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Sample records for q2 jan-mar q3

  1. Q2 Q3 Season Q2 Q3 Season Q2 Q3 Season

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

    Q2 Q3 Season Q2 Q3 Season Q2 Q3 Season Nominal Prices (dollars per gallon) WTI Crude Oil (Spot) a 1.38 1.11 1.24 1.08 1.06 1.07 -21.4 -4.5 -13.7 Brent Crude Oil Price (Spot) 1.47 1.20 1.33 1.08 1.08 1.08 -26.1 -10.2 -18.8 U.S. Refiner Average Crude Oil Cost 1.37 1.14 1.25 1.00 1.03 1.02 -26.6 -8.8 -18.5 Wholesale Gasoline Price b 2.01 1.84 1.93 1.58 1.46 1.52 -21.6 -20.6 -21.1 Wholesale Diesel Fuel Price b 1.89 1.61 1.75 1.41 1.43 1.42 -25.4 -11.4 -18.8 Regular Gasoline Retail Price c 2.67 2.60

  2. Sep Nov Jan Mar May Jul Sep Nov Jan Mar May Jul Sep Nov Jan

    Office of Legacy Management (LM)

    Nov Jan Mar May Jul Sep Nov Jan Mar May Jul Sep Nov Jan 2008 2009 2010 Mound Site Transition Created with Timeline Maker Professional on May 06 2008 Sep 2008 Phase I Parcel Deed...

  3. Small- and Medium-Size Building Automation and Control System...

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

    ... Milestones & Deliverables (Actual) Q3 (Apr-Jun) Q4 (Jul-Sep) Q1 (Oct-Dec) Legend Summary Q2 (Jan-Mar) Q3 (Apr-Jun) Q4 (Jul-Sep) Q3 (Apr-Jun) Q1 (Oct-Dec) Q2 (Jan-Mar) FY2012 FY2013 ...

  4. Retrofitting Doors on Open Refrigerated Cases

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

    ... Q2 (Jan-Mar) FY2012 FY2013 Legend Q2 (Jan-Mar) Q3 (Apr-Jun) Q4 (Jul-Sep) Q3 (Apr-Jun) Q4 (Jul-Sep) Q1 (Octt-Dec) * Met all original project milestones to date * Original project ...

  5. Rooftop Unit Campaign

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

    ... Future work Report on first year's impact Final achievement recognitions (November 2014) Q1 (Octt-Dec) Q2 (Jan-Mar) Q1 (Octt-Dec) Legend Q2 (Jan-Mar) Q3 (Apr-Jun) Q4 (Jul-Sep) Q4 ...

  6. Lone Star I (Q3) Wind Farm | Open Energy Information

    Open Energy Info (EERE)

    Q3) Wind Farm Jump to: navigation, search Name Lone Star I (Q3) Wind Farm Facility Lone Star I (Q3) Sector Wind energy Facility Type Commercial Scale Wind Facility Status In...

  7. FOIA Quarterly Reports (Q2 2016)

    Office of Energy Efficiency and Renewable Energy (EERE)

    DOE FOIA Quarterly Reports for Q2 2016. This information will be displayed on the DOJ http://www.foia.gov

  8. Lone Star I (Q2) Wind Farm | Open Energy Information

    Open Energy Info (EERE)

    Q2) Wind Farm Jump to: navigation, search Name Lone Star I (Q2) Wind Farm Facility Lone Star I (Q2) Sector Wind energy Facility Type Commercial Scale Wind Facility Status In...

  9. Domestic Coal Distribution 2009 Q2 by Origin State: Alabama

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

    Q2 by Origin State: Alabama (1000 Short Tons) 1 58 Domestic Coal Distribution 2009 Q2 by Origin State: Alabama (1000 Short Tons) Destination State Transportation Mode Electricity...

  10. Domestic Coal Distribution 2009 Q2 by Destination State: Alabama

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

    61 Domestic Coal Distribution 2009 Q2 by Destination State: Alabama (1000 Short Tons) 1 61 Domestic Coal Distribution 2009 Q2 by Destination State: Alabama (1000 Short Tons)...

  11. Q3dComms Version 0.9

    Energy Science and Technology Software Center (OSTI)

    2012-01-05

    Q3dComms provides an interface to the commercial package Quest30 . Quest30 connectors called "channels" can be directly mapped to Umbra connectors using this tool. Furthermore, virtual 30 worlds created in Quest30 can be connected to Umbra with this tool.

  12. Electrolux: ENERGY STAR Referral (GAH105Q2T1)

    Broader source: Energy.gov [DOE]

    DOE referred the matter of Electrolux room air conditioner model GAH105Q2T1 to the EPA for appropriate action after DOE testing showed that the model does not meet the ENERGY STAR specification.

  13. Dish Stirling High Performance Thermal Storage FY15Q3 Quad Chart...

    Office of Scientific and Technical Information (OSTI)

    Technical Report: Dish Stirling High Performance Thermal Storage FY15Q3 Quad Chart ... Visit OSTI to utilize additional information resources in energy science and technology. A ...

  14. Microsoft Word - S06430_JanMar.doc

    Office of Legacy Management (LM)

    Heavy snow cover inhibits normal use of the park. 1.3 Peripheral Properties (Private and City-Owned) * No land use or supplemental standards compliance issues were observed or ...

  15. SPEAR3 Jan-Mar 03 Qtrly Rpt.doc

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

    3 2 TABLE OF CONTENTS Page A. Project Summary 1. Technical Progress 3 2. Future Reporting 5 2. Current Costs 7 B. Detailed Reports 1.1 Magnets & Supports 10 1.2 Vacuum System 10 1.3 Power Supplies 16 1.4 RF System 18 1.5 Instrumentation & Co ntrols 20 1.6 Cable Plant 22 1.7 Beam Line Front Ends 22 1.8 Facilities 23 1.9 Installation 24 2.1 Accelerator Physics 25 3 A. SPEAR 3 PROJECT SUMMARY 1. Technical Progress In general most of the technical systems have been completed; howeve r,

  16. Integrated Solar Thermochemical Reaction System - FY13 Q2 | Department of

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

    Energy Integrated Solar Thermochemical Reaction System - FY13 Q2 Integrated Solar Thermochemical Reaction System - FY13 Q2 This document summarizes the progress of this PNNL project, funded by SunShot, for the second quarter of fiscal year 2013. progress_report_sunshot_pnnl_fy13_q2.pdf (274.11 KB) More Documents & Publications Integrated Solar Thermochemical Reaction System for High Efficiency Production of Electricity Highly Efficient Solar Thermochemical Reaction Systems Integrated

  17. Dish Stirling High Performance Thermal Storage FY14Q3 Quad Chart.

    Office of Scientific and Technical Information (OSTI)

    (Technical Report) | SciTech Connect Dish Stirling High Performance Thermal Storage FY14Q3 Quad Chart. Citation Details In-Document Search Title: Dish Stirling High Performance Thermal Storage FY14Q3 Quad Chart. Abstract not provided. Authors: Andraka, Charles E. Publication Date: 2014-07-01 OSTI Identifier: 1171437 Report Number(s): SAND2014-15691R 533649 DOE Contract Number: AC04-94AL85000 Resource Type: Technical Report Research Org: Sandia National Laboratories (SNL-NM), Albuquerque, NM

  18. Dish Stirling High Performance Thermal Storage FY15Q3 Quad Chart (Technical

    Office of Scientific and Technical Information (OSTI)

    Report) | SciTech Connect Dish Stirling High Performance Thermal Storage FY15Q3 Quad Chart Citation Details In-Document Search Title: Dish Stirling High Performance Thermal Storage FY15Q3 Quad Chart Abstract not provided. Authors: Andraka, Charles E. [1] + Show Author Affiliations Sandia National Lab. (SNL-NM), Albuquerque, NM (United States) Publication Date: 2015-08-01 OSTI Identifier: 1211552 Report Number(s): SAND2015--6472R 598782 DOE Contract Number: AC04-94AL85000 Resource Type:

  19. Dish Stirling High Performance Thermal Storage FY15Q2 Quad Chart (Technical

    Office of Scientific and Technical Information (OSTI)

    Report) | SciTech Connect Technical Report: Dish Stirling High Performance Thermal Storage FY15Q2 Quad Chart Citation Details In-Document Search Title: Dish Stirling High Performance Thermal Storage FY15Q2 Quad Chart Abstract not provided. Authors: Andraka, Charles E. [1] + Show Author Affiliations Sandia National Lab. (SNL-NM), Albuquerque, NM (United States) Publication Date: 2015-04-01 OSTI Identifier: 1178621 Report Number(s): SAND2015-2914R 583301 DOE Contract Number: AC04-94AL85000

  20. SRS Employee Headcount by County of Residence Q3 FY15

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

    3 rd Quarter FY 2015 *Data does not include MOX, Parsons and some small subcontractors SRS Employee Headcount by County of Residence Q3 FY15 GA County SRNS SRR Centerra Ameresco DOE-SR County Total Burke 34 3 4 0 0 41 Columbia 777 260 100 6 42 1185 Jefferson 2 2 0 0 0 4 Lincoln 8 1 2 0 0 11 McDuffie 8 6 0 0 2 16 Richmond 548 160 102 4 29 843 Screven 23 6 1 0 0 30 Other 35 8 3 0 0 46 GA TOTAL 1435 446 212 10 73 2176 SC County SRNS SRR Centerra Ameresco DOE-SR County Total Aiken 2613 852 353 9 158

  1. TOTAL ARRA Homes Weatherized thru Q2 2010 8.19.10.xls | Department of

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

    Energy TOTAL ARRA Homes Weatherized thru Q2 2010 8.19.10.xls (14.26 KB) More Documents & Publications U.S. Department of Energy Weatherization Assistance Program Homes Weatherized By State through 06/30/2010 (Calendar Year) Homes Weatherized by State March 2010 ARRA Homes Weatherized by Grantee

  2. High Precision Measurement of the Proton Elastic Form Factor Ratio at Low Q2

    SciTech Connect (OSTI)

    Xiaohui Zhan

    2009-12-01

    A high precision measurement of the proton elastic form factor ratio µpGEp/GMp in the range Q2 = 0.3–0.7 GeV2/c2 was performed using recoil polarimetry in Jefferson Lab Hall A. In this low Q2 range, previous data from LEDEX [5] along with many fits and calculations [2, 3, 4] indicate substantial deviations of the ratio from unity. In this new measurement, with 80% polarized electron beam for 24 days, we are able to achieve <1% statistical uncertainty. Preliminary results are a few percent lower than expected from previous world data and fits, indicating a smaller GEp at this region. Beyond the intrinsic interest in nucleon structure, the improved form factor measurements also have implications for DVCS, determinations of the proton Zemach radius and strangeness form factors through parity violation experiments.

  3. High Precision Measurement of the Proton Elastic Form Factor Ratio at Low Q2

    SciTech Connect (OSTI)

    Xiaohui Zhan

    2010-01-31

    Experiment E08-007 measured the proton elastic form factor ratio ?pGE/GM in the range of Q2 = 0.3?0.7(GeV/c)2 by recoil polarimetry. Data were taken in 2008 at the Thomas Jefferson National Accelerator Facility in Virginia, USA. A 1.2 GeV polarized electron beam was scattered off a cryogenic hydrogen target. The recoil proton was detected in the left HRS in coincidence with the elasticly scattered electrons tagged by the BigBite spectrometer. The proton polarization was measured by the focal plane polarimeter (FPP). In this low Q2 region, previous measurement from Jefferson Lab Hall A (LEDEX) along with various fits and calculations indicate substantial deviations of the ratio from unity. For this new measurement, the proposed statistical uncertainty (< 1%) was achieved. These new results are a few percent lower than expected from previous world data and fits, which indicate a smaller GEp at this region. Beyond the intrinsic interest in nucleon structure, the new results also have implications in determining the proton Zemach radius and the strangeness form factors from parity violation experiments.

  4. Neutral Pion Electroproduction in the Resonance Region at High $Q^2$

    SciTech Connect (OSTI)

    Villano, A N; Bosted, P E; Connell, S H; Dalton, M M; Jones, M K; Adams, G S; Afanasev, A; Ahmidouch, A; Angelescu, T; Arrington, J; Asaturyan, R; Baker, O K; Benmouna, N; Berman, B L; Breuer, H; Christy, M E; Cui, Y; Danagoulian, S; Day, D; Dodario, T; Dunne, J A; Dutta, D; El Khayari, N; Elliot, B; Ent, R; Fenker, H C; Frolov, V V; Gan, L; Gaskell, D; Gasparian, A; Grullon, S; Hafidi, K; Hinton, W; Holt, R J; Huber, G M; Hungerford, E; Joo, K; Kalantarians, N; Keppel, C E; Kinney, E R; Kubarovsky, V; Li, Y; Liang, Y; Lu, M; Lung, A; Mack, D; Malace, S; Markowitz, P; McKee, P; Meekins, D G; Mkrtchhyan, H; Napolitano, J; Niculescu, G; Niculescu, I; Opper, A K; Pamela, P; Potterveld, D H; Reimer, Paul E; Reinhold, J; Roche, J; Rock, S E; Schulte, E; Segbefia, E; Smith, C; Smith, G R

    2009-09-01

    The process $ep \\to e^{\\prime}p^{\\prime}\\pi^0$ has been measured at $Q^2$ = 6.4 and 7.7 \\ufourmomts in Jefferson Lab's Hall C. Unpolarized differential cross sections are reported in the virtual photon-proton center of mass frame considering the process $\\gamma^{\\ast}p \\to p^{\\prime}\\pi^0$. Various details relating to the background subtractions, radiative corrections and systematic errors are discussed. The usefulness of the data with regard to the measurement of the electromagnetic properties of the well known $\\Delta(1232)$ resonance is covered in detail. Specifically considered are the electromagnetic and scalar-magnetic ratios $R_{EM}$ and $R_{SM}$ along with the magnetic transition form factor $G_M^{\\ast}$. It is found that the rapid fall off of the $\\Delta(1232)$ contribution continues into this region of momentum transfer and that other resonances

  5. SRS Employee Headcount by County of Residence Q2, FY 15

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

    2 nd Quarter, FY 2015 *Data does not include MOX, Parsons and some small subcontractors SRS Employee Headcount by County of Residence Q2, FY 15 GA County SRNS SRR Centerra Ameresco DOE-SR County Total Burke 34 3 4 0 0 41 Columbia 769 249 102 7 45 1172 Jefferson 2 2 0 0 0 4 Lincoln 9 1 2 0 0 12 McDuffie 9 6 0 0 2 17 Richmond 558 146 103 3 29 839 Screven 23 6 1 0 0 30 Other 36 1 3 0 0 40 GA TOTAL 1440 414 215 10 76 2155 SC County SRNS SRR Centerra Ameresco DOE-SR County Total Aiken 2597 829 360 9

  6. Report to Congress on abnormal occurrences. Quarterly report Jan-Mar 81

    SciTech Connect (OSTI)

    Not Available

    1981-07-01

    Section 208 of the Energy Reorganization Act of 1974 identified an abnormal occurrence as an unscheduled incident or event which the Nuclear Regulatory Commission determined to be significant from the standpoint of public health or safety and requires a quarterly report of such events to be made to Congress. This report covers the period January 1 to March 31, 1981. There was one abnormal occurrence at the nuclear power plants licensed to operate; the event involved an inadvertent disconnection of station batteries. There were no abnormal occurrences at the fuel cycle facilities (other than nuclear power plants). There was one abnormal occurrence at other licensee facilities; the event involved occupational overexposures. There were no abnormal occurrences reported by the Agreement States. This report also contains information updating some previously reported abnormal occurrences.

  7. On the determination of the polarized parton distribution in the (x,Q2)-plane: a relativistic quark exchange approach

    SciTech Connect (OSTI)

    Yazdanpanah, M.M.; Modarres, M.

    2005-05-06

    We perform a next-to-leading order QCD analysis of polarized distribution functions of proton in the (x,Q2)-plane within the scheme of the radiative parton model. The flavor-broken light sea quark distributions is investigated and a comparison is made with the corresponding available experimental data.

  8. High-precision measurement of the proton elastic form factor ratio μpGE/GM at low Q2

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

    Zhan, X.; Allada, K.; Armstrong, D. S.; Arrington, J.; Bertozzi, W.; Boeglin, W.; Chen, J. -P.; Chirapatpimol, K.; Choi, S.; Chudakov, E.; et al

    2011-10-06

    Here, we report a new high precision measurement of the proton elastic form factor ratio μpGE/GM for the four-momentum transfer squared Q2 = 0.3-0.7 (GeV/c)2. The measurement was performed at Jefferson Lab (JLab) in Hall A using recoil polarimetry. With the achieved ~1% total uncertainty, the new data clearly show that the deviation of the ratio μpGE/GM from unity observed in previous polarization measurements at high Q2 continues down to the lowest Q2 value of this measurement. The updated global fit that includes the new results yields in this Q2 range an electric (magnetic) form factor ~2% smaller (~1% larger)more » than the previous global fit. We obtain new extractions of the proton electric and magnetic radii, which are (rE2)1/2 = 0.875 ± 0.010 fm and (rM2)1/2 = 0.867 ± 0.020 fm. Moreover, the charge radius is consistent with other recent extractions based on the electron-proton interaction, including the atomic hydrogen Lamb shift measruements, which suggests a missing correction in the comparison of measurements of the proton charge radius using electron probes and the recent extraction from the muonic hydrogen Lamb shift.« less

  9. The Salt Defense Disposal Investigations (SDDI)

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

    Q4 Q2 Q1 Q3 Q4 Q2 Q1 Q3 Q4 Q2 Q1 Q3 Q4 Q2 Q1 Q3 Q4 Q2 Q1 Q3 Q4 Q2 Q1 Q3 Q4 Q2 Q1 Q3 Task Name ID 1 2 3 4 5 6 7 8 9 Mine and Construct the Test Commit to Major Procurements...

