosseini Nejad; Manfried Faber; Roman Höllwieser

    2015-09-25

    We investigate plane vortices with color structure. The topological charge and gauge action of such colorful plane vortices are studied in the continuum and on the lattice. These configurations are vacuum to vacuum transitions changing the winding number between the two vacua, leading to a topological charge $Q=-1$ in the continuum. After growing temporal extent of these vortices, the lattice topological charge approaches $-1$ and the index theorem is fulfilled. We analyze the low lying modes of the overlap Dirac operator in the background of these colorful plane vortices and compare them with those of spherical vortices. They show characteristic properties for spontaneous chiral symmetry breaking.

  18. Auditory evoked potentials and electroencephalograms correlates to intracranial pressure 

    E-Print Network [OSTI]

    Chandrasekhar, Mahesh

    1992-01-01

    Tracheal tube RESPIRATOR STRIPCH ART RECORDER Fig. 10. The overall equipment setup for the experiment. +9 V 270 Q 1MQ 8 4 6 Earphone 4. 7 F, F LM555 3 1 KQ 2N2222 O. 1 ltF LM386 1 2 4 . 01 lt $ 10KQ Fig. 11. The circuit diagram...&Is were extracted and analyses oi' variance show no siginficant statistical difference be- tween the respective means. To 1VIy Uncle Dr. N. S. Umanath ACKNOWLEDGMENTS I would like to deeply thank Dr. Charles Lessard for serving as Chairman of my...

  19. Applications of algebraic geometry to object/image recognition 

    E-Print Network [OSTI]

    Abbott, Kevin Toney

    2009-06-02

    (the object/image relations) for the Qi to be a generalized weak perspective projection of the Pi. Recall that we view our object space Ok as a subvariety of P( n 4)?1 R and our image space Ik as a subvariety of P( n 3)?1 R . As such, we want to view.... Two configurations P1,P2,...,Pk and Q1,Q2,...,Qk of points in Rn have the same shape if there is a similarity transformation T ?Sim(n) such that T(Pi) = Qi for i = 1,...,k. The shape of a configuration of k points in Rn is its equivalence class under...

  20. Double vector meson production in the International Linear Collider

    E-Print Network [OSTI]

    Carvalho, F; Moreira, B D; Navarra, F S

    2015-01-01

    In this paper we study double vector meson production in $\\gamma \\gamma$ interactions at high energies and, using the color dipole picture, estimate the main observables which can be probed at the International Linear Collider (ILC). The total $\\gamma (Q_1^2) + \\gamma (Q_2^2) \\rightarrow V_1 + V_2$ cross-sections for $V_i = \\rho$, $\\phi$, $J/\\psi$ and $\\Upsilon$ are computed and the energy and virtuality dependencies are studied in detail. Our results demonstrate that the experimental analysis of this process is feasible at the ILC and it can be useful to constrain the QCD dynamics at high energies.

  1. From $sl_q(2)$ to a parabosonic Hopf algebra

    E-Print Network [OSTI]

    Tsujimoto, Satoshi; Zhedanov, Alexei

    2011-01-01

    A Hopf algebra with four generators among which an involution (reflection) operator, is introduced. The defining relations involve commutators and anticommutators. The discrete series representations are developed. Designated by $sl_{-1}(2)$, this algebra encompasses the Lie superalgebra $osp(1|2)$. It is obtained as a $q=-1$ limit of the $sl_q(2)$ algebra and seen to be equivalent to the parabosonic oscillator algebra in irreducible representations. It possesses a noncocommutative coproduct. The Clebsch-Gordan coefficients (CGC) of $sl_{-1}(2)$ are obtained and expressed in terms of the dual -1 Hahn polynomials. A generating function for the CGC is derived using a Bargmann realization.

  2. CONFIDENTIAL -encanadacgpss2013reports.xlsx All Respondents (No Filter) CANADIAN GRADUATE AND PROFESSIONAL STUDENT SURVEY -2013 NATIONAL DATA -ALL CANADA

    E-Print Network [OSTI]

    Wang, Hao "Howard"

    Responses 51,621 Valid 51,634 Total Responses 51,682 Total 51,682 Q2: In what disciplinary area are you.3% 32,705 3.0% 1,559 6.5% 3,358 32.4% 16,720 30.2% 15,619 Valid Responses 51,682 Valid 51,682 Total Responses 51,682 Total 51,682 SECTION 1 - EDUCATIONAL STATUS Q1: At which degree level are you currently

  3. From $sl_q(2)$ to a Parabosonic Hopf Algebra

    E-Print Network [OSTI]

    Satoshi Tsujimoto; Luc Vinet; Alexei Zhedanov

    2011-10-07

    A Hopf algebra with four generators among which an involution (reflection) operator, is introduced. The defining relations involve commutators and anticommutators. The discrete series representations are developed. Designated by $sl_{-1}(2)$, this algebra encompasses the Lie superalgebra $osp(1|2)$. It is obtained as a $q=-1$ limit of the $sl_q(2)$ algebra and seen to be equivalent to the parabosonic oscillator algebra in irreducible representations. It possesses a noncocommutative coproduct. The Clebsch-Gordan coefficients (CGC) of $sl_{-1}(2)$ are obtained and expressed in terms of the dual -1 Hahn polynomials. A generating function for the CGC is derived using a Bargmann realization.

  4. Extracting meson-baryon contributions to the electroexcitation of the N (1675)-5/2 nucleon resonance

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

    Aznauryan, Inna G.; Burkert, Volker D.

    2015-07-01

    We report on the determination of the electrocouplings for the transition from the proton to the N (1675)-5/2 resonance state using recent differential cross section data on ep ? e?+n by the CLAS collaboration at 1.8 ? Q² -5/2 helicity amplitudes show considerable coupling through the AP1/2 amplitude, that is significantly larger than predicted three-quark contribution to this amplitude. The amplitude AP3/2 is much smaller. Both results are consistent with the predicted sizes of the meson-baryonmore »contributions at Q² ? 1.8 GeV² from the dynamical coupled-channel model.« less

  5. Piezoelectric energy harvesting from colored fat-tailed fluctuations: An electronic analogy

    E-Print Network [OSTI]

    J. I. Peña Rosselló; R. R. Deza; J. I. Deza; H. S. Wio

    2015-10-17

    Aiming to optimize piezoelectric energy harvesting from strongly colored fat-tailed fluctuations, we have recently studied the performance of a monostable inertial device under a noise whose statistics depends on a parameter $q$ (bounded for $q1$). We have studied the interplay between the potential shape (interpolating between square-well and harmonic-like behaviors) and the noise's statistics and spectrum, and showed that its output power grows as $q$ increases above 1. We now report a real experiment on an electronic analog of the proposed system, which sheds light on its operating principle.

  6. A CAD tool for the power estimation of CMOS, BiCMOS and BiNMOS gates 

    E-Print Network [OSTI]

    Islam, Kazi Inamul

    1995-01-01

    bias depletion capacitance Base-collector built-in voltage Base-collector profile exponent Fraction of B/C depletion capacitance connected to internal base node CJS VJS MJS FC TF Collector-substrate, zero bias capacitance Collector... carrier charge in the base. The normalized majority carrier charge in the base QB is given by an equation of the form: QB = ? + ? +Qs (2 4) where Q 1 BC BE (2. 5) (2. 6) VzF is the forward Early voltage and V~B is an equivalent reverse Early...

  7. FY 2013 Metric Summary | Department of Energy

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergy A plug-inPPLforLDRD Report to Congress MoreHyd rog en Tan41FY 2013 Q1 Metric

  8. FY 2014 Consolidated Innovative Nuclear Research FOA | Department of Energy

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergy A plug-inPPLforLDRD Report to Congress MoreHyd rog en Tan41FY 2013 Q1

  9. FY 2014 EM Budget Rollout Presentation | Department of Energy

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergy A plug-inPPLforLDRD Report to Congress MoreHyd rog en Tan41FY 2013 Q1Provides keyEM

  10. FY 2014 Excess Elimination Report FINAL | Department of Energy

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergy A plug-inPPLforLDRD Report to Congress MoreHyd rog en Tan41FY 2013 Q1Provides

  11. FY 2014 Federal Real Property Reporting Requirement | Department of Energy

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergy A plug-inPPLforLDRD Report to Congress MoreHyd rog en Tan41FY 2013 Q1ProvidesFIMS

  12. FY 2014 Metric Summary | Department of Energy

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergy A plug-inPPLforLDRD Report to Congress MoreHyd rog en Tan41FY 2013 Q1ProvidesFIMSFY

  13. FY 2015 METRIC SUMMARY | Department of Energy

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

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergy A plug-inPPLforLDRD Report to Congress MoreHyd rog en Tan41FYFY 2014,byFY 2015 Q1

  14. Tank Closure and Waste Management Environmental Impact Statement for the Hanford Site, Richland, Washington

    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: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorking With U.S. Coal StocksSuppliers Tag:Take Action toTandeepH-1L-1P-1Q-1

  15. 3dtab.xlsx

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.10 CoolingNotes &* j o n5 1:2:1 AlgeriaQ1

  16. Monthly Energy Review - August 2001

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1Markets See(STEO), 19992,BiodieselU.S.3 E nQ1 E n

  17. Monthly Energy Review - August 2002

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1Markets See(STEO), 19992,BiodieselU.S.3 E nQ1 E n2

  18. Monthly Energy Review - August 2003

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1Markets See(STEO), 19992,BiodieselU.S.3 E nQ1 E

  19. Monthly Energy Review - August 2004

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1Markets See(STEO), 19992,BiodieselU.S.3 E nQ1 E4 E

  20. Monthly Energy Review - August 2005

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1Markets See(STEO), 19992,BiodieselU.S.3 E nQ1 E4

  1. Monthly Energy Review - August 2006

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1Markets See(STEO), 19992,BiodieselU.S.3 E nQ1 E46

  2. Monthly Energy Review - August 2007

    Gasoline and Diesel Fuel Update (EIA)

    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 Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1Markets See(STEO), 19992,BiodieselU.S.3 E nQ1

  3. Charge dependent relation between the masses of different generations and Neutrino masses

    E-Print Network [OSTI]

    Branislav Sazdovic

    2015-01-29

    Despite the enormous achievements, the Standard model of Particle physics can not be consider as complete theory of fundamental interactions. Among other things, it can not describe the gravitational interaction and it depends on 19 parameters. The Standard model includes 12 fermions (matter elementary particles with spin $\\frac{1}{2}$) which are divided in three generations, groups with same interactions but different masses. Each generation can be classified into two leptons (with electric charges $Q=-1$, electron-like and $Q=0$, neutrino) and two quarks (with electric charges $Q=-\\frac{1}{3}$, down-type and $Q=\\frac{2}{3}$, up-type). However, the understanding of the relationship between generations and ratio of masses of different generations are unknown. Here we show that there exists the simple relation between masses of different generations which depend only on the electric charges for $Q=-1,\\, \\, Q=-\\frac{1}{3}$ and $Q=\\frac{2}{3}$. It is in pretty good agreement with experimental data. Assuming that the same relation valid for $Q=0$, we are able to calculate neutrino masses. Therefore, our results could pave the way for further investigations beyond Standard model.

  4. Charge dependent relation between the masses of different generations and Neutrino masses

    E-Print Network [OSTI]

    Sazdovic, Branislav

    2015-01-01

    Despite the enormous achievements, the Standard model of Particle physics can not be consider as complete theory of fundamental interactions. Among other things, it can not describe the gravitational interaction and it depends on 19 parameters. The Standard model includes 12 fermions (matter elementary particles with spin $\\frac{1}{2}$) which are divided in three generations, groups with same interactions but different masses. Each generation can be classified into two leptons (with electric charges $Q=-1$, electron-like and $Q=0$, neutrino) and two quarks (with electric charges $Q=-\\frac{1}{3}$, down-type and $Q=\\frac{2}{3}$, up-type). However, the understanding of the relationship between generations and ratio of masses of different generations are unknown. Here we show that there exists the simple relation between masses of different generations which depend only on the electric charges for $Q=-1,\\, \\, Q=-\\frac{1}{3}$ and $Q=\\frac{2}{3}$. It is in pretty good agreement with experimental data. Assuming that...

  5. Formation of an internal transport barrier and magnetohydrodynamic activity in experiments with the controlled density of rational magnetic surfaces in the T-10 Tokamak

    SciTech Connect (OSTI)

    Razumova, K. A., E-mail: razumova@nfi.kiae.ru; Andreev, V. F.; Bel’bas, I. S.; Gorshkov, A. V.; Dnestrovskij, A. Yu.; Dyabilin, K. S.; Kislov, A. Ya.; Lysenko, S. E.; Notkin, G. E.; Timchenko, N. N.; Chudnovskiy, A. N.; Shelukhin, D. A. [National Research Centre Kurchatov Institute (Russian Federation)] [National Research Centre Kurchatov Institute (Russian Federation)

    2013-09-15

    Results are presented from experiments on the formation of an internal electron transport barrier near the q = 1.5 rational surface in the T-10 tokamak. The experiments were carried out in the regime with off-axis electron cyclotron resonance (ECR) heating followed by a fast plasma current ramp-up. After suppressing sawtooth oscillations by off-axis ECR heating, an internal transport barrier began to form near the q = 1.5 rational surface. In the phase of the current ramp-up, the quality of the transport barrier improved; as a result, the plasma energy confinement time increased 2–2.5 times. The intentionally produced flattening of the profile of the safety factor q(r) insignificantly affected magnetohydrodynamic activity in the plasma column in spite of the theoretical possibility of formation of substantial m/n = 3/2 and 2/1 magnetic islands. Conditions are discussed under which the flattening of the profile of the safety factor q near low-order rational surfaces leads to the formation of either an internal transport barrier or the development of an island magnetic structure induced by tearing modes.

  6. Chemical non-equilibrium and deconfinement in 200 A GeV Sulphur induced reactions

    E-Print Network [OSTI]

    Jean Letessier; Johann Rafelski

    1998-10-06

    We interpret hadronic particle abundances produced in S--Au/W/Pb 200 A GeV reactions in terms of the final state hadronic phase space model and determine by a data fit of the chemical hadron freeze-out parameters. Allowing for the flavor abundance non-equilibrium a highly significant fit to experimental particle abundance data emerges, which supports possibility of strangeness distillation. We find under different strategies stable values for freeze-out temperature T_f=143\\pm3 MeV, baryochemical potential \\mu_B= 173\\pm6 MeV, ratio of strangeness (\\gamma_s) and light quark (\\gamma_q) phase space occupancies \\gamma_s/\\gamma_q=0.60\\pm0.02, and \\gamma_q=1.22\\pm0.05 without accounting for collective expansion (radial flow). When introducing flow effects which allow a consistent description of the transverse mass particle spectra, yielding |v_c|=0.49\\pm0.01c, we find \\gamma_s/\\gamma_q=0.69\\pm0.03, \\gamma_q=1.41\\pm0.08. The strange quark fugacity is fitted at \\lambda_s=1.00\\pm0.02 suggesting chemical freeze-out directly from the deconfined phase.

  7. TRANSITION FROM THE SECTOR ZONE TO THE UNIPOLAR ZONE IN THE HELIOSHEATH: VOYAGER 2 MAGNETIC FIELD OBSERVATIONS

    SciTech Connect (OSTI)

    Burlaga, L. F. [NASA Goddard Space Flight Center, Code 673, Greenbelt, MD 20771 (United States); Ness, N. F., E-mail: lburlagahsp@verizon.net, E-mail: nfnudel@yahoo.com [Institute for Astrophysics and Computational Sciences, Catholic University of America, Washington, DC 20064 (United States)

    2011-08-10

    The magnetic polarity pattern observed by Voyager 2 (V2) evolved with time from a nearly equal mixture of positive and negative polarity sectors in the sector zone from 2007.00 to 2007.67 to nearly uniform positive polarity (magnetic fields directed away from the Sun) in the unipolar zone from 2009.6 to 2010.3. This change was caused by the decreasing latitudinal extent of the sector zone, when the minimum extent of the heliospheric current sheet moved northward toward the solar equator as the solar activity associated with solar cycle 23 decreased a minimum in 2010. In the heliosheath, the distribution of daily averages of the magnetic field strength B was lognormal in the sector zone from 2008.83 to 2009.57 and Gaussian in the unipolar zone from 2009.57 to 2010.27. The distribution of daily increments of B was a Tsallis distribution (q-Gaussian distribution) with q = 1.66 {+-} 0.01 in the sector zone and {approx}Gaussian (q = 1.01 {+-} 0.29) in the unipolar zone. The unipolar region appears to be in a relatively undisturbed equilibrium state.

  8. Emergent AdS3 and BTZ Black Hole from Weakly Interacting Hot 2d CFT

    E-Print Network [OSTI]

    Soo-Jong Rey; Yasuaki Hikida

    2006-05-02

    We investigate emergent holography of weakly coupled two-dimensional hyperK\\"ahler sigma model on cotangent bundle of (N-1)-dimensional complex projective space at zero and finite temperature. The sigma model is motivated by the spacetime conformal field theory dual to the near-horizon geometry of Q1 D1-brane bound to Q5 D5-brane wrapped on four-torus times circle, where N = Q1*Q5. The sigma model admits nontrivial instanton for all N greater than or equal to 2, which serves as a local probe of emergent holographic spacetime. We define emergent geometry of the spacetime as that of instanton moduli space via Hitchin's information metric. At zero temperature, we find that emergent geometry is AdS3. At finite temperature, time-periodic instanton is mappable to zero temperature instanton via conformal transformation. Utilizing the transformation, we show that emergent geometry is precisely that of the non-extremal, non-rotating BTZ black hole.

  9. Extreme event statistics of daily rainfall: Dynamical systems approach

    E-Print Network [OSTI]

    G. Cigdem Yalcin; Pau Rabassa; Christian Beck

    2015-08-15

    We analyse the probability densities of daily rainfall amounts at a variety of locations on the Earth. The observed distributions of the amount of rainfall fit well to a q-exponential distribution with exponent q close to q=1.3. We discuss possible reasons for the emergence of this power law. On the contrary, the waiting time distribution between rainy days is observed to follow a near-exponential distribution. A careful investigation shows that a q-exponential with q=1.05 yields actually the best fit of the data. A Poisson process where the rate fluctuates slightly in a superstatistical way is discussed as a possible model for this. We discuss the extreme value statistics for extreme daily rainfall, which can potentially lead to flooding. This is described by Frechet distributions as the corresponding distributions of the amount of daily rainfall decay with a power law. On the other hand, looking at extreme event statistics of waiting times between rainy days (leading to droughts for very long dry periods) we obtain from the observed near-exponential decay of waiting times an extreme event statistics close to Gumbel distributions. We discuss superstatistical dynamical systems as simple models in this context.

  10. Extreme event statistics of daily rainfall: Dynamical systems approach

    E-Print Network [OSTI]

    Yalcin, G Cigdem; Beck, Christian

    2015-01-01

    We analyse the probability densities of daily rainfall amounts at a variety of locations on the Earth. The observed distributions of the amount of rainfall fit well to a q-exponential distribution with exponent q close to q=1.3. We discuss possible reasons for the emergence of this power law. On the contrary, the waiting time distribution between rainy days is observed to follow a near-exponential distribution. A careful investigation shows that a q-exponential with q=1.05 yields actually the best fit of the data. A Poisson process where the rate fluctuates slightly in a superstatistical way is discussed as a possible model for this. We discuss the extreme value statistics for extreme daily rainfall, which can potentially lead to flooding. This is described by Frechet distributions as the corresponding distributions of the amount of daily rainfall decay with a power law. On the other hand, looking at extreme event statistics of waiting times between rainy days (leading to droughts for very long dry periods) w...