  10. 2014_Q3.indd

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

    July-September 2014 issue of the U.S. Department of Energy Offce of Legacy Management Quarterly Program Update. This publication is designed to provide a status of activities within LM. Please direct all comments and inquiries to lm@hq.doe.gov. July-September 2014 Visit us at http://energy.gov/lm/ Goal 5 2014 LM All-Hands Training The U.S. Department of Energy (DOE) Offce of Legacy Management (LM) 2014 All-Hands Training was held the week of July 28, 2014, in Albuquerque, New Mexico. The week

  11. Measurement of the generalized form factors near threshold via γ*p → nπ+ at high Q2

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

    Park, K.; Adhikari, K. P.; Adikaram, D.; Anghinolfi, M.; Baghdasaryan, H.; Ball, J.; Battaglieri, M.; Batourine, V.; Bedlinskiy, I.; Bennett, R. P.; et al

    2012-03-26

    We report the first extraction of the pion-nucleon multipoles near the production threshold for the nπ+ channel at relatively high momentum transfer (Q2 up to 4.2 GeV2). The dominance of the s-wave transverse multipole (E0+), expected in this region, allowed us to access the generalized form factor G1 within the light-cone sum rule (LCSR) framework as well as the axial form factor GA. The data analyzed in this work were collected by the nearly 4π CEBAF Large Acceptance Spectrometer (CLAS) using a 5.754-GeV electron beam on a proton target. The differential cross section and the π-N multipole E0+/GD were measuredmore » using two different methods, the LCSR and a direct multipole fit. The results from the two methods are found to be consistent and almost Q2 independent.« less

  12. Measurement of the generalized form factors near threshold via γ*p → nπ+ at high Q2

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

    Park, K.; Adhikari, K. P.; Adikaram, D.; Anghinolfi, M.; Baghdasaryan, H.; Ball, J.; Battaglieri, M.; Batourine, V.; Bedlinskiy, I.; Bennett, R. P.; et al

    2012-03-26

    We report the first extraction of the pion-nucleon multipoles near the production threshold for the nπ+ channel at relatively high momentum transfer (Q2 up to 4.2 GeV2). The dominance of the s-wave transverse multipole (E0+), expected in this region, allowed us to access the generalized form factor G1 within the light-cone sum rule (LCSR) framework as well as the axial form factor GA. The data analyzed in this work were collected by the nearly 4π CEBAF Large Acceptance Spectrometer (CLAS) using a 5.754-GeV electron beam on a proton target. The differential cross section and the π-N multipole E0+/GD were measuredmore »using two different methods, the LCSR and a direct multipole fit. The results from the two methods are found to be consistent and almost Q2 independent.« less

  13. Ocean thermal energy at the Johns Hopkins University Applied Physics Laboratory, quarterly report. Report for Jan-Mar 82

    SciTech Connect (OSTI)

    Not Available

    1982-01-01

    The following are included: Ocean thermal energy conversion (OTEC)--OTEC pilot plant conceptual design review; OTEC methanol; review of electrolyzer development programs and requirements; financial and legal considerations in OTEC implementation; potential navy sites for GEOTEC systems; hybrid geothermal-OTEC power plants: single-cycle performance estimates; and supervision of testing of pneumatic wave energy conversion system.

  14. Theoretical investigations of the IO,{sup q+} (q = 2, 3, 4) multi-charged ions: Metastability, characterization and spectroscopy

    SciTech Connect (OSTI)

    Hammami, H.; Yazidi, O.; Ben El Hadj Rhouma, M.; Al Mogren, M. M.; Hochlaf, M.

    2014-07-07

    Using ab initio methodology, we studied the IO{sup q+} (q = 2, 3, 4) multi-charged ions. Benchmark computations on the IO(X{sup 2}Π) neutral species allow validate the current procedure. For IO{sup 2+}, several potential wells were found on the ground and the electronic excited states potentials with potential barriers with respect to dissociation, where this dication can exist in the gas phase as long-lived metastable molecules. We confirm hence the recent observation of the dication by mass spectrometry. Moreover, we predict the existence of the metastable IO{sup 3+} trication, where a shallow potential well along the IO internuclear distance is computed. This potential well supports more than 10 vibrational levels. The IO{sup 3+} excited states are repulsive in nature, as well as the computed potentials for the IO{sup 4+} tetracation. For the bound states, we give a set of spectroscopic parameters including excitation transition energies, equilibrium distances, harmonic and anharmonic vibrational terms, and rotational constants. At the MRCI + Q/aug-cc-pV5Z(-PP) level, the adiabatic double and triple ionization energies of IO are computed to be ∼28.1 eV and ∼55.0 eV, respectively.

  15. Final analysis of proton form factor ratio data at Q2 = 4.0, 4.8, and 5.6 GeV2

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

    Puckett, A. J. R.; Brash, E. J.; Gayou, O.; Jones, M. K.; Pentchev, L.; Perdrisat, C. F.; Punjabi, V.; Aniol, K. A.; Averett, T.; Benmokhtar, F.; et al

    2012-04-11

    Recently published measurements of the proton electromagnetic form factor ratio R = μp GEp/GMp at momentum transfers Q2 up to 8.5 GeV2 in Jefferson Lab Hall C deviate from the linear trend of previous measurements in Jefferson Lab Hall A, favoring a slower rate of decrease of R with Q2. While statistically compatible in the region of overlap with Hall A, the Hall C data hint at a systematic difference between the two experiments. This possibility was investigated in a reanalysis of the Hall A data. We find that the original analysis underestimated the background in the selection of elasticmore » events. The application of an additional cut to further suppress the background increases the results for R, improving the consistency between Halls A and C.« less

  16. Exclusive single pion electroproduction off the proton in the high-lying resonances at Q2 < 5 GeV2 from CLAS

    SciTech Connect (OSTI)

    Park, Kijun

    2014-09-01

    The differential cross sections and structure functions for the exclusive electroproduction process ep --> e'n pi+ were measured in the range of the invariantmass for the np+ system 1.6 GeV lte W lte 2.0 GeV, and the photon virtuality 1.8 GeV2 lte Q2 lte 4.0 GeV2 using CLAS at Jefferson Lab. For the first time, these kinematics are probed in the exclusive p+ production from the protons with nearly full coverage in the azimuthal and polar angles of the np+ center-of-mass system. In this analysis, approximately 39,000 differential cross-section data points in terms of W, Q2, cosq theta* _ pi, and phi?_p-, were obtained. The preliminary differential cross section and structure function analyses are carried out, which allow us to extract the helicity amplitudes in high-lying resonances.

  17. Q3 1997 STEO, Final

    Gasoline and Diesel Fuel Update (EIA)

    7 (Released July 8, 1997) Energy Information Administration DOE/EIA-0202(97/3Q) Distribution Category UC-950 Short-Term Energy Outlook Quarterly Projections Third Quarter 1997 Energy Information Administration Office of Energy Markets and End Use U.S. Department of Energy Washington, DC 20585 This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the Department of Energy. The information contained herein should not be construed

  18. Measurement of the Neutron (3He) Spin Structure at Low Q2 and the Extended Gerasimov-Drell-Hearn Sum Rule

    SciTech Connect (OSTI)

    Ioannis Kominis

    2001-01-31

    This thesis presents the results of E-94010, an experiment at Thomas Jefferson National Accelerator Facility (TJNAF) designed to study the spin structure of the neutron at low momentum transfer, and to test the extended Gerasimov-Drell-Hearn (GDH) sum rule. The first experiment of its kind, it was performed in experimental Hall-A of TJNAF using a new polarized 3He facility. It has recently been shown that the GDH sum rule and the Bjorken sum rule are both special examples of a more general sum rule that applies to polarized electron scattering off nucleons. This generalized sum rule, due to Ji and Osborne, reduces to the GDH sum rule at Q2 = 0 and to the Bjorken sum rule at Q2 >> 1 GeV2. By studying the Q2 evolution of the extended GDH sum, one learns about the transition from quark-like behavior to hadronic-like behavior. We measured inclusive polarized cross sections by scattering high energy polarized electrons off the new TJNAF polarized 3He target with both longitudinal and transverse target orientations. The high density 3He target, based on optical pumping and spin exchange, was used as an effective neutron target. The target maintained a polarization of about 35% at beam currents as high as 151tA. We describe the precision 3He polarimetry leading to a systematic uncertainty of the target polarization of 4% (relative). A strained GaAs photocathode was utilized in the polarized electron gun, which provided an electron beam with a polarization of about 70%, known to 3% (relative). By using six different beam energies (between 0.86 and 5.06 GeV) and a fixed scattering angle of 15.5, a wide kinematic coverage was achieved, with 0.02 GeV2< Q2 <1 GcV2 and 0.5 GeV< W < 2.5 GeV for the squared momentum transfer and invariant mass, respectively. From the measured cross sections we extract the 3He spin structure functions He and g1e Finally, we determine the extended GDH sum for the range 0.1 GeV2< Q2 <1 GeV2 for 3He and the neutron.

  19. ACBEDGF1DIH P Q2R§STDVU@DVW RYX1`bacSedVagf ShFiSpaqSTr1H£s)t

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

    ¢¤¥§¦©¨ ¥! ¥ " ¥#¢ $ %¡'&( $ %&()0&1%234 ¥5¨  6§!7580 9 @&1¢2 ACBEDGF1DIH P Q2R§STDVU@DVW RYX1`bacSedVagf ShFiSpaqSTr1H£s)t Wvuwr1HxHbD y €B‚Sƒr„Hx€†…0‡ˆ€†‰@rW‘€’B‚rwWq` “•”!–˜—w™edgfih j rkD Pl€†Wv…eacr1H£sm‡r„ant …o€p r1a q DrH y rw…ƒ…TDGBcBIsmt Wvuwr„H¤HbD s

  20. Precise determination of the deuteron spin structure at low to moderate Q2 with CLAS and extraction of the neutron contribution

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

    Guler, N.; Fersch, R. G.; Kuhn, S. E.; Bosted, P.; Griffioen, K. A.; Keith, C.; Minehart, R.; Prok, Y.; Adhikari, K. P.; Adikaram, D.; et al

    2015-11-02

    In this study, we present the final results for the deuteron spin structure functions obtained from the full data set collected with Jefferson Lab's CLAS in 2000-2001. Polarized electrons with energies of 1.6, 2.5, 4.2 and 5.8 GeV were scattered from deuteron (15ND3) targets, dynamically polarized along the beam direction, and detected with CLAS. From the measured double spin asymmetry, the virtual photon absorption asymmetry Ad1 and the polarized structure function gd1 were extracted over a wide kinematic range (0.05 GeV2 < Q2 < 5 GeV2 and 0.9 GeV < W < 3 GeV). We use an unfolding procedure andmore » a parametrization of the corresponding proton results to extract from these data the polarized structure functions An1 and g1n of the (bound) neutron, which are so far unknown in the resonance region, W < 2 GeV. We compare our final results, including several moments of the deuteron and neutron spin structure functions, with various theoretical models and expectations as well as parametrizations of the world data. The unprecedented precision and dense kinematic coverage of these data can aid in future extractions of polarized parton distributions, tests of perturbative QCD predictions for the quark polarization at large x, a better understanding of quark-hadron duality, and more precise values for higher-twist matrix elements in the framework of the Operator Product Expansion.« less

  1. Measurements of the Electric Form Factor of the Neutron up to Q2 = 3.4 GeV2 using the Reaction He-3(e,e'n)pp

    SciTech Connect (OSTI)

    Riordan, Seamus; Craver, Brandon; Kelleher, Aidan; Kolarkar, Ameya; Miller, Jonathan; Cates, Gordon; Liyanage, Nilanga; Wojtsekhowski, Bogdan; Quimper, Armando Acha; Allada, Kalyan; Anderson, Byron; Aniol, Konrad; Annand, John; Arrington, John; Averett, Todd; Beck, Arie; Bellis, Matthew; Boeglin, Werner; Breuer, Herbert; Calarco, John; Chen, Jian-Ping; Chudakov, Eugene; Coman, Luminita; Crowe, Benjamin; Cusanno, Francesco; Day, Donal; Degtiarenko, Pavel; Dolph, P.A.M.; Dutta, Chiranjib; Ferdi, Catherine; Fernandez-Ramirez, Cezar; Feuerbach, Robert; Fraile Prieto, Luis; Franklin, Gregg; Frullani, Salvatore; Fuchs, Sabine; Garibaldi, Franco; Gevorgyan, Nerses; Gilman, Ronald; Glazmazdin, Oleksandr; Gomez, Javier; Grimm, Klaus; Hansen, Jens-Ole; Herraiz, Joaquin Lopez; Higinbotham, Douglas; Holmes, Richard; Holmstrom, Timothy; Howell, David; De Jager, Cornelis; Jiang, Xiaodong; Jones, Mark; Katich, Joseph; Kaufman, Lisa; Khandaker, Mahbubul; Kelly, James; Kiselev, Daniela; Korsch, Wolfgang; LeRose, John; Markowitz, Pete; Margaziotis, Demetrius; May-Tal Beck, Sharon; Mayilyan, Samvel; McCormick, Kathy; Meziani, Zein-Eddine; Michaels, Robert; Moffit, Bryan; Nanda, Sirish; Nelyubin, Vladimir; Ngo, Tim; Nikolenko, Dmitri; Norum, Blaine; Pentchev, Lubomir; Perdrisat, Charles; Piasetzky, Eliazer; Pomatsalyuk, Roman; Protopoescu, Dan; Puckett, Andrew; Punjabi, Vina; Qian, XIn; Qiang, Yi; Quinn, Brian; Rachek, Igor; Ransome, Ronald; Reimer, Paul; Reitz, Bodo; Roche, Julie; Ron, Guy; Rondon-Aramayo, Oscar; Rosner, Guenther; Saha, Arunava; Sargsian, Misak; Sawatzky, Bradley; Segal, John; Shabestari, Mitra Hashemi; Shahinyan, Albert; Singh, Jaideep; Sirca, Simon; Souder, Paul; Stepanyan, Samuel; Stibunov, Victor; Sulkosky, Vince; Sulkosky, Vincent; Tajima, Shigeyuki; Tobias, William; Moinelo, Jose Udias; Urciuoli, Guido; Vlahovic, Branislav; Voskanyan, Hakob; Wang, Kebin; Wesselmann, Frank; Vignote, Javier Rodriguez; Wood, Stephen; Wright, Justin; Yao, Huan

    2010-12-01

    The electric form factor of the neutron was determined from studies of the reaction \\rea{} in quasi-elastic kinematics in Hall A at Jefferson Lab. Longitudinally polarized electrons were scattered off a polarized target in which the nuclear polarization was oriented perpendicular to the momentum transfer. The scattered electrons were detected in a magnetic spectrometer in coincidence with neutrons that were registered in a large-solid-angle detector. More than doubling the $Q^2$-range over which it is known, we find \\GEn{}$ = 0.0225 \\pm 0.0017 (stat) \\pm 0.0024 (syst)$, $0.0200 \\pm 0.0023 \\pm 0.0018$, and $0.0142 \\pm 0.0019 \\pm 0.0013$ for $Q^2$ = 1.72, 2.48, and 3.41~\\gevsq, respectively.

  2. FOIA Quarterly Reports (Q3 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...

  3. FOIA Quarterly Reports (Q3 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.

  4. FOIA Quarterly Reports (Q3 2016)

    Broader source: Energy.gov [DOE]

    The Department of Energy (DOE) 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 environmental cleanup of the national nuclear weapons complex. The records maintained by the DOE often involve proprietary matters, classified matters, innovation matters, and environmental matters. The DOE invokes several of the FOIA’s exemptions to protect information that is: •classified as restricted data or formerly restricted data; •proprietary; •personal; and •pre-decisional and deliberative. These types of information may not be granted under the FOIA to protect national security, proprietary interests of submitters; personal privacy of individuals, and open and frank discussion.

  5. Q3 1996 STEO TEXT/TABLES

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

    ... are based on annual data for coal-fired generation at nonutilities reported on Form EIA-867. Data for 1994 and 1995 are estimates. d Synfuels plant demand in 1993 was 1.7 million ...

  6. Beam-Target Double-Spin Asymmetry ALT in Charged Pion Production from Deep Inelastic Scattering on a Transversely Polarized He3 Target at 1.4<Q2<2.7 GeV2

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

    Huang, J.; Allada, K.; Dutta, C.; Katich, J.; Qian, X.; Wang, Y.; Zhang, Y.; Aniol, K.; Annand, J. R. M.; Averett, T.; et al

    2012-01-01

    We report the first measurement of the double-spin asymmetry ALT for charged pion electroproduction in semi-inclusive deep inelastic electron scattering on a transversely polarized 3He target. The kinematics focused on the valence quark region, 0.16 < x < 0.35 with 1.4 < Q2 < 2.7 GeV2. The corresponding neutron ALT asymmetries were extracted from the measured 3He asymmetries and proton/3He cross section ratios using the effective polarization approximation. These new data probe the transverse momentum dependent parton distribution function g1Tq and therefore provide access to quark spin-orbit correlations. Our results indicate a positive azimuthal asymmetry for π- production on 3Hemore » and the neutron, while our π+ asymmetries are consistent with zero.« less

  7. fu-q(2)-99.pdf

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

    FDTD Scheme for Light Scattering by Dielectric Particles with Large Complex Refractive Index Q. Fu and W. B. Sun Dalhousie University Halifax, Nova Scotia, Canada Numerical solution for light scattering by highly refractive dielectric particles is examined with the finite-difference time domain (FDTD) technique. In the FDTD, the computational domain is truncated using the perfectly matched layer (PML) absorbing boundary condition (Sun et al. 1999). It is found that for dielectric particles with

  8. Microchannel Receiver Development- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  9. FOIA Quarterly Reports (Q2 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...

  10. FOIA QUARTERLY REPORTS (Q2-2014)

    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...

  11. Q2 External Package.xls

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

    376,031 285,072 76% 214,494 57% Interest Expense and (Income) 33 Interest Expense 352,982 351,730 331,697 94% 158,351 45% 34 AFUDC (43,062) (43,204) (45,230) 105% (26,819)...

  12. compare_tables.xlsx

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

    ... Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 2014 2015 2016 2017 2014-2015 2015-2016 2016-2017 U.S. Petroleum WTI spot (barrel) Current 48.48 57.85 46.55 41.94 33.35 44.52 46.00 47.00 ...

  13. Final Meeting Summary Page 1

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

    committee and introductions were made. The committee approved the June meeting summary. ... Assessment, Q2 * Natural Gas Pipeline Environmental Impact Statement (EIS), Q3 ...

  14. Slide 1

    Energy Savers [EERE]

    ... Nigeria - 2.9 Trinidad &Tobago - 2.1 Equitorial Guinea - 0.5 Oman - 1.5 UAE - 0.8 USA - 0.2 Peru - 0.6 Source: Waterborne, Cheniere Research 26 Q4 Q1 Q1 Q1 Q1 Q1 Q2 Q2 Q1 Q2 Q3 Q2 ...

  15. Observations from The EV Project in Q3 2013

    SciTech Connect (OSTI)

    John Smart

    2013-12-01

    This is a brief report that summarizes results published in numerous other reports. It describes the usage of electric vehicles and charging units in the EV Project over the past 3 months. There is no new data or information provided in this report, only summarizing of information published in other reports (which have all been approved for unlimited distribution publication). This report will be posted to the INL/AVTA website for viewing by the general public.

  16. Flexible Assembly Solar Technology- FY13 Q3

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this BrightSource Energy project, funded by SunShot, for the second quarter of fiscal year 2013.

  17. FY 2014 Q3 Metric Summary | Department of Energy

    Office of Environmental Management (EM)

    FY 2014 Overall Contract and Project Management Improvement Performance Metrics and Targets FY 2015 Overall Contract and Project Management Improvement Performance Metrics and ...

  18. FY 2016 Q3 Metrics Summary.xlsx

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

    FY 2016 Target 95% 95% 90% 85% 90% 90% FY 2016 3rd Qtr Actual Comment FY 2016 Forecast ... Schedule Compliance, Projects Less Than 5 Years Duration: Projects will meet the project ...

  19. Microsoft Word - DOE_ANNUAL_METRICS_2009Q3.docx

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

    14404 Third Quarter 2009 Modeling Program Metric: Coupled model comparison with observations using improved dynamics at coarse resolution Quantifying the impact of a finite volume dynamical core in CCSM3 on simulated precipitation over major catchment areas July 2009 Peter J. Gleckler and Karl E. Taylor Lawrence Livermore National Laboratory Livermore, CA Work supported by the U.S. Department of Energy, Office of Science, Office of Biological and Environmental Research 
 2
 Disclaimer This

  20. Tensor spin observables and spin stucture at low Q2

    SciTech Connect (OSTI)

    Slifer, Karl J.

    2015-04-01

    We discuss recent spin structure results from Jefferson Lab, and outline an emerging program to study tensor spin observables using solid deuteron targets. These new experiments open the potential to study hidden color, the tensor nature of short range correlations, and to probe for exotic gluonic states.

  1. SU{sub {ital q}}(2) lattice gauge theory

    SciTech Connect (OSTI)

    Bimonte, G.; Stern, A.; Vitale, P.

    1996-07-01

    We reformulate the Hamiltonian approach to lattice gauge theories such that, at the classical level, the gauge group does not act canonically, but instead as a Poisson-Lie group. At the quantum level, the symmetry gets promoted to a quantum group gauge symmetry. The theory depends on two parameters: the deformation parameter {lambda} and the lattice spacing {ital a}. We show that the system of Kogut and Susskind is recovered when {lambda}{r_arrow}0, while QCD is recovered in the continuum limit (for any {lambda}). We, thus, have the possibility of having a two-parameter regularization of QCD. {copyright} {ital 1996 The American Physical Society.}

  2. 10-Megawatt Supercritical Carbon Dioxide Turbine- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  3. Flexible Assembly Solar Technology- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  4. Shorepower Truck Electrification Project (STEP) - 1Q - 2Q 2013

    SciTech Connect (OSTI)

    2014-02-01

    The Fleet Test and Evaluation Team at the U.S. Department of Energy's National Renewable Energy Laboratory is evaluating and documenting the use of shorepower at 50 planned American Recovery and Reinvestment Act (ARRA)-funded truck stop electrification (TSE) sites across the nation. Trucks participating in the study have idle-reduction equipment installed that was purchased with rebates through the ARRA. A total of 5,000 rebates will be approved. the ARRA. A total of 5,000 rebates will be approved.

  5. High-Performance Nanostructured Coating- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  6. NBB Enclosed Particle Receiver- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  7. Low-Cost, Lightweight Solar Concentrators FY13 Q2

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Jet Propulsion Laboratory project, funded by SunShot, for the second quarter of fiscal year 2013.

  8. Presentation title: This can be up to 2 lines

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

    to continued declines in profits. * Capital expenditure per barrel produced was the ... Q1 Q2 Q3 Q4 2011 2012 2013 2014 2015 Capital expenditure decreased 11 billion since ...

  9. Transport Studies Enabling Efficiency Optimization of Cost-Competitive...

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

    the PEM Stack Transport Studies Transport Studies Enabling Efficiency Optimization of Cost-Competitive Fuel Cell ... 11 Q1 12 Q2 12 Q3 12 1. Systems Analysis NFC 2. Test ...

  10. Attachment 1 - PIC Transcribed Flip Chart Notes Final Meeting Summary Page 12

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

    - PIC Transcribed Flip Chart Notes Final Meeting Summary Page 12 Public Involvement Committee September 4, 2013 Strategic Planning: Quarters by month * Q1: Oct. - Dec. * Q2: Jan - March * Q3: April - June * Q4: July - Sept. Page 1 Strategic Planning: 2014 Topics (Interactive activity) * = priority topic for discussion at meeting; �= priority for future discussion | Quarter prioritized for discussion (Q1, Q2, Q3, Q4) * 100-F Proposed Plan | *** Q2 * 100 D-H Proposed Plan * Draft Land

  11. Dish Stirling High Performance Thermal Storage FY14Q3 Quad Chart...

    Office of Scientific and Technical Information (OSTI)

    Report Number(s): SAND2014-15691R 533649 DOE Contract Number: AC04-94AL85000 Resource Type: Technical Report Research Org: Sandia National Laboratories (SNL-NM), Albuquerque, NM ...

  12. Dish Stirling High Performance Thermal Storage FY14Q3 Quad Chart

    Office of Scientific and Technical Information (OSTI)

    coatings to short-term test initiated * Enhanced powder screening method initiated * Heat pipe advanced wick development * Two heat pipe wicks assembled into bench scale devices...

  13. High-Efficiency Receivers for Supercritical Carbon Dioxide Cycles- FY13 Q3

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Brayton Energy project, funded by SunShot, for the third quarter of fiscal year 2013.

  14. FY 2014 Q3 RCA CAP Performance Metrics Report 2014-09-05.xlsx

    Energy Savers [EERE]

    ContractProject Management Performance Metrics FY 2014 Target FY 2014 Pre- & Post- CAP* ... TPC is Total Project Cost. No. FY 2014 Target FY 2014 3rd Qtr Actual 2 95% 92% 3 95% ...

  15. Microsoft Word - Q3 MDA 8_11_2015 Update of $172M for Reposting...

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

    to deliver on its mission. BPA also funds regional efforts to protect and enhance fish and wildlife populations affected by hydropower development in the Columbia River...

  16. Dish Stirling High Performance Thermal Storage FY15Q3 Quad Chart...

    Office of Scientific and Technical Information (OSTI)

    Close Cite: Bibtex Format Close 0 pages in this document matching the terms "" Search For Terms: Enter terms in the toolbar above to search the full text of this document for ...

  17. Low-Cost Metal Hydride TES Systems- FY13 Q3

    Broader source: Energy.gov [DOE]

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

  18. High-Efficiency Thermal Energy Storage System for CSP- FY13 Q3

    Broader source: Energy.gov [DOE]

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

  19. Dish/Stirling High-Performance Thermal Storge- FY13 Q3

    Broader source: Energy.gov [DOE]

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

  20. Advanced Low-Cost Recievers for Parabolic Troughs- FY13 Q3

    Broader source: Energy.gov [DOE]

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

  1. Enclosure - FY 2015 Q3 Metrics Report 2015-08-12.xlsx

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

    ContractProject Management Performance Metrics FY 2015 Target FY 2015 Pre- & Post- CAP* Forecast Comment 1 Capital Asset Project Management Success: Complete 90% of capital asset ...

  2. bbnp_bb_an_0003578_pmc_dashboard_y13-q3.xls

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

    ... Number Of Tenants Tenancy Assessed Value Down Payment First Trust Deed Balance First Trust Deed Lender First Trust Deed Payment First Trust Deed Terms Second Trust Deed Balance ...

  3. bbnp_bb_an_0004442_pmc_dashboard_y13-q3.xls

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

    ... Number Of Tenants Tenancy Assessed Value Down Payment First Trust Deed Balance First Trust Deed Lender First Trust Deed Payment First Trust Deed Terms Second Trust Deed Balance ...

  4. bbnp_bb_an_0003562_pmc_dashboard_y13-q3_0.xls

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

    ... Number Of Tenants Tenancy Assessed Value Down Payment First Trust Deed Balance First Trust Deed Lender First Trust Deed Payment First Trust Deed Terms Second Trust Deed Balance ...

  5. bbnp_bb_an_0003576_pmc_dashboard_y13-q3.xls

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

    ... Number Of Tenants Tenancy Assessed Value Down Payment First Trust Deed Balance First Trust Deed Lender First Trust Deed Payment First Trust Deed Terms Second Trust Deed Balance ...

  6. connecticut_bb_an_0003806_pmc_dashboard_y13-q3.xls

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

    ... Number Of Tenants Tenancy Assessed Value Down Payment First Trust Deed Balance First Trust Deed Lender First Trust Deed Payment First Trust Deed Terms Second Trust Deed Balance ...

  7. bbnp_bb_an_0003566_pmc_dashboard_y13-q3.xls

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

    ... Number Of Tenants Tenancy Assessed Value Down Payment First Trust Deed Balance First Trust Deed Lender First Trust Deed Payment First Trust Deed Terms Second Trust Deed Balance ...

  8. bbnp_bb_an_0003572_pmc_dashboard_y13-q3.xls

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

    ... Number Of Tenants Tenancy Assessed Value Down Payment First Trust Deed Balance First Trust Deed Lender First Trust Deed Payment First Trust Deed Terms Second Trust Deed Balance ...

  9. bbnp_bb_an_0003809_pmc_dashboard_y13-q3.xls

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

    ... Number Of Tenants Tenancy Assessed Value Down Payment First Trust Deed Balance First Trust Deed Lender First Trust Deed Payment First Trust Deed Terms Second Trust Deed Balance ...

  10. bbnp_bb_an_0003569_pmc_dashboard_y13-q3.xls

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

    ... Number Of Tenants Tenancy Assessed Value Down Payment First Trust Deed Balance First Trust Deed Lender First Trust Deed Payment First Trust Deed Terms Second Trust Deed Balance ...

  11. bbnp_bb_an_0003580_pmc_dashboard_y13-q3.xls

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

    ... Number Of Tenants Tenancy Assessed Value Down Payment First Trust Deed Balance First Trust Deed Lender First Trust Deed Payment First Trust Deed Terms Second Trust Deed Balance ...

  12. TOTAL_ARRA_Homes_Weatherized_thru_Q3_2010_11_9_10.pdf | Department of

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

    Energy (73.65 KB) More Documents & Publications TOTAL_ARRA_Homes_Weatherized_thru_Q4_2010_3.7.11.pdf ARRA_Homes_Weatherized_by_State_for_February_4.14.11.pdf Homes_Weatherized_State_July_10.15.10.pdf

  13. High-Temperature Falling-Particle Receiver- FY13 Q3

    Broader source: Energy.gov [DOE]

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

  14. A Small Particle Solar Receiver for High Temperature Brayton Power Cycles- FY13 Q3

    Broader source: Energy.gov [DOE]

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

  15. High Operating Temperature Liquid Metal Heat Transfer Fluids- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  16. Lowest Q2 Measurement of the gamma*p-> Delta Reaction: Probing...

    Office of Scientific and Technical Information (OSTI)

    While there is qualitative agreement with the models, there is no quantitative agreement thus indicating the need for further improvement of the models. Temp HTML Storage 2: Stave, ...

  17. The proton and deuteron F2 structure function at low Q2 (Journal...

    Office of Scientific and Technical Information (OSTI)

    ; Lorenzon, Wolfgang ; Mammei, Juliette ; Martin, J W ; Mkrtchyan, Hamlet ; Niculescu, Maria-Ioana more ; Piercey, Rodney ; Potterveld, David ; Smith, Gregory ; Spurlock, Kurt ; ...

  18. Dish Stirling High Performance Thermal Storage FY15Q2 Quad Chart...

    Office of Scientific and Technical Information (OSTI)

    Authors: Andraka, Charles E. 1 + Show Author Affiliations Sandia National Lab. (SNL-NM), ... Resource Type: Technical Report Research Org: Sandia National Laboratories (SNL-NM), ...

  19. Dish Stirling High Performance Thermal Storage FY15Q2 Quad Chart

    Office of Scientific and Technical Information (OSTI)

    storage module * Module design complete * Major elements ordered and in fabrication Heat pipe advanced wick development * Complete 5000 hours of wick operation at...

  20. Self-Cleaning CSP Optics with EDS- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  1. Baseload CSP Generation Integrated with Sulfur-Based Thermochemical Heat Storage- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  2. High-Temperature Solar Selective Coating Development for Power Tower Receivers- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  3. Low-Cost Self-Cleaning Reflector Coatings for CSP Collectors- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  4. Dish/Stirling High-Performance Thermal Storage- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  5. Next-Generation Solar Collectors for CSP- FY13 Q2

    Office of Energy Efficiency and Renewable Energy (EERE)

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

  6. Low-Cost Metal Hydride Thermal Energy Storage System- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  7. High-Efficiency Thermal Energy Storage System for CSP- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  8. Advanced Low-Cost Receivers for Parabolic Troughs- FY13 Q2

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Norwich Technologies project, funded by SunShot, for the second quarter of fiscal year 2013.

  9. New parton distributions from large-x and low-Q2 data

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

    Alberto Accardi; Christy, M. Eric; Keppel, Cynthia E.; Melnitchouk, Wally; Monaghan, Peter A.; Morfin, Jorge G.; Owens, Joseph F.

    2010-02-11

    We report results of a new global next-to-leading order fit of parton distribution functions in which cuts on W and Q are relaxed, thereby including more data at high values of x. Effects of target mass corrections (TMCs), higher twist contributions, and nuclear corrections for deuterium data are significant in the large-x region. The leading twist parton distributions are found to be stable to TMC model variations as long as higher twist contributions are also included. Furthermore, the behavior of the d quark as x → 1 is particularly sensitive to the deuterium corrections, and using realistic nuclear smearing modelsmore » the d-quark distribution at large x is found to be softer than in previous fits performed with more restrictive cuts.« less

  10. Enclosure - FY 2016 Q2 Metrics Report 2016-05-03.xlsx

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

    FY 2016 Target 95% 95% 90% 85% 90% 90% FY 2016 2nd Qtr Actual Comment FY 2016 Forecast ... Schedule Compliance, Projects Less Than 5 Years Duration: Projects will meet the project ...

  11. Next-Generation Thermionic Solar Energy Conversion- FY13 Q2

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Stanford/SLAC project, funded by SunShot, for the second quarter of fiscal year 2013.

  12. Microsoft Word - EE0003005-2016Q2-Final Technical Report FTR

    Office of Scientific and Technical Information (OSTI)

    005 RiverHeath: Neighborhood Loop Geothermal Exchange System RiverHeath LLC Final Technical Report (FTR) for DOE/EERE Project Title: RiverHeath: Neighborhood Loop Geothermal Exchange System Covering Period: January 29, 2010 - June 30, 2015 Approved Project Period: 1/29/2010 - 6/30/2015 Submission Date: Recipient: Website (if available) Award Number: 07/11/2016 RiverHeath LLC 201 S RiverHeath Way, Suite 1800 Appleton Wl 54915 www.riverheath.com DE-EE0003005 PI: Submitted by: (if other than PI)

  13. High-Temperature Falling-Particle Receiver- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  14. High-Temperature Thermal Array for Next Generation Solar Thermal Power Production- FY12 Q2

    Broader source: Energy.gov [DOE]

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

  15. Direct s-CO2 Receiver Development- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  16. PowerPoint Presentation

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

    Management Advisory Board Meeting May 11, 2016 1 We do the right thing. Nuclear Workforce Initiative Larry Ling Chief of Staff Acting Director of Administrative Services Savannah River Remediation Environmental Management Advisory Board Meeting May 11, 2016 2 We do the right thing. SRR Contract Headcount 0 500 1000 1500 2000 2500 3000 Q4-09 Q2-10 Q4-10 Q2-11 Q4-11 Q2-12 Q4-12 Q2-13 Q4-13 Q2-14 Q4-14 Q1-15 Q2-15 Q3-15 Q4-15 Q1-16 SRR Headcount (December 31, 2009 through March 2016) All data at

  17. Directives Quarterly Updates - DOE Directives, Delegations, and

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

    Requirements Quarterly Updates by Diane Johnson Listings of new Justification Memoranda and new or revised Directives that have been posted to the DOE Directives, Delegations, and Requirements Portal. Updated quarterly. FY2016 FY 16, Q2 - January through March 2016 FY2015 FY15, Q1 - October through December 2014 FY15, Q3 - April through June 2015 FY15, Q4 - July through September 2015 FY 2014 FY14, Q1 - October through December 2013 FY14, Q2 - January through March 2014 FY14, Q3 - April

  18. Matt Schatzman € Houston € 22 October 2007

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

    ... Belgium Japan France Italy Mexico Norway* South Korea Spain Taiwan Turkey UAE US UK India ... Jan Mar May Jul Sep Nov Other Mexico (east) UK EU Main China India Taiwan S Korea Japan ...