  11. Semiclassical energy formulas for power-law and log potentials in quantum mechanics

    E-Print Network [OSTI]

    Richard L. Hall; Qutaibeh D. Katatbeh

    2003-05-09

    We study a single particle which obeys non-relativistic quantum mechanics in R^N and has Hamiltonian H = -Delta + V(r), where V(r) = sgn(q)r^q. If N \\geq 2, then q > -2, and if N = 1, then q > -1. The discrete eigenvalues E_{n\\ell} may be represented exactly by the semiclassical expression E_{n\\ell}(q) = min_{r>0}\\{P_{n\\ell}(q)^2/r^2+ V(r)}. The case q = 0 corresponds to V(r) = ln(r). By writing one power as a smooth transformation of another, and using envelope theory, it has earlier been proved that the P_{n\\ell}(q) functions are monotone increasing. Recent refinements to the comparison theorem of QM in which comparison potentials can cross over, allow us to prove for n = 1 that Q(q)=Z(q)P(q) is monotone increasing, even though the factor Z(q)=(1+q/N)^{1/q} is monotone decreasing. Thus P(q) cannot increase too slowly. This result yields some sharper estimates for power-potential eigenvlaues at the bottom of each angular-momentum subspace.

  12. Evidence for a disaggregation of the universe

    E-Print Network [OSTI]

    Antonio Alfonso-Faus

    2011-04-19

    Combining the kinematical definitions of the two dimensionless parameters, the deceleration q(x) and the Hubble t0H(x), we get a differential equation (where x = t/t0 is the age of the universe relative to its present value t0). First integration gives the function H(x). The present values of the Hubble parameter H(1) [approximately t0H(1) \\approx 1], and the deceleration parameter [approximately q(1)\\approx - 0.5], determine the function H(x). A second integration gives the cosmological scale factor a(x). Differentiation of a(x) gives the speed of expansion of the universe. The evolution of the universe that results from our approach is: an initial extremely fast exponential expansion (inflation), followed by an almost linear expansion (first decelerated, and later accelerated). For the future, at approximately t \\approx 3t0 there is a final exponential expansion, a second inflation that produces a disaggregation of the universe to infinity. We find the necessary and sufficient conditions for this disaggregation to occur. The precise value of the final age is given only with one parameter: the present value of the deceleration parameter q(1) \\approx - 0.5]. This emerging picture of the history of the universe represents an important challenge, an opportunity for the immediate research on the Universe. These conclusions have been elaborated without the use of any particular cosmological model of the universe.

  13. Latent instabilities in metallic LaNiO? films by strain control of Fermi-surface topology

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

    Yoo, Hyang Keun; Hyun, Seung Ill; Moreschini, Luca; Kim, Hyeong -Do; Chang, Young Jun; Sohn, Chang Hee; Jeong, Da Woon; Sinn, Soobin; Kim, Yong Su; Bostwick, Aaron; et al

    2015-03-04

    Strain control is one of the most promising avenues to search for new emergent phenomena in transition metal-oxide films. Here, we investigate the strain-induced changes of electronic structures in strongly correlated LaNiO? (LNO) films, using angle-resolved photoemission spectroscopy and the dynamical mean-field theory. The strongly renormalized eg-orbital bands are systematically rearranged by misfit strain to change its fermiology. As tensile strain increases, the hole pocket centered at the A point elongates along the kz-axis and seems to become open, thus changing Fermi-surface (FS) topology from three- to quasi-two-dimensional. Concomitantly, the FS shape becomes flattened to enhance FS nesting. A FSmore »superstructure withQ? = (1/2,1/2,1/2) appears in all LNO films, while a tensile-strained LNO film has an additional Q? = (1/4,1/4,1/4) modulation, indicating that some instabilities are present in metallic LNO films. Charge disproportionation and spin-density-wave fluctuations observed in other nickelates might be their most probable origins« less

  14. Trends in U.S. Venture Capital Investments Related to Energy: 1980 through the Third Quarter of 2010

    SciTech Connect (OSTI)

    Dooley, James J.

    2010-11-08

    This report documents trends in U.S. venture capital investments over the period 1980 through the third quarter of calendar year 2010 (2010 Q1+Q2+Q3). Particular attention is given to U.S. venture capital investments in the energy/industrial sector over the period 1980-2010 Q1+Q2+Q3 as well as in the more recently created cross-cutting category of CleanTech over the period 1995-2010 Q1+Q2+Q3. During the early 1980s, U.S. venture capital investments in the energy/industrial sector accounted for more than 20% of all venture capital investments. However subsequent periods of low energy prices, the deregulation of large aspects of the energy industry, and the emergence of fast growing new industries like computers (both hardware and software), biotechnology and the Internet quickly reduced the priority accorded to energy/industrial investments. To wit, venture capital investments related to the energy/industrial sector accounted for only 1% of the $132 billion (in real 2010 US$) invested in 2000 by the U.S. venture capital community. The significant increase in the real price of oil that began in 2003-2004 correlates with renewed interest and increased investment by the venture capital community in energy/industrial investment opportunities. Venture capital investments for 2009 for the energy/industrial sector accounted for $2.4 billion or slightly more than 13% of all venture capital invested that year. The total venture capital invested in energy/industrial during the first three quarters of 2010 is close to $2.4 billion accounting for slightly less than 15% of all venture capital investments during the first three quarters of 2010. In 2009, the aggregate amount invested in CleanTech was $2.1 billion (11% of the total US venture capital invested in that lean year) and for the first three quarters of 2010 US venture capital investments in CleanTech have already exceeded $2.8 billion (18% of all US venture capital investments made during the first three quarters of 2010). Between 2004 and 2009, U.S. venture capital investments in energy/industrial as well as CleanTech have more than quadrupled in real terms.

  15. Trends in U.S. Venture Capital Investments Related to Energy: 1980 through the Second Quarter of 2010

    SciTech Connect (OSTI)

    Dooley, James J.

    2010-07-29

    This report documents trends in U.S. venture capital investments over the period 1980 through the second quarter of calendar year 2010 (2010Q1+Q2). Particular attention is given to U.S. venture capital investments in the energy/industrial sector over the period 1980-2010Q1+Q2 as well as in the more recently created cross-cutting category of CleanTech over the period 1995-2010Q1+Q2. During the early 1980s, U.S. venture capital investments in the energy/industrial sector accounted for more than 20% of all venture capital investments. However subsequent periods of low energy prices, the deregulation of large aspects of the energy industry, and the emergence of fast growing new industries like computers (both hardware and software), biotechnology and the Internet quickly reduced the priority accorded to energy/industrial investments. To wit, venture capital investments related to the energy/industrial sector accounted for only 1% of the $119 billion dollars invested in 2000 by the U.S. venture capital community. The significant increase in the real price of oil that began in 2003-2004 correlates with renewed interest and increased investment by the venture capital community in energy/industrial investment opportunities. Venture capital investments for 2009 for the energy/industrial sector accounted for $2.1 billion or slightly more than 13% of all venture capital invested that year. The total venture capital invested in energy/industrial during the first two quarters of 2010 is close to $1.8 billion accounting for 17% of all venture capital investments during the first two quarters of 2010. In 2009, the aggregate amount invested in CleanTech was $1.8 billion (30% of the total US venture capital invested in that lean year) and for the first two quarters of 2010 US venture capital investments in CleanTech have already exceeded $1.9 billion (19% of all US venture capital investments made during the first half of 2010). Between 2004 and 2009, U.S. venture capital investments in energy/industrial as well as CleanTech have more than quadrupled in real terms.

  16. An economic analysis of the income of rural families in the low income farm area of Northeast Texas 

    E-Print Network [OSTI]

    Wright, Richard Hill

    1958-01-01

    " -. 39 V: . 22~9 . . $2~Q: IvO. Q . 56 l. '' 2Qe9 . ', ' 19oQ . '. : Xtl+9 - ' - k$al '1QQeQ 9~7: . : ?:-:&+1, -: . @ 3. . . . ' Q' Q 1~% Q 62 1Q+Q. '- -'. , g'~$ -", '1(@+Q. 95~5 ';- ';':, RzjQ:;" 39ig::". '", ?$';. 1QQ~Q::$7:~";:":: ', , 'I ''2 6...'Qoc~~s' to iL?n klux'$1 D8-'?eiQQT??alt Pz'+, , e~ '~? 2g'ZkpQ ~+~~@~: ~+ion& 99? f&QM8e;k~, ~~~+/?, 1~. '&7+ . , 80958@?' Geke? INES -Ai'L&ate@&m 9~Vg ~A ~3r~~~a yf' ~tz iQ&w~~vm' 'q'~g &~q x'ig@1t~g . '-'ypng%n~~ 8'49tio?? 40118ge tgtegioo? . '~@Me...

  17. Nonconvex programming techniques based on functional moments 

    E-Print Network [OSTI]

    Martin, Jacques

    1976-01-01

    functions of the form The citations on the following pages follow the style of the Annals of Statistics. (1 9) n f (x) n II (p cos v. x v v ~ ~ . v . v. v+v+ +u &m 1 2'' nj 1 j 1 2 n v. integer, for all j 's j + q sin v, x, ) v. j j j andp + q =1 2... is k (1) Z B. = 0; jt j = 1, 2, . . . , n n (2) 2 ~B. ) &m; t=1, 2, . . . , k j=l (226) Os D 5 (3) 0 II 0 and only one of the two 0 and -0 is represented in D (4) Only one member of the permutation family s (0 ) on a given 0 s D is present (5) B...