  19. Measurement of the Neutron electric form factor at Q2=0.8 2(GeV\\\\c)

    SciTech Connect (OSTI)

    Derek Glazier

    2007-09-30

    Nucleon form factors allow a sensitive test for models of the nucleon. Recent experiments utilising polarisation observables have resulted, for the first time, in a model-independent determination of the neutron electric form factor GnE. This method employed an 80% longitudinally polarised, high intensity (10 uA) electon beam (883 MeV) that was quasi-elastically scattered off a liquid deuterium target in the reaction D (e, en)p. A neutron polarimeter was designed and installed to measure the ratio of transverse-to-longitudinal polarisation using neutron scattering asymmetries. This ratio allowed a determination of the neutron elastic form factor, GnE, free of the previous large systematic uncertainties associated with the deuterium wave function. The experiment took place in the A1 experimental hall at MAMI taking advantage of a high resolution magnetic spectrometer. A detailed investigation was carried out into the performance of the neutron polarimeter.

  20. Charged pion form factor between $Q^2$=0.60 and 2.45 GeV$^2$...

    Office of Scientific and Technical Information (OSTI)

    ... Paul ; Reinhold, Joerg ; Roche, Julie ; Roos, Philip ; Sarty, Adam ; Shin, Ilkyoung ; Smith, Gregory ; Stepanyan, Stepan ; Tang, Liguang ; Tvaskis, Vladas ; van der Meer, Rob ; ...

  1. Charged pion form factor between $Q^2$=0.60 and 2.45 GeV$^2$...

    Office of Scientific and Technical Information (OSTI)

    Paul ; Reinhold, Joerg ; Roche, Julie ; Roos, Philip ; Sarty, Adam ; Shin, Ilkyoung ; Smith, Gregory ; Stepanyan, Stepan ; Tang, Liguang ; Tvaskis, Vladas ; van der Meer, Rob ; ...

  2. Fundamental Corrosion Studies in High-Temperature Molten Salt Systems for Next-Generation CSP Systems- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  3. Quarterly Report for LANL Activities: FY12-Q2 National Risk Assessment Partnership (NRAP): Industrial Carbon Capture Program

    SciTech Connect (OSTI)

    Pawar, Rajesh J.

    2012-04-17

    This report summarizes progress of LANL activities related to the tasks performed under the LANL FWP FE102-002-FY10, National Risk Assessment Partnership (NRAP): Industrial Carbon Capture Program. This FWP is funded through the American Recovery and Reinvestment Act (ARRA). Overall, the NRAP activities are focused on understanding and evaluating risks associated with large-scale injection and long-term storage of CO{sub 2} in deep geological formations. One of the primary risks during large-scale injection is due to changes in geomechanical stresses to the storage reservoir, to the caprock/seals and to the wellbores. These changes may have the potential to cause CO{sub 2} and brine leakage and geochemical impacts to the groundwater systems. While the importance of these stresses is well recognized, there have been relatively few quantitative studies (laboratory, field or theoretical) of geomechanical processes in sequestration systems. In addition, there are no integrated studies that allow evaluation of risks to groundwater quality in the context of CO{sub 2} injection-induced stresses. The work performed under this project is focused on better understanding these effects. LANL approach will develop laboratory and computational tools to understand the impact of CO{sub 2}-induced mechanical stress by creating a geomechanical test bed using inputs from laboratory experiments, field data, and conceptual approaches. The Geomechanical Test Bed will be used for conducting sensitivity and scenario analyses of the impacts of CO{sub 2} injection. The specific types of questions will relate to fault stimulation and fracture inducing stress on caprock, changes in wellbore leakage due to evolution of stress in the reservoir and caprock, and the potential for induced seismicity. In addition, the Geomechanical Test Bed will be used to investigate the coupling of stress-induced leakage pathways with impacts on groundwater quality. LANL activities are performed under two tasks: (1) develop laboratory and computational tools to understand CO{sub 2}-induced mechanical impacts and (2) use natural analog sites to determine potential groundwater impacts. We are using the Springerville-St. John Dome as a field site for collecting field data on CO{sub 2} migration through faults and groundwater impacts as well as developing and validating computational models. During the FY12 second quarter we have been working with New England Research Company to construct a tri-axial core-holder. We have built fluid control system for the coreflood system that can be ported to perform in-situ imaging of core. We have performed numerical simulations for groundwater impacts of CO{sub 2} and brine leakage using the reservoir model for Springerville-St John's Dome site. We have analyzed groundwater samples collected from Springerville site for major ion chemistry and isotopic composition. We are currently analyzing subsurface core and chip samples acquired for mineralogical composition.

  4. A Small-Particle Solar Receiver for High-Temperature Brayton Power Cycles- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  5. Low-Cost, Highly Transparent Flexible low-e Coating Film to Enable Electrochromic Windows with Increased Energy Savings

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

    Berland, bberland@itnes.com ITN Energy Systems Low-Cost, Highly Transparent Flexible low-e Coating Film to Enable Electrochromic Windows with Increased Energy Savings 2014 Building Technologies Office Peer Review 2 Project Summary Timeline: Start date: October 1, 2013 Planned end date: September 30, 2014 Key Milestones 1.Low-e Film: 90% T,vis & R,ir (100 cm 2 ) (Q2) 2.Low-e Film: 90% T,vis & R,ir (2m long, %T,%R variation < 2% cross web) (Q3) 3.Demonstrate Low-e/EC Film (Q3) Budget:

  6. completed_td_projects | netl.doe.gov

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

    Forecast: August 9, 2016; Previous Forecast: July 12, 2016 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 2014 2015 2016 2017 2014-2015 2015-2016 2016-2017 U.S. Energy Supply U.S. Crude Oil Production (million barrels per day) Current 9.48 9.50 9.43 9.32 9.17 8.87 8.45 8.44 8.42 8.36 8.16 8.29 8.71 9.43 8.73 8.31 8.3% -7.4% -4.9% Previous 9.48 9.50 9.43 9.32 9.17 8.79 8.26 8.23 8.24 8.21 8.09 8.27 8.71 9.43 8.61 8.20 8.3% -8.7% -4.8% Percent Change 0.0% 0.0% 0.0% 0.0% 0.1% 0.9% 2.3% 2.5% 2.2% 1.8% 0.9%

  7. Quarterly Research Performance Progress Report (2015 Q3). Ultrasonic Phased Arrays and Interactive Reflectivity Tomography for Nondestructive Inspection of Injection and Production Wells in Geothermal Energy Systems

    SciTech Connect (OSTI)

    Santos-Villalobos, Hector J; Polsky, Yarom; Kisner, Roger A; Johnson, Christi R; Collins, Case; Bouman, Charles; Abdulrahman, Hani; Foster, Benjamin

    2015-09-01

    For the past quarter, we have placed our effort in implementing the first version of the ModelBased Iterative Reconstruction (MBIR) algorithm, assembling and testing the electronics, designing transducers mounts, and defining our laboratory test samples. We have successfully developed the first implementation of MBIR for ultrasound imaging. The current algorithm was tested with synthetic data and we are currently making new modifications for the reconstruction of real ultrasound data. Beside assembling and testing the electronics, we developed a LabView graphic user interface (GUI) to fully control the ultrasonic phased array, adjust the time-delays of the transducers, and store the measured reflections. As part of preparing for a laboratory-scale demonstration, the design and fabrication of the laboratory samples has begun. Three cement blocks with embedded objects will be fabricated, characterized, and used to demonstrate the capabilities of the system. During the next quarter, we will continue to improve the current MBIR forward model and integrate the reconstruction code with the LabView GUI. In addition, we will define focal laws for the ultrasonic phased array and perform the laboratory demonstration. We expect to perform laboratory demonstration by the end of October 2015.

  8. Halide and Oxy-Halide Eutectic Systems for High-Performance, High-Temperature Heat Transfer Fluids- FY13 Q2

    Broader source: Energy.gov [DOE]

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

  9. Nuclear Transparency and Single Particle Spectral Functions from Quasielastic A(e,e'p) Reactions up to Q2=8.1 GeV2

    SciTech Connect (OSTI)

    David McKee

    2003-05-01

    High statistics elastic and quasielastic scattering measurements were performed on hydrogen, deuterium, carbon, and iron at squared momentum transfers up to 8.1 GeV2. Both the nuclear transparency and the single particle spectral functions were extracted by means of comparison with a Plane- Wave Impulse Approximation calculation. Our data provide no evidence of the onset of color transparency within our kinematic range.

  10. A Measurement of the Neutron Electric Form Factor in Dvec (evec,e'n)p Quasielastic Scattering at Q2=0.5(GeV/c)2

    SciTech Connect (OSTI)

    Hongguo Zhu

    2000-08-01

    The form factors of the neutron give information on fundamental properties of the nucleons and provide a critical testing ground for models based on QCD. In late 1998, Jefferson Lab (JLAB) experiment E93-026 measured the spin-dependent part of the exclusive (e, e'n) scattering cross section from a polarized deuterated ammonia ({sup 15}ND{sub 3}) target at a four momentum transfer squared of Q{sup 2} = 0.5 (GeV/c){sub 2}. A longitudinally polarized electron beam was scattered from the polarized target and the quasi-elastically scattered electron was detected in coincidence with the knocked-out neutron. The data have been analyzed in terms of the spin-correlation parameter, or the electron-deuteron vector asymmetry (A{sub ed}{sup V}), of (e, e'n) to determine the neutron electric form factor G{sub E}{sup n}. The result is consistent with data from existing experiments and shows a good agreement with the Galster parameterization of G{sub E}{sup n} within experimental uncertainty.

  11. Recoil Polarization Measurements for Neutral Pion Electroproduction at Q^2=1 (GeV/c)^2 Near the Delta Resonance

    SciTech Connect (OSTI)

    James Kelly; et. Al.

    2005-09-01

    We measured angular distributions of differential cross section, beam analyzing power, and recoil polarization for neutral pion electroproduction at Q{sup 2} = 1.0 (GeV/c){sup 2} in 10 bins of W across the Delta resonance. A total of 16 independent response functions were extracted, of which 12 were observed for the first time. Comparisons with recent model calculations show that response functions governed by real parts of interference products are determined relatively well near 1.232 GeV, but variations among models is large for response functions governed by imaginary parts and for both increases rapidly with W. We performed a nearly model-independent multipole analysis that adjusts complex multipoles with high partial waves constrained by baseline models. Parabolic fits to the W dependence of the multipole analysis around the Delta mass gives values for SMR = (-6.61 +/- 0.18)% and EMR = (-2.87 +/- 0.19)% that are distinctly larger than those from Legendre analysis of the same data. Similarly, the multipole analysis gives Re(S0+/M1+) = (+7.1 +/- 0.8)% at W=1.232 GeV, consistent with recent models, while the traditional Legendre analysis gives the opposite sign because its truncation errors are quite severe. Finally, using a unitary isobar model (UIM), we find that excitation of the Roper resonance is dominantly longitudinal with S1/2 = (0.05 +/- 0.01) GeV{sup (-1/2)} at Q{sup 2}=1. The ReS0+ and ReE0+ multipoles favor pseudovector coupling over pseudoscalar coupling or a recently proposed mixed-coupling scheme, but the UIM does not reproduce the imaginary parts of 0+ multipoles well.

  12. PowerPoint Presentation

    Energy Savers [EERE]

    Paul Schwartz, pschwartz@tm-lift.com DE-FOA-0000823 Grantee The Natural Gas Heat Pump and Air Conditioner 2014 Building Technologies Office Peer Review FREE Heat from Ambient (10 kW) Heat from Burner (15 kW) Combined Heat Delivered (25 kW) New Project 2 Project Summary Timeline: Start date: 10/1/2013 (8/1/2013) Planned end date: 9/30/2014 Key Milestones 1. Concept & CAD model; Q1 FY2014 2. Thermal Simulation; Q2 FY2014 3. 20kW Demonstrator; Q3-Q4 FY2014 4. Testing at Oak Ridge; Q4 FY2014?

  13. Hanford Advisory Board Fiscal Year 2016 Work Plan

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

    Updated 05.18.16 *Indicates lead committee 1 Hanford Advisory Board Fiscal Year Draft 2017 Work Plan (FY 2017 Action Overview) Topic Committee Assignment Potential FY 2017 Action/Product Action Q1 Q2 Q3 Q4 1. 100-N Proposed Plan RAP Advice [X] 2. Critical Infrastructure Updates *RAP/HSEP/TWC Advice [X] 3. PFP Progress *RAP/HSEP Agency briefing X 4. Sludge retrieval RAP Agency briefing X 5. WESF preparations to move capsules to dry storage RAP Agency briefing, advice [X] 6. Risk-based retrieval,

  14. Hanford Advisory Board Fiscal Year 2016 Work Plan

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

    July 24, 2015) 1 Hanford Advisory Board Fiscal Year 2016 Work Plan (FY 2016 Action Overview) Topic Committee Assignment Potential FY 2016 Action/Product Action Q1 Q2 Q3 Q4 1. 100 Area retrieval process, K Basin RAP Informational x x 2. 100 D/H Proposed Plan RAP Informational x x 3. 100-N Proposed Plan RAP Policy discussion, Potential Advice x 4. 324 Waste Sites RAP Informational 5. 618-10 VPU remediation RAP Informational 6. Central Plateau Inner Area Guidelines RAP Informational x 7. ERDF RAP

  15. Hanford Advisory Board Fiscal Year 2016 Work Plan

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

    Adopted by the Hanford Advisory Board on 11/5/2015, updated 12/21/15 1 Hanford Advisory Board Fiscal Year 2016 Work Plan (FY 2016 Action Overview and RAP Issue Manager Assignments) Topic Committee Assignment Issue Managers (lead noted in bold) Action Q1 Q2 Q3 Q4 1. 100 Area retrieval process, K Basin RAP Mattson, Suyama x 2. 100 D/H Proposed Plan RAP Engstrom, Mattson, Garnant, Leckband x 3. 100-N Proposed Plan RAP Cimon, Mattson x 4. Central Plateau Inner Area Guidelines RAP Cimon, Catrell,

  16. Hanford Advisory Board Fiscal Year 2016 Work Plan

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

    June 19, 2015June 18, 2015) 1 Hanford Advisory Board Fiscal Year 2016 Work Plan (FY 2016 Action Overview) Topic Committee Assignment Potential FY 2016 Action/Product Action Q1 Q2 Q3 Q4 1. 100 Area retrieval process, K Basin RAP Project update x 2. 100 D/H Proposed Plan RAP Project update x 3. 100-N Proposed Plan RAP Policy discussion, Potential Advice x 4. Central Plateau Inner Area Guidelines RAP Project update x 5. ERDF RAP Project update x 6. Groundwater updates RAP Project update 7.

  17. Hanford Advisory Board Fiscal Year 2016 Work Plan

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

    Updated December 21, 2015 1 Hanford Advisory Board Fiscal Year 2016 Work Plan (FY 2016 Action Overview) Topic Committee Assignment Potential FY 2016 Action/Product Action Q1 Q2 Q3 Q4 1. 100 Area retrieval process, K Basin RAP Project update x 2. 100 D/H Proposed Plan RAP Project update x 3. 100-N Proposed Plan RAP Policy discussion, Potential Advice x 4. Central Plateau Inner Area Guidelines RAP Project update x 5. ERDF RAP Project update x 6. Groundwater updates RAP Project update 7.

  18. Hanford Advisory Board Fiscal Year 2016 Work Plan

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

    Fiscal Year 2016 Work Plan Working draft - reflects comments received from PIC, HSEP, TWC and RAP committees (updated October 22, 2015) 1 Hanford Advisory Board Draft Fiscal Year 2016 Work Plan (FY 2016 Action Overview) Topic Committee Assignment Potential FY 2016 Action/Product Action Q1 Q2 Q3 Q4 1. 100 Area retrieval process, K Basin RAP Project update x 2. 100 D/H Proposed Plan RAP Project update x 3. 100-N Proposed Plan RAP Policy discussion, Potential Advice x 4. Central Plateau Inner Area

  19. Hanford Advisory Board Fiscal Year 2016 Work Plan

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

    Updated 8/31/2016 * Indicates lead committee 1 Hanford Advisory Board Fiscal Year Draft 2017 Work Plan (FY 2017 Action Overview) Topic Committee Assignment Potential FY 2017 Action/Product Action Q1 Q2 Q3 Q4 1. 100-N Proposed Plan RAP Agency briefing, advice [x] 2. Sludge retrieval RAP Agency briefing x x 3. WESF preparations to move capsules to dry storage RAP Agency briefing, advice [x] 4. River Corridor updates RAP Agency briefing 5. Groundwater updates RAP Agency briefing x x x x 6. Central

  20. request.pdf

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

    Advisory Board Draft Fiscal Year 2016 Work Plan Adopted March 18, 2016; updated per EIC discussion 01.13.16 1 Hanford Advisory Board Fiscal Year 2016 Work Plan (FY 2016 Action Overview) Topic Committee Assignment Potential FY 2016 Action/Product Action Q1 Q2 Q3 Q4 1. 100 Area retrieval process, K Basin RAP Project update x 2. 100 D/H Proposed Plan RAP Project update x x 3. 100-N Proposed Plan RAP Policy discussion, Potential Advice x 4. Central Plateau Inner Area Guidelines RAP Project update x

  1. PowerPoint Presentation

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

    Schwartz, pschwartz@tm-lift.com DE-FOA-0000823 Grantee The Natural Gas Heat Pump and Air Conditioner 2014 Building Technologies Office Peer Review FREE Heat from Ambient (10 kW) Heat from Burner (15 kW) Combined Heat Delivered (25 kW) New Project 2 Project Summary Timeline: Start date: 10/1/2013 (8/1/2013) Planned end date: 9/30/2014 Key Milestones 1. Concept & CAD model; Q1 FY2014 2. Thermal Simulation; Q2 FY2014 3. 20kW Demonstrator; Q3-Q4 FY2014 4. Testing at Oak Ridge; Q4 FY2014? Budget:

  2. Microsoft Word - 2015_0211_Joint FY2015HABWorkPlan_TWC Issue Managers.docx

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

    Updated February 11, 2015; incorporates comments from February 2015 EIC discussion Hanford Advisory Board Fiscal Year 2015 Work Plan (FY 2015 Action Overview) - ISSUE MANAGER ASSIGNMENTS Topic Committee Assignment Issue managers (lead in bold) Potential FY 2015 Action/Product Action Q1 Q2 Q3 Q4 1 Deferred Maintenance Plan RAP/HSEP Discussion; sounding board x 2 100 D/H Proposed Plan for ROD RAP Public involvement x 3 Central Plateau Inner Area Principles RAP Policy discussion; advice x x x x 4

  3. Microsoft Word - 2015_0914_FY2016HABWorkPlan_v1.docx

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

    Hanford Advisory Board Fiscal Year 2016 Work Plan Updated October 22, 2015 1 Hanford Advisory Board Fiscal Year 2016 Work Plan (FY 2016 Action Overview) Topic Committee Assignment Potential FY 2016 Action/Product Action Q1 Q2 Q3 Q4 1. 100 Area retrieval process, K Basin RAP Project update x 2. 100 D/H Proposed Plan RAP Project update x 3. 100-N Proposed Plan RAP Policy discussion, Potential Advice x 4. Central Plateau Inner Area Guidelines RAP Project update x 5. ERDF RAP Project update x 6.

  4. Systematics of ground-state quadrupole moments of odd-A deformed nuclei determined with muonic M x rays

    SciTech Connect (OSTI)

    Tanaka, Y.; Steffen, R.M.; Shera, E.B.; Reuter, W.; Hoehn, M.V.; Zumbro, J.D.

    1984-05-01

    The ground-state quadrupole moments of /sup 151/Eu, /sup 153/Eu, /sup 159/Tb, /sup 163/Dy, /sup 167/Er, /sup 177/Hf, /sup 179/Hf, /sup 191/Ir, and /sup 193/Ir were determined by measuring the quadrupole hyperfine-splitting energies of muonic M x rays. The results are Q = 0.903(10) e b for /sup 151/Eu, Q = 2.412(21) e b for /sup 153/Eu, Q = 1.432(8) e b for /sup 159/Tb, Q = 2.648(21) e b for /sup 163/Dy, Q = 3.565(29) e b for /sup 167/Er, Q = 3.365(29) e b for /sup 177/Hf, Q = 3.793(33) e b for /sup 179/Hf, Q = 0.816(9) e b for /sup 191/Ir, and Q = 0.751(9) e b for /sup 193/Ir. The present quadrupole moments, compared with values obtained from electronic-atom hyperfine measurements, show that the Sternheimer correction factors used in the rare-earth electronic-atom analysis are unreliable. Systematics of deformation parameters ..beta../sub 2/ calculated from the present quadrupole moments for odd-A nuclei, and from B(E2) values of Coulomb excitation measurements for even-A nuclei, also indicate that the largest deformation change so far known exists between /sup 151/Eu and /sup 153/Eu. Except at the onset of nuclear deformation, the deformation parameters of the odd-A nuclei are quite consistent with those of the even-A neighbors.

  5. U.S. Department of Energy Weatherization Assistance Program

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

    Weatherization Assistance Program Homes Weatherized By State through 03/31/2010 (Calendar Year) *State Total Number of Homes Weatherized 2009 Calendar Year Number of Homes Weatherized in 1st Quarter 2010 Total Number Homes Weatherized through March 2010 Total Number of Homes Weatherized through March 2010 (Calendar Year 2009 - March 2010) ***January 2010 February 2010 March 2010 **Breakdown of Homes Weatherized in 1st Quarter 2010 (Jan-Mar) [Recovery Act] 2009 Calendar Year [Recovery Act] 1st

  6. Measurements of the Proton Electromagnetic Form Factor Ratio From Elastic e + p -> e + p Scattering at Momentum Transfer Q^2 = 2.5, 5.2, 6.7 and 8.5 (GeV/c)^2

    SciTech Connect (OSTI)

    Arthur Mkrtchyan

    2012-05-31

    Among the fundamental observables of nucleon structure, electromagnetic form factors are a crucial benchmark for modern calculations describing the strong interaction dyna mics of the nucleon's quark constituents. Electromagnetic probes are traditionally preferered to the hadronic beams. The electromagnetic interaction is a powerful tool for investigating the nucleon structure since it is well understood and it reveals observables that can be directly interpreted in terms of the current carried by the quarks. Elastic scattering leads to the form factors that describe the spatial charge a nd current distributions inside the nucleon. The reaction mechanism is assumed to be one photon exchange, the electromagnetic interaction is exactly calculable in QED, and one can safely extract the information on the hadronic vertex. The most important feature of early measurements of proton form factor ratio G{sub E}{sup p}/G{sub M}{sup p} with recoil polarization technique at Q{sup 2} up to 5.6 (GeV/c){sup 2} is the sharp decline of the ratio with Q{sup 2} increases, indicating that G{sub E}{sup p} falls much faster than G{sub M}{sup p}. This contradicts to data obtained by Rosenbluth separation method. An intriguing question was whether G{sub E}{sup p} will continue to decrease or become constant when Q{sup 2} increases. New set of measurements of proton form factor ratio G{sub E}{sup p}/G{sub M}{sup p} at Q{sup 2} = 2.5, 5.2, 6.7 and 8.5 (GeV/c){sup 2} have been conducted at JLab Hall C using {approx}85% longitudinally polarized electron elastic scattering from unpolarized hydrogen target. Recoil protons were detected in the HMS magnetic spectrometer with the standard detector package, combined with newly installed trigger scintillators and Focal Plane Polarimeter. The BigCal electromagnetic calorimeter (1744 channel) have been used for electron detection. Data obtained in this experiment show that G{sub E}{sup p}/G{sub M}{sup p} ratio continued to drop with Q{sup 2} and may cross 'zero' at Q{sup 2} > 10-15 (GeV/c){sup 2}. Intensive theoretical and experimental efforts over the past decade have aimed at explaining the discrepancy between data for the proton form factor ratio G{sub E}{sup p}/G{sub M}{sup p} obtained from cross section and polarization measurements. It was assumed that the two photon exchange contribution might be responsible for difference of G{sub E}{sup p}/G{sub M}{sup p} ratio obtained by Rosenbluth separation method and recoil polarization technique. The kinematical dependence of polarization transfer observables in elastic electron-proton scattering at Q{sup 2} = 2.5 (GeV/c){sup 2} have been used in search of effects of 2{gamma} contribution. For a wide range of values of the virtual photon polarization {epsilon} ({epsilon} = 0.15, 0.63, and 0.77), the proton form factor ratio and longitudinal polarization transfer component were measured with statistical uncertainties of {+-}0.01 and {+-}0.005, respectively. Our data provide significant constraints on models of nucleon structure.

  7. 1Q/2Q00 M-Area and Metallurgical Laboratory Hazardous Waste Management Facilities Groundwater Monitoring and Corrective-Action Report - First and Second Quarters 2000 - Volumes I, II, and II

    SciTech Connect (OSTI)

    Chase, J.

    2000-10-24

    This report describes the groundwater monitoring and corrective-action program at the M-Area Hazardous Waste Management Facility (HWMF) and the Metallurgical Laboratory (Met Lab) HWMF at the Savannah River site (SRS) during first and second quarters of 2000.

  8. 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

  9. 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

  10. b35.pdf

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

    .. 67,338 58,474 8,329 9,147 14,276 2,750 12,909 36,527 2,219 1,312 Building Floorspace (Square Feet) 1,001 to 5,000 .............................................. 6,774 4,879 890 700 962 Q Q 2,613 253 Q 5,001 to 10,000 ............................................ 8,238 6,212 1,606 707 1,396 Q Q 3,197 181 Q 10,001 to 25,000 .......................................... 11,153 9,530 1,420 1,270 2,482 Q 307 6,031 207 Q 25,001 to 50,000 .......................................... 9,311 8,116 860 1,304

  11. A numerical test of KPZ scaling; Potts models coupled to two-dimensional quantum gravity

    SciTech Connect (OSTI)

    Baillie, C.F. , 91 - Nozay ); Johnston, D.A. . Dept. of Mathematics)

    1992-06-07

    In this paper, the authors perform Monte-Carlo simulations using the Wolff cluster algorithm of the q = 2 (Ising), 3, 4 and q = 10 Potts models on dynamical phi-cubed graphs of spherical topology with up to 5000 nodes. The authors find that the measured critical exponents are in reasonable agreement with those from the exact solution of the Ising model and with those calculated from KPZ scaling for q = 3, 4 where no exact solution is available. Using Binder's cumulant, the authors find that the q = 10 Potts model displays a first order phase transition on a dynamical graph, as it does on a fixed lattice. The authors also examine the internal geometry of the graphs generated in the simulation, finding a linear relationship between ring length probabilities and the central charge of the Potts model.

  12. A=7B (1974AJ01)

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

    4AJ01) (See the Isobar Diagram for 7B) 1. 10B(3He, 6He)7B Qm = -18.55 A 6He group corresponding to the unbound ground state of 7B has been identified at E(3He) = 50 MeV: M - A (7B) = 27.94 ± 0.10, Γ = 1.4 ± 0.2 MeV. The isobaric quartet mass law would predict M - A = 27.76 ± 0.17 MeV. 7B is unbound with respect to 6Be + p (Q = 2.27), 5Li + 2p (Q = 1.68), 4He + 3p (Q = 3.65). The expected single-particle width is Γ = 0.64 MeV: it is suggested that the two-proton and three-proton decays make

  13. A=7B (1979AJ01)

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

    9AJ01) (See the Isobar Diagram for 7B) GENERAL: See also (1974DA1B, 1974IR04, 1975BE31, 1975BE56, 1976IR1B, 1977SP1B). 1. 10B(3He, 6He)7B Qm = -18.55 A 6He group corresponding to the unbound ground state of 7B has been identified at E(3He) = 50 MeV: M - A (7B) = 27.94 ± 0.10, Γ = 1.4 ± 0.2 MeV. The isobaric quartet mass law would predict M - A = 27.76 ± 0.17 MeV. 7B is unbound with respect to 6Be + p (Q = 2.27), 5Li + 2p (Q = 1.68), 4He + 3p (Q = 3.65). The expected single-particle width is

  14. A=8C (1974AJ01)

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

    4AJ01) (Not illustrated) 8C has been observed in the 12C(α, 8He)8C reaction at Eα = 156 MeV: M - A = 35.30 ± 0.20 MeV, Γc.m. = 220+80-140 keV [the differential cross section at 2° (lab) is ≈ 20 nb/sr] (R.G.H. Robertson, S. Martin, W.R. Falk, D. Ingham and A. Djaloeis, private communication). 8C is then unstable with respect to 7B + p (Q = 0.1), 6Be + 2p (Q = 2.3), 5Li + 3p (Q = 1.8), 4He + 4p (Q = 3.7). See also (1960GO1B, 1966KE16, 1970WA1G).

  15. A=8C (1979AJ01)

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

    9AJ01) (See the Isobar Diagram for 8C) Mass of 8C: The atomic mass excess of 8C is 35096 ± 26 keV, Γc.m. = 230 ± 50 keV: see (1977TR07). See also (1974AJ01, 1974RO17, 1976TR1B, 1978RO01). 8C is stable with respect to 7B + p (Q = -0.13 MeV) and unstable with respect to 6Be + 2p (Q = 2.143), 5Li + 3p (Q = 1.55), 4He + 4p (Q = 3.514). At E(3He) = 76 MeV the differential cross section for formation of 8Cg.s. in the 14N(3He, 9Li) reaction is ≈ 5 nb/sr at θlab = 10° (1976RO04). The 12C(α,

  16. A=8C (1984AJ01)

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

    4AJ01) (See the Isobar Diagram for 8C) Mass of 8C: The atomic mass excess of 8C is 35095 ± 23 keV (A.H. Wapstra, private communication). Γc.m. = 230 ± 50 keV: see (1979AJ01). 8C is stable with respect to 7B + p (Q = -0.13 MeV) and unstable with respect to 6Be + 2p (Q = 2.14), 5Li + 3p (Q = 1.55), 4He + 4p (Q = 3.51). At E(3He) = 76 MeV the differential cross section for formation of 8Cg.s. in the 14N(3He, 9Li) reaction is ~ 5 nb/sr at θlab = 10°. The 12C(α, 8He)8C reaction has been studied

  17. A=8C (2004TI06)

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

    2004TI06) (See the Isobar Diagram for 8C) Mass of 8C: The atomic mass excess of 8C is 35094 ± 23 keV (2003AU03); Γcm = 230 ± 50 keV [Jπ = 0+; T = 2]: see (1979AJ01). 8C is stable with respect to 7B + p (Q = -0.07 MeV) and unstable with respect to 6Be + 2p (Q = 2.14), 5Li + 3p (Q = 1.55) and 4He + 4p (Q = 3.51). At E(3He) = 76 MeV the differential cross section for formation of 8Cg.s. in the 14N(3He, 9Li) reaction is ~ 5 nb/sr at θlab = 10°. The 12C(α, 8He)8C reaction has been studied at

  18. All

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

    87,093 15,952 13,077 4,630 11,330 4,557 12,239 5,559 Building floorspace (square feet) 1,001 to 5,000 8,041 1,520 1,127 1,031 730 572 391 498 5,001 to 10,000 8,900 1,663 1,329 1,051 1,052 790 353 536 10,001 to 25,000 14,105 2,012 2,331 1,253 1,821 1,443 1,212 1,108 25,001 to 50,000 11,917 2,333 1,814 607 1,648 926 1,492 861 50,001 to 100,000 13,918 2,203 1,632 Q 1,909 585 3,363 627 100,001 to 200,000 12,415 2,054 1,946 Q 2,178 Q 3,020 553 200,001 to 500,000 10,724 1,946 1,827 Q 1,264 Q 2,358 748

  19. HSEP Committee FY 2016 Work Plan

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

    FY 2016 Work Plan Updated 12/10/2015 during the committee meeting Beryllium program update  Placeholder Annual Employee Concerns Program  Placeholder  Hear from new program director at WRPS  Quarter 1 (Oct-Dec) Quarter 2 (Jan-Mar) Quarter 3 (Apr-Jun) Quarter 4 (July-Sept) Holding Bin Transportation Effects on Worker Safety - draft advice  Review of draft advice Safety culture improvement efforts (joint with TWC)  Discuss Sounding Board for upcoming Board meeting o Review

  20. Measurements of the neutron electric to magnetic form-factor ratio G(En) / G(Mn) via the H-2(polarized-e, e-prime,polarized-n)H-1 reaction to Q**2 = 1.45-(GeV/c)**2

    SciTech Connect (OSTI)

    Bradley Plaster; A.Yu. Semenov; A. Aghalaryan; Erick Crouse; Glen MacLachlan; Shigeyuki Tajima; William Tireman; Abdellah Ahmidouch; Brian Anderson; Hartmuth Arenhovel; Razmik Asaturyan; O. Baker; Alan Baldwin; David Barkhuff; Herbert Breuer; Roger Carlini; Michael Christy; Steve Churchwell; Leon Cole; Samuel Danagoulian; Donal Day; T. Eden; Mostafa Elaasar; Rolf Ent; Manouchehr Farkhondeh; Howard Fenker; John Finn; Liping Gan; Ashot Gasparian; Kenneth Garrow; Paul Gueye; Calvin Howell; Bitao Hu; Mark Jones; James Kelly; Cynthia Keppel; Mahbubul Khandaker; Wooyoung Kim; Stanley Kowalski; Allison Lung; David Mack; Richard Madey; D. Manley; Pete Markowitz; Joseph Mitchell; Hamlet Mkrtchyan; Allena Opper; Charles Perdrisat; Vina Punjabi; Brian Raue; Tilmann Reichelt; Joerg Reinhold; Julie Roche; Yoshinori Sato; Nikolai Savvinov; Irina Semenova; Wonick Seo; Neven Simicevic; Gregory Smith; Stepan Stepanyan; Vardan Tadevosyan; Liguang Tang; Shawn Taylor; Paul Ulmer; William Vulcan; John Watson; Steven Wells; Frank Wesselmann; Stephen Wood; Seunghoon Yang; Lulin Yuan; Wei-Ming Zhang; Hong Guo Zhu; Xiaofeng Zhu

    2006-02-01

    We report values for the neutron electric to magnetic form factor ratio, G{sub En}/G{sub Mn}, deduced from measurements of the neutron's recoil polarization in the quasielastic {sup 2}H({rvec e}, e{prime}{rvec n}) {sup 1}H reaction, at three Q{sup 2} values of 0.45, 1.13, and 1.45 (GeV/c){sup 2}. The data at Q{sup 2} = 1.13 and 1.45 (GeV/c){sup 2} are the first direct experimental measurements of GEn employing polarization degrees of freedom in the Q{sup 2} > 1 (GeV/c){sup 2} region and stand as the most precise determinations of GEn for all values of Q{sup 2}.