  18. A torsional vibration analysis of synchronous motor driven trains by the modal method 

    E-Print Network [OSTI]

    Jung, Si Young

    1986-01-01

    3 IS n Q Q O J (S C3 Q u I) I I c CO (0 cn c I 73 ?Q C cn O 6 3 u c cr u p nj c -a a 6 4) l - i 3 O J [ Z L | ] X a u s n b a J j . a C9 en (3 (9 03 S3 S3 ID S3 S3 i n S) S i S3 m S3 CVJ (3 s ) 0 o... CO cn c t a I cn O s 13 C 0> C c ? C H CO bo CVJ [ zt|] Xouanba J > - ( 9 01 s - ( S n CD U CI (A ( 9 1 - a _Q 1 C (3 a CD ? ' a at LD CD c a ? - a E ft* "0 a m ( 3 (3 0 J (3 (S ? * (3 ?4-

  19. Joint convergence along different subsequences of the signed cubic variation of fractional Brownian motion II

    E-Print Network [OSTI]

    Nualart, David; Swanson, Jason

    2013-10-13

    . Taking in to account that the ?n’s are integers, this implies that L ? N and ?n = L for all but finitely many n. We therefore have an|?n| = |bn ? anL| = k, for large enough n. In this case, using p = L and q = 1 and the fact that fL is periodic... ? anL| = 2n+ 1??. Therefore, ?(t) = 3 4 ? 1 0 f1(x) dx. If an = 2n and bn = 3n+1, then Ln ? 3/2 and an|?n| = |bn?anL| = 1 for all n. Therefore, ?(t) = 1 4 ( f3/2 ( 1 2 + t ) + f3/2(t) ) . ECP 18 (2013), paper 81. Page 10/11 ecp.ejpecp.org Correlations...

  20. Cyclotomic and simplicial matroids

    E-Print Network [OSTI]

    Martin, Jeremy L.; Reiner, Victor

    2005-12-01

    of variables in TG := TM(G) which gives Crapo’s coboundary polynomial G(q; t) [18, x6.3F]: G(q; t) := q 1 X vertex colorings f: V !f1;2;:::;qg tjffv1;v2g2E: f(v1)=f(v2)gj = (t 1)jV j c(G) TG q + t 1 t 1 ; t ; (7) where c(G) denotes the number... of connected components of G. Note that TG(x; y) may be recovered from G(x; y) via the substitution q = (x 1)(y 1); t = y, and that the usual chromatic polynomial G(q) is the specialization q G(q; 0). In this section, we consider the special case that n = pm...

  1. A Development Path for the Stabilized Spheromak

    SciTech Connect (OSTI)

    Fowler, T K

    2007-07-13

    In Refs. [1] - [3], I suggest a concerted computational effort to study profile control of spheromaks, in anticipation that it is timely to incorporate the q < 1 regime of RFP's and spheromaks into an integrated advanced toroidal confinement program, together with improvements in tokamaks and stellarators now being pursued. For profile control of spheromaks by neutral beam injection, with care to avoid super-Alfvenic beam instability the main issue is excitation of tearing modes that can be studied using the NIMROD code already calibrated to MST and SSPX. In this note, I show that profile control on spheromaks could be demonstrated in a device the size of SSPX, leading ultimately to a very compact ignition facility, and possibly modular fusion reactors with a shorter development path.

  2. Minimal regularity conditions for the end-point estimate of bilinear Calderón-Zygmund operators

    E-Print Network [OSTI]

    Perez, Carlos; Torres, Rodolfo H.

    2014-01-09

    , in Rn it can be written in the more geometric form (1.4) sup Q sup y?Q ? Rn\\Q? |K(x, y)?K(x, yQ)| dx < ?, where the supremum is taken over all cubes Q in Rn with sides parallel to the axes, and where Q? is the cube with the same center yQ as Q and side... on the full range of exponents is known. In particular, it was shown in [11] that a bilinear operator bounded from Lp×Lq ? Lr for some 1/p+ 1/q = 1/r, and given by T (f, g)(x) = ? R2n K(x, y, z)f(y)g(z) dydz for x /? supp f ? supp g, also satisfies T : L1 ×L1...

  3. Search for CP violation in tau -> K pi nu(tau) decays

    E-Print Network [OSTI]

    Ammar, Raymond G.; Besson, David Zeke; Zhao, X.

    2002-03-01

    of the amplitude in terms of experimentally jAj 2 H11011 jf V j 2 H208512H20849q ? QH20850H20849Q ? kH20850 2 H20849q 1 2 ReH20849LH20850 ReH20849f S f H11569 V H20850Mm t H20849Q where q and k are the four-vectors of the t lepton and the neutrino, respectively... is constructed from the above quantities. 111803-2 H20850Q 2 H20852 1 jLj 2 jf S j 2 M 2 H20849q ? kH20850 H20850 2 2 ImH20849LH20850 ImH20849f S f H11569 V H20850Mm t H20849Q ? kH20850, (3) To construct the optimal observable we need to express H20849q ? QH20850...

  4. Is nonextensive statistics applicable to continuous Hamiltonian systems?

    E-Print Network [OSTI]

    J. P. Boon; J. F. Lutsko

    2010-06-30

    The homogeneous entropy for continuous systems in nonextensive statistics reads $S^{H}_{q}=k_B\\,{(1 - (K \\int d\\Gamma \\rho^{1/q}(\\Gamma))^{q})}/({1-q})$, where $\\Gamma$ is the phase space variable. Optimization of $S^{H}_{q}$ combined with normalization and energy constraints gives an implicit expression of the distribution function $\\rho (\\Gamma)$ which can be computed explicitly for the ideal gas. From this result, we compute properties such as the energy fluctuations and the specific heat. Similar results are also presented using the formulation based on the Tsallis entropy. From the analysis, we discuss the validity of the application of the nonextensive formalism to continuous Hamiltonian systems which is found to be restricted to the range $qpower law decay.

  5. Coincidence of collective relaxation anomaly and specific heat peak in a bulk metallic glass-forming liquid

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

    Jaiswal, Abhishek; Podlesynak, Andrey; Ehlers, Georg; Mills, Rebecca; O'Keeffe, Stephanie; Stevick, Joseph; Kempton, James; Jelbert, Glenton; Dmowski, Wojciech; Lokshin, Konstantin; et al

    2015-07-21

    The study of multicomponent metallic liquids' relaxational behavior is still the key to understanding and improving the glass-forming abilities of bulk metallic glasses. Here, we report measurements of the collective relaxation times in a melted bulk metallic glass (LM601Zr51Cu36Ni4Al9) in the kinetic regime (Q: 1.5–4.0Å–1) using quasielastic neutron scattering. The results reveal an unusual slope change in the Angell plots of this metallic liquid's collective relaxation time around 950°C, beyond the material's melting point. Measurement of specific heat capacity also reveals a peak around the same temperature. Adams-Gibbs theory is used to rationalize the coincidence, which motivates more careful experimentalmore »and computational studies of the metallic liquids in the future.« less

  6. Big-Bang Nucleosynthesis verifies classical Maxwell-Boltzmann distribution

    E-Print Network [OSTI]

    S. Q. Hou; J. J. He; A. Parikh; K. Daid; C. Bertulani

    2014-08-15

    We provide the most stringent constraint to date on possible deviations from the usually-assumed Maxwell-Boltzmann (MB) velocity distribution for nuclei in the Big-Bang plasma. The impact of non-extensive Tsallis statistics on thermonuclear reaction rates involved in standard models of Big-Bang Nucleosynthesis (BBN) has been investigated. We find that the non-extensive parameter $q$ may deviate by, at most, $|\\delta q|$=6$\\times$10$^{-4}$ from unity for BBN predictions to be consistent with observed primordial abundances; $q$=1 represents the classical Boltzmann-Gibbs statistics. This constraint arises primarily from the {\\em super}sensitivity of endothermic rates on the value of $q$, which is found for the first time. As such, the implications of non-extensive statistics in other astrophysical environments should be explored. This may offer new insight into the nucleosynthesis of heavy elements.

  7. Study of five corrugated case designs 

    E-Print Network [OSTI]

    Rogers, Roxanne Russell

    1996-01-01

    . BEGINNING OF TEST OEC. 12, 1995. END OF TEST AUG. 14, M 1996 2. 5 Z UJ Q 1. 5 NOTE: THIS DATA IS FROM THE TOTAL SAMPLE AS OF 14 AUG 1996. 05? -V- C -r-- D -~- E -A- F -+- G 2/14 2/20 2/22 2/27 3/13 3/27 4/19 4/29 5/01 5/13 2/19 2/22 2/23 3/01 3/20... in the overafl mean trip life and the mean trip life of the correctly printed cases is larger than the same comparison for design codes F and G. I- UJ O CL' UJ 0 110% 100%? 90% ep 7p 6p 5p 40% 30%? 20% 10% p CORRECT INCORRECT D E F...

  8. Equipment balancing and cost estimating a computer approach 

    E-Print Network [OSTI]

    Cottrell, David Sherman

    1987-01-01

    Selection(13. 4) REM Selection (13. 4) = Selection (Capacity. Iieneuver, Lode, No. of Dozers) FOR Q=1 TO 13 FOR R=l TO 4 29 READ Selection(Q, R) SolutionScraper (Q, R) = Selection(Q. R) DATA 11, 0. 7, 0. 9, 0, 16, 0. 7, 0. 9. 0, 20. 0. 7. 0. 7. 1. 22... Cos(Scraper(53, 4) FOR I = I T09 READ CostDozer g(l) NEXT I FOR I I T09 FORJ=I T03 READ CostDozer(I J) NEXT J CostDozer(l, 4) = CostDozer(l, 2) NEXT I DATA D38 . D4E . DSB . 06D DATA 07G, 07H, DBL . 09L, D I IN DATA 7, 10, 17, 10, 13. 20...

  9. Structural assembly of two-domain proteins by rigid-body docking

    E-Print Network [OSTI]

    Cheng, Tammy; Blundell, Tom L.; Fernandez-Recio, Juan

    2008-10-16

    _A(1–123)/2cgp_A(8–207) 1pii 3 (14.0)b 6 (15.9)b 1jcm_P(4–253)/1nsj_-(1–201) 1qcs 1 (7.0) 1 (7.0) 1cr5_B(23–103)/1qdn_A(91–183) 1nkr 37 (10.3)c 6 (10.3)c 1m4k_A(8–102)/2dli_A(109–200) 1a6q 41 (10.8)b 2 (10.8)b 2p8e_A(4–295)/1q1v_A(309–378) 1clc 1291 (7...

  10. A photoelastic study of the stresses in simple beams in pure bending due to loads applied through pins at third points in the beam 

    E-Print Network [OSTI]

    Slagle, Grady Moreland

    1949-01-01

    2 BEAM A X= O. ~ CURVES OF (P Q) AWO 8 '4 g /0 075 050 025 0 -025' -050 -075 -/0 010 TA IIIcE / ROPrt CE/v TER F/G VRE /6 27 SEAM A X= 0. 5 C ALC. VI AT (ON OF SHEAR 5 yRE66 IIVCHE5 /. 0 n FRIIV GE5 8 DEGREES 28 DE6RFE5 Sw28 7iy... 70 70 /40 /+0 . 643 / 6'0 . 032/ . 7/ -+ 7 ?. &3/ ?. /2/9 ?. /999 -/0 7 ABLE /9 8t Abt C X=/. 0 CCIRVES OF (P-Q) AFID g D g '4 4g 4p I PA) 4q 1 6 I /0 075' 050 OZ5' 0 -825 %50 -07$' +0 0/$ 7 ANCE FROID CEA/7 ER F/UVRE 93 BEAJH...

  11. Nuclear electron capture rate in stellar interiors and the case of 7Be

    E-Print Network [OSTI]

    P. Quarati; A. M. Scarfone

    2008-11-25

    Nuclear electron capture rate from continuum in an astrophysical plasma environment (like solar core) is calculated using a modified Debye-Huckel screening potential and the related non-Gaussian q-distribution of electron momenta. For q=1 the well-known Debye-Huckel results are recovered. The value of q can be derived from the fluctuation of number of particles and temperature inside the Debye sphere. For 7Be continuum electron capture in solar core, we find an increase of 7 -- 10 percent over the rate calculated with standard Debye-Huckel potential. The consequence of this results is a reduction of the same percentage of the SSM 8B solar neutrino flux, leaving unchanged the SSM 7Be flux.

  12. The Role of Final State Interactions in Quasielastic $^{56}$Fe$(e,e')$ Reactions at large $|\\vec q|$

    E-Print Network [OSTI]

    C. R. Chinn

    1994-10-21

    A relativistic finite nucleus calculation using a Dirac optical potential is used to investigate the importance of final state interactions [FSI] at large momentum transfers in inclusive quasielastic electronuclear reactions. The optical potential is derived from first-order multiple scattering theory and then is used to calculate the FSI in a nonspectral Green's function doorway approach. At intermediate momentum transfers excellent predictions of the quasielastic $^{56}$Fe$(e,e')$ experimental data for the longitudinal response function are obtained. In comparisons with recent measurements at $|{\\vec q|}=1.14$~GeV/c the theoretical calculations of $R_L$ give good agreement for the quasielastic peak shape and amplitude, but place the position of the peak at an energy transfer of about $40$~MeV higher than the data.

  13. High resolution linkage and association study of quantitative trait loci 

    E-Print Network [OSTI]

    Jung, Jeesun

    2005-11-01

    allele marker, p1 = 0.50,k1 = k2 = 100; For a 3 allele marker, p1 = 0.4,p2 = 0.3,k1 = 100,k2 = k3 = 50; For a 4 allele marker, pi = 0.25,ki = 50,i = 1,???,4. . . . . . . . . . . . . . . . . . . . . . 24 4 Power curves of FGen Nuc,singleton,sibs for 2, 3... curves of FGen Nuc,singleton for 2, 3 and 4 allele markers against the recombination fraction at 0.05 significant level, when q1 = 0.25,?2G = 0.75,A = 20,h2 = 0.25 for a dominant trait a = d = 1.0, Graph I; and a recessive trait a = 1.0 and d = ?0...

  14. The rate of entropy increase at the edge of chaos

    E-Print Network [OSTI]

    V. Latora; M. Baranger; A. Rapisarda; C. Tsallis

    2000-07-07

    Under certain conditions, the rate of increase of the statistical entropy of a simple, fully chaotic, conservative system is known to be given by a single number, characteristic of this system, the Kolmogorov-Sinai entropy rate. This connection is here generalized to a simple dissipative system, the logistic map, and especially to the chaos threshold of the latter, the edge of chaos. It is found that, in the edge-of-chaos case, the usual Boltzmann-Gibbs-Shannon entropy is not appropriate. Instead, the non-extensive entropy $S_q\\equiv \\frac{1-\\sum_{i=1}^W p_i^q}{q-1}$, must be used. The latter contains a parameter q, the entropic index which must be given a special value $q^*\

  15. Bronze Age Representations of Aegean Bull-Games, III

    E-Print Network [OSTI]

    Younger, John G.

    1995-01-01

    ttlen, !v{:iir tlrsir hltir l*ng {il*ntx 5? lPl. l.Xlnl.7fi l}}Y f"rr:sccl. ?{tl. Whitr-p*intetl leuperx itt fr*lco-;tr*rr.llrrr:rl thfrq:frlre tt.r b* rf,{rn}*rr. a}l lr*;rr theil }uir llrrrg ir{clrr{ 4},4V.57 lPl. i-Xlrr|, 7q,1**j. il{her leapcrs r...", uncastrated = "tauros"), he suggests "ta-to-mo" (l.e.. orcr0pQ) "at the farmstead" or "at pasture". E. DAVIS The Vapheio Cups and Aegean GoId and Silver Ware (1977),256-257 & passim, cat. 103; Sp. MARINATOS & M. HIRMER, Crete and Mycenae (1960), pls. 182...

  16. Coupled symplectic maps as models for subdiffusive processes in disordered Hamiltonian lattices

    E-Print Network [OSTI]

    Chris G. Antonopoulos; Tassos Bountis; Lambros Drossos

    2015-08-01

    We investigate dynamically and statistically diffusive motion in a chain of linearly coupled 2-dimensional symplectic McMillan maps and find evidence of subdiffusion in weakly and strongly chaotic regimes when all maps of the chain possess a saddle point at the origin and the central map is initially excited. In the case of weak coupling, there is either absence of diffusion or subdiffusion with $q>1$-Gaussian probability distributions, characterizing weak chaos. However, for large enough coupling and already moderate number of maps, the system exhibits strongly chaotic ($q\\approx 1$) subdiffusive behavior, reminiscent of the subdiffusive energy spreading observed in a disordered Klein-Gordon Hamiltonian. Our results provide evidence that coupled symplectic maps can exhibit physical properties similar to those of disordered Hamiltonian systems, even though the local dynamics in the two cases is significantly different.

  17. An application of Laplace transforms to a machine maintenance problem 

    E-Print Network [OSTI]

    Boone, James Robert

    1962-01-01

    are: (1) P (t) Ll -'(m-n)kh][l-noh], where [14m-n)), h] is the probability n of no failure and [1 - noh] is the probability of no repair. (2) P (t) [m-n+1)Th][l - (n-1) Ph], where [(m-n+1)Xh] is the n-1 probability of one failure and [1 ? (n-1) Wh... is in state 0 and no possibility 0 of failure if the system is in the state 0 . The probabilities of the system being in states 0, 0, 0 at time t + h are then: o' n' m P (t+h) = P (t) [1-(m-n)Q][1-noh] + P (t)[(m-n+l))h][l-(n-l)gh] n n n-1 + P (t)[l-(m...

  18. Equilibrium and Stability of Partial Toroidal Plasma Discharges

    SciTech Connect (OSTI)

    Oz, E.; Myers, C. E.; Yamada, M.; Ji, H.; Kulsrud, R.; Xie, J.

    2011-01-04

    The equilibrium and stability of partial toroidal flux ropes are studied in detail in the laboratory, motivated by ubiquitous loop structures on the solar surface. The flux ropes studied here are magnetized arc discharges formed in the Magnetic Reconnection Experiment (MRX). It is found that these loops robustly maintain their equilibrium on time scales much longer than the Alfven time over a wide range of plasma current, guide eld strength, and angle between electrodes, even in the absence of a strapping fi eld. Additionally, the external kink stability of these flux ropes is found to be governed by the Kruskal-Shafranov limit for a flux rope with line-tied boundary conditions at both ends (q > 1).

  19. On the solutions to the string equation

    E-Print Network [OSTI]

    A. Schwarz

    1991-09-10

    The set of solutions to the string equation $[P,Q]=1$ where $P$ and $Q$ are differential operators is described.It is shown that there exists one-to-one correspondence between this set and the set of pairs of commuting differential operators.This fact permits us to describe the set of solutions to the string equation in terms of moduli spa- ces of algebraic curves,however the direct description is much simpler. Some results are obtained for the superanalog to the string equation where $P$ and $Q$ are considered as superdifferential operators. It is proved that this equation is invariant with respect to Manin-Radul, Mulase-Rabin and Kac-van de Leur KP-hierarchies.

  20. Route to chaos in generalized logistic map

    E-Print Network [OSTI]

    Rafa? Rak; Ewa Rak

    2015-02-01

    Motivated by a possibility to optimize modelling of the population evolution we postulate a generalization of the well-know logistic map. Generalized difference equation reads: \\begin{equation} x_{n+1}=rx^p_n(1-x^q_n), \\end{equation} $x\\in[0,1],\\;(p,q)>0,\\;n=0,1,2,...$, where the two new parameters $p$ and $q$ may assume any positive values. The standard logistic map thus corresponds to the case $p=q=1$. For such a generalized equation we illustrate the character of the transition from regularity to chaos as a function of $r$ for the whole spectrum of $p$ and $q$ parameters. As an example we consider the case for $p=1$ and $q=2$ both in the periodic and chaotic regime. We focus on the character of the corresponding bifurcation sequence and on the quantitative nature of the resulting attractor as well as its universal attribute (Feigenbaum constant).

  1. A Proof of Selection Rules for Critical Dense Polymers

    E-Print Network [OSTI]

    Alexi Morin-Duchesne

    2011-09-29

    Among the lattice loop models defined by Pearce, Rasmussen and Zuber (2006), the model corresponding to critical dense polymers ($\\beta = 0$) is the only one for which an inversion relation for the transfer matrix $D_N(u)$ was found by Pearce and Rasmussen (2007). From this result, they identified the set of possible eigenvalues for $D_N(u)$ and gave a conjecture for the degeneracies of its relevant eigenvalues in the link representation, in the sector with $d$ defects. In this paper, we set out to prove this conjecture, using the homomorphism of the $TL_N (\\beta)$ algebra between the loop model link representation and that of the XXZ model for $\\beta = -(q+q^{-1})$.

  2. Theoretical investigation of projectile angular dependence of the ratio of double to single ionization of helium by fast proton impact 

    E-Print Network [OSTI]

    Fang, Xushan

    1990-01-01

    and the ejected electron taken into account, by dp 2s /. UZscis 'i dn, , i 2 It, (1 ? eicp(2nir)) 0 J& ('2. 27u ) where I'(1 ? iN)l (in ? 2 - i V) It? I'(in ? 2) ] F(in 2+ iN iN 1 () (2 27$) ((Q ? ' k)2 ? cr2]?+2+iN (kb+ Qb)' (k+ Q)2 ? ' or ' ( 2. '27c... j ail cl ? iN f dqb 2 1 t' J (qb Qb)2+2iN [(q+ k)2+ cr2]in+2 2 s( ? [q +(cr ? ip)2]an-t[q +(1 ? in)q k] ? [Q +(c ? ip)2]?[Q2+(I ? in)Q. k]) q & qi=tqs (2. 27d) The calculated results for projectile energies of 0 3, 1, 3 and 6 Me...

  3. The strict-weak lattice polymer

    E-Print Network [OSTI]

    Ivan Corwin; Timo Seppäläinen; Hao Shen

    2015-07-06

    We introduce the strict-weak polymer model, and show the KPZ universality of the free energy fluctuation of this model for a certain range of parameters. Our proof relies on the observation that the discrete time geometric q-TASEP model, studied earlier by A. Borodin and I. Corwin, scales to this polymer model in the limit q->1. This allows us to exploit the exact results for geometric q-TASEP to derive a Fredholm determinant formula for the strict-weak polymer, and in turn perform rigorous asymptotic analysis to show KPZ scaling and GUE Tracy-Widom limit for the free energy fluctuations. We also derive moments formulae for the polymer partition function directly by Bethe ansatz, and identify the limit of the free energy using a stationary version of the polymer model.

  4. Resistive stability of 2/1 modes near 1/1 resonance

    SciTech Connect (OSTI)

    Brennan, D. P.; Turnbull, A. D.; Chu, M. S.; La Haye, R. J.; Lao, L. L.; Osborne, T. H.; Galkin, S. A. [University of Tulsa, 600 South College Avenue, Tulsa, Oklahoma 74104 (United States); General Atomics, 3550 General Atomics Court, San Diego, California 92121 (United States); Far-Tech, 3550 General Atomics Court, San Diego, California 92121 (United States)

    2007-05-15

    The stability of resistive modes is examined using reconstructions of experimental equilibria in the DIII-D tokamak [J. L. Luxon and L. G. Davis, Fusion Technol. 8, 441 (1985)], revealing the important physics in mode onset as discharges evolve to instability. Experimental attempts to access the highest {beta} in tokamak discharges, including 'hybrid' discharges, are typically terminated by the growth of a large 2/1 tearing mode. Model equilibria, based on experimental reconstructions from one of these discharges with steady state axial q{sub 0}{approx_equal}1, are generated varying q{sub 0} and pressure. For each equilibrium, the PEST-III code [A. Pletzer, A. Bondeson, and R. L. Dewar, J. Comput. Phys. 115, 530 (1994)] is used to determine the ideal magnetohydrodynamic solution including both tearing and interchange parities. This outer region solution must be matched to the resistive inner layer solutions at the rational surface to determine resistive mode stability. From this analysis it is found that the approach to q=1 simultaneously causes the 2/1 mode to become unstable and the nonresonant 1/1 displacement to become large, as the ideal {beta} limit rapidly decreases toward the experimental value. However, the 2/2 harmonic on axis, which is also large and is coupled to the saturated steady state 3/2 mode, is thought to contribute to the current drive sustaining q{sub 0} above 1 in these hybrid discharges. Thus, the approach to the q=1 resonance is self-limiting in this context. This work suggests that sustaining q{sub 0} slightly above 1 will avoid the 2/1 instability and will allow access to significantly higher {beta} values in these discharges.

  5. A model for motor-mediated bidirectional transport along an antipolar microtubule bundle

    E-Print Network [OSTI]

    Congping Lin; Peter Ashwin; Gero Steinberg

    2012-11-21

    Long-distance bidirectional transport of organelles depends on the motor proteins kinesin and dynein. Using quantitative data obtained from a fungal model system, we previously developed ASEP-models of bidirectional motion of motors along unipolar microtubules (MTs) near the cell ends of the elongated hyphal cells (herein referred as "unipolar section"). However, recent quantitative live cell imaging in this system has demonstrated that long-range motility of motors and their endosomal cargo mainly occurs along extended antipolar microtubule bundles within the central part of the cell (herein referred to as "bipolar section"). Dynein and kinesin-3 motors coordinate their activity to move early endosomes (EEs) in a bidirectional fashion, with dynein mediating retrograde motility along the unipolar section near the cell poles, whereas kinesin-3 is responsible for bidirectional motions along the antipolar section. Here we extend our modelling approach to simulate bidirectional motility along an antipolar microtubule bundle. In our model, cargos (particles) change direction on each MT with a turning rate $\\Omega$ and the MTs are linked to each other at the minus ends where particles can hop between MTs with a rate $q_1$ (obstacle-induced switching rate) or $q_2$ (end-induced switching rate). By numerical simulations and mean-field approximations, we investigate the distribution of particles along the MTs for different overall densities $\\Theta$. We find that even if $\\Theta$ is low, the system can exhibit shocks in the density profiles near plus and minus ends caused by queueing of particles. We also discuss how the switching rates $q_{1,2}$ influence the type of motor that dominates the active transport in the bundle.

  6. MAGNETIC FIELD STRENGTH FLUCTUATIONS AND THE q-TRIPLET IN THE HELIOSHEATH: VOYAGER 2 OBSERVATIONS FROM 91.0 TO 94.2 AU AT LATITUDE 30 Degree-Sign S

    SciTech Connect (OSTI)

    Burlaga, L. F. [Geospace Physics Laboratory, Code 673, NASA Goddard Space Flight Center, Greenbelt, MD 20771 (United States)] [Geospace Physics Laboratory, Code 673, NASA Goddard Space Flight Center, Greenbelt, MD 20771 (United States); Ness, N. F., E-mail: lburlagahsp@verizon.net, E-mail: nfnudel@yahoo.com [Institute for Astrophysics and Computational Sciences, Catholic University of America, Washington, DC 20064 (United States)

    2013-03-01

    Voyager 2 (V2) was in the heliosheath during 2010, at (91.0-94.2) AU from the Sun and at the latitudes (28. Degree-Sign 8-29. Degree-Sign 3 S) AU, observing solar wind that left the Sun during 2009, when solar activity was very low. There was no feature in B(t) associated with the changes in the plasma parameters observed near 2010.4. The CR-B relation was satisfied. The fluctuations of daily averages of B showed (1) a Gaussian distribution of B, (2) a q-Gaussian of the daily increments of B with q = 1.6, (3) a power-law correlation of B on scales from 1 to 16 days, (4) multifractal structure of B on scales from 1 to 8 days, and (5) a 1/f spectrum of B on scales from 1 to 100 days. The amplitude of the compressive microscale fluctuations of B during several hours on each day is described by the standard deviation (SD) of the 48 s averages of B during the day. Items 2, 3, and 4 determine a 'q-triplet' in the heliosheath. Large-scale fluctuations of SD show (1) a lognormal distribution of SD; (2) an average value of SD = 0.19, 20% of the average B; (3) a q-Gaussian distribution of the increments of SD with q = 1.4; (4) a power-law correlation on scales from 1 to 16 days; and (5) a 1/f spectrum on scales from 1 to 100 days. The heliosheath was in a quasi-stationary, metastable equilibrium state with well-defined structure over a wide range of scales near V2 during 2010.

  7. Radiofrequency Ablation of Liver Metastases-Software-Assisted Evaluation of the Ablation Zone in MDCT: Tumor-Free Follow-Up Versus Local Recurrent Disease

    SciTech Connect (OSTI)

    Keil, Sebastian, E-mail: keil@rad.rwth-aachen.de; Bruners, Philipp [University Hospital, RWTH Aachen University, Department of Diagnostic Radiology (Germany); Schiffl, Katharina [University Hospital, RWTH Aachen University, Institute of Medical Statistics (Germany); Sedlmair, Martin [Siemens Healthcare (Germany); Muehlenbruch, Georg; Guenther, Rolf W.; Das, Marco; Mahnken, Andreas H. [University Hospital, RWTH Aachen University, Department of Diagnostic Radiology (Germany)

    2010-04-15

    The purpose of this study was to investigate differences in change of size and CT value between local recurrences and tumor-free areas after CT-guided radiofrequency ablation (RFA) of hepatic metastases during follow-up by means of dedicated software for automatic evaluation of hepatic lesions. Thirty-two patients with 54 liver metastases from breast or colorectal cancer underwent triphasic contrast-enhanced multidetector-row computed tomography (MDCT) to evaluate hepatic metastatic spread and localization before CT-guided RFA and for follow-up after intervention. Sixteen of these patients (65.1 {+-} 10.3 years) with 30 metastases stayed tumor-free (group 1), while the other group (n = 16 with 24 metastases; 62.0 {+-} 13.8 years) suffered from local recurrent disease (group 2). Applying an automated software tool (SyngoCT Oncology; Siemens Healthcare, Forchheim, Germany), size parameters (volume, RECIST, WHO) and attenuation were measured within the lesions before, 1 day after, and 28 days after RFA treatment. The natural logarithm (ln) of the quotient of the volume 1 day versus 28 days after RFA treament was computed: lnQ1//28/0{sub volume}. Analogously, ln ratios of RECIST, WHO, and attenuation were computed and statistically evaluated by repeated-measures ANOVA. One lesion in group 2 was excluded from further evaluation due to automated missegmentation. Statistically significant differences between the two groups were observed with respect to initial volume, RECIST, and WHO (p < 0.05). Furthermore, ln ratios corresponding to volume, RECIST, and WHO differed significantly between the two groups. Attenuation evaluations showed no significant differences, but there was a trend toward attenuation assessment for the parameter lnQ28/0{sub attenuation} (p = 0.0527), showing higher values for group 1 (-0.4 {+-} 0.3) compared to group 2 (-0.2 {+-} 0.2). In conclusion, hepatic metastases and their zone of coagulation necrosis after RFA differed significantly between tumor-free and local-recurrent ablation zones with respect to the corresponding size parameters. A new parameter (lnQ1//28/0{sub volume/RECIST/WHO/attenuation}) was introduced, which appears to be of prognostic value at early follow-up CT.

  8. Local inverse scattering at a fixed energy for radial Schr{ö}dinger operators and localization of the Regge poles

    E-Print Network [OSTI]

    Thierry Daudé; Francois Nicoleau

    2015-06-12

    We study inverse scattering problems at a fixed energy for radial Schr\\"{o}dinger operators on $\\R^n$, $n \\geq 2$. First, we consider the class $\\mathcal{A}$ of potentials $q(r)$ which can be extended analytically in $\\Re z \\geq 0$ such that $\\mid q(z)\\mid \\leq C \\ (1+ \\mid z \\mid )^{-\\rho}$, $\\rho \\textgreater{} \\frac{3}{2}$. If $q$ and $\\tilde{q}$ are two such potentials and if the corresponding phase shifts $\\delta\\_l$ and $\\tilde{\\delta}\\_l$ are super-exponentially close, then $q=\\tilde{q}$. Secondly, we study the class of potentials $q(r)$ which can be split into $q(r)=q\\_1(r) + q\\_2(r)$ such that $q\\_1(r)$ has compact support and $q\\_2 (r) \\in \\mathcal{A}$. If $q$ and $\\tilde{q}$ are two such potentials, we show that for any fixed $a\\textgreater{}0$, ${\\ds{\\delta\\_l - \\tilde{\\delta}\\_l \\ = \\ o \\left( \\frac{1}{l^{n-3}} \\ \\left( {\\frac{ae}{2l}}\\right)^{2l}\\right)}}$ when $l \\rightarrow +\\infty$ if and only if $q(r)=\\tilde{q}(r)$ for almost all $r \\geq a$. The proofs are close in spirit with the celebrated Borg-Marchenko uniqueness theorem, and rely heavily on the localization of the Regge poles that could be defined as the resonances in the complexified angular momentum plane. We show that for a non-zero super-exponentially decreasing potential, the number of Regge poles is always infinite and moreover, the Regge poles are not contained in any vertical strip in the right-half plane. For potentials with compact support, we are able to give explicitly their asymptotics. At last, for potentials which can be extended analytically in $\\Re z \\geq 0$ with $\\mid q(z)\\mid \\leq C \\ (1+ \\mid z \\mid )^{-\\rho}$, $\\rho \\textgreater{}1$ , we show that the Regge poles are confined in a vertical strip in the complex plane.

  9. Effective field theory and integrability in two-dimensional Mott transition

    SciTech Connect (OSTI)

    Bottesi, Federico L.; Zemba, Guillermo R.

    2011-08-15

    Highlights: > Mott transition in 2d lattice fermion model. > 3D integrability out of 2D. > Effective field theory for Mott transition in 2d. > Double Chern-Simons. > d-Density waves. - Abstract: We study the Mott transition in a two-dimensional lattice spinless fermion model with nearest neighbors density-density interactions. By means of a two-dimensional Jordan-Wigner transformation, the model is mapped onto the lattice XXZ spin model, which is shown to possess a quantum group symmetry as a consequence of a recently found solution of the Zamolodchikov tetrahedron equation. A projection (from three to two space-time dimensions) property of the solution is used to identify the symmetry of the model at the Mott critical point as U{sub q}(sl(2)-circumflex)xU{sub q}(sl(2)-circumflex), with deformation parameter q = -1. Based on this result, the low-energy effective field theory for the model is obtained and shown to be a lattice double Chern-Simons theory with coupling constant k = 1 (with the standard normalization). By further employing the effective filed theory methods, we show that the Mott transition that arises is of topological nature, with vortices in an antiferromagnetic array and matter currents characterized by a d-density wave order parameter. We also analyze the behavior of the system upon weak coupling, and conclude that it undergoes a quantum gas-liquid transition which belongs to the Ising universality class.

  10. Quantum computation with moving quantum dots generated by surface acoustic waves

    E-Print Network [OSTI]

    X. Shi; M. Zhang; L. F. Wei

    2011-02-15

    Motivated by the recent experimental observations [M. Kataoka et al., Phys. Rev. Lett. {\\bf102}, 156801 (2009)], we propose here an theoretical approach to implement quantum computation with bound states of electrons in moving quantum dots generated by the driving of surface acoustic waves. Differing from static quantum dots defined by a series of static electrodes above the two-dimensional electron gas (2DEG), here a single electron is captured from a 2DEG-reservoir by a surface acoustic wave (SAW) and then trapped in a moving quantum dot (MQD) transporting across a quasi-one dimensional channel (Q1DC), wherein all the electrons have been excluded out by the actions of the surface gates. The flying qubit introduced here is encoded by the two lowest adiabatic levels of the electron in the MQD, and the Rabi oscillation between these two levels could be implemented by applying finely-selected microwave pulses to the surface gates. By using the Coulomb interaction between the electrons in different moving quantum dots, we show that a desirable two-qubit operation, i.e., i-SWAP gate, could be realized. Readouts of the present flying qubits are also feasible with the current single-electron detected technique.

  11. q-deformed statistics and the role of a light fermionic dark matter in the supernovae SN1987A cooling

    E-Print Network [OSTI]

    Atanu Guha; Selvaganapathy. J; Prasanta Kumar Das

    2015-09-19

    Light dark matter($\\simeq 1-30~\\rm{MeV}$) particles, pair produced in electron-positron annihilation $ e^-e^+ \\stackrel{\\gamma}{\\longrightarrow} \\chi \\bar{\\chi}$ inside the core of the supernovae, can take away the energy released in the supernovae SN1987A explosion. Using the Raffelt's criterion on the emissivity rate of energy loss for any new channel $\\dot{\\varepsilon}(e^+ e^- \\to \\chi \\overline{\\chi}) \\le 10^{19}~{erg~g^{-1}s^{-1}}$ and working within the formalism of $q$-deformed statistics, we obtain a lower bound on the scale $\\Lambda$ of the dark matter effective theory. As the deformation parameter $q$ varies from $1.01$ to $1.10$, we find that the bound on $\\Lambda$ changes from $3.4\\times 10^6~\\rm{GeV}$ to $2.5\\times 10^7~\\rm{GeV}$ for a light dark matter of mass $m_\\chi = 30~\\rm{MeV}$. For $q=1$ (the undeformed scenario where fermions and bosons obey the normal Fermi-Dirac and Bose-Einstein statistics) we find $\\Lambda = 2.5\\times 10^6~\\rm{GeV}$ for $m_\\chi = 30~\\rm{MeV}$.

  12. Two relations that generalize the $q$-Serre relations and the Dolan-Grady relations

    E-Print Network [OSTI]

    Paul Terwilliger

    2003-07-01

    We define an algebra on two generators which we call the Tridiagonal algebra, and we consider its irreducible modules. The algebra is defined as follows. Let K denote a field, and let $\\beta, \\gamma, \\gamma^*, \\varrho, \\varrho^*$ denote a sequence of scalars taken from K. The corresponding Tridiagonal algebra $T$ is the associative K-algebra with 1 generated by two symbols $A$, $A^*$ subject to the relations (i) \\lbrack A,A^2A^*-\\beta AA^*A + A^*A^2 -\\gamma (AA^*+A^*A)- \\varrho A^*\\rbrack = 0, (ii) \\lbrack A^*,A^{*2}A-\\beta A^*AA^* + AA^{*2} -\\gamma^* (A^*A+AA^*)- \\varrho^* A\\rbrack = 0, where $\\lbrack r,s\\rbrack $ means $rs-sr$. We call these relations the Tridiagonal relations. For $\\beta = q+q^{-1}$, $\\gamma = \\gamma^*=0$, $\\varrho=\\varrho^*=0$, the Tridiagonal relations are the $q$-Serre relations. For $\\beta = 2$, $\\gamma = \\gamma^*=0$, $\\varrho=b^2$, $\\varrho^*=b^{*2}$, the Tridiagonal relations are the Dolan-Grady relations. In the first part of this paper, we survey what is known about irreducible finite dimensional $T$-modules. We focus on how these modules are related to the Leonard pairs recently introduced by the present author, and the more general Tridiagonal pairs recently introduced by Ito, Tanabe, and the present author. In the second part of the paper, we construct an infinite dimensional irreducible $T$-module based on the Askey-Wilson polynomials.

  13. Erosion of a granular bed driven by laminar fluid flow

    E-Print Network [OSTI]

    A. E. Lobkovsky; A. V. Orpe; R. Molloy; A. Kudrolli; D. H. Rothman

    2008-05-01

    Motivated by examples of erosive incision of channels in sand, we investigate the motion of individual grains in a granular bed driven by a laminar fluid to give us new insights into the relationship between hydrodynamic stress and surface granular flow. A closed cell of rectangular cross-section is partially filled with glass beads and a constant fluid flux $Q$ flows through the cell. The refractive indices of the fluid and the glass beads are matched and the cell is illuminated with a laser sheet, allowing us to image individual beads. The bed erodes to a rest height $h_r$ which depends on $Q$. The Shields threshold criterion assumes that the non-dimensional ratio $\\theta$ of the viscous stress on the bed to the hydrostatic pressure difference across a grain is sufficient to predict the granular flux. Furthermore, the Shields criterion states that the granular flux is non-zero only for $\\theta >\\theta_c$. We find that the Shields criterion describes the observed relationship $h_r \\propto Q^{1/2}$ when the bed height is offset by approximately half a grain diameter. Introducing this offset in the estimation of $\\theta$ yields a collapse of the measured Einstein number $q^*$ to a power-law function of $\\theta - \\theta_c$ with exponent $1.75 \\pm 0.25$. The dynamics of the bed height relaxation are well described by the power law relationship between the granular flux and the bed stress.

  14. Stellar and Gaseous Disk Structures in Cosmological Galaxy Equilibrium Models

    E-Print Network [OSTI]

    Rathaus, Ben

    2015-01-01

    We present "radially-resolved-equilibrium-models" for the growth of stellar and gaseous disks in cosmologically accreting massive halos. Our focus is on objects that evolve to redshifts $z\\sim 2$. We solve the time-dependent equations that govern the radially dependent star-formation rates, inflows and outflows from and to the inter- and circum-galactic medium, and inward radial gas flows within the disks. The stellar and gaseous disks reach equilibrium configurations on dynamical time scales much shorter than variations in the cosmological dark matter halo growth and baryonic accretions rates. We show analytically that mass and global angular momentum conservation naturally give rise to exponential gas and stellar disks over many radial length scales. The gaseous disks are more extended as set by the condition Toomre $Q<1$ for star-formation. The disks rapidly become baryon dominated. For massive, $5\\times 10^{12}M_\\odot$ halos at redshift $z=2$, we reproduced the typical observed star-formation rates of ...

  15. Neutron diffraction studies on chemical and magnetic structure of multiferroic PbFe{sub 0.67}W{sub 0.33}O{sub 3}

    SciTech Connect (OSTI)

    Matteppanavar, Shidaling Angadi, Basavaraj; Rayaprol, Sudhindra

    2014-04-24

    We report on the single phase synthesis and room temperature structural characterization of PbFe{sub 0.67}W{sub 0.33}O{sub 3} (PFW) multiferroic. The PFW was synthesized by low temperature sintering, Columbite method. Analysis of powder XRD pattern exhibits single phase formation of PFW with no traces of pyrochlore phase. Detailed analysis of room temperature neutron diffraction (ND) reveals cubic phase at room temperature, space group Pm-3m. The ND pattern clearly reveals magnetic Bragg peak at 2? = 18.51° (Q = 1.36Å{sup ?1}). The refinement of magnetic structure reveals G-type antiferromagnetic structure in PFW at room temperature. The dielectric constant and loss tangent decreases with increasing frequency. The room temperature P-E measurements shows a non-linear slim hysteresis, typical nature of relaxor multiferroics, with saturation and remnant polarizations of P{sub s} = 1.50 ?C/cm{sup 2} and P{sub r} = 0.40 ?C/cm{sup 2}, respectively.

  16. Selfishness, fraternity, and other-regarding preference in spatial evolutionary games

    E-Print Network [OSTI]

    Szabo, Gyorgy; 10.1016/j.jtbi.2011.03.015

    2011-01-01

    Spatial evolutionary games are studied with myopic players whose payoff interest, as a personal character, is tuned from selfishness to other-regarding preference via fraternity. The players are located on a square lattice and collect income from symmetric two-person two-strategy (called cooperation and defection) games with their nearest neighbors. During the elementary steps of evolution a randomly chosen player modifies her strategy in order to maximize stochastically her utility function composed from her own and the co-players' income with weight factors $1-Q$ and Q. These models are studied within a wide range of payoff parameters using Monte Carlo simulations for noisy strategy updates and by spatial stability analysis in the low noise limit. For fraternal players ($Q=1/2$) the system evolves into ordered arrangements of strategies in the low noise limit in a way providing optimum payoff for the whole society. Dominance of defectors, representing the "tragedy of the commons", is found within the region...

  17. Observations on the vitamin B12 binding substance of egg yolk 

    E-Print Network [OSTI]

    Ener, Huseyin Siret

    1953-01-01

    ~gg~ ?'~ ?@T PtETT P W43@QgSJ, '98-Q9~6fx ". ~vs "(&gal 'e. 'w~?-mPva~~r~, S~ ~~m=~A~&~ *ting ~g' Pttgggbf $0'3/36+6'fg(R@TT~5[ g '+PI/ /gal'Pft??'?Q' ?Q 'Q~? " f, , ggttTQI? *'m't Air Il?II'I I0 I? '0 'II ?I??T ll 0 't 000 t. ' t'?00'0 Wt Ill t?LII TT...A, Thesis "yi""ih eQ Le Qhe *~pe'j ~'j e *ese' 1 A: gicQ1+MQ1'5716';, :!eshs'51Q91, . P911e:, :, 6 'Qf Text's , i~ yeW~ial fM "i11'. e~h. i=" ". '. he ie~ixemenPs 'e= -~he Pi~w'x s. pZ"' ' ACKhG~KEEC~L::ai?iT The anterior w1shes to, express...

  18. An ATCA survey of debris disks at 7 millimeters

    E-Print Network [OSTI]

    Ricci, L; Wilner, D; MacGregor, M A; Ubach, C; Carpenter, J M; Testi, L

    2015-01-01

    We present ATCA continuum observations at a wavelength of 6.8 mm of five debris disks: $\\beta$ Pictoris, q$^1$ Eridani, HD 107146, HD 181327, and HD 95086. These observations provide the detection at the longest wavelengths obtained to date for all these debris disks. By combining our 6.8 mm data with previous detections at shorter sub-millimeter/millimeter wavelengths we measure the long wavelength spectral index of these sources. We then use previous estimates for the temperature of the emitting dust to derive the spectral index of the dust emissivity. Under the assumption that all the detected flux comes from dust only, we constrain the slope of the solid size distribution, assumed to be a power-law. The values that we infer for the slope of the size distribution range between about 3.36 and 3.50. We compare our findings with the case of the Fomalhaut debris disk and use these results to test the predictions of collisional cascades of planetesimal belts.

  19. Coordinating Tectons: Bipyridyl Terminated Allenylidene Complexes

    SciTech Connect (OSTI)

    Cifuentes, Marie P.; Humphrey, Mark G.; Koutsantonis, George A.; Lengkeek, Nigel A.; Petrie, Simon; Sanford, Vanessa; Schauer, Phil A.; Skelton, Brian W.; Stranger, Robert; White, Allan H.

    2009-01-15

    A series of complexes with {pi}-conjugated carbon chains terminated by bipyridyl moieties has been prepared. These allenylidene complexes were derived from 9-hydroxy-9-ethynyl-4,5-diazafluorene, the preparation of which is reported; the new allenylidene complexes are highly colored with the cumulated carbon chain terminating in a bipyridyl unit providing a site for further coordination. The synthesis, characterization, and X-ray structure determination of trans-[MCl(P{intersection}P){sub 2}{sub {double_bond}}C{sub {double_bond}}C{sub {double_bond}}(4,5-diazafluoren-9-yl)]PF{sub 6} (M = Ru, P{intersection}P = bis(diphenylphosphino)methane (dppm), 1,2-bis(diphenylphosphino)ethane (dppe), 1,2-bis(dimethylphosphino)ethane (dmpe); M = Os, P{intersection}P = dppm) are described. The effect of the variation in metal and ligand on electronic and electrochemical characteristics of these complexes has been investigated by using UV-vis, solution electrochemistry, and a combination of these techniques in spectroelectrochemical experiments. DFT calculations have been performed on trans-[RuCl(P{intersection}P){sub 2}{sub {double_bond}}C{sub {double_bond}}C{sub {double_bond}}(4,5-diazafluoren-9-yl)]{sup q} (P{intersection}P = dppm, bis(dimethylphosphino)methane (dmpm); q = -1, 0, +1, +2) and subsequently solvent-corrected calculations with use of COSMO were also undertaken to examine the nature of electronic transitions in various oxidation states.

  20. Neutrinoless Double Beta Decay with R-parity Violation

    E-Print Network [OSTI]

    Yosuke Uehara

    2002-06-26

    We consider recently observed neutrinoless double beta decay in the context of the minimal supersymmetric standard model with R-parity violating couplings lambda^{'}. We observe that most of the current experimental bounds on the R-parity violating couplings do not exclude the possibility that the neutrinoless double beta decay is caused by R-parity violation. But if we consider K-bar{K} oscillation, we observe that we have to make the R-parity violating couplings generation-dependent to accomodate with the observed neutrinoless double beta decay. And furthermore, we need some mechanism to cancel the contribution to K-bar{K} mixing from a large R-parity violating coupling. We realized this cancellation by assuming that the first- and the second- generation of quark sector do not couple with the first-generation lepton sector by R-parity violating couplings except the term W=lambda_{111}^{'} L_{1} Q_{1} D_{1}^{c}, which is responsible for the observed neutrinoless double beta decay.