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

    SciTech Connect (OSTI)

    Azuah, Richard T; Omar Diallo, Souleymane; Adams, Mark A.; Kirichek, Oleg; Glyde, Henry R

    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.

  2. Energy Information Administration - Commercial Energy Consumption...

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

    ... 8 Q 2 1 Q 2 Q Q Q 1 Principal Building Activity Education ... 386 Q 21 34 29 87 Q 56 39 97 Food Sales...

  3. 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 inmorethis 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

  4. 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.

  5. All

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

    87,093 67,550 30,637 26,115 8,873 1,925 19,543 1,573 5,539 12,431 Building floorspace (square feet) 1,001 to 5,000 8,041 7,077 3,871 2,526 382 298 964 Q 230 713 5,001 to 10,000 8,900 7,953 4,118 2,932 635 267 947 Q Q 765 10,001 to 25,000 14,105 11,987 6,045 4,149 1,305 488 2,117 Q 621 1,373 25,001 to 50,000 11,917 9,482 4,067 3,656 1,353 Q 2,435 Q 647 1,649 50,001 to 100,000 13,918 9,104 3,712 4,051 1,106 Q 4,814 Q 1,327 3,351 100,001 to 200,000 12,415 8,905 4,306 3,493 1,025 Q 3,510 Q 1,392

  6. Minimally nonlocal nucleon-nucleon potentials with chiral two-pion exchange including Δ 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 Δ-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 Χ2 /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

  7. CaCl 2 -Accelerated Hydration of Tricalcium Silicate: A STXM Study Combined with 29 Si MAS NMR

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

    Li, Qinfei; Ge, Yong; Geng, Guoqing; Bae, Sungchul; Monteiro, Paulo J. M.

    2015-01-01

    Tmore » he effect of calcium chloride (CaCl 2 ) on tricalcium silicate (C 3 S) hydration was investigated by scanning transmission X-ray microscopy (STXM) with Near Edge X-ray Absorption Fine Structure (NEXAFS) spectra and 29 Si MAS NMR. STXM is demonstrated to be a powerful tool for studying the chemical composition of a cement-based hydration system.he Ca L 3,2 -edge NEXAFS spectra obtained by examining C 3 S hydration in the presence of CaCl 2 showed that this accelerator does not change the coordination of calcium in the calcium silicate hydrate (C-S-H), which is the primary hydration product. O K-edge NEXAFS is also very useful in distinguishing the chemical components in hydrated C 3 S. Based on the Ca L 3,2 -edge spectra and chemical component mapping, we concluded that CaCl 2 prefers to coexist with unhydrated C 3 S instead of C-S-H. In Si K-edge NEXAFS analysis, CaCl 2 increases the degree of silicate polymerization of C-S-H in agreement with the 29 Si CP/MAS NMR results, which show that the presence of CaCl 2 in hydrated C 3 S considerably accelerates the formation of middle groups ( Q 2 ) and branch sites ( Q 3 ) in the silicate chains of C-S-H gel at 1-day hydration.« less

  8. Resid-

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

    87,093 79,294 14,765 12,538 12,420 4,608 17,041 45,153 1,918 328 Building floorspace (square feet) 1,001 to 5,000 8,041 6,124 2,350 983 1,027 Q Q 2,154 155 Q 5,001 to 10,000 8,900 7,304 2,968 1,193 972 Q Q 3,082 Q N 10,001 to 25,000 14,105 12,357 3,883 1,457 1,855 145 631 6,557 Q Q 25,001 to 50,000 11,917 10,813 2,526 1,866 1,606 Q 1,095 6,466 Q Q 50,001 to 100,000 13,918 13,069 1,395 2,825 1,956 567 2,724 8,705 441 Q 100,001 to 200,000 12,415 12,152 895 1,718 1,652 1,273 3,211 7,447 Q Q 200,001

  9. DC Fast Charge Effects on Battery Life and Performance Study - 50,000 Mile Update

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

    11 L2 4582 L2 2183 DCFC 2078 DCFC 0-10k Miles (Oct-Jan) 28.6 28.6 32.7 32.5 10-20k Miles (Jan-Mar) 22.7 22.5 27.6 27.3 20-30k Miles (Apr-Jul) 35.7 36.0 39.8 39.5 30-40k Miles (Jul-Oct) 38.2 38.4 40.8 40.6 40-50k Miles (Oct-Mar) 23.2 23.6 27.3 26.8 1. Capacity and Peak Power tests based on tests from USABC Electric Vehicle Battery Test Procedures Manual Revision 2. Electric Vehicle Power Characterization test adapted from the Hybrid Pulse Power Characterization Test from the FreedomCAR Battery

  10. Advanced, Low/Zero Emission Boiler Design and Operation

    SciTech Connect (OSTI)

    Babcock Illinois State Geological; Worley Parsons; Parsons Infrastructure /Technology Group

    2007-06-30

    In partnership with the U.S. Department of Energy's National Energy Technology Laboratory, B&W and Air Liquide are developing and optimizing the oxy-combustion process for retrofitting existing boilers as well as new plants. The main objectives of the project is to: (1) demonstrate the feasibility of the oxy-combustion technology with flue gas recycle in a 5-million Btu/hr coal-fired pilot boiler, (2) measure its performances in terms of emissions and boiler efficiency while selecting the right oxygen injection and flue gas recycle strategies, and (3) perform technical and economic feasibility studies for application of the technology in demonstration and commercial scale boilers. This document summarizes the work performed during the period of performance of the project (Oct 2002 to June 2007). Detailed technical results are reported in corresponding topical reports that are attached as an appendix to this report. Task 1 (Site Preparation) has been completed in 2003. The experimental pilot-scale O{sub 2}/CO{sub 2} combustion tests of Task 2 (experimental test performance) has been completed in Q2 2004. Process simulation and cost assessment of Task 3 (Techno-Economic Study) has been completed in Q1 2005. The topical report on Task 3 has been finalized and submitted to DOE in Q3 2005. The calculations of Task 4 (Retrofit Recommendation and Preliminary Design of a New Generation Boiler) has been completed in 2004. In Task 6 (engineering study on retrofit applications), the engineering study on 25MW{sub e} unit has been completed in Q2, 2008 along with the corresponding cost assessment. In Task 7 (evaluation of new oxy-fuel power plants concepts), based on the design basis document prepared in 2005, the design and cost estimate of the Air Separation Units, the boiler islands and the CO{sub 2} compression and trains have been completed, for both super and ultra-supercritical case study. Final report of Task-7 is published by DOE in Oct 2007.

  11. Search for: All records | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    ... detail and add significantly to the DIS data set at low to moderate Q2 and moderate to ... detail and add significantly to the DIS data set at low to moderate Q2 and moderate to ...

  12. Threshold Reflectivity Zc

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

    The black and red colors represent those for 0.33 (q 3) and 1(q 1), respectively. The dependency exhibits two distinct regimes: threshold function ...

  13. Energy Department Invests $13 Million to Drive Innovative U.S...

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

    of efficient, affordable photovoltaic and concentrating solar power technologies. ... In Q3 2013, the United States installed 930 megawatts of photovoltaic, up 20 percent over ...

  14. PowerPoint Presentation

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

    FY10 JFR activities in Q3 focused on data analysis and refurbishment of divertor heat flux instrumentation LH2 launcher installed and operational Progress thus far: * P...

  15. Energy Information Administration - Commercial Energy Consumption...

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

    500,000 ... 8 3 1 Q Q 3 Q Principal Building Activity Education ... 386 360 21 Q N N N Food Sales...

  16. --No Title--

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

    3 Q 9 Q 3 Q 6 Central Chillers ... 111 3 6 18 11 31 8 11 6 16 Packaged Air Conditioning Units ... 1,613 42...

  17. Integrated Biomass Gasification with Catalytic Partial Oxidation for Selective Tar Conversion

    SciTech Connect (OSTI)

    Zhang, Lingzhi; Wei, Wei; Manke, Jeff; Vazquez, Arturo; Thompson, Jeff; Thompson, Mark

    2011-05-28

    . Major milestones include identification of syngas cleaning requirements for proposed system design, identification and selection of tar compounds and 2 mixtures for use in CPO tests, and preparation of CPO catalysts for validation. (Q3 2009 ~ Q4 2009) - Task C: Test CPO with biomass gasification product gas. Optimize CPO performance with selected tar compounds. Optimize CPO performance with multi-component mixtures. Milestones include optimizing CPO catalysts design, collecting CPO experimental data for next stage kinetic modeling and understanding the effect of relative reactivities on ultimate tar conversion and syngas yields. (Q1 2010 ~ Q3 2010) - Task D: Develop tar CPO kinetic model with CPO kinetic model and modeling results as deliverables. (Q3 2010 ~ Q2 2011) - Task E: Project management and reporting. Milestone: Quarterly reports and presentations, final report, work presented at national technical conferences (Q1 2009 ~ Q2 2011) At the beginning of the program, IP landscaping was conducted to understand the operation of various types of biomass gasifiers, their unique syngas/tar compositions and potential tar mitigation options using the catalytic partial oxidation technology. A process simulation model was developed to quantify the system performance and economics impact of CPO tar removal technology. Biomass gasification product compositions used for performance evaluation tests were identified after literature review and system modeling. A reaction system for tar conversion tests was designed, constructed, with each individual component shaken-down in 2009. In parallel, University of Minnesota built a lab-scale unit and evaluated the tar removal performance using catalytic reforming. Benzene was used as the surrogate compound. The biomass gasification raw syngas composition was provided by GE through system studies. In 2010, GE selected different tar compounds and evaluated the tar removal effectiveness of the CPO catalyst. The catalytic performance was

  18. Search for: All records | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    ... of National Environmental Policy Act (United States) USDOE ... F2 and, by including other world data, we studied the Q2 ... phenomenological analysis indicates an excess of the ...

  19. Search for: All records | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    ...circ in the scaled differential cross section, s7 fracdsigmadt. ... The proton electric to magnetic form factor ratio (Gsub Esup pGsub Msup p) at Q2 ...

  20. Slide 1

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

    Direct + Diffuse Direct (all sky) Direct (clear sky) Diffuse (all sky) > Diffuse (clear sky) Q2: Reflectance Enhancement Enhancement (3D-1D) depends on cloud...

  1. b26.xls

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

    79 Q N Q Q Food Service ...... 297 282 125 171 Q Q 31 Q Health Care ...... 129 124 62 68 Q 2 Q Q Inpatient ...

  2. Implementation of ORR Groundwater Strategy

    Office of Environmental Management (EM)

    ... modeling * Summary of progress in annual Remediation Effectiveness Report Groundwater Program ... * first sampling event in FY 2015 Q2 was successfully completed ...

  3. NREL-BA Team CARB

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

    & Review; Q2 3. Project Execution and Ongoing Evaluation; ... 2 Purpose and Objectives Problem Statement: * Builders , ... cost-effective efficiency strategy - maximize insulation * ...

  4. Building America - IBACOS

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

    & Review; Q2 3. Project Execution and Ongoing Evaluation; ... - IBACOS Focus Areas Problem Statement: Support RBI ... in low load homes, regardless of HVAC system strategy. ...

  5. Empirical Fit to Precision Inclusive Electron-Proton Cross Sections in the Resonance Region

    SciTech Connect (OSTI)

    M.E. Christy; Peter Bosted

    2010-05-01

    An empirical fit is described to measurements of inclusive inelastic electron-proton cross sections in the kinematic range of four-momentum transfer $0 \\le Q^2<8$ GeV$^2$ and final state invariant mass $1.1<3.1$ GeV. The fit is constrained by the recent high precision longitudinal and transverse (L/T) separated cross section measurements from Jefferson Lab Hall C, un-separated Hall C measurements up to $Q^2$ $\\approx 7.5$ ${\\rm GeV}^2$, and photoproduction data at $Q^2 = 0$. Compared to previous fits, the present fit covers a wider kinematic range, fits both transverse and longitudinal cross sections, and features smooth transitions to the photoproduction data at $Q^2=0$ and DIS data at high $Q^2$ and $W$.

  6. 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...

  7. --No Title--

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

    Q Q Q 505 Q Q 22.0 Q Buildings without Cooling ... 2 1 Q 634 623 Q 3.1 2.1 Q Water-Heating Energy Sources Electricity ... 29 126 26...

  8. c15.xls

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

    without Cooling ... 7 Q 3 6 1,855 2,232 1,214 1,080 3.6 6.4 2.6 5.8 Water-Heating Energy Sources Electricity ... 57 86...

  9. Low-Cost MHTES Systems for CSP | Department of Energy

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

    More Documents & Publications Low-Cost Metal Hydride TES Systems - FY13 Q1 Low-Cost Metal Hydride TES Systems - FY13 Q3 Low-Cost Metal Hydride Thermal Energy Storage System - FY13 ...

  10. c1.xls

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

    Q District Heat ... 27 3,088 8,155 4,241 218 Q 3,690 Propane ... 128 1,422 1,871 1,734 Q Q Q Cooking...

  11. Energy Information Administration - Commercial Energy Consumption...

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

    ... 7,660 2,756 800 Q Q 3,274 Q Principal Building Activity Education ... 9,874 8,714 946 Q N N N Food Sales...

  12. Paraquantization and supersymmetric intertwining

    SciTech Connect (OSTI)

    Morchedi, O.; Mebarki, N.

    2012-06-27

    A two dimensional paraquantum system of order Q=3,5 along one direction is shown to be a supersymetric intertwining. The expressions of the partners pairs of the Hamiltonian and supercharge verifying the intertwining relations are obtained.

  13. Southface Advanced Commercial Buildings Initiative (ABCI)

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

    ... of Atlanta: Development of Commercial Benchmarking ordinance to include small commercial ... with the Boys and Girls Club. Budget History Q3FY2013 - FY2013 (past) FY2014 (current) ...

  14. THE AEROSPACE CORPORATION '

    Office of Legacy Management (LM)

    q 3 THE AEROSPACE CORPORATION ' Suite 4000, 955 L' Enant Plaza, S. W., Warhington, D.C. 20024, Telephone: (202) 488-6000 7117-01.87.sej.16 28 July 1987 . Mr. Andrew Wallo, III,...

  15. The pMSSM10 after LHC run 1

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

    de Vries, K. J.; Bagnaschi, E. A.; Buchmueller, O.; Cavanaugh, R.; Citron, M.; De Roeck, A.; Dolan, M. J.; Ellis, J. R.; Flächer, H.; Heinemeyer, S.; et al

    2015-09-01

    We present a frequentist analysis of the parameter space of the pMSSM10, in which the following ten soft SUSY-breaking parameters are specified independently at the mean scalar top mass scale MSUSY ≡ √mmore » $$\\tilde{t}$$1m$$\\tilde{t}$$2 : the gaugino masses M1,2,3 , the first-and second-generation squark masses m$$\\tilde{q}$$1 = m$$\\tilde{q}$$2 , the third-generation squark mass m$$\\tilde{q}$$3, a common slepton mass m$$\\tilde{ℓ}$$ and a common trilinear mixing parameter A , as well as the Higgs mixing parameter μ , the pseudoscalar Higgs mass MA and tanβ , the ratio of the two Higgs vacuum expectation values. We use the MultiNest sampling algorithm with ∼ 1.2 ×109 points to sample the pMSSM10 parameter space. A dedicated study shows that the sensitivities to strongly interacting sparticle masses of ATLAS and CMS searches for jets, leptons + E-slashT signals depend only weakly on many of the other pMSSM10 parameters. With the aid of the Atom and Scorpion codes, we also implement the LHC searches for electroweakly interacting sparticles and light stops, so as to confront the pMSSM10 parameter space with all relevant SUSY searches. In addition, our analysis includes Higgs mass and rate measurements using the HiggsSignals code, SUSY Higgs exclusion bounds, the measurements of BR(Bs→μ+μ-) by LHCb and CMS, other B -physics observables, electroweak precision observables, the cold dark matter density and the XENON100 and LUX searches for spin-independent dark matter scattering, assuming that the cold dark matter is mainly provided by the lightest neutralino χ-tilde10 . We show that the pMSSM10 is able to provide a supersymmetric interpretation of (g-2)μ , unlike the CMSSM, NUHM1 and NUHM2. As a result, we find (omitting Higgs rates) that the minimum χ2=20.5 with 18 degrees of freedom (d.o.f.) in the pMSSM10, corresponding to a χ2 probability of 30.8 %, to be compared with χ2/d.o.f.=32.8/24(31.1/23)(30.3/22) in the CMSSM (NUHM1) (NUHM2). We

  16. Quercetin 3-O-methyl ether protects FL83B cells from copper induced oxidative stress through the PI3K/Akt and MAPK/Erk pathway

    SciTech Connect (OSTI)

    Tseng, Hsiao-Ling; Li, Chia-Jung; Huang, Lin-Huang; Chen, Chun-Yao; Tsai, Chun-Hao; Lin, Chun-Nan; Department of Biological Science and Technology, School of Medicine, China Medical University, Taichung, Taiwan ; Hsu, Hsue-Yin

    2012-10-01

    Quercetin is a bioflavonoid that exhibits several biological functions in vitro and in vivo. Quercetin 3-O-methyl ether (Q3) is a natural product reported to have pharmaceutical activities, including antioxidative and anticancer activities. However, little is known about the mechanism by which it protects cells from oxidative stress. This study was designed to investigate the mechanisms by which Q3 protects against Cu{sup 2+}-induced cytotoxicity. Exposure to Cu{sup 2+} resulted in the death of mouse liver FL83B cells, characterized by apparent apoptotic features, including DNA fragmentation and increased nuclear condensation. Q3 markedly suppressed Cu{sup 2+}-induced apoptosis and mitochondrial dysfunction, characterized by reduced mitochondrial membrane potential, caspase-3 activation, and PARP cleavage, in Cu{sup 2+}-exposed cells. The involvement of PI3K, Akt, Erk, FOXO3A, and Mn-superoxide dismutase (MnSOD) was shown to be critical to the survival of Q3-treated FL83B cells. The liver of both larval and adult zebrafish showed severe damage after exposure to Cu{sup 2+} at a concentration of 5 μM. Hepatic damage induced by Cu{sup 2+} was reduced by cotreatment with Q3. Survival of Cu{sup 2+}-exposed larval zebrafish was significantly increased by cotreatment with 15 μM Q3. Our results indicated that Cu{sup 2+}-induced apoptosis in FL83B cells occurred via the generation of ROS, upregulation and phosphorylation of Erk, overexpression of 14-3-3, inactivation of Akt, and the downregulation of FOXO3A and MnSOD. Hence, these results also demonstrated that Q3 plays a protective role against oxidative damage in zebrafish liver and remarked the potential of Q3 to be used as an antioxidant for hepatocytes. Highlights: ► Protective effects of Q3 on Cu{sup 2+}-induced oxidative stress in vitro and in vivo. ► Cu{sup 2+} induced apoptosis in FL83B cells via ROS and the activation of Erk. ► Q3 abolishes Cu{sup 2+}-induced apoptosis through the PI3K/Akt and MAPK

  17. PowerPoint Presentation - FY13 Q1 | Department of Energy

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

    More 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 ...

  18. Stuart R Hudson | Princeton Plasma Physics Lab

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

    was introduced. After completing his doctorate, Stuart worked as a Research Fellow at the Japan Atomic Energy Research Institute. During this time, he studied the overlap of q2...

  19. MHK Projects/CETO La Reunion | Open Energy Information

    Open Energy Info (EERE)

    of the single, stand-alone unit due in Q2 2012. Stage 1 has been awarded 5M of French Government funding. Project Installed Capacity (MW) 0 Number of Devices Deployed 1...

  20. c21.xls

    Gasoline and Diesel Fuel Update (EIA)

    Q 14.5 18.7 Buildings without Cooling ... 11 8 Q 2,142 2,757 Q 5.2 2.8 7.7 Water-Heating Energy Sources Electricity ... 88 163...

  1. --No Title--

    Gasoline and Diesel Fuel Update (EIA)

    ... 110 52 88 6,834 3,186 6,328 16.1 16.4 13.9 Other Excluding Electricity ... Q Q Q Q Q Q Q Q Q Buildings without Cooling ... Q 2...

  2. --No Title--

    Gasoline and Diesel Fuel Update (EIA)

    Q 14.5 18.7 Buildings without Cooling ... 11 8 Q 2,142 2,757 Q 5.2 2.8 7.7 Water-Heating Energy Sources Electricity ... 88 163...

  3. Search for: All records | SciTech Connect

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    differential cross section, ssup 7(dsigmadt) and a rapid fall-off in a ... The proton electric to magnetic form factor ratio (Gsub Esup pGsub Msup p) at Q2 ...

  4. file://C:\\Documents and Settings\\bh5\\My Documents\\Energy Effici

    Gasoline and Diesel Fuel Update (EIA)

    Metals 758 646 529 332 Fabricated Metal Products 3 1 1 333 Machinery Q 2 * 334 Computer and Electronic Products * 1 1 335 Electrical Equip., Appliances, and Components 27 69...

  5. Electrolux Gibson Air Conditioner and Equator Clothes Washer Fail DOE Energy Star Testing

    Broader source: Energy.gov [DOE]

    DOE testing in support of the ENERGY STAR program has revealed that an Electrolux Gibson air conditioner (model GAH105Q2T1) and an Equator clothes washer (model EZ 3720 CEE), both of which claimed...

  6. Search for: All records | DOE PAGES

    Office of Scientific and Technical Information (OSTI)

    ; Carlin, C. ; Keith, C. D. ; Meekins, D. G. ; et al Full Text Available April 2016, Elsevier Precise determination of the deuteron spin structure at low to moderate Q2 with CLAS...

  7. Electrolux Gibson Air Conditioner and Equator Clothes Washer...

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

    ENERGY STAR program has revealed that an Electrolux Gibson air conditioner (model GAH105Q2T1) and an Equator clothes washer (model EZ 3720 CEE), both of which claimed ENERGY STAR...

  8. Financial Management for Retail Energy Efficiency

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

    ... Budget History April 9, 2015 - FY 2015 (past) FY 2016 (current) FY 2017 - Dec. 31, 2018 ... retail financial calendars 3.1 Program Benchmarking Calls Q1, Q2 Q1 delayed less than a ...

  9. Atmospheric Pressure Deposition for Electrochromic Windows

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

    ... Study of Doped NiO Counter Electrode Materials FY12-Q2 Milestone: Synthesize VO2 Nanoparticles and Charcaterize Performance FY12-Q4 Milestone: Demonstration Liquid Phase Spray ...

  10. --No Title--

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

    Distributed System ... Q 120 244 Q 2,566 5,478 Q 46.9 44.6 Energy-Related Space Functions (more than one may apply) Commercial Food Preparation ... 185 298 483...

  11. SENDECO2 | Open Energy Information

    Open Energy Info (EERE)

    search Name: SENDECO2 Place: Barcelona, Spain Zip: 11 08034 Sector: Carbon Product: A Spanish exchange for CO2 allowances and carbon credits, intended to go live by the end of Q2...

  12. DOE MURI: Hig-Operating Temperature Heat Transfer Fluids for...

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

    High Operating Temperature Liquid Metal Heat Transfer Fluids - FY13 Q2 High Operating Temperature Heat Transfer Fluids for Solar Thermal Power Generation FY13 Q1 Corrosion in Very ...

  13. Low-Cost, Lightweight Solar Concentrators - FY13 Q1 | Department...

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

    KB) More Documents & Publications Low-Cost, Lightweight Solar Concentrators FY13 Q2 Low-Cost, Lightweight Solar Concentrator Low-Cost Light Weigh Thin Film Solar Concentrators

  14. Low-Cost Light Weigh Thin Film Solar Concentrators | Department...

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    313ganapathi.pdf (6.65 MB) More Documents & Publications Low-Cost, Lightweight Solar Concentrators - FY13 Q1 Low-Cost, Lightweight Solar Concentrators FY13 Q2

  15. HUD Updated Supplemental Lists - February 18, 2016 | Department of Energy

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

    Updated Supplemental Lists - February 18, 2016 HUD Updated Supplemental Lists - February 18, 2016 HUD Updated Supplemental Lists - February 18, 2016 Updated_supplemental_lists_1Q_2Q_ 2-18-16.xlsx (23.23 KB) More Documents & Publications updated_supplemental_lists_1n-2n-3m_07-06-2012.xlsx updated_supplemental_lists_1m-2m-3l-04-05-2012.xlsx updated_supplemental_lists_1p_2p_3o_04302013.xlsx

  16. $$B\\to Kl^+l^-$$ decay form factors from three-flavor lattice QCD

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

    Bailey, Jon A.

    2016-01-27

    We compute the form factors for the B → Kl+l- semileptonic decay process in lattice QCD using gauge-field ensembles with 2+1 flavors of sea quark, generated by the MILC Collaboration. The ensembles span lattice spacings from 0.12 to 0.045 fm and have multiple sea-quark masses to help control the chiral extrapolation. The asqtad improved staggered action is used for the light valence and sea quarks, and the clover action with the Fermilab interpretation is used for the heavy b quark. We present results for the form factors f+(q2), f0(q2), and fT(q2), where q2 is the momentum transfer, together with a comprehensivemore » examination of systematic errors. Lattice QCD determines the form factors for a limited range of q2, and we use the model-independent z expansion to cover the whole kinematically allowed range. We present our final form-factor results as coefficients of the z expansion and the correlations between them, where the errors on the coefficients include statistical and all systematic uncertainties. Lastly, we use this complete description of the form factors to test QCD predictions of the form factors at high and low q2.« less

  17. Clean measurements of the nucleon axial-vector and free-neutron magnetic form factors

    SciTech Connect (OSTI)

    Deur, Alexandre P.

    2013-11-01

    We discuss the feasibility of a weak charged current experiment using a low energy electron beam. A first goal is to measure the Q^2 dependence of the axial-vector form factor g_a(Q^2). It can be measured model-independently and as robustly as for electromagnetic form factors from typical electron scattering experiments, in contrast to the methods used so far to measure g_a(Q^2). If g_a(Q^2) follows a dipole form, the axial mass can be extracted with a better accuracy than the world data altogether. The most important detection equipment would be a segmented neutron detector with good momentum and angular resolution that is symmetric about the beam direction, and covers a moderate angular range. A high intensity beam (100 uA) is necessary. Beam polarization is highly desirable as it provides a clean measurement of the backgrounds. Beam energies between 70 and 110 MeV are ideal. This range would provide a Q^2 mapping of g_a between 0.01

  18. Precision Measurements of the Proton Elastic Form Factor Ratio

    SciTech Connect (OSTI)

    Douglas Higinbotham

    2010-08-01

    New high precision polarization measurements of the proton elastic form factor ratio in the Q^2 from 0.3 to 0.7 [GeV/c]^2 have been made. These elastic H(e,e'p) measurementswere done in Jefferson Lab's Hall A using 80% longitudinally polarized electrons and recoil polarimetry. For Q^2 greater than 1 [GeV/c]^2, previous polarization data indicated a strong deviation of the form factor ratio from unity which sparked renewed theoretical and experimental interest in how two-photon diagrams have been taken into account. The new high precision data indicate that the deviation from unity, while small, persists even at Q^2 less than 1 [GeV/c]^2.

  19. Impact of hadronic and nuclear corrections on global analysis of spin-dependent parton distributions

    SciTech Connect (OSTI)

    Jimenez-Delgado, Pedro; Accardi, Alberto; Melnitchouk, Wally

    2014-02-01

    We present the first results of a new global next-to-leading order analysis of spin-dependent parton distribution functions from the most recent world data on inclusive polarized deep-inelastic scattering, focusing in particular on the large-x and low-Q^2 regions. By directly fitting polarization asymmetries we eliminate biases introduced by using polarized structure function data extracted under nonuniform assumptions for the unpolarized structure functions. For analysis of the large-x data we implement nuclear smearing corrections for deuterium and 3He nuclei, and systematically include target mass and higher twist corrections to the g_1 and g_2 structure functions at low Q^2. We also explore the effects of Q^2 and W^2 cuts in the data sets, and the potential impact of future data on the behavior of the spin-dependent parton distributions at large x.

  20. Measurements of $$ep \\to e^\\prime π^+n$$ at W = 1.6 - 2.0 GeV and extraction of nucleon resonance electrocouplings at CLAS

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

    Park, Kijun; Aznauryan, I. G.; Burkert, V. D.; Adhikari, K. P.; Amaryan, M. J.; Pereira, S. Anefalos; Avakian, H.; Battaglieri, M.; Badui, R.; Bedlinskiy, I.; et al

    2015-04-01

    Differential cross sections of the exclusive processmore » $$e p \\to e^\\prime \\pi^+ n$$ were measured with good precision in the range of the photon virtuality $Q^2 = 1.8 - 4.5$ GeV$^2$, and the invariant mass range of the $$\\pi^+ n$$ final state W = 1.6 - 2.0 GeV using the CEBAF Large Acceptance Spectrometer. Data were collected with nearly complete coverage in the azimuthal and polar angles of the $$n\\pi^+$$ center-of-mass system. More than 37,000 cross section points were measured. The contributions of the isospin $$I = {1\\over 2}$$ resonances $$N(1675){5\\over 2}^-$$, $$N(1680){5\\over 2}^+$$ and $$N(1710){1\\over 2}^+$$ were extracted at different values of $Q^2$ using a single-channel, energy-dependent resonance amplitude analysis. Two different approaches, the unitary isobar model and the fixed-$t$ dispersion relations, were employed in the analysis. We observe significant strength of the $$N(1675){5\\over 2}^-$$ in the $$A_{1/2}$$ amplitude, which is in strong disagreement with quark models that predict both transverse amplitudes to be strongly suppressed. For the $$N(1680){5\\over 2}^+$$ we observe a slow changeover from the dominance of the $$A_{3/2}$$ amplitude at the real photon point ($Q^2=0$) to a $Q^2$ where $$A_{1/2}$$ begins to dominate. The scalar amplitude $$S_{1/2}$$ drops rapidly with $Q^2$ consistent with quark model prediction. For the $$N(1710){1\\over 2}^+$$ resonance our analysis shows significant strength for the $$A_{1/2}$$ amplitude at $Q^2 < 2.5$ GeV$^2$.« less

  1. Measurements of $ep \\to e^\\prime π^+n$ at W = 1.6 - 2.0 GeV and extraction of nucleon resonance electrocouplings at CLAS

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

    Park, Kijun; Aznauryan, I. G.; Burkert, V. D.; Adhikari, K. P.; Amaryan, M. J.; Pereira, S. Anefalos; Avakian, H.; Battaglieri, M.; Badui, R.; Bedlinskiy, I.; et al

    2015-04-01

    Differential cross sections of the exclusive process $e p \\to e^\\prime \\pi^+ n$ were measured with good precision in the range of the photon virtuality $Q^2 = 1.8 - 4.5$ GeV$^2$, and the invariant mass range of the $\\pi^+ n$ final state W = 1.6 - 2.0 GeV using the CEBAF Large Acceptance Spectrometer. Data were collected with nearly complete coverage in the azimuthal and polar angles of the $n\\pi^+$ center-of-mass system. More than 37,000 cross section points were measured. The contributions of the isospin $I = {1\\over 2}$ resonances $N(1675){5\\over 2}^-$, $N(1680){5\\over 2}^+$ and $N(1710){1\\over 2}^+$ were extracted atmore »different values of $Q^2$ using a single-channel, energy-dependent resonance amplitude analysis. Two different approaches, the unitary isobar model and the fixed-$t$ dispersion relations, were employed in the analysis. We observe significant strength of the $N(1675){5\\over 2}^-$ in the $A_{1/2}$ amplitude, which is in strong disagreement with quark models that predict both transverse amplitudes to be strongly suppressed. For the $N(1680){5\\over 2}^+$ we observe a slow changeover from the dominance of the $A_{3/2}$ amplitude at the real photon point ($Q^2=0$) to a $Q^2$ where $A_{1/2}$ begins to dominate. The scalar amplitude $S_{1/2}$ drops rapidly with $Q^2$ consistent with quark model prediction. For the $N(1710){1\\over 2}^+$ resonance our analysis shows significant strength for the $A_{1/2}$ amplitude at $Q^2 « less

  2. Measurements of $ep \\to e^\\prime ?^+n$ at W = 1.6 - 2.0 GeV and extraction of nucleon resonance electrocouplings at CLAS

    SciTech Connect (OSTI)

    Park, Kijun; Aznauryan, I. G.; Burkert, V. D.; Adhikari, K. P.; Amaryan, M. J.; Pereira, S. Anefalos; Avakian, H.; Battaglieri, M.; Badui, R.; Bedlinskiy, I.; Biselli, A. S.; Bono, J.; Briscoe, W. J.; Brooks, W. K.; Carman, D. S.; Celentano, A.; Chandavar, S.; Charles, G.; Colaneri, L.; Cole, P. L.; Contalbrigo, M.; Cortes, O.; Crede, V.; D'Angelo, A.; Dashyan, N.; De Vita, R.; De Sanctis, E.; Deur, A.; Djalali, C.; Doughty, D.; Dupre, R.; Egiyan, H.; Alaoui, A. El; Elouadrhiri, L.; Fassi, L. El; Eugenio, P.; Fedotov, G.; Fegan, S.; Fersch, R.; Filippi, A.; Fleming, J. A.; Garillon, B.; Garcon, M.; Gevorgyan, N.; Gilfoyle, G. P.; Giovanetti, K. L.; Girod, F. X.; Joo, H. S.; Goetz, J. T.; Golovatch, E.; Gothe, R. W.; Griffioen, K. A.; Guegan, B.; Guidal, M.; Guo, L.; Hakobyan, H.; Hanretty, C.; Hattawy, M.; Hicks, K.; Holtrop, M.; Hughes, S. M.; Hyde, C. E.; Ilieva, Y.; Ireland, D. G.; Ishkhanov, B. S.; Isupov, E. L.; Jenkins, D.; Jiang, H.; Jo, H. S.; Joo, K.; Joosten, S.; Keller, D.; Khandaker, M.; Kim, A.; Kim, W.; Klein, A.; Klein, F. J.; Kubarovsky, V.; Kuhn, S. E.; Kuleshov, S. V.; Lenisa, P.; Livingston, K.; Lu, H. Y.; MacGregor, I. J.; Markov, N.; Martinez, D.; McKinnon, B.; Mokeev, V.; Montgomery, R. A.; Moutarde, H.; Camacho, C. Munoz; Nadel-Turonski, P.; Niccolai, S.; Niculescu, G.; Niculescu, I.; Osipenko, M.; Ostrovidov, A. I.; Paolone, M.; Pasyuk, E.; Peng, P.; Phelps, W.; Phillips, J. J.; Pisano, S.; Pogorelko, O.; Price, J. W.; Procureur, S.; Prok, Y.; Protopopescu, D.; Puckett, A. J.; Raue, B. A.; Ripani, M.; Rizzo, A.; Rosner, G.; Rossi, P.; Roy, P.; Sabati??, F.; Salgado, C.; Schott, D.; Schumacher, R. A.; Seder, E.; Sharabian, Y. G.; Simonyan, A.; Skorodumina, Iu.; Smith, E. S.; Smith, G. D.; Sparveris, N.; Stoler, P.; Strakovsky, I. I.; Strauch, S.; Sytnik, V.; Taiuti, M.; Tang, W.; Taylor, C. E.; Tian, Ye; Trivedi, A.; Ungaro, M.; Voskanyan, H.; Voutier, E.; Walford, N. K.; Watts, D. P.; Wei, X.; Weinstein, L. B.; Wood, M. H.; Zachariou, N.; Zana, L.; Zhang, J.; Zhao, Z. W.; Zonta, I.

    2015-04-01

    Differential cross sections of the exclusive process $e p \\to e^\\prime \\pi^+ n$ were measured with good precision in the range of the photon virtuality $Q^2 = 1.8 - 4.5$ GeV$^2$, and the invariant mass range of the $\\pi^+ n$ final state W = 1.6 - 2.0 GeV using the CEBAF Large Acceptance Spectrometer. Data were collected with nearly complete coverage in the azimuthal and polar angles of the $n\\pi^+$ center-of-mass system. More than 37,000 cross section points were measured. The contributions of the isospin $I = {1\\over 2}$ resonances $N(1675){5\\over 2}^-$, $N(1680){5\\over 2}^+$ and $N(1710){1\\over 2}^+$ were extracted at different values of $Q^2$ using a single-channel, energy-dependent resonance amplitude analysis. Two different approaches, the unitary isobar model and the fixed-$t$ dispersion relations, were employed in the analysis. We observe significant strength of the $N(1675){5\\over 2}^-$ in the $A_{1/2}$ amplitude, which is in strong disagreement with quark models that predict both transverse amplitudes to be strongly suppressed. For the $N(1680){5\\over 2}^+$ we observe a slow changeover from the dominance of the $A_{3/2}$ amplitude at the real photon point ($Q^2=0$) to a $Q^2$ where $A_{1/2}$ begins to dominate. The scalar amplitude $S_{1/2}$ drops rapidly with $Q^2$ consistent with quark model prediction. For the $N(1710){1\\over 2}^+$ resonance our analysis shows significant strength for the $A_{1/2}$ amplitude at $Q^2 < 2.5$ GeV$^2$.

  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. "Table HC1.2.3 Living Space Characteristics by Average Floorspace...

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

    ...357,2492,2103,1096,"Q","Q","Q" "3,000 or 3,499",6.7,6.6,3014,2175,1438,3047,2079,1108,"N","N","N" "3,500 to 3,999",5.2,5.1,3549,2505,1518,"Q","Q","Q","N","N","N" "4,000 or ...

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

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

    "3 or More",0.6,"Q","Q","Q" "Plasma Television Sets",3.6,0.7,0.6,"Q" ... "3 or More",22.3,37.5,49,58.8 "Plasma Television Sets",10.8,29.6,32.8,57.2 ...

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

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

    "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",... "3 or More",22.3,24,26.1,96.9,0,75.1,0 "Plasma Television Sets",10.8,11.6,13.3,39.5,54.7...

  7. " Million U.S. Housing Units"

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

    "3 or More",0.6,0.4,"Q","N","Q","N" "Plasma Television Sets",3.6,2.6,0.3,"Q",0.4,"Q" ... "3 or More",22.3,26.1,96.8,0,46.6,0 "Plasma Television Sets",10.8,13,32.3,38.4,26.5,5...

  8. Science Headlines

    Office of Science (SC) Website

    -0500 12B69234-E106-461C-B008-1A4F342D3F6Dhttp:1.usa.gov20feQ3S A Respiratory Virus Provides Clues to Possible Treatments Purdue University researchers, working at the...

  9. News

    Office of Science (SC) Website

    glaciers. 12B69234-E106-461C-B008-1A4F342D3F6Dhttp:1.usa.gov20feQ3S A Respiratory Virus Provides Clues to Possible Treatments Purdue University researchers, working at the...

  10. table2.1_02.xls

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

    Total United States RSE Column Factors: 1.4 0.4 1.6 1.2 1.2 1.1 0.7 1.2 ... 0 0 0 0 * 324 Petroleum and Coal Products 3,689 * * * 0 Q * 3,407 324110 Petroleum Refineries 3,307 0 0 0 0 ...

  11. New insight on global QCD fits using Regge theory

    SciTech Connect (OSTI)

    Soyez, G.

    2005-06-14

    In global QCD fits, one has to choose an initial parton distribution at Q{sup 2} = Q{sub 0}{sup 2}. I shall argue that the initial condition chosen in usual standard sets is inconsistent with analytic S-matrix theory. I shall show how one can combine these two approaches, leading to a Regge-compatible next-to-leading order global QCD fit. This allows one to extend the parametrisation in the low-Q2 region. Finally, I shall discuss how it it possible to use the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) equation to obtain information on Regge models at high Q2.

  12. Unitary constraints on neutral pion electroproduction

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

    Laget, J -M

    2011-01-01

    At large virtualitymore » $Q^2$, the coupling to the vector meson production channels provides us with a natural explanation of the surprisingly large cross section of the neutral pion electroproduction recently measured at Jefferson Laboratory, without destroying the good agreement between the Regge pole model and the data at the real photon point. Elastic rescattering of the $$\\pi^0$$ provides us with a way to explain why the node, that appears at $$t\\sim -0.5$$~GeV$^2$ at the real photon point, disappears as soon as $Q^2$ differs from zero.« less

  13. Table 5.14. U.S. Vehicle Fuel Consumption by Vehicle Type, 1994

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

    or More ... 11.9 7.0 6.6 0.4 0.7 1.4 Q 2.0 Q 23.6 Below Poverty Line 100 Percent ... 6.9 4.9 4.6 0.3 Q Q Q 1.2 Q...

  14. Characteristics RSE Column Factor: All Vehicle Types

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

    or More ... 19.1 13.0 12.3 0.7 1.0 1.7 Q 2.7 Q 21.8 Below Poverty Line 100 Percent ... 12.4 9.5 8.9 0.5 Q Q Q 1.8 Q...

  15. Search for: All records | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    ... GeV electron beam, covers a range of 1.72 GeV, which is non-zero at the 2.75sigma level. ... (APS) Measurements of the Electric Form Factor of the Neutron up to Q2 3.4 GeV2 using ...

  16. Search for: All records | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    GeV electron beam, covers a range of 1.72 GeV, which is non-zero at the 2.75sigma level. ... (APS) Measurements of the Electric Form Factor of the Neutron up to Q2 3.4 GeV2 using ...

  17. c35.xls

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

    Water ... 574 40 47 Q 2,577 1,652 2,380 1,081 0.22 0.02 0.02 Q Separate Computer Area ... 560 41 59 35 3,623 1,957 2,916 1,756 0.15 0.02 0.02 Q HVAC...

  18. Hard diffractive production of vector mesons

    SciTech Connect (OSTI)

    Kirschner, R.

    2005-06-14

    The large Q2 behaviour of diffractive electroproduction and the large t behaviour of diffractive photoproduction are considered relying on models of the meson and real photon light-cone wave functions. The large size quark-antiquark dipole contribution to the impact factors of all helicity configurations are discussed.

  19. table2.2_02.xls

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

    Total United States RSE Column Factors: 1.4 0.4 1.6 1.2 1.2 1.1 0.7 1.2 ... 0 0 * 0 324 Petroleum and Coal Products 3,689 * 2 * 0 Q 2 3,407 4.4 324110 Petroleum Refineries 3,307 0 0 0 ...

  20. Study of quasielastic scattering using charged-current νμ-iron interactions in the MINOS near detector

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

    Adamson, P.

    2015-01-08

    Kinematic distributions from an inclusive sample of 1.41×106 charged-current νμ interactions on iron, obtained using the MINOS near detector exposed to a wide-band beam with peak flux at 3 GeV, are compared to a conventional treatment of neutrino scattering within a Fermi gas nucleus. Results are also used to guide the selection of a subsample enriched in quasielastic νμFe interactions, containing an estimated 123,000 quasielastic events of incident energies 1 < Eν < 8 GeV, with < Eν > = 2.79 GeV. Four additional subsamples representing topological and kinematic sideband regions to quasielastic scattering are also selected for the purposemore » of evaluating backgrounds. Comparisons using subsample distributions in four-momentum transfer Q2 show the Monte Carlo model to be inadequate at low Q2. Its shortcomings are remedied via inclusion of a Q2-dependent suppression function for baryon resonance production, developed from the data. A chi-square fit of the resulting Monte Carlo simulation to the shape of the Q2 distribution for the quasielastic-enriched sample is carried out with the axial-vector mass MA of the dipole axial-vector form factor of the neutron as a free parameter. Furthermore, the effective MA which best describes the data is 1.23+0.13-0.09(fit)+0.12-0.15(syst) GeV.« less

  1. Induced polarization of Lambda(1116) in kaon electroproduction

    SciTech Connect (OSTI)

    Gabrielyan, M.; Raue, B.A.; Carman, D.S.; Park, K.; Adhikari, K.P.; Adikaram, D.; Amaryan, M.J.; Anefalos Pereira, S.; Avakian, H.; Ball, J.; Baltzell, N.A.; Battaglieri, M.; Baturin, V.; Bedlinskiy, I.; Biselli, A.S.; Bono, J.; Boiarinov, S.; Briscoe, W.J.; Brooks, W.K.; Burkert, V.D.; Cao, T.; Celentano, A.; Chandavar, S.; Charles, G.; Cole, P.L.; Contalbrigo, M.; Cortes, O.; Crede, V.; DAngelo, A.; Dashyan, N.; De Vita, R.; De Sanctis, E.; Deur, A.; Djalali, C.; Doughty, D.; Dupre, R.; ElFassi, L.; Eugenio, P.; Fedotov, G.; Fegan, S.; Fleming, J.A.; Forest, T.A.; Garillon, B.; Gevorgyan, N.; Ghandilyan, Y.; Gilfoyle, G.P.; Giovanetti, K.L.; Girod, F.X.; Goetz, J.T.; Golovatch, E.; Gothe, R.W.; Griffioen, K.A.; Guidal, M.; Guo, L.; Hafidi, K.; Hakobyan, H.; Hattawy, M.; Hicks, K.; Ho, D.; Holtrop, M.; Hughes, S.M.; Ilieva, Y.; Ireland, D.G.; Ishkhanov, B.S.; Jenkins, D.; Jiang, H.; Jo, H.S.; Joo, K.; Keller, D.; Khandaker, M.; Kim, W.; Klein, F.J.; Koirala, S.; Kubarovsky, V.; Kuhn, S.E.; Kuleshov, S.V.; Lenisa, P.; Levine, W.I.; Livingston, K.; MacGregor, I.J.D.; Mayer, M.; McKinnon, B.; Meyer, C.A.; Mestayer, M.D.; Mirazita, M.; Mokeev, V.; Moody, C.I.; Moutarde, H.; Movsisyan, A; Munevar, E.; Munoz Camacho, C.; Nadel-Turonski, P.; Niccolai, S.; Niculescu, G.; Osipenko, M.; Pappalardo, L.L.; Paremuzyan, R.; Pasyuk, E.; Peng, P.; Phelps, W.; Phillips, J.J.; Pisano, S.; Pogorelko, O.; Pozdniakov, S.; Price, J.W.; Procureur, S.; Protopopescu, D.; Rimal, D.; Ripani, M.; Rizzo, A.; Sabatie, F.; Salgado, C.; Schott, D.; Schumacher, R.A.; Simonyan, A.; Smith, G.D.; Sober, D.I.; Sokhan, D.; Stepanyan, S.S.; Stepanyan, S.; Strakovsky, I.I.; Strauch, S.; Sytnik, V.; Tang, W.; Ungaro, M.; Vlassov, A.V.; Voskanyan, H.; Voutier, E.; Walford, N.K.; Watts, D.P.; Wei, X.; Weinstein, L.B.; Zachariou, N.; Zana, L.; Zhang, J.

    2014-09-01

    We have measured the induced polarization of the ?(1116) in the reaction ep?e?K+?, detecting the scattered e? and K+ in the final state along with the proton from the decay ??p??.The present study used the CEBAF Large Acceptance Spectrometer (CLAS), which allowed for a large kinematic acceptance in invariant energy W (1.6?W?2.7 GeV) and covered the full range of the kaon production angle at an average momentum transfer Q2=1.90 GeV2.In this experiment a 5.50 GeV electron beam was incident upon an unpolarized liquid-hydrogen target. We have mapped out the W and kaon production angle dependencies of the induced polarization and found striking differences from photoproduction data over most of the kinematic range studied. However, we also found that the induced polarization is essentially Q2 independent in our kinematic domain, suggesting that somewhere below the Q2 covered here there must be a strong Q2 dependence. Along with previously published photo- and electroproduction cross sections and polarization observables, these data are needed for the development of models, such as effective field theories, and as input to coupled-channel analyses that can provide evidence of previously unobserved s-channel resonances.

  2. Jefferson Lab Hosts 2012 SPAFOA Members Meeting (Meyer Cryogenic, Vacuum

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

    and Pressure Technologies) | Jefferson Lab Hosts 2012 SPAFOA Members Meeting (Meyer Cryogenic, Vacuum and Pressure Technologies) External Link: http://ourmailer.com/Z2U-TRYV-D24Q2F5T0E/cr.aspx?b=32

  3. Build-

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

    Air Condi- tioners","District Chilled Water","Central Chillers","Pack- aged Air Condi- ...Q",2,13,25,15,8,"Q","Q" "District Chilled Water ......",33,33,"Q",1,2,33,"Q",4,"Q","Q" ...

  4. Separated response functions in exclusive, forward π± electroproduction on deuterium

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

    Huber, G. M.; Blok, H. P.; Butuceanu, C.; Gaskell, D.; Horn, T.; Mack, D. J.; Abbott, D.; Aniol, K.; Anklin, H.; Armstrong, C.; et al

    2015-01-07

    Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in π⁻ and π⁺ electroproduction are particularly informative. Ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method:more » Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q2 values of 0.6, 1.0, 1.6 GeV2 at W=1.95 GeV, and Q2=2.45 GeV2 at W=2.22 GeV. There was significant coverage in Φ And ϵ, which allowed separation of σL,T,LT,TT. Results: σL shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, σT is much flatter versus t. The longitudinal/transverse ratios evolve with Q2 and t, and at the highest Q2=2.45 GeV2 show a slight enhancement for π⁻ Production compared to π⁺. The π⁻/π⁺+ ratio for transverse photons exhibits only a small Q2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The σTT/σT ratio also drops rapidly with Q2, qualitatively consistent with s-channel helicity conservation. The π⁻/π⁺ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics.« less

  5. NERSC-ScienceHighlightSlidesSeptember2010.ppt

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

    2010 NERSC Science Highlights NERSC Scientific Accomplishments, Q3CY2010 2 Energy Resources State-of-the-art electronic structure and first-principles molecular- dynamics show why enzymes may be good models for hydrogen production catalysts. (R. Car, Princeton) . Astrophysics A quantum leap in supernova understanding has been obtained by researchers using a 3-D radiation-hydro code on NERSC's Franklin. (Burrows, Princeton; Bell, LBNL) Nuclear Physics NERSC's PDSF and HPSS are the main U.S.

  6. "Table HC4.2 Living Space Characteristics by Renter-Occupied...

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

    "2,500 to 2,999",10.3,9.3,8.6,0.5,"Q","Q","Q" "3,000 to 3,499",6.7,6.1,5.8,0.3,"Q","N","N" "3,500 to 3,999",5.2,4.9,4.7,"Q","Q","Q","N" "4,000 or More",13.3,12.6,12,0.5,"Q","Q",...

  7. "Table HC3.2 Living Space Characteristics by Owner-Occupied...

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

    "2,500 to 2,999",10.3,9.3,8.6,0.5,"Q","Q","Q" "3,000 to 3,499",6.7,6.1,5.8,0.3,"Q","N","N" "3,500 to 3,999",5.2,4.9,4.7,"Q","Q","Q","N" "4,000 or More",13.3,12.6,12,0.5,"Q","Q",...

  8. " Million U.S. Housing Units"

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

    "2,500 to 2,999",10.3,9.4,0.6,"Q","Q","Q" "3,000 to 3,499",6.7,6.3,0.3,"Q","N","N" "3,500 to 3,999",5.2,4.9,"Q","Q","Q","N" "4,000 or More",13.3,12.7,0.6,"Q","Q","N" ...

  9. Monthly energy review, May 1995

    SciTech Connect (OSTI)

    1995-05-24

    Energy production during Feb 95 totaled 5.4 quadrillion Btu (Q), 3.1% over Feb 94. Energy consumption totaled 7.4 Q, 0.7% below Feb 94. Net imports of energy totaled 1.3 Q, 5.6% below Feb 94. This publication is divided into energy overview, energy consumption, petroleum, natural gas, oil and gas resource development, coal, electricity, nuclear energy, energy prices, and international energy.

  10. Innovative Exploration Technologies Maui Hawaii & Glass Buttes, Oregon

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

    Innovative Exploration Technologies Maui Hawaii & Glass Buttes, Oregon Kyle Snyder Ezra Zemach Ormat Nevada Inc. Project Officer: Ava Coy Total Project Funding: Maui-$4.9M, GB- $4.4M April 23rd, 2013 This presentation does not contain any proprietary confidential, or otherwise restricted information. Ulupalakua, Maui Glass Buttes, Oregon 2 | US DOE Geothermal Program eere.energy.gov Maui Overview * Timeline * Project start date 10/29/2009 * Project end date Q3 2013 * Well sites permitting: