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1

Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4  

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

Current Forecast: December 10, 2013; Previous Forecast: November 13, 2013 Current Forecast: December 10, 2013; Previous Forecast: November 13, 2013 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 2011 2012 2013 2014 2011-2012 2012-2013 2013-2014 U.S. Energy Supply U.S. Crude Oil Production (million barrels per day) Current 6.22 6.29 6.42 7.02 7.11 7.29 7.61 7.97 8.26 8.45 8.57 8.86 5.65 6.49 7.50 8.54 14.8% 15.6% 13.8% Previous 6.22 6.30 6.43 7.04 7.13 7.30 7.60 7.91 8.22 8.40 8.52 8.80 5.65 6.50 7.49 8.49 15.0% 15.2% 13.3% Percent Change 0.0% -0.1% -0.2% -0.2% -0.3% -0.1% 0.1% 0.7% 0.5% 0.5% 0.6% 0.6% 0.0% -0.1% 0.1% 0.6% U.S. Dry Natural Gas Production (billion cubic feet per day) Current 65.40 65.49 65.76 66.34 65.78 66.50 67.11 67.88 67.99 67.74 67.37 67.70 62.74 65.75 66.82 67.70 4.8% 1.6% 1.3% Previous 65.40 65.49 65.76 66.34 65.78 66.50 67.11 67.30 67.47 67.41 67.04 67.37 62.74 65.75 66.68 67.32

2

"State","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Sep","Q3 Total","Oct","Nov","Dec","Q4 Total","2002 Total"  

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

Jun","Q2 Total","Jul","Aug","Sep","Q3 Total","Oct","Nov","Dec","Q4 Total","2002 Total" Jun","Q2 Total","Jul","Aug","Sep","Q3 Total","Oct","Nov","Dec","Q4 Total","2002 Total" "Alabama",1595069,1422595,1446039,4463703,1651900,1673270,1619686,4944856,1609758,1743418,1702481,5055657,1618031,1459125,1520148,4597304,19061520 "Alaska",132989,119164,123742,375895,111713,113169,109538,334420,76798,83175,78226,238199,80312,66775,50123,197210,1145724 "Arizona",1158076,1038925,1084980,3281981,1017804,1030975,974342,3023121,988049,1095624,1063939,3147612,1183635,1062729,1104980,3351344,12804058 "Arkansas",978,1085,2107,4170,1565,1582,1524,4671,636,689,971,2296,935,843,871,2649,13786 "Colorado",3163974,2824806,2885394,8874174,2997782,3036576,2869817,8904175,2629615,2915930,3075236,8620781,3004721,2814415,2884793,8703929,35103059

3

After starting with a 12,000-job bang in 2010-Q2, Connecticut's  

E-Print Network [OSTI]

Sales -0.1% State Exports -2.9% Personal Income (est.) +3.2% Coincident GDI +0.6% Indicators of Future GDI +4.1% TAKING STOCK 'TIS THE SEASON? -10 -8 -6 -4 -2 0 2 4 6 8 Retail Construction Q4Q3Q2Q1 CT JOBS

Holsinger, Kent

4

Electric Field How does a charge, q1, exert a force on  

E-Print Network [OSTI]

Electric Field How does a charge, q1, exert a force on another charge, q2, when the charges don't touch? The charge, q1, sets up an electric field in its surrounding space This electric field has both magnitude and direction which determine the magnitude and direction of the force acting on q2 #12;Electric

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

5

"State","Jan","Feb","Mar","Q1 Total","Apr","May","Jun ","Q2 Total","Jul","Aug","Sep","Q3 Total","Oct","Nov","Dec","Q4 Total","2003 Total"  

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

3 Total" 3 Total" "Alabama",1771113,1510892,1622954,4904959,1863504,1845388,1776824,5485716,1600128,1565897,1672632,4838657,1763889,1479114,1734574,4977577,20206909 "Alaska",87443,76405,79754,243602,62928,62232,69581,194741,67907,66760,67789,202456,156990,131143,152391,440524,1081323 "Arizona",1073559,941887,1030496,3045942,943093,932681,884672,2760446,1040168,1016416,1058519,3115103,1107584,941831,1088188,3137603,12059094 "Arkansas",829,426,1561,2816,484,478,264,1226,442,432,494,1368,769,439,946,2154,7564 "Colorado",2846715,2541328,2830992,8219035,2865526,2903720,2827776,8597022,3131374,3268010,3269638,9669022,3014173,2950843,3381090,9346106,35831185 "Illinois",2961000,2440349,2876040,8277389,2706876,2702220,3169886,8578982,2373950,2388551,2344648,7107149,2993442,2346572,2456095,7796109,31759629

6

"State","Jan","Feb","Mar","Q1 Total","Apr","May","Jun ","Q2 Total","Jul","Aug","Sep","Q3 Total","Oct","Nov","Dec","Q4 Total","2004 Total"  

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

4 Total" 4 Total" "Alabama",1725998,1581616,2004066,5311680,1926051,1739300,2099141,5764492,1605125,1654151,1850943,5110219,1976865,2078720,2086665,6142250,22328641 "Alaska",140314,131982,185547,457843,61887,55405,120646,237938,131114,130814,96529,358457,149748,156396,151405,457549,1511787 "Arizona",977250,897698,1100939,2975887,1049375,950831,1069753,3069959,1098199,1113785,977716,3189700,1129140,1195127,1171016,3495283,12730829 "Arkansas",1133,1013,845,2991,679,692,1274,2645,411,400,432,1243,170,166,113,449,7328 "Colorado",3527103,3179582,3398625,10105310,3407363,3451070,3468743,10327176,3293260,3357952,3258228,9909440,3172777,3167266,3188128,9528171,39870097 "Illinois",2888652,2695556,3272892,8857100,2664839,2497528,2930733,8093100,2657588,2695324,2480874,7833786,2322429,2411032,2394081,7127542,31911528

7

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

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

"Arkansas",218,114,136,468,174,172,167,513,253,283,245,781,341,303,157,801,2563 "Colorado",3339797,3246183,3644547,10230527,3101948,3095295,3141507,9338750,3284972,3442912...

8

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

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

901,5222,5790,16913,6096,6383,6653,19132,8430,9527,8169,26126,5636,7084,7786,20506,82677 "Colorado",2732284,2480711,2775220,7988215,3264406,3408511,3417513,10090430,2999471,3278170...

9

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

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

7135,7446,22132,3555,3697,3686,10938,9304,10021,8613,27938,12782,12327,12004,37113,98121 "Colorado",2551829,2353617,2123193,7028639,2286316,2208508,2390122,6884946,2544298,2770090,...

10

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

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

611611,596681,1843797,3813909 "Arkansas",5862,5366,5865,17093,8039,7743,7457,23239,40332 "Colorado",1750313,1873107,1653903,5277323,2284260,1942356,2289442,6516058,11793381...

11

R Measurements at High Q^2  

E-Print Network [OSTI]

Previous Measurements of R at high Q^2 are reviewed. Recent R measurement results, including those from the Beijing Spectrometer Experiment, are described. The present status of R measurements and future measurement possiblities are summarized.

F. A. Harris

2001-06-01T23:59:59.000Z

12

Observations from The EV Project in Q4 2013  

SciTech Connect (OSTI)

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.

John Smart

2014-02-01T23:59:59.000Z

13

Bloo Solar formerly Q1 Nanosystems | Open Energy Information  

Open Energy Info (EERE)

Solar formerly Q1 Nanosystems Jump to: navigation, search Name: Bloo Solar (formerly Q1 Nanosystems) Place: West Sacramento, California Zip: 95691 Sector: Solar Product: String...

14

Minimally non-local nucleon-nucleon potentials in $?$EFT at order $Q^4$  

E-Print Network [OSTI]

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

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

2014-12-19T23:59:59.000Z

15

Prova Scritta di Robotica I 4 Dicembre 2006  

E-Print Network [OSTI]

cartesiane ammesse sono pari a Vmax = 1 m/s e, rispettivamente, Amax = 4 m/s2 . Determinare la legge oraria A4(q3, q4) = 2 R4(q3, q4) 0 Nc4 q3 + Ns4 0T 1 1 A4(q2, q3, q4) = 1 R4(q2, q3, q4) s2(q3 + Ns4) -c2(q3 + Ns4) Nc4 0T 1 0 A4(q1, q2, q3, q4) = 0 R4(q1, q2, q3, q4) Mc1 + c1s2(q3

De Luca, Alessandro

16

Domestic Coal Distribution 2009 Q2 by Origin State: Alabama  

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

Q2 by Origin State: Alabama 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 Generation Coke Plants Industrial Plants Excluding Coke Commercial & Institutional Total Alabama Railroad 875 12 33 - 920 Alabama River 855 - - - 855 Alabama Truck 155 84 230 - 469 Alabama Total 1,885 96 263 - 2,244 Florida Railroad - - 8 - 8 Georgia Railroad 118 - - - 118 Georgia Truck s - 15 - 15 Georgia Total 118 - 15 - 133 Indiana Railroad - 83 - - 83 Indiana Truck 17 34 - - 50 Indiana Total 17 116 - - 133 Kentucky Railroad 83 - - - 83 Pennsylvania Railroad 95 - - - 95 Origin State Total 2,197 212 285 - 2,695 Railroad 1,171 95 40 - 1,305 River 855 - - - 855 Truck 171 118 245 - 534 2 / 58 Domestic Coal Distribution 2009 Q2 by Origin State: Alaska

17

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.

18

FOIA Quarterly Reports (Q2 2013) | Department of Energy  

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

Q2 2013) Q2 2013) FOIA Quarterly Reports (Q2 2013) 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 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

19

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

Open Energy Info (EERE)

Q2) Wind Farm 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 Service Owner Horizon Developer RES/Horizon Energy Purchaser Direct Energy Location Callahan and Shackelford counties TX Coordinates 32.594885°, -99.506464° Loading map... {"minzoom":false,"mappingservice":"googlemaps3","type":"ROADMAP","zoom":14,"types":["ROADMAP","SATELLITE","HYBRID","TERRAIN"],"geoservice":"google","maxzoom":false,"width":"600px","height":"350px","centre":false,"title":"","label":"","icon":"","visitedicon":"","lines":[],"polygons":[],"circles":[],"rectangles":[],"copycoords":false,"static":false,"wmsoverlay":"","layers":[],"controls":["pan","zoom","type","scale","streetview"],"zoomstyle":"DEFAULT","typestyle":"DEFAULT","autoinfowindows":false,"kml":[],"gkml":[],"fusiontables":[],"resizable":false,"tilt":0,"kmlrezoom":false,"poi":true,"imageoverlays":[],"markercluster":false,"searchmarkers":"","locations":[{"text":"","title":"","link":null,"lat":32.594885,"lon":-99.506464,"alt":0,"address":"","icon":"","group":"","inlineLabel":"","visitedicon":""}]}

20

Domestic Coal Distribution 2009 Q1 by Origin State: Alabama  

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

Q1 by Origin State: Alabama Q1 by Origin State: Alabama (1000 Short Tons) 1 / 58 Domestic Coal Distribution 2009 Q1 by Origin State: Alabama (1000 Short Tons) Destination State Transportation Mode Electricity Generation Coke Plants Industrial Plants Excluding Coke Commercial & Institutional Total Alabama Railroad 950 4 84 - 1,038 Alabama River 1,110 - - - 1,110 Alabama Truck 37 170 249 - 456 Alabama Total 2,096 174 333 - 2,603 Florida Railroad - - 22 - 22 Georgia Railroad 45 - - - 45 Georgia Truck s - 20 - 21 Georgia Total 45 - 20 - 65 Hawaii Ocean Vessel s - - - s Indiana Railroad - 78 - - 78 Indiana Truck - 32 - - 32 Indiana Total - 110 - - 110 South Carolina Truck - - 2 - 2 Tennessee Truck - - 1 - 1 Texas Railroad 72 - - - 72 Origin State Total 2,213 284 378 - 2,875 Ocean Vessel s - - - s Railroad 1,066 82 106 - 1,255 River 1,110 - - - 1,110 Truck 37 202 272 - 511 2 / 58

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


21

FOIA Quarterly Reports (Q1 2013) | Department of Energy  

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

Q1 2013) Q1 2013) FOIA Quarterly Reports (Q1 2013) 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 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

22

Domestic Coal Distribution 2009 Q2 by Destination State: Alabama  

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

61 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) Origin State Transportation Mode Electricity Generation Coke Plants Industrial Plants Excluding Coke Commercial & Institutional Total Alabama Railroad 875 12 33 - 920 Alabama River 855 - - - 855 Alabama Truck 155 84 230 - 469 Alabama Total 1,885 96 263 - 2,244 Colorado Railroad 123 - - - 123 Illinois River 145 - - - 145 Indiana River 246 - - - 246 Indiana Truck 37 - - - 37 Indiana Total 283 - - - 283 Kentucky Railroad 426 - 30 - 457 Kentucky (East) Railroad 172 - 30 - 202 Kentucky (West) Railroad 255 - - - 255 Oklahoma Railroad - 6 - - 6 Utah Railroad 30 - - - 30 Virginia Railroad - 14 - - 14 West Virginia Railroad - 75 - -

23

Domestic Coal Distribution 2009 Q1 by Destination State: Alabama  

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

4 4 Domestic Coal Distribution 2009 Q1 by Destination State: Alabama (1000 Short Tons) 1 / 64 Domestic Coal Distribution 2009 Q1 by Destination State: Alabama (1000 Short Tons) Origin State Transportation Mode Electricity Generation Coke Plants Industrial Plants Excluding Coke Commercial & Institutional Total Alabama Railroad 950 4 84 - 1,038 Alabama River 1,110 - - - 1,110 Alabama Truck 37 170 249 - 456 Alabama Total 2,096 174 333 - 2,603 Arkansas Railroad - 6 - - 6 Colorado Railroad 279 - - - 279 Illinois Railroad 11 - - - 11 Illinois River 109 - - - 109 Illinois Total 119 - - - 119 Indiana River 197 - - - 197 Kentucky Railroad 442 - 28 - 471 Kentucky Truck - - 2 - 2 Kentucky Total 442 - 31 - 473 Kentucky (East) Railroad 357 - 28 - 385 Kentucky (East) Truck - - 2 - 2 Kentucky (East)

24

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

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

Advanced Low-Cost Receivers for Parabolic Troughs - FY13 Q2 Advanced Low-Cost Receivers for Parabolic Troughs - FY13 Q2 This document summarizes the progress of this Norwich...

25

Low-Cost, Lightweight Solar Concentrators FY13 Q2 | Department...  

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

FY13 Q2 Low-Cost, Lightweight Solar Concentrators FY13 Q2 This document summarizes the progress of this Jet Propulsion Laboratory project, funded by SunShot, for the second quarter...

26

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

Energy Savers [EERE]

TOTAL ARRA Homes Weatherized thru Q2 2010 8.19.10.xls TOTAL ARRA Homes Weatherized thru Q2 2010 8.19.10.xls TOTAL ARRA Homes Weatherized thru Q2 2010 8.19.10.xls More Documents &...

27

Next Generation Solar Collectors for CSP - FY13 Q1 | Department...  

Office of Environmental Management (EM)

Next Generation Solar Collectors for CSP - FY13 Q1 Next Generation Solar Collectors for CSP - FY13 Q1 This document summarizes the progress of this 3M project, funded by SunShot,...

28

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

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

GA County SRNS SRR WSI *Parsons GA County SRNS SRR WSI *Parsons Amer- esco MOX DOE-SR GA County Total Burke 23 15 4 17 0 24 0 83 Columbia 719 258 101 75 6 148 44 1351 Jefferson 2 3 0 1 0 3 0 9 Lincoln 11 1 2 1 0 4 0 19 McDuffie 10 8 0 5 0 13 2 38 Richmond 508 184 110 117 2 215 34 1170 Screven 20 7 1 6 0 4 0 38 Other 24 12 3 91 0 162 0 292 Total 1317 488 221 313 * 8 573 80 3000 SRS Employee Headcount by County of Residence Q4, FY 13

29

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

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

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

30

Domestic Uranium Production Report - Quarterly - Energy Information  

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

All Nuclear Reports All Nuclear Reports Domestic Uranium Production Report - Quarterly Data for 3rd Quarter 2013 | Release Date: October 31, 2013 | Next Release Date: February 2014 | full report Previous Issues Year: 2013-Q2 2013-Q1 2012-Q4 2012-Q3 2012-Q2 2012-Q1 2011-Q4 2011-Q3 2011-Q2 2011-Q1 2010-Q4 2010-Q3 2010-Q2 2010-Q1 2009-Q4 2009-Q3 2009-Q2 2009-Q1 2008-Q4 2008-Q3 2008-Q2 2008-Q1 Go 3rd Quarter 2013 U.S. production of uranium concentrate in the third quarter 2013 was 1,171,278 pounds U3O8, down 16 percent from the previous quarter and up 12 percent from the third quarter 2012. Third quarter 2013 uranium production is at its highest level since 1999. During the third quarter 2013, U.S. uranium was produced at six U.S. uranium facilities. U.S. Uranium Mill in Production (State)

31

A measurement of $alpha_s(Q^2)$ from the Gross-Llewellyn Smith Sum Rule  

E-Print Network [OSTI]

We extract a set of values for the Gross-Llewellyn Smith sum rule at different values of 4-momentum transfer squared ($Q^{2}$), by combining revised CCFR neutrino data with data from other neutrino deep-inelastic scattering experiments for $1 < Q^2 < 15 GeV^2/c^2$. A comparison with the order $\\alpha^{3}_{s}$ theoretical predictions yields a determination of $\\alpha_{s}$ at the scale of the Z-boson mass of $0.114 \\pm^{.009}_{.012}$. This measurement provides a new and useful test of perturbative QCD at low $Q^2$, because of the low uncertainties in the higher order calculations.

J. H. Kim; D. A. Harris

1998-08-19T23:59:59.000Z

32

On the roughening transition in the Potts model (q=2, 3) in two and three dimensions  

Science Journals Connector (OSTI)

Roughening-respectively depinning-transitions of interfaces between regions...q-state Potts model (q=2, 3) in two and three dimensions. For two dimensions the depinning temperatureT ...

I. Schmidt; W. Pesch

1984-01-01T23:59:59.000Z

33

Shielded Payload Containers Will Enhance the Safety and  

E-Print Network [OSTI]

Drop Test #12;End Drop Test Results · Pre- and post-drop position of SCAs and radial shock absorber configuration in HalfPACT under current design and licensing bases: - 7,600 lb max payload - 30 watts max decay Q-2 Q-3 Q-4 Q-1 Q-2 Q-3 Q-4 2007 2008 2009 Engineering and testing Stakeholder meeting 11/29/07 EPA

34

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Year total  

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

Year total" Year total" "Alabama",1562473,1400113,1447708,4410294,1592661,1584520,1474279,4651460,9061754 "Alaska",102639,95553,102206,300398,151343,155955,134279,441577,741975 "Arizona",626131,579206,619554,1824891,748419,751109,684147,2183675,4008566 "Arkansas",1344,1241,1331,3916,572,572,538,1682,5598 "Colorado",2049961,1815249,1916126,5781336,1708460,1651160,1937762,5297382,11078718 "Illinois",4897036,4449010,4664902,14010948,4596761,4692289,4224673,13513723,27524671 "Indiana",3304230,2985013,3132637,9421880,3242977,3260643,3012840,9516460,18938340 "Kansas",1589,1462,1564,4615,1627,1605,1527,4759,9374 "Kentucky Total",7194068,6511926,6926423,20632417,7065146,7169716,6488303,20723165,41355582

35

Jefferson Lab's results on the Q^2-evolution of moments of spin structure functions  

E-Print Network [OSTI]

We present the recent JLab measurements on moments of spin structure functions at intermediate and low Q^2. The Bjorken sum and Burkhardt-Cottingham sum on the neutron are presented. The later appears to hold. Higher moments (generalized spin polarizabilities and d_2^n) are shown and compared to chiral perturbation theory and lattice QCD respectively.

A. Deur

2005-07-15T23:59:59.000Z

36

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

E-Print Network [OSTI]

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

A. Gardestig

2006-04-16T23:59:59.000Z

37

Applicability of InSAR to tropical volcanoes: insights from Central AmericaQ1  

E-Print Network [OSTI]

volcanoes: insights from Central AmericaQ1 S. K. EBMEIER1*, J. BIGGS2,3, T. A. MATHER1 & F. AMELUNG3 1 COMET+, Department of Earth Sciences, University of Oxford, South Parks Road, Oxford OX1 3AN, UK 2 COMET+, Department rapid in southern Central America where Evergreen broad- leaf vegetation dominates. Land

Biggs, Juliet

38

Moments of the neutron $g_2$ structure function at intermediate $Q^2$  

E-Print Network [OSTI]

We present new experimental results of the $^3$He spin structure function $g_2$ in the resonance region at $Q^2$ values between 1.2 and 3.0 (GeV/c)$^2$. Spin dependent moments of the neutron were then extracted. Our main result, the resonance contribution to the neutron $d_2$ matrix element, was found to be small at $$=2.4 (GeV/c)$^2$ and in agreement with the Lattice QCD calculation. The Burkhardt-Cottingham sum rule for $^3$He and the neutron was tested with the measured data and using the Wandzura-Wilczek relation for the low $x$ unmeasured region. A small deviation was observed at $Q^2$ values between 0.5 and 1.2 (GeV/c)$^2$ for the neutron.

P. Solvignon; N. Liyanage; J. -P. Chen; Seonho Choi; K. Slifer; K. Aniol; T. Averett; W. Boeglin; A. Camsonne; G. D. Cates; C. C. Chang; E. Chudakov; B. Craver; F. Cusanno; A. Deur; D. Dutta; R. Ent; R. Feuerbach; S. Frullani; H. Gao; F. Garibaldi; R. Gilman; C. Glashausser; V. Gorbenko; O. Hansen; D. W. Higinbotham; H. Ibrahim; X. Jiang; M. Jones; A. Kelleher; J. Kelly; C. Keppel; W. Kim; W. Korsch; K. Kramer; G. Kumbartzki; J. J. LeRose; R. Lindgren; B. Ma; D. J. Margazioti; P. Markowitz; K. McCormick; Z. -E. Meziani; R. Michaels; B. Moffit; P. Monaghan; C. Munoz Camacho; K. Paschke; B. Reitz; A. Saha; R. Shneor; J. Singh; V. Sulkosky; A. Tobias; G. M. Urciuoli; K. Wang; K. Wijesooriya; B. Wojtsekhowski; S. Woo; J. -C. Yang; X. Zheng; L. Zhu

2014-03-14T23:59:59.000Z

39

Measurement of the generalized form factors near threshold via ?*p ? n?+ at high Q2  

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

We report the first extraction of the pion-nucleon multipoles near the production threshold for the n?+ 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 4? CEBAF Large Acceptance Spectrometer (CLAS) using a 5.754-GeV electron beam on a proton target. The differential cross section and the ?-N multipole E0+/GD were measured 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.

Park, K; Adhikari, K P; Adikaram, D; Anghinolfi, M; Baghdasaryan, H; Ball, J; Battaglieri, M; Batourine, V; Bedlinskiy, I; Bennett, R P; Biselli, A S; Bookwalter, C; Boiarinov, S; Branford, D; Briscoe, W J; Brooks, W K; Burkert, V D; Carman, D S; Celentano, A; Chandavar, S; Charles, G; Cole, P L; Contalbrigo, M; Crede, V; D'Angelo, A; Daniel, A; Dashyan, N; De Vita, R; De Sanctis, E; Deur, A; Djalali, C; Doughty, D; Dupre, R; El Alaoui, A; El Fassi, L; Euginio, P; Fedotov, G; Fradi, A; Gabrielyan, M Y; Gevorgyan, N; Gilfoyle, G P; Giovanetti, K L; Girod, F X; Goetz, J T; Gohn, W; Golovatch, E; Graham, L; Griffioen, K A; Guidal, M; Guo, L; Hafidi, K; Hakobyan, H; Hanretty, C; Heddle, D; Hicks, K; Holtrop, M; Ilieva, Y; Ireland, D G; Ishkhanov, B S; Isupov, E L; Jenkins, D; Jo, H S; Joo, K; Khandaker, M; Khertarpal, P; Kim, A; Kim, W; Klein, F J; Kubarovsky, A; Kubarovsky, V; Kuhn, S E; Kuleshov, S V; Kvaltine, N D; Livingston, K; Lu, H Y; MacGregor, J D; Markov, N; Mayer, M; McKinnon, B; Mestayer, M D; Meyer, C A; Mineeva, T; Mirazita, M; Mokeev, V; Moutarde, H; Munevar, E; Nadel-Turonski, P; Nasseripour, R; Niccolai, S; Niculescu, G; Niculescu, I; Osipenko, M; Ostrovidov, A I; Paolone, M; Pappalardo, L; Paremuzyan, R; Park, S; Anefalos Pereira, S; Phelps, E; Pisano, S; Pogorelko, O; Pozdniakov, S; Price, J W; Procureur, S; Prok, Y; Ricco, G; Rimal, D; Ripani, M; Ritchie, B G; Rosner, G; Rossi, P; Sabati ee, F; Saini, M S; Salgado, C; Schott, D; Schumacher, R A; Seraydaryan, H; Sharabian, Y G; Smith, E S; Smith, G D; Sober, D I; Sokhan, D; Stepanyan, S S; Stepanyan, S; Stoler, P; Strakovsky, I I; Strauch, S; Taiuti, M; Tang, W; Taylor, C E; Tian, Y; Tkachenko, S; Trivedi, A; Ungaro, M; Vernarsky, B; Vlassov, A V; Voutier, E; Watts, D P; Weygand, D P; Wood, M H; Zachariou, N; Zhao, B; Zhao, Z W

2012-03-26T23:59:59.000Z

40

Measurement of the proton structure function $F_L(x,Q^2)$ at low x  

E-Print Network [OSTI]

A first measurement is reported of the longitudinal proton structure function F_L(x,Q^2) at the ep collider HERA. It is based on inclusive deep inelastic e^+p scattering cross section measurements with a positron beam energy of 27.5 GeV and proton beam energies of 920, 575 and 460 GeV. Employing the energy dependence of the cross section, F_L is measured in a range of squared four-momentum transfers 12 < Q^2 < 90 GeV^2 and low Bjorken x 0.00024 < x < 0.0036. The F_L values agree with higher order QCD calculations based on parton densities obtained using cross section data previously measured at HERA.

Aaron, F D; Andreev, V; Antunovic, B; Aplin, S; Asmone, A; Astvatsatourov, A; Bacchetta, A; Backovic, S; Baghdasaryan, A; Baranov, P; Barrelet, E; Bartel, Wulfrin; Beckingham, M; Begzsuren, K; Behnke, O; Belousov, A; Berger, N; Bizot, J C; Boenig, M O; Boudry, V; Bozovic-Jelisavcic, I; Bracinik, J; Brandt, G; Brinkmann, M; Brisson, V; Bruncko, D; Bunyatyan, A; Buschhorn, G; Bystritskaya, L; Campbell, A J; Cantun Avila, K B; Cassol-Brunner, F; Cerny, K; Cerny, V; Chekelian, V; Cholewa, A; Contreras, J G; Coughlan, J A; Cozzika, G; Cvach, J; Dainton, J B; Daum, K; de Roeck, A; De Wolf, E A; Del Degan, M; Delcourt, B; Delvax, J; Dek, M; Diaconu, C; Dodonov, V; Dossanov, A; Dubak, A; Eckerlin, G; Efremenko, V; Egli, S; Eliseev, A; Elsen, E; Essenov, S; Falkiewicz, A; Faulkner, P J W; Favart, L; Fedotov, A; Felst, R; Feltesse, J; Ferencei, J; Finke, L; Fleischer, M; Fomenko, A; Gabathuler, E; Gayler, J; Ghazaryan, S; Glazov, A; Glushkov, I; Grlich, L; Goettlich, M; Gogitidze, N; Gouzevitch, M; Grab, C; Greenshaw, T; Grell, B R; Grindhammer, G; Habib, S; Haidt, D; Hansson, M; Helebrant, C; Henderson, R C W; Henschel, H; Herrera-Corral, G; Hildebrandt, M; Hiller, K H; Hoffmann, D; Horisberger, R; Hovhannisyan, A; Hreus, T; Jacquet, M; Janssen, M E; Janssen, X; Jemanov, V; Jhnson, D P; Jung, A W; Jung, H; Jnsson, L; Kapichine, M; Katzy, J; Kenyon, I R; Kiesling, C; Klein, M; Kleinwort, C; Klimkovich, T; Kluge, T; Knutsson, A; Kogler, R; Korbel, V; Kostka, P; Krmer, M; Krastev, K; Kretzschmar, J; Kropivnitskaya, A; Krger, K; Kutak, K; Landon, M P J; Lange, W; Lastoviicka-Medin, G; Laycock, P; Lebedev, A; Leibenguth, G; Lendermann, V; Levonian, S; Li, G; Lipka, K; Liptaj, A; List, B; List, J; Loktionova, N; Lpez-Fernandez, R; Lubimov, V; Lucaci-Timoce, A I; Lytkin, L; Makankine, A; Malinovski, E; Marage, P; Marti, Ll; Martyn, H U; Maxfield, S J; Mehta, A; Meier, K; Meyer, A B; Meyer, H; Meyer, J; Michels, V; Mikocki, S; Milcewicz-Mika, I; Moreau, F; Morozov, A; Morris, J V; Mozer, M U; Mudrinic, M; Murn, P; Mller, K; Nankov, K; Naroska, B; Naumann, Th; Newman, P R; Niebuhr, C; Nikiforov, A; Nowak, G; Nowak, K; Nozicka, M; Olivier, B; Olsson, J E; Osman, S; Ozerov, D; Palichik, V; Panagoulias, I; Pandurovic, M; Papadopoulou, Th; Pascaud, C; Patel, G D; Pejchal, O; Peng, H; Prez, E; Petrukhin, A; Picuric, I; Piec, S; Pitzl, D; Placakyte, R; Polifka, R; Povh, B; Preda, T; Radescu, V; Rahmat, A J; Raicevic, N; Raspiareza, A; Ravdandorj, T; Reimer, P; Rizvi, E; Robmann, P; Roland, B; Roosen, R; Rostovtsev, A; Rotaru, M; Ruiz Tabasco, J E; Rurikova, Z; Rusakov, S; Salek, D; Salvaire, F; Sankey, D P C; Sauter, M; Sauvan, E; Schmidt, S; Schmitt, S; Schmitz, C; Schoeffel, L; Schultz-Coulon, H C; Schning, A; Sefkow, F; Shaw-West, R N; Shevyakov, I; Shtarkov, L N; Shushkevich, S; Sloan, T; Smiljanic, I; Smirnov, P; Soloviev, Yu; Sopicki, P; South, D; Spaskov, V; Specka, A; Staykova, Z; Steder, M; Stella, B; Straumann, U; Sunar, D; Sykora, T; Tchoulakov, V; Thompson, G; Thompson, P D; Toll, T; Tomasz, F; Tran, T H; Traynor, D; Trinh, T N; Trul, P; Tsakov, I; Tseepeldorj, B; Tsurin, I; Turnau, J; Tzamariudaki, E; Urban, K; Valkrov, A; Valle, C; Van Mechelen, P; Vargas-Trevino, A; Vazdik, Y; Vinokurova, S; Volchinski, V; Wegener, D; Wessels, M; Wissing, Ch; Wnsch, E; Yeganov, V; Zhang, Z; Zhelezov, A; Zhokin, A; Zhu, Y C; Zimmermann, T; Zohrabyan, H; Zomer, F; Zcek, J; Zlesk, J; De Boer, Y

2008-01-01T23:59:59.000Z

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41

Jet Production in ep Collisions at High $Q^2$ and Determination of $\\alpha_s$  

E-Print Network [OSTI]

The production of jets is studied in deep-inelastic ep scattering at large negative four momentum transfer squared 150<Q^2<15000 GeV^2 using HERA data taken in 1999-2007, corresponding to an integrated luminosity of 395 pb^-1. Inclusive jet, 2-jet and 3-jet cross sections, normalised to the neutral current deep-inelastic scattering cross sections, are measured as functions of Q^2, jet transverse momentum and proton momentum fraction. The measurements are well described by perturbative QCD calculations at next-to-leading order corrected for hadronisation effects. The strong coupling as determined from these measurements is alpha_s(M_Z) = 0.1168 +/-0.0007 (exp.) +0.0046/-0.0030 (th.) +/-0.0016(pdf).

Aaron, FD; Alimujiang, K; Andreev, V; Antunovic, B; Asmone, A; Backovic, S; Baghdasaryan, A; Barrelet, E; Bartel, W; Begzsuren, K; Belousov, A; Bizot, J C; Boudry, V; Bozovic-Jelisavcic, I; Bracinik, J; Brandt, G; Brinkmann, M; Brisson, V; Bruncko, D; Bunyatyan, A; Buschhorn, G; Bystritskaya, L; Campbell, A J; Cantun Avila, K B; Cassol-Brunner, F; Cerny, K; Cerny, V; Chekelian, V; Cholewa, A; Contreras, J G; Coughlan, J A; Cozzika, G; Cvach, J; Dainton, J B; Daum, K; Deak, M; de Boer, Y; Delcourt, B; Del Degan, M; Delvax, J; De Roeck, A; De Wolf, E A; Diaconu, C; Dodonov, V; Dossanov, A; Dubak, A; Eckerlin, G; Efremenko, V; Egli, S; Eliseev, A; Elsen, E; Falkiewicz, A; Faulkner, P J W; Favart, L; Fedotov, A; Felst, R; Feltesse, J; Ferencei, J; Fischer, D -J; Fleischer, M; Fomenko, A; Gabathuler, E; Gayler, J; Ghazaryan, Samvel; Glazov, A; Glushkov, I; Goerlich, L; Gogitidze, N; Gouzevitch, M; Grab, C; Greenshaw, T; Grell, B R; Grindhammer, G; Habib, S; Haidt, D; Helebrant, C; Henderson, R C W; Hennekemper, E; Henschel, H; Herbst, M; Herrera, G; Hildebrandt, M; Hiller, K H; Hoffmann, D; Horisberger, R; Hreus, T; Jacquet, M; Janssen, M E; Janssen, X; Jemanov, V; Jonsson, L; Jung, Andreas Werner; Jung, H; Kapichine, M; Katzy, J; Kenyon, I R; Kiesling, C; Klein, M; Kleinwort, C; Kluge, T; Knutsson, A; Kogler, R; Korbel, V; Kostka, P; Kraemer, M; Krastev, K; Kretzschmar, J; Kropivnitskaya, A; Kruger, K; Kutak, K; Landon, M P J; Lange, W; Lastovicka-Medin, G; Laycock, P; Lebedev, A; Leibenguth, G; Lendermann, V; Levonian, S; Li, G; Lipka, K; Liptaj, A; List, B; List, J; Loktionova, N; Lopez-Fernandez, R; Lubimov, V; Lytkin, L; Makankine, A; Malinovski, E; Marage, P; Marti, Ll; Martyn, H -U; Maxfield, S J; Mehta, A; Meyer, A B; Meyer, H; Meyer, H; Meyer, J; Michels, V; Mikocki, S; Milcewicz-Mika, I; Moreau, F; Morozov, A; Morris, J V; Mozer, Matthias Ulrich; Mudrinic, M; Muller, K; Murin, P; Naroska, B; Naumann, Th; Newman, P R; Niebuhr, C; Nikiforov, A; Nowak, G; Nowak, K; Nozicka, M; Olivier, B; Olsson, J E; Osman, S; Ozerov, D; Palichik, V; Panagoulias, I; Pandurovic, M; Papadopoulou, Th; Pascaud, C; Patel, G D; Pejchal, O; Perez, E; Petrukhin, A; Picuric, I; Piec, S; Pitzl, D; Placakyte, R; Pokorny, B; Polifka, R; Povh, B; Preda, T; Radescu, V; Rahmat, A J; Raicevic, N; Raspiareza, A; Ravdandorj, T; Reimer, P; Rizvi, E; Robmann, P; Roland, B; Roosen, R; Rostovtsev, A; Rotaru, M; Ruiz Tabasco, J E; Rurikova, Z; Rusakov, S; Salek, D; Sankey, D P C; Sauter, M; Sauvan, E; Schmitt, S; Schmitz, C; Schoeffel, L; Schoning, A; Schultz-Coulon, H -C; Sefkow, F; Shaw-West, R N; Sheviakov, I; Shtarkov, L N; Shushkevich, S; Sloan, T; Smiljanic, Ivan; Soloviev, Y; Sopicki, P; South, D; Spaskov, V; Specka, Arnd E; Staykova, Z; Steder, M; Stella, B; Stoicea, G; Straumann, U; Sunar, D; Sykora, T; Tchoulakov, V; Thompson, G; Thompson, P D; Toll, T; Tomasz, F; Tran, T H; Traynor, D; Trinh, T N; Truol, P; Tsakov, I; Tseepeldorj, B; Turnau, J; Urban, K; Valkarova, A; Vallee, C; Van Mechelen, P; Vargas Trevino, A; Vazdik, Y; Vinokurova, S; Volchinski, V; von den Driesch, M; Wegener, D; Wissing, Ch; Wunsch, E; Zacek, J; Zalesak, J; Zhang, Z; Zhokin, A; Zimmermann, T; Zohrabyan, H; Zomer, F; Zus, R

2010-01-01T23:59:59.000Z

42

Jet Production in ep Collisions at Low Q^2 and Determination of $\\alpha_{s}$  

E-Print Network [OSTI]

The production of jets is studied in deep-inelastic e+p scattering at low negative four momentum transfer squared 5<Q^2<100 GeV^2 and at inelasticity 0.2Q^2 and jet transverse momentum. The 2-jet cross section is also measured as a function of the proton momentum fraction xi. The measurements are well described by perturbative quantum chromodynamics at next-to-leading order corrected for hadronisation effects and are subsequently used to extract the strong coupling alpha_s.

Aaron, FD; Alexa, C; Andreev, V; Antunovic, B; Backovic, S; Baghdasaryan, A; Barrelet, E; Bartel, W; Begzsuren, K; Belousov, A; Bizot, J C; Boudry, V; Bozovic-Jelisavcic, I; Bracinik, J; Brandt, G; Brinkmann, M; Brisson, V; Bruncko, D; Bunyatyan, A; Buschhorn, G; Bystritskaya, L; Campbell, A J; Cantun Avila, K B; Cerny, K; Cerny, V; Chekelian, V; Cholewa, A; Contreras, J G; Coughlan, J A; Cozzika, G; Cvach, J; Dainton, J B; Daum, K; Deak, M; Delcourt, B; Delvax, J; De Wolf, E A; Diaconu, C; Dodonov, V; Dossanov, A; Dubak, A; Eckerlin, G; Efremenko, V; Egli, S; Eliseev, A; Elsen, E; Falkiewicz, A; Favart, L; Fedotov, A; Felst, R; Feltesse, J; Ferencei, J; Fischer, D J; Fleischer, M; Fomenko, A; Gabathuler, E; Gayler, J; Ghazaryan, Samvel; Glazov, A; Glushkov, I; Goerlich, L; Gogitidze, N; Gouzevitch, M; Grab, C; Greenshaw, T; Grell, B R; Grindhammer, G; Habib, S; Haidt, D; Helebrant, C; Henderson, R C W; Hennekemper, E; Henschel, H; Herbst, M; Herrera, G; Hildebrandt, M; Hiller, K H; Hoffmann, D; Horisberger, R; Hreus, T; Jacquet, M; Janssen, X; Jonsson, L; Jung, A W; Jung, H; Kapichine, M; Katzy, J; Kenyon, I R; Kiesling, C; Klein, M; Kleinwort, C; Kluge, T; Knutsson, A; Kogler, R; Kosior, E; Kostka, P; Kraemer, M; Krastev, K; Kretzschmar, J; Kropivnitskaya, A; Kruger, K; Kutak, K; Landon, M P J; Lange, W; Lastovicka-Medin, G; Laycock, P; Lebedev, A; Lendermann, V; Levonian, S; Li, G; Lipka, K; Liptaj, A; List, B; List, J; Loktionova, N; Lopez-Fernandez, R; Lubimov, V; Makankine, A; Malinovski, E; Marage, P; Marti, Ll; Martyn, H U; Maxfield, S J; Mehta, A; Meyer, A B; Meyer, H; Meyer, H; Meyer, J; Mikocki, S; Milcewicz-Mika, I; Moreau, F; Morozov, A; Morris, J V; Mozer, M U; Mudrinic, M; Muller, K; Murin, P; Naumann, Th; Newman, P R; Niebuhr, C; Nikiforov, A; Nikitin, D; Nowak, G; Nowak, K; Olsson, J E; Osman, S; Ozerov, D; Palichik, V; Panagoulias, I; Pandurovic, M; Papadopoulou, Th; Pascaud, C; Patel, G D; Pejchal, O; Perez, E; Petrukhin, A; Picuric, I; Piec, S; Pitzl, D; Placakyte, R; Pokorny, B; Polifka, R; Povh, B; Radescu, V; Rahmat, A J; Raicevic, N; Raspiareza, A; Ravdandorj, T; Reimer, P; Rizvi, E; Robmann, P; Roland, B; Roosen, R; Rostovtsev, A; Rotaru, M; Tabasco, J E Ruiz; Rusakov, S; Salek, D; Sankey, D P C; Sauter, M; Sauvan, E; Schmitt, S; Schoeffel, L; Schoning, A; Schultz-Coulon, H C; Sefkow, F; Shaw-West, R N; Shtarkov, L N; Shushkevich, S; Sloan, T; Smiljanic, Ivan; Soloviev, Y; Sopicki, P; South, D; Spaskov, V; Specka, A; Staykova, Z; Steder, M; Stella, B; Stoicea, G; Straumann, U; Sunar, D; Sykora, T; Tchoulakov, V; Thompson, G; Thompson, P D; Toll, T; Tomasz, F; Tran, T H; Traynor, D; Trinh, T N; Truol, P; Tsakov, I; Tseepeldorj, B; Turnau, J; Urban, K; Valkarova, A; Vallee, C; Van Mechelen, P; Trevino, A Vargas; Vazdik, Y; Vinokurova, S; Volchinski, V; von den Driesch, M; Wegener, D; Wissing, Ch; Wunsch, E; Zacek, J; Zalesak, J; Zhang, Z; Zhokin, A; Zimmermann, T; Zohrabyan, H; Zomer, F

2010-01-01T23:59:59.000Z

43

The Mathieu group M12 and the M13 game  

E-Print Network [OSTI]

). The permutation induced by the entire path is (0 8)(7 12) (1 8)(4 9) (1 12)(5 10) (6 12)(3 9) (0 6)(4 5) = (1 7 12 6 8)(3 4 10 5 9). Two paths are called equivalent if they induce the same permutation. We readily check that if p, q, r are collinear..., the points q1, q2, q3, q4 form an oval. Thus we may adopt the labelling (2.1), with q5 = q1q2 ? q3q4 = r1, q6 = q1q3 ? q2q4 = r2, y = s12. If s12 = 0, then the paths [s12, r2, s23] and [s12, r3, r1, s14] induce the permuta- tions ? = (s12 s23 r2)(r3 s34)(r1 s...

Conway, John H.; Elkies, Noam D.; Martin, Jeremy L.

2006-01-01T23:59:59.000Z

44

Quarterly SSP Experiment Summary-FY13-1Q 1  

National Nuclear Security Administration (NNSA)

3-1Q 1 3-1Q 1 Summary of Experiments Conducted in Support of Stockpile Stewardship January 2013 The U.S. Stockpile Stewardship Program is a robust program of scientific inquiry used to sustain and assess the nuclear weapons stockpile without the use of underground nuclear tests. The experiments carried out within the program are used in combination with Advanced Simulation and Computing (ASC) to continually assess the stockpile to ensure it is safe, secure, and effective. (For links to the ASC program, see: http://nnsa.energy.gov/asc) For a link to the Nuclear Posture Review 2010, see: http://www.defense.gov/npr/docs/2010%20nuclear%20posture%20review%20report.pdf . An extraordinary set of science, technology, and engineering (ST&E) facilities have been established and are active everyday in support of the

45

Flavor decomposition of the nucleon electromagnetic form factors at low $Q^2$  

E-Print Network [OSTI]

The spatial distribution of charge and magnetization within the proton is encoded in the elastic form factors. These have been precisely measured in elastic electron scattering, and the combination of proton and neutron form factors allows for the separation of the up- and down-quark contributions. In this work, we extract the proton and neutron form factors from world's data with an emphasis on precise new data covering the low-momentum region, which is sensitive to the large-scale structure of the nucleon. From these, we separate the up- and down-quark contributions to the proton form factors. We combine cross section and polarization measurements of elastic electron-proton scattering to separate the proton form factors and two-photon exchange (TPE) contributions. We combine the proton form factors with parameterization of the neutron form factor data and uncertainties to separate the up- and down-quark contributions to the proton's charge and magnetic form factors. The extracted TPE corrections are compared to previous phenomenological extractions, TPE calculations, and direct measurements from the comparison of electron and positron scattering. The flavor-separated form factors are extracted and compared to models of the nucleon structure. With the inclusion of the precise new data, the extracted TPE contributions show a clear change ofsign at low $Q^2$, necessary to explain the high-$Q^2$ form factor discrepancy while being consistent with the known $Q^2 \\to 0$ limit. We find that the new Mainz data yield a significantly different result for the proton magnetic form factor and its flavor-separated contributions. We also observe that the RMS radius of both the up- and down-quark distributions are smaller than the RMS charge radius of the proton.

I. A. Qattan; J. Arrington; A. Alsaad

2015-02-10T23:59:59.000Z

46

Electroproduction of $\\phi(1020)$ Mesons at High $Q^2$ with CLAS  

SciTech Connect (OSTI)

http://dx.doi.org/10.1103/PhysRevC.78.025210
Electroproduction of exclusive $\\phi$ vector mesons has been studied with the CLAS detector in the kinematical range $1.6\\leq Q^2\\leq 3.8$ GeV$^{2}$, $0.0\\leq t^{\\prime}\\leq 3.6$ GeV$^{2}$, and $2.0\\leq W\\leq 3.0$ GeV. The scaling exponent for the total cross section as $1/(Q^2+M_{\\phi}^2)^n$ was determined to be $n=2.49\\pm 0.33$. The slope of the four-momentum transfer $t'$ distribution is $b_{\\phi}=0.98 \\pm 0.17$ GeV$^{-2}$. The data are consistent with the assumption of s-channel helicity conservation (SCHC). Under this assumption, we determine the ratio of longitudinal to transverse cross sections to be $R=0.86 \\pm 0.24$. A 2-gluon exchange model is able to reproduce the main features of the data.

Santoro, Joseph; Smith, Elton; Garcon, Michel; Guidal, Michel; Laget, Jean; Weiss, Christian; Adams, Gary; Amaryan, Moscov; Amaryan, Moskov; Anghinolfi, Marco; Asryan, Gegham; Audit, Gerard; Avagyan, Harutyun; Baghdasaryan, Hovhannes; Baillie, Nathan; Ball, J.P.; Ball, Jacques; Ball, J.P.; Ball, Jacques; Ball, James; Baltzell, Nathan; Barrow, Steve; Battaglieri, Marco; Bedlinskiy, Ivan; Bektasoglu, Mehmet; Bellis, Matthew; Benmouna, Nawal; Berman, Barry; Biselli, Angela; Blaszczyk, Lukasz; Bonner, Billy; Bookwalter, Craig; Bouchigny, Sylvain; Bouchigny, Sylvain; Bradford, Robert; Branford, Derek; Briscoe, William; Brooks, William; Bultmann, S.; Bueltmann, Stephen; Bultmann, S.; Bueltmann, Stephen; Burkert, Volker; Butuceanu, Cornel; Calarco, John; Careccia, Sharon; Carman, Daniel; Casey, Liam; Cazes, Antoine; Chen, Shifeng; Cheng, Lu; Cole, Philip; Collins, Patrick; Coltharp, Philip; Cords, Dieter; Corvisiero, Pietro; Crabb, Donald; Crannell, Hall; Crede, Volker; Cummings, John; Dale, Daniel; Dashyan, Natalya; De Masi, Rita; De Sanctis, Enzo; De Vita, Raffaella; Degtiarenko, Pavel; Denizli, Haluk; Dennis, Lawrence; Deur, Alexandre; Dhamija, Seema; Dharmawardane, Kahanawita; Dhuga, Kalvir; Dickson, Richard; Djalali, Chaden; Dodge, Gail; Doughty, David; Dugger, Michael; Dytman, Steven; Dzyubak, Oleksandr; Egiyan, Hovanes; Egiyan, Kim; Elfassi, Lamiaa; Elouadrhiri, Latifa; Eugenio, Paul; Fatemi, Renee; Fedotov, Gleb; Feuerbach, Robert; Ficenec, John; Forest, Tony; Fradi, Ahmed; Funsten, Herbert; Gavalian, Gagik; Gevorgyan, Nerses; Gilfoyle, Gerard; Giovanetti, Kevin; Girod, Francois-Xavier; Goetz, John; Gohn, Wesley; Gordon, Christopher; Gothe, Ralf; Graham, Lewis; Griffioen, Keith; Guillo, Matthieu; Guler, Nevzat; Guo, Lei; Gyurjyan, Vardan; Hadjidakis, Cynthia; Hafidi, Kawtar; Hakobyan, Hayk; Hanretty, Charles; Hardie, John; Hassall, Neil; Heddle, David; Hersman, F.; Hicks, Kenneth; Hleiqawi, Ishaq; Holtrop, Maurik; Hyde, Charles; Ilieva, Yordanka; Ireland, David; Ishkhanov, Boris; Isupov, Evgeny; Ito, Mark; Jenkins, David; Jo, Hyon-Suk; Johnstone, John; Joo, Kyungseon; Juengst, Henry; Kalantarians, Narbe; Keller, Dustin; Kellie, James; Khandaker, Mahbubul; Kim, Wooyoung; Klein, Andreas; Klein, Franz; Klimenko, Alexei; Kossov, Mikhail; Krahn, Zebulun; Kramer, Laird; Kubarovsky, Valery; Kuhn, Joachim; Kuhn, Sebastian; Kuleshov, Sergey; Kuznetsov, Viacheslav; Lachniet, Jeff; Langheinrich, Jorn; Lawrence, David; Livingston, Kenneth; Lu, Haiyun; MacCormick, Marion; Marchand, Claude; Markov, Nikolai; Mattione, Paul; McAleer, Simeon; McKinnon, Bryan; McNabb, John; Mecking, Bernhard; Mehrabyan, Surik; Melone, Joseph; Mestayer, Mac; Meyer, Curtis; Mibe, Tsutomu; Mikhaylov, Konstantin; Minehart, Ralph; Mirazita, Marco; Miskimen, Rory; Mokeev, Viktor; Morand, Ludyvine; Moreno, Brahim; Moriya, Kei; Morrow, Steven; Moteabbed, Maryam; Mueller, James; Munevar Espitia, Edwin; Mutchler, Gordon; Nadel-Turonski, Pawel; Nasseripour, Rakhsha; Niccolai, Silvia; Niculescu, Gabriel; Niculescu, Maria-Ioana; Niczyporuk, Bogdan; Niroula, Megh; Niyazov, Rustam; Nozar, Mina; O'Rielly, Grant; Osipenko, Mikhail; Ostrovidov, Alexander; Park, Kijun; Park, Sungkyun; Pasyuk, Evgueni; Paterson, Craig; Pereira, Sergio; Philips, Sasha; Pierce, Joshua; Pivnyuk, Nikolay; Pocanic, Dinko; Pogorelko, Oleg; Popa, Iulian; Pozdnyakov, Sergey; Preedom, Barry; Price, John; Procureur, Sebastien; Prok, Yelena; Protopopescu, Dan; Qin, Liming; Raue, Brian; Riccardi, Gregory; Ricco, Giovanni; Ripani, Marco; Ritchie, Barry; Rosner, Guenther; Rossi, Patrizia; Sabatie, Franck; Saini, Mukesh; Salamanca, Julian; Salgado, Carlos; Sapunenko, Vladimir; Schott, Diane; Schumacher, Reinhard; Serov, Vladimir; Sharabian, Youri; Sharov, Dmitri; Shvedunov, Nikolay; Skabelin, Alexander; Smith, Lee; Sober, Daniel; Sokhan, Daria; Stavinsky, Aleksey; Stepanyan, Samuel; Stepanyan, Stepan; Stokes, Burnham; Stoler, Paul; Strakovski, Igor; Strauch, Steffen; Taiuti, Mauro; Tedeschi, David; Tkabladze, A

2008-08-01T23:59:59.000Z

47

2012_Q4  

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

2 2 - Visit us at www.lm.doe.gov Welcome to the October-December 2012 issue of the U.S. Department of Energy (DOE) Office of Legacy Management (LM) . This publication is designed to provide a Program Update status of activities within LM. Please direct all comments and inquiries to . lm@hq.doe.gov Program Update Legacy Management The U.S. Department of Energy Office of Legacy Management has completed the stakeholder satisfaction survey. Thanks to everyone who participated in the survey. We are in the process of reviewing your responses in order to address your comments, suggestions, and concerns. The summary survey report will be available on the LM website in January 2013. v Goal 2 LM Communication and Stakeholder Satisfaction Independent Survey Goal 1 Saw What? Saw-Whet!

48

2013_Q4.indd  

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

Update Update Welcome to the October-December 2013 issue of the U.S. Department of Energy (DOE) Offi ce of Legacy Management (LM) 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. October-December 2013 Visit us at http://energy.gov/lm/ Goal 4 Agencies Assist LM to Develop Reports on Defense-Related Uranium Mines The U.S. Department of Energy (DOE) Offi ce of Legacy Management (LM) has made substantial progress researching and consulting with the U.S. Environmental Protection Agency (EPA), the U.S. Department of the Interior (DOI), other relevant federal agencies, affected states and tribes, and the interested public to obtain data and other technical information that will inform the Report to Congress

49

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

E-Print Network [OSTI]

The process $ep \\to e^{\\prime}p^{\\prime}\\pi^0$ has been measured at $Q^2$ = 6.4 and 7.7 GeV/c$^2$)$^2$ 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

A. N. Villano; P. Stoler; P. E. Bosted; S. H. Connell; M. M. Dalton; M. K. Jones; V. Kubarovsky; G. S Adams; A. Ahmidouch; J. Arrington; R. Asaturyan; O. K. Baker; H. Breuer; M. E. Christy; S. Danagoulian; D. Day; J. A. Dunne; D. Dutta; R. Ent; H. C. Fenker; V. V. Frolov; L. Gan; D. Gaskell; W. Hinton; R. J. Holt; T. Horn; G. M. Huber; K. Joo; N. Kalantarians; C. E. Keppel; Y. Li; A. Lung; D. Mack; S. Malace; P. Markowitz; D. G. Meekins; H. Mkrtchyan; J. Napolitano; G. Niculescu; I. Niculescu; D. H. Potterveld; Paul E. Reimer; J. Reinhold; J. Roche; S. E. Rock; G. R. Smith; S. Stepanyan; V. Tadevosyan; V. Tvaskis; M. Ungaro; A. Uzzle; S. Vidakovic; F. R. Wesselmann; B. Wojtsekhowski; S. A. Wood; L. Yuan; X. Zheng; H. Zhu

2009-09-26T23:59:59.000Z

50

Strangeness Production at low $Q^2$ in Deep-Inelastic ep Scattering at HERA  

E-Print Network [OSTI]

The production of neutral strange hadrons is investigated using deep-inelastic scattering events measured with the H1 detector at HERA. The measurements are made in the phase space defined by the negative four-momentum transfer squared of the photon 2 < Q^2 < 100 GeV^2 and the inelasticity 0.1 < y < 0.6. The K_s and Lambda production cross sections and their ratios are determined. K_s production is compared to the production of charged particles in the same region of phase space. The Lambda - anti-Lambda asymmetry is also measured and found to be consistent with zero. Predictions of leading order Monte Carlo programs are compared to the data.

Aaron, F D; Andreev, V; Antunovic, B; Aplin, S; Asmone, A; Astvatsatourov, A; Bacchetta, A; Backovic, S; Baghdasaryan, A; Barrelet, E; Bartel, W; Beckingham, M; Begzsuren, K; Behnke, O; Belousov, A; Berger, N; Bizot, J C; Boenig, M O; Boudry, V; Bozovic-Jelisavcic, I; Bracinik, J; Brandt, G; Brinkmann, M; Brisson, V; Bruncko, D; Bunyatyan, A; Buschhorn, G; Bystritskaya, L; Campbell, A J; Cantun Avila, K B; Cassol-Brunner, F; Cerny, K; Cerny, V; Chekelian, V; Cholewa, A; Contreras, J G; Coughlan, J A; Cozzika, G; Cvach, J; Dainton, J B; Daum, K; Deak, M; de Boer, Y; Delcourt, B; Del Degan, M; Delvax, J; De Roeck, A; De Wolf, E A; Diaconu, C; Dodonov, V; Dossanov, A; Dubak, A; Eckerlin, G; Efremenko, V; Egli, S; Eichler, R; Eliseev, A; Elsen, E; Essenov, S; Falkiewicz, A; Faulkner, P J W; Favart, L; Fedotov, A; Felst, R; Feltesse, J; Ferencei, J; Fleischer, M; Fomenko, A; Gabathuler, E; Gayler, J; Ghazaryan, S; Glazov, A; Glushkov, I; Goerlich, L; Goettlich, M; Gogitidze, N; Gouzevitch, M; Grab, C; Greenshaw, T; Grell, B R; Grindhammer, G; Habib, S; Haidt, D; Hansson, M; Helebrant, C; Henderson, R C W; Hennekemper, E; Henschel, H; Herrera, G; Hildebrandt, M; Hiller, K H; Hoffmann, D; Horisberger, R; Hovhannisyan, A; Hreus, T; Jacquet, M; Janssen, M E; Janssen, X; Jemanov, V; Jonsson, L; Jung, Andreas Werner; Jung, H; Kapichine, M; Katzy, J; Kenyon, I R; Kiesling, C; Klein, M; Kleinwort, C; Klimkovich, T; Kluge, T; Knutsson, A; Kogler, R; Korbel, V; Kostka, P; Kraemer, M; Krastev, K; Kretzschmar, J; Kropivnitskaya, A; Kruger, K; Kutak, K; Landon, M P J; Lange, W; Lastovicka-Medin, G; Laycock, P; Lebedev, A; Leibenguth, G; Lendermann, V; Levonian, S; Li, G; Lipka, K; Liptaj, A; List, B; List, J; Loktionova, N; Lopez-Fernandez, R; Lubimov, V; Lucaci-Timoce, A.-I; Lytkin, L; Makankine, A; Malinovski, E; Marage, P; Marti, Ll; Martyn, H.-U; Maxfield, S J; Mehta, A; Meier, K; Meyer, A B; Meyer, H; Meyer, H; Meyer, J; Michels, V; Mikocki, S; Milcewicz-Mika, I; Moreau, F; Morozov, A; Morris, J V; Mozer, Matthias Ulrich; Mudrinic, M; Muller, K; Murin, P; Nankov, K; Naroska, B; Naumann, Th; Newman, Paul R; Niebuhr, C; Nikiforov, A; Nowak, G; Nowak, K; Nozicka, M; Olivier, B; Olsson, J E; Osman, S; Ozerov, D; Palichik, V; Panagoulias, I; Pandurovic, M; Papadopoulou, Th; Pascaud, C; Patel, G D; Pejchal, O; Peng, H; Perez, E; Petrukhin, A; Picuric, I; Piec, S; Pitzl, D; Placakyte, R; Polifka, R; Povh, B; Preda, T; Radescu, V; Rahmat, A J; Raicevic, N; Raspiareza, A; Ravdandorj, T; Reimer, P; Rizvi, E; Robmann, P; Roland, B; Roosen, R; Rostovtsev, A; Rotaru, M; Ruiz Tabasco, J E; Rurikova, Z; Rusakov, S; Salek, D; Salvaire, F; Sankey, D P C; Sauter, M; Sauvan, E; Schmidt, S; Schmitt, S; Schmitz, C; Schoeffel, L; Schoning, A; Schultz-Coulon, H.-C; Sefkow, F; Shaw-West, R N; Sheviakov, I; Shtarkov, L N; Shushkevich, S; Sloan, T; Smiljanic, Ivan; Smirnov, P; Soloviev, Y; Sopicki, P; South, D; Spaskov, V; Specka, Arnd E; Staykova, Z; Steder, M; Stella, B; Straumann, U; Sunar, D; Sykora, T; Tchoulakov, V; Thompson, G; Thompson, P D; Toll, T; Tomasz, F; Tran, T H; Traynor, D; Trinh, T N; Truol, P; Tsakov, I; Tseepeldorj, B; Tsurin, I; Turnau, J; Tzamariudaki, E; Urban, K; Valkarova, A; Vallee, C; Van Mechelen, P; Vargas Trevino, A; Vazdik, Y; Vinokurova, S; Volchinski, V; Wegener, D; Wessels, M; Wissing, Ch; Wunsch, E; Yeganov, V; Zacek, J; Zalesak, J; Zhang, Z; Zhelezov, A; Zhokin, A; Zhu, Y C; Zimmermann, T; Zohrabyan, H; Zomer, F

2009-01-01T23:59:59.000Z

51

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

National Nuclear Security Administration (NNSA)

2-12-06 Quarterly SSP Experiment Summary-FY12-4Q 1 2-12-06 Quarterly SSP Experiment Summary-FY12-4Q 1 Summary of Experiments Conducted in Support of Stockpile Stewardship October 2012 The U.S. Stockpile Stewardship Program is a robust program of scientific inquiry used to sustain and assess the nuclear weapons stockpile without the use of underground nuclear tests. The experiments carried out within the program are used in combination with Advanced Simulation and Computing (ASC) to continually assess the stockpile to ensure it is safe, secure, and effective. (For links to the ASC program, see: http://nnsa.energy.gov/asc) For a link to the Nuclear Posture Review 2010, see: http://www.defense.gov/npr/docs/2010%20nuclear%20posture%20review%20report.pdf . An extraordinary set of science, technology, and engineering (ST&E) facilities have been established and are active everyday in support of the

52

Recoil Polarization Measurements of the Proton Electromagnetic Form Factor Ratio to Q^2 = 8.5 GeV^2  

SciTech Connect (OSTI)

Among the most fundamental observables of nucleon structure, electromagnetic form factors are a crucial benchmark for modern calculations describing the strong interaction dynamics of the nucleons quark constituents; indeed, recent proton data have attracted intense theoretical interest. In this Letter, we report new measurements of the proton electromagnetic form factor ratio using the recoil polarization method, at momentum transfers Q2=5.2, 6.7, and 8.5??GeV2. By extending the range of Q2 for which GEp is accurately determined by more than 50%, these measurements will provide significant constraints on models of nucleon structure in the nonperturbative regime.

Puckett, A J.R.; Jones, M K; Luo, W; Meziane, M; Pentchev, L; Perdrisat, C F; Punjabi, V; Wesselmann, F R; Ahmidouch, A; Albayrak, I; Aniol, K A; Arrington, J; Asaturyan, A; Baghdasaryan, H; Benmokhtar, F; Bertozzi, W; Bimbot, L; Bosted, P; Boeglin, W; Butuceanu, C; Carter, P; Chernenko, S; Christy, E; Commisso, M; Cornejo, J C; Covrig, S; Danagoulian, S; Daniel, A; Davidenko, A; Day, D; Dhamija, S; Dutta, D; Ent, R; Frullani, S; Fenker, H; Frlez, E; Garibaldi, F; Gaskell, D; Gilad, S; Gilman, R; Goncharenko, Y; Hafidi, K; Hamilton, D; Higinbotham, D W; Hinton, W; Horn, T; Hu, B; Huang, J; Huber, G M; Jensen, E; Keppel, C; Khandaker, M; King, P; Kirillov, D; Kohl, M; Kravtsov, V; Kumbartzki, G; Li, Y; Mamyan, V; Margaziotis, D J; Marsh, A; Matulenko, Y; Maxwell, J; Mbianda, G; Meekins, D; Melnik, Y; Miller, J; Mkrtchyan, A; Mkrtchyan, H; Moffit, B; Moreno, O; Mulholland, J; Narayan, A; Nedev, S; Nuruzzaman,; Piasetzky, E; Pierce, W; Piskunov, N M; Prok, Y; Ransome, R D; Razin, D S; Reimer, P; Reinhold, J; Rondon, O; Shabestari, M; Shahinyan, A; Shestermanov, K; Sirca, S; Sitnik, I; Smykov, L; Smith, G; Solovyev, L; Solvingnon, P; Subedi, R; Tomasi-Gustafsson, E; Vasiliev, A; Veilleux, M; Wojtsekhowski, B B; Wood, S; Ye, Z; Zanevsky, Y; Zhang, X; Zhang, Y; Zheng, X; Zhu, L

2010-06-01T23:59:59.000Z

53

Warm water occupancy by North Sea cod  

Science Journals Connector (OSTI)

...Southern Bight), 963, 861 (German Bight), 3443 (Flamborough), 10401 (Eastern...the year (Q) for cod from the Southern Bight and west Shetland. region Q1 Q2 Q3 Q4...Gillibrand1996Hydrography of the East Shetland Basin in relation to decadal North Sea variability...

2007-01-01T23:59:59.000Z

54

P2Q2Iso2D = 2D ISOPARAMETRIC FEM IN MATLAB S. BARTELS, C. CARSTENSEN  

E-Print Network [OSTI]

P2Q2Iso2D = 2D ISOPARAMETRIC FEM IN MATLAB S. BARTELS, C. CARSTENSEN , AND A. HECHT Abstract. A short Matlab implementation realizes a flexible isoparametric finite element method up to quadratic a short Matlab implementation of this finite element method for the Laplace equation in two dimensions

Bartels, Soeren

55

Q1, gender 1 = male, 2 = female. (1 occurence of "Not answered" (0) changed to median value 1).  

E-Print Network [OSTI]

, average time per week used on AoC 1 = less than 1 hour, 2 = 1-3 hours, 3 = 3-5 hours, 4 = 5-7 hours, 5 = more than 7 hours Q4, "Compared with an average student in the course I used ... on AoC" 1 = much less would definitely benefit from using a system like AoC" followed Likert scale where 1 = strongly disagree

Natvig, Lasse

56

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

SciTech Connect (OSTI)

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

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

2014-10-01T23:59:59.000Z

57

BPS M2-branes in AdS4Q1,1,1 and their dual loop operators  

Science Journals Connector (OSTI)

In this paper, we first compute the Killing spinors of AdS4Q1,1,1 and its certain orbifolds. Based on this, two classes of M2-brane solutions are found. The first class of solutions includes M2-branes dual to Wilson loops in the fundamental representation as a special case. The second class includes the candidates of the holographic description of vortex loops in the dual field theories.

Jun-Bao Wu and Meng-Qi Zhu

2014-06-05T23:59:59.000Z

58

Angular analysis of the $B^0 \\rightarrow K^{*0} e^+ e^-$ decay in the low-$q^2$ region  

E-Print Network [OSTI]

An angular analysis of the $B^0 \\rightarrow K^{*0} e^+ e^-$ decay is performed using a data sample, corresponding to an integrated luminosity of 3.0 ${\\mbox{fb}^{-1}}$, collected by the LHCb experiment in $pp$ collisions at centre-of-mass energies of 7 and 8 TeV during 2011 and 2012. For the first time several observables are measured in the dielectron mass squared ($q^2$) interval between 0.002 and 1.120${\\mathrm{\\,Ge\\kern -0.1em V^2\\!/}c^4}$. The angular observables $F_{\\mathrm{L}}$ and $A_{\\mathrm{T}}^{\\mathrm{Re}}$ which are related to the $K^{*0}$ polarisation and to the lepton forward-backward asymmetry, are measured to be $F_{\\mathrm{L}}= 0.16 \\pm 0.06 \\pm0.03$ and $A_{\\mathrm{T}}^{\\mathrm{Re}} = 0.10 \\pm 0.18 \\pm 0.05$, where the first uncertainty is statistical and the second systematic. The angular observables $A_{\\mathrm{T}}^{(2)}$ and $A_{\\mathrm{T}}^{\\mathrm{Im}}$ which are sensitive to the photon polarisation in this $q^2$ range, are found to be $A_{\\mathrm{T}}^{(2)} = -0.23 \\pm 0.23 \\pm 0.05$ a...

Aaij, Roel; Adinolfi, Marco; Affolder, Anthony; Ajaltouni, Ziad; Akar, Simon; Albrecht, Johannes; Alessio, Federico; Alexander, Michael; Ali, Suvayu; Alkhazov, Georgy; Alvarez Cartelle, Paula; Alves Jr, Antonio Augusto; Amato, Sandra; Amerio, Silvia; Amhis, Yasmine; An, Liupan; Anderlini, Lucio; Anderson, Jonathan; Andreassen, Rolf; Andreotti, Mirco; Andrews, Jason; Appleby, Robert; Aquines Gutierrez, Osvaldo; Archilli, Flavio; Artamonov, Alexander; Artuso, Marina; Aslanides, Elie; Auriemma, Giulio; Baalouch, Marouen; Bachmann, Sebastian; Back, John; Badalov, Alexey; Baesso, Clarissa; Baldini, Wander; Barlow, Roger; Barschel, Colin; Barsuk, Sergey; Barter, William; Batozskaya, Varvara; Battista, Vincenzo; Bay, Aurelio; Beaucourt, Leo; Beddow, John; Bedeschi, Franco; Bediaga, Ignacio; Belogurov, Sergey; Belyaev, Ivan; Ben-Haim, Eli; Bencivenni, Giovanni; Benson, Sean; Benton, Jack; Berezhnoy, Alexander; Bernet, Roland; Bertolin, Alessandro; Bettler, Marc-Olivier; van Beuzekom, Martinus; Bien, Alexander; Bifani, Simone; Bird, Thomas; Bizzeti, Andrea; Blake, Thomas; Blanc, Frdric; Blouw, Johan; Blusk, Steven; Bocci, Valerio; Bondar, Alexander; Bondar, Nikolay; Bonivento, Walter; Borghi, Silvia; Borgia, Alessandra; Borsato, Martino; Bowcock, Themistocles; Bowen, Espen Eie; Bozzi, Concezio; Brett, David; Britsch, Markward; Britton, Thomas; Brodzicka, Jolanta; Brook, Nicholas; Bursche, Albert; Buytaert, Jan; Cadeddu, Sandro; Calabrese, Roberto; Calvi, Marta; Calvo Gomez, Miriam; Campana, Pierluigi; Campora Perez, Daniel; Capriotti, Lorenzo; Carbone, Angelo; Carboni, Giovanni; Cardinale, Roberta; Cardini, Alessandro; Carson, Laurence; Carvalho Akiba, Kazuyoshi; Casanova Mohr, Raimon; Casse, Gianluigi; Cassina, Lorenzo; Castillo Garcia, Lucia; Cattaneo, Marco; Cauet, Christophe; Cenci, Riccardo; Charles, Matthew; Charpentier, Philippe; Chefdeville, Maximilien; Chen, Shanzhen; Cheung, Shu-Faye; Chiapolini, Nicola; Chrzaszcz, Marcin; Cid Vidal, Xabier; Ciezarek, Gregory; Clarke, Peter; Clemencic, Marco; Cliff, Harry; Closier, Joel; Coco, Victor; Cogan, Julien; Cogneras, Eric; Cogoni, Violetta; Cojocariu, Lucian; Collazuol, Gianmaria; Collins, Paula; Comerma-Montells, Albert; Contu, Andrea; Cook, Andrew; Coombes, Matthew; Coquereau, Samuel; Corti, Gloria; Corvo, Marco; Counts, Ian; Couturier, Benjamin; Cowan, Greig; Craik, Daniel Charles; Crocombe, Andrew Christopher; Cruz Torres, Melissa Maria; Cunliffe, Samuel; Currie, Robert; D'Ambrosio, Carmelo; Dalseno, Jeremy; David, Pascal; David, Pieter; Davis, Adam; De Bruyn, Kristof; De Capua, Stefano; De Cian, Michel; De Miranda, Jussara; De Paula, Leandro; De Silva, Weeraddana; De Simone, Patrizia; Dean, Cameron Thomas; Decamp, Daniel; Deckenhoff, Mirko; Del Buono, Luigi; Dlage, Nicolas; Derkach, Denis; Deschamps, Olivier; Dettori, Francesco; Dey, Biplab; Di Canto, Angelo; Di Domenico, Antonio; Di Ruscio, Francesco; Dijkstra, Hans; Donleavy, Stephanie; Dordei, Francesca; Dorigo, Mirco; Dosil Surez, Alvaro; Dossett, David; Dovbnya, Anatoliy; Dreimanis, Karlis; Dujany, Giulio; Dupertuis, Frederic; Durante, Paolo; Dzhelyadin, Rustem; Dziurda, Agnieszka; Dzyuba, Alexey; Easo, Sajan; Egede, Ulrik; Egorychev, Victor; Eidelman, Semen; Eisenhardt, Stephan; Eitschberger, Ulrich; Ekelhof, Robert; Eklund, Lars; El Rifai, Ibrahim; Elsasser, Christian; Ely, Scott; Esen, Sevda; Evans, Hannah Mary; Evans, Timothy; Falabella, Antonio; Frber, Christian; Farinelli, Chiara; Farley, Nathanael; Farry, Stephen; Fay, Robert; Ferguson, Dianne; Fernandez Albor, Victor; Ferreira Rodrigues, Fernando; Ferro-Luzzi, Massimiliano; Filippov, Sergey; Fiore, Marco; Fiorini, Massimiliano; Firlej, Miroslaw; Fitzpatrick, Conor; Fiutowski, Tomasz; Fol, Philip; Fontana, Marianna; Fontanelli, Flavio; Forty, Roger; Francisco, Oscar; Frank, Markus; Frei, Christoph; Frosini, Maddalena; Fu, Jinlin; Furfaro, Emiliano; Gallas Torreira, Abraham; Galli, Domenico; Gallorini, Stefano; Gambetta, Silvia; Gandelman, Miriam; Gandini, Paolo; Gao, Yuanning; Garca Pardias, Julin; Garofoli, Justin; Garra Tico, Jordi; Garrido, Lluis; Gascon, David; Gaspar, Clara; Gastaldi, Ugo; Gauld, Rhorry; Gavardi, Laura; Gazzoni, Giulio; Geraci, Angelo; Gersabeck, Evelina; Gersabeck, Marco; Gershon, Timothy; Ghez, Philippe; Gianelle, Alessio; Gian, Sebastiana; Gibson, Valerie; Giubega, Lavinia-Helena; Gligorov, Vladimir; Gbel, Carla; Golubkov, Dmitry; Golutvin, Andrey; Gomes, Alvaro; Gotti, Claudio; Grabalosa Gndara, Marc; Graciani Diaz, Ricardo; Granado Cardoso, Luis Alberto; Graugs, Eugeni; Graverini, Helena

2015-01-01T23:59:59.000Z

59

Angular analysis of the $B^0 \\rightarrow K^{*0} e^+ e^-$ decay in the low-$q^2$ region  

E-Print Network [OSTI]

An angular analysis of the $B^0 \\rightarrow K^{*0} e^+ e^-$ decay is performed using a data sample, corresponding to an integrated luminosity of 3.0 ${\\mbox{fb}^{-1}}$, collected by the LHCb experiment in $pp$ collisions at centre-of-mass energies of 7 and 8 TeV during 2011 and 2012. For the first time several observables are measured in the dielectron mass squared ($q^2$) interval between 0.002 and 1.120${\\mathrm{\\,Ge\\kern -0.1em V^2\\!/}c^4}$. The angular observables $F_{\\mathrm{L}}$ and $A_{\\mathrm{T}}^{\\mathrm{Re}}$ which are related to the $K^{*0}$ polarisation and to the lepton forward-backward asymmetry, are measured to be $F_{\\mathrm{L}}= 0.16 \\pm 0.06 \\pm0.03$ and $A_{\\mathrm{T}}^{\\mathrm{Re}} = 0.10 \\pm 0.18 \\pm 0.05$, where the first uncertainty is statistical and the second systematic. The angular observables $A_{\\mathrm{T}}^{(2)}$ and $A_{\\mathrm{T}}^{\\mathrm{Im}}$ which are sensitive to the photon polarisation in this $q^2$ range, are found to be $A_{\\mathrm{T}}^{(2)} = -0.23 \\pm 0.23 \\pm 0.05$ ...

LHCb Collaboration

2015-01-01T23:59:59.000Z

60

Moments of the Spin Structure Functions g1p and g1d for 0.05 < Q2 < 3.0 GeV2  

SciTech Connect (OSTI)

The spin structure functions $g_1$ for the proton and the deuteron have been measured over a wide kinematic range in $x$ and \\Q2 using 1.6 and 5.7 GeV longitudinally polarized electrons incident upon polarized NH$_3$ and ND$_3$ targets at Jefferson Lab. Scattered electrons were detected in the CEBAF Large Acceptance Spectrometer, for $0.05 < Q^2 < 5 $\\ GeV$^2$ and $W < 3$ GeV. The first moments of $g_1$ for the proton and deuteron are presented -- both have a negative slope at low \\Q2, as predicted by the extended Gerasimov-Drell-Hearn sum rule. The first result for the generalized forward spin polarizability of the proton $\\gamma_0^p$ is also reported, and shows evidence of scaling above $Q^2$ = 1.5 GeV$^2$. Although the first moments of $g_1$ are consistent with Chiral Perturbation Theory (\\ChPT) calculations up to approximately $Q^2 = 0.06$ GeV$^2$, a significant discrepancy is observed between the $\\gamma_0^p$ data and \\ChPT\\ for $\\gamma_0^p$,even at the lowest \\Q2.

Prok, Yelena; Bosted, Peter; Burkert, Volker; Deur, Alexandre; Dharmawardane, Kahanawita; Dodge, Gail; Griffioen, Keith; Kuhn, Sebastian; Minehart, Ralph; Adams, Gary; Amaryan, Moscov; Amaryan, Moskov; Anghinolfi, Marco; Asryan, G.; Audit, Gerard; Avagyan, Harutyun; Baghdasaryan, Hovhannes; Baillie, Nathan; Ball, J.P.; Ball, Jacques; Baltzell, Nathan; Barrow, Steve; Battaglieri, Marco; Beard, Kevin; Bedlinskiy, Ivan; Bektasoglu, Mehmet; Bellis, Matthew; Benmouna, Nawal; Berman, Barry; Biselli, Angela; Blaszczyk, Lukasz; Boyarinov, Sergey; Bonner, Billy; Bouchigny, Sylvain; Bradford, Robert; Branford, Derek; Briscoe, William; Brooks, William; Bultmann, S.; Bueltmann, Stephen; Butuceanu, Cornel; Calarco, John; Careccia, Sharon; Carman, Daniel; Casey, Liam; Cazes, Antoine; Chen, Shifeng; Cheng, Lu; Cole, Philip; Collins, Patrick; Coltharp, Philip; Cords, Dieter; Corvisiero, Pietro; Crabb, Donald; Crede, Volker; Cummings, John; Dale, Daniel; Dashyan, Natalya; De Masi, Rita; De Vita, Raffaella; De Sanctis, Enzo; Degtiarenko, Pavel; Denizli, Haluk; Dennis, Lawrence; Dhuga, Kalvir; Dickson, Richard; Djalali, Chaden; Doughty, David; Dugger, Michael; Dytman, Steven; Dzyubak, Oleksandr; Egiyan, Hovanes; Egiyan, Kim; Elfassi, Lamiaa; Elouadrhiri, Latifa; Eugenio, Paul; Fatemi, Renee; Fedotov, Gleb; Feldman, Gerald; Fersch, Robert; Feuerbach, Robert; Forest, Tony; Fradi, Ahmed; Funsten, Herbert; Garcon, Michel; Gavalian, Gagik; Gevorgyan, Nerses; Gilfoyle, Gerard; Giovanetti, Kevin; Girod, Francois-Xavier; Goetz, John; Golovach, Evgeny; Gothe, Ralf; Guidal, Michel; Guillo, Matthieu; Guler, Nevzat; Guo, Lei; Gyurjyan, Vardan; Hadjidakis, Cynthia; Hafidi, Kawtar; Hakobyan, Hayk; Hanretty, Charles; Hardie, John; Hassall, Neil; Heddle, David; Hersman, F.; Hicks, Kenneth; Hleiqawi, Ishaq; Holtrop, Maurik; Huertas, Marco; Hyde, Charles; Ilieva, Yordanka; Ireland, David; Ishkhanov, Boris; Isupov, Evgeny; Ito, Mark; Jenkins, David; Jo, Hyon-Suk; Johnstone, John; Joo, Kyungseon; Juengst, Henry; Kalantarians, Narbe; Keith, Christopher; Kellie, James; Khandaker, Mahbubul; Kim, Kui; Kim, Kyungmo; Kim, Wooyoung; Klein, Andreas; Klein, Franz; Klusman, Mike; Kossov, Mikhail; Krahn, Zebulun; Kramer, Laird; Kubarovsky, Valery; Kuhn, Joachim; Kuleshov, Sergey; Kuznetsov, Viacheslav; Lachniet, Jeff; Laget, Jean; Langheinrich, Jorn; Lawrence, Dave; Lima, Ana; Livingston, Kenneth; Lu, Haiyun; Lukashin, K.; MacCormick, Marion; Marchand, Claude; Markov, Nikolai; Mattione, Paul; McAleer, Simeon; McKinnon, Bryan; McNabb, John; Mecking, Bernhard; Mestayer, Mac; Meyer, Curtis; Mibe, Tsutomu; Mikhaylov, Konstantin; Mirazita, Marco; Miskimen, Rory; Mokeev, Viktor; Morand, Ludyvine; Moreno, Brahim; Moriya, Kei; Morrow, Steven; Moteabbed, Maryam; Mueller, James; Munevar Espitia, Edwin; Mutchler, Gordon; Nadel-Turonski, Pawel; Nasseripour, Rakhsha; Niccolai, Silvia; Niculescu, Gabriel; Niculescu, Maria-Ioana; Niczyporuk, Bogdan; Niroula, Megh; Niyazov, Rustam; Nozar, Mina; O'Rielly, Grant; Osipenko, Mikhail; Ostrovidov, Alexander; Park, Kijun; Pasyuk, Evgueni; Paterson, Craig; Anefalos Pereira, S.; Philips, Sasha; Pierce, J.; Pivnyuk, Nikolay; Pocanic, Dinko; Pogorelko, Oleg; Popa, Iulian; Pozdnyakov, Sergey; Preedom, Barry; Price, John; Procureur, Sebastien; Protopopescu, Dan; Qin, Liming; Raue, Brian; Riccardi, Gregory; Ricco, Giovanni; Ripani, Marco; Ritchie, Barry; Rosner, Guenther; Rossi, Patrizia; Rowntree, David; Rubin, Philip; Sabatie, Franck; Salamanca, Julian; Salgado, Carlos; Santoro, Joseph; Sapunenko, Vladimir; Schumacher, Reinhard; Seely, Mikell; Serov, Vladimir; Sharabian, Youri; Sharov, Dmitri; Shaw, Jeffrey; Shvedunov, Nikolay; Skabelin, Alexander; Smith, Elton; Smith, Lee; Sober, Daniel; Sokhan, Daria; Stavinskiy, Aleksey; Stepanyan, Samuel; Stepanyan, Stepan; Stokes, Burnham; Stoler, Paul; Strakovski, Igor; Strauch, Steffen; Suleiman, Riad; Taiuti, Mauro; Tedeschi, David; Tkabladze, Avtandil; Tkachenko, Svyatoslav; Todor, Luminita; Ungaro, Maurizio; V

2009-02-01T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
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61

Electroexcitation of the Roper resonance for 1.7 < Q**2 < 4.5 -GeV2 in vec-ep ---> en pi+  

SciTech Connect (OSTI)

DOI: http://dx.doi.org/10.1103/PhysRevC.78.045209
The helicity amplitudes of the electroexcitation of the Roper resonance are extracted for 1.7 < Q2 < 4.5 GeV2 from recent high precision JLab-CLAS cross section and longitudinally polarized beam asymmetry data for pi+ electroproduction on protons at W=1.15-1.69 GeV. The analysis is made using two approaches, dispersion relations and a unitary isobar model, which give consistent results. It is found that the transverse helicity amplitude A_{1/2} for the gamma* p -> N(1440)P11 transition, which is large and negative at Q2=0, becomes large and positive at Q2 ~ 2 GeV2, and then drops slowly with Q2. The longitudinal helicity amplitude S_{1/2}, which was previously found from CLAS ep -> eppi0,enpi+ data to be large and positive at Q2=0.4,0.65 GeV2, drops with Q2. Available model predictions for gamma* p -> N(1440)P11 allow us to conclude that these results provide strong evidence in favor of N(1440)P11 as a first radial excitation of

Aznauryan, Inna; Burkert, Volker; Kim, Wooyoung; Park, Kil; Adams, Gary; Amaryan, Moscov; Amaryan, Moskov; Ambrozewicz, Pawel; Anghinolfi, Marco; Asryan, Gegham; Avagyan, Harutyun; Bagdasaryan, H.; Baillie, Nathan; Ball, J.P.; Ball, Jacques; Baltzell, Nathan; Barrow, Steve; Batourine, V.; Battaglieri, Marco; Bedlinskiy, Ivan; Bektasoglu, Mehmet; Bellis, Matthew; Benmouna, Nawal; Berman, Barry; Biselli, Angela; Blaszczyk, Lukasz; Bonner, Billy; Bookwalter, Craig; Bouchigny, Sylvain; Boyarinov, Sergey; Bradford, Robert; Branford, Derek; Briscoe, Wilbert; Brooks, William; Bultmann, S.; Bueltmann, Stephen; Butuceanu, Cornel; Calarco, John; Careccia, Sharon; Carman, Daniel; Casey, Liam; Cazes, Antoine; Chen, Shifeng; Cheng, Lu; Cole, Philip; Collins, Patrick; Coltharp, Philip; Cords, Dieter; Corvisiero, Pietro; Crabb, Donald; Crede, Volker; Cummings, John; Dale, Daniel; Dashyan, Natalya; De Masi, Rita; De Vita, Raffaella; De Sanctis, Enzo; Degtiarenko, Pavel; Denizli, Haluk; Dennis, Lawrence; Deur, Alexandre; Dhamija, Seema; Dharmawardane, Kahanawita; Dhuga, Kalvir; Dickson, Richard; Djalali, Chaden; Dodge, Gail; Donnelly, J.; Doughty, David; Dugger, Michael; Dytman, Steven; Dzyubak, Oleksandr; Egiyan, Hovanes; Egiyan, Kim; Elfassi, Lamiaa; Elouadrhiri, Latifa; Eugenio, Paul; Fatemi, Renee; Fedotov, Gleb; Feldman, Gerald; Feuerbach, Robert; Forest, Tony; Fradi, Ahmed; Funsten, Herbert; Gabrielyan, Marianna; Garcon, Michel; Gavalian, Gagik; Gevorgyan, Nerses; Gilfoyle, Gerard; Giovanetti, Kevin; Girod, Francois-Xavier; Goetz, John; Gohn, Wesley; Golovach, Evgeny; Gonenc, Atilla; Gordon, Christopher; Gothe, Ralf; Graham, L.; Griffioen, Keith; Guidal, Michel; Guillo, Matthieu; Guler, Nevzat; Guo, Lei; Gyurjyan, Vardan; Hadjidakis, Cynthia; Hafidi, Kawtar; Hafnaoui, Khadija; Hakobyan, Hayk; Hakobyan, Rafael; Hanretty, Charles; Hardie, John; Hassall, Neil; Heddle, David; Hersman, F.; Hicks, Kenneth; Hleiqawi, Ishaq; Holtrop, Maurik; Hyde, Charles; Ilieva, Yordanka; Ireland, David; Ishkhanov, Boris; Isupov, Evgeny; Ito, Mark; Jenkins, David; Jo, Hyon-Suk; Johnstone, John; Joo, Kyungseon; Juengst, Henry; Kalantarians, Narbe; Keller, Dustin; Kellie, James; Khandaker, Mahbubul; Kim, Kui; Klein, Andreas; Klein, Andreas; Klimenko, Alexei; Kossov, Mikhail; Krahn, Zebulun; Kramer, Laird; Kubarovsky, Valery; Kuhn, Joachim; Kuhn, Sebastian; Kuleshov, Sergey; Kuznetsov, Viacheslav; Lachniet, Jeff; Laget, Jean; Langheinrich, Jorn; Lawrence, Dave; Lee, T.; Lima, Ana; Livingston, Kenneth; Lu, Haiyun; Lukashin, Konstantin; MacCormick, Marion; Markov, Nikolai; Mattione, Paul; McAleer, Simeon; McKinnon, Bryan; McNabb, John; Mecking, Bernhard; Mehrabyan, Surik; Melone, Joseph; Mestayer, Mac; Meyer, Curtis; Mibe, Tsutomu; Mikhaylov, Konstantin; Minehart, Ralph; Mirazita, Marco; Miskimen, Rory; Mokeev, Viktor; Morand, Ludyvine; Moreno, Brahim; Moriya, Kei; Morrow, Steven; Moteabbed, Maryam; Mueller, James; Munevar Espitia, Edwin; Mutchler, Gordon; Nadel-Turonski, Pawel; Nasseripour, Rakhsha; Niccolai, Silvia; Niculescu, Gabriel; Niculescu, Maria-Ioana; Niczyporuk, Bogdan; Niroula, Megh; Niyazov, Rustam; Nozar, Mina; O'Rielly, Grant; Osipenko, Mikhail; Ostrovidov, Alexander; Park, S.; Pasyuk, Evgueni; Paterson, Craig; Anefalos Pereira, S.; Philips, Sasha; Pierce, Jerome; Pivnyuk, Nikolay; Pocanic, Dinko; Pogorelko, Oleg; Polli, Ermanno; Popa, Iulian; Pozdnyakov, Sergey; Preedom, Barry; Price, John; Prok, Yelena; Protopopescu, Dan; Qin, Liming; Raue, Brian; Riccardi, Gregory; Ricco, Giovanni; Ripani, Marco; Ritchie, Barry; Rosner, Guenther; Rossi, Patrizia; Rowntree, David; Rubin, Philip; Sabatie, Franck; Saini, Mukesh; Salamanca, Julian; Salgado, Carlos; Santoro, Joseph; Sapunenko, Vladimir; Schott, Diane; Schumacher, Reinhard; Serov, Vladimir; Sharabian, Youri; Sharov, Dmitri; Shaw, J.; Shvedunov, Nikolay; Skabelin, Alexander; Smith, Elton; Smith, Lee; Sober, Daniel; Sokhan, Daria; Stavinskiy, Aleksey; Stepanyan, Samuel; Stepanyan, Stepan; Stokes, Burnham

2008-10-01T23:59:59.000Z

62

Measurement of high-Q2 deep inelastic scattering cross sections with longitudinally polarised positron beams at HERA  

E-Print Network [OSTI]

The first measurements of the cross sections for neutral and charged current deep inelastic scattering in e+p collisions with longitudinally polarised positron beams are presented. The total cross section for e+p charged current deep inelastic scattering is presented at positive and negative values of positron beam longitudinal polarisation for an integrated luminosity of 37.0 pb^-1 H1 data and 30.5 pb^-1 ZEUS data collected in 2003 and 2004 at a centre-of-mass energy of 319 GeV. In addition, the ZEUS collaboration measured the single differential cross sections for charged and neutral current deep inelastic scattering in the kinematic region Q^2>200 GeV^2. The measured cross sections are compared with the predictions of the Standard Model. The H1 collaboration extrapolate the cross section to a fully left handed positron beam and find it to be consistent with the Standard Model expectation.

Julian Rautenberg

2005-06-15T23:59:59.000Z

63

Separated cross sections in ?^0 electroproduction at threshold at Q^2 = 0.05 GeV^2/c^2  

E-Print Network [OSTI]

The differential cross sections \\sigma_0=\\sigma_T+\\epsilon \\sigma_L, \\sigma_{LT}, and \\sigma_{TT} of \\pi^0 electroproduction from the proton were measured from threshold up to an additional center of mass energy of 40 MeV, at a value of the photon four-momentum transfer of Q^2= 0.05 GeV^2/c^2 and a center of mass angle of \\theta=90^\\circ. By an additional out-of-plane measurement with polarized electrons \\sigma_{LT'} was determined. This showed for the first time the cusp effect above the \\pi^+ threshold in the imaginary part of the s-wave. The predictions of Heavy Baryon Chiral Perturbation Theory are in disagreement with these data. On the other hand, the data are somewhat better predicted by the MAID phenomenological model and are in good agreement with the dynamical model DMT.

M. Weis; P. Bartsch; D. Baumann; J. Bermuth; A. M. Bernstein; K. Bohinc; R. Bhm; M. Ding; M. O. Distler; I. Ewald; J. M. Friedrich; J. Friedrich; M. Kahrau; M. Kohl; K. W. Krygier; A. Liesenfeld; H. Merkel; P. Merle; U. Mller; R. Neuhausen; M. M. Pavan; Th. Pospischil; M. Potokar; G. Rosner; H. Schmieden; M. Seimetz; S. irca; A. Wagner; Th. Walcher

2007-05-25T23:59:59.000Z

64

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

E-Print Network [OSTI]

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

Aksay, Ilhan A.

65

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Se  

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

89641,1665248,1813673,5268562,1605603,1418925,1574797,4599325,1560226,1520979,1548087,4629292,1595758,1512352,1566079,4674189,19171368 89641,1665248,1813673,5268562,1605603,1418925,1574797,4599325,1560226,1520979,1548087,4629292,1595758,1512352,1566079,4674189,19171368 "Alaska",157348,149707,163004,470059,165229,146865,163558,475652,126370,123922,126533,376825,179973,172560,185294,537827,1860363 "Arizona",615155,578338,629726,1823219,607331,529736,589913,1726980,684161,661439,675382,2020982,662176,605888,634784,1902848,7474029 "Arkansas",1368,1265,1373,4006,44,42,49,135,75,63,73,211,100,84,102,286,4638 "Colorado",2598599,2398691,2624231,7621521,2480199,2301680,2410596,7192475,2455799,2551386,2458359,7465544,2080422,1958496,1948749,5987667,28267207 "Illinois",2808999,2634005,2873292,8316296,3159879,2871581,3122311,9153771,2831358,2822706,2817902,8471966,2751380,2615582,2712181,8079143,34021176

66

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Se  

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

590156,1549121,1890240,5029517,1837008,1612832,1817764,5267604,1748827,1836260,1829250,5414337,1492063,1580746,1611253,4684062,20395520 590156,1549121,1890240,5029517,1837008,1612832,1817764,5267604,1748827,1836260,1829250,5414337,1492063,1580746,1611253,4684062,20395520 "Alaska",169145,171367,209428,549940,173925,153851,175804,503580,157110,166999,164746,488855,199224,205990,203505,608719,2151094 "Arizona",570518,563089,688183,1821790,656991,574518,646273,1877782,632198,671964,662911,1967073,683134,705482,697016,2085632,7752277 "Arkansas",61,21,38,120,21,20,42,83,2070,2222,2243,6535,8094,8775,8694,25563,32301 "Colorado",2322065,2187158,2595450,7104673,2124653,2012449,1834574,5971676,1808658,1912885,2451386,6172929,2126637,1895802,1890809,5913248,25162526 "Illinois",2562464,2507353,3029909,8099726,2908053,2654999,2859539,8422591,2736555,2873367,2839818,8449740,2744642,2850172,2897794,8492608,33464665

67

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Se  

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

55341,1681343,1892574,5329258,1658658,1670531,1742534,5071723,1410575,1654603,1555258,4620436,1414541,1475429,1469622,4359592,19381009 55341,1681343,1892574,5329258,1658658,1670531,1742534,5071723,1410575,1654603,1555258,4620436,1414541,1475429,1469622,4359592,19381009 "Alaska",192973,186567,214662,594202,157877,160560,166491,484928,147331,177894,166088,491313,191081,196389,191013,578483,2148926 "Arizona",642124,620818,714289,1977231,669838,675081,709437,2054356,609976,734758,686039,2030773,676671,695481,676430,2048582,8110942 "Arkansas",11974,11580,13334,36888,13213,13591,14398,41202,7961,9719,9086,26766,9411,9673,9407,28491,133347 "Colorado",1929471,1900070,2298696,6128237,2283478,1810220,2149953,6243651,2060280,2721721,2820414,7602415,2775211,1986851,2153267,6915329,26889632 "Illinois",2989525,2827862,3153966,8971353,2967621,3035216,3035405,9038242,3187769,3653573,3443141,10284483,3162324,3233725,3247382,9643431,37937509

68

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Se  

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

72722,1652685,1998911,5524318,1471117,1597213,1449134,4517464,1423501,1603213,1457981,4484695,1605882,1508880,1380680,4495442,19021919 72722,1652685,1998911,5524318,1471117,1597213,1449134,4517464,1423501,1603213,1457981,4484695,1605882,1508880,1380680,4495442,19021919 "Alaska",114843,99176,120137,334156,121810,134985,129878,386673,99616,112621,101599,313836,138523,130333,121502,390358,1425023 "Arizona",716328,607106,761870,2085304,550294,596655,802028,1948977,665397,763415,690796,2119608,735514,692009,634843,2062366,8216255 "Arkansas",1133,1091,1358,3582,363,400,3739,4502,1808,2040,1864,5712,2692,2525,3739,8956,22752 "Colorado",2387855,2081513,2450873,6920241,3801879,3949839,2602952,10354670,3080487,3253632,3429159,9763278,3286901,3017466,2979227,9283594,36321783 "Illinois",2785216,2462110,2950202,8197528,2491704,2687396,2573207,7752307,2694833,2967093,2729343,8391269,2968605,2766731,2652360,8387696,32728800

69

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Se  

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

37013,1847191,1852958,5637162,1679453,1697484,1543327,4920264,1696796,1671906,1699481,5068183,1984467,1700253,1847148,5531868,21157477 37013,1847191,1852958,5637162,1679453,1697484,1543327,4920264,1696796,1671906,1699481,5068183,1984467,1700253,1847148,5531868,21157477 "Alaska",129329,125265,125952,380546,108802,109831,102313,320946,107919,106795,108897,323611,161955,136692,153265,451912,1477015 "Arizona",666141,615518,614586,1896245,554503,559721,651658,1765882,787471,774751,790062,2352284,723180,613209,674173,2010562,8024973 "Arkansas",4995,4715,4674,14384,5556,5604,3913,15073,5154,5056,5144,15354,8839,7448,8083,24370,69181 "Colorado",2775379,2662914,2807565,8245858,2749564,2843044,2837128,8429736,2646860,2778764,2672384,8098008,2586749,2325481,2342628,7254858,32028460 "Illinois",2630380,2533189,2580968,7744537,2648952,2698785,2302695,7650432,2901260,2937658,2923435,8762353,3168268,2775871,2973000,8917139,33074461

70

2014_Q1.indd  

Energy Savers [EERE]

environmental analyses; complying with regulatory orders; responding to dangers to public health, safety, and the environment; and maintaining the lease tracts and their existing...

71

Applications of the LM392 Comparator Op Amp IC  

E-Print Network [OSTI]

Applications of the LM392 Comparator Op Amp IC The LM339 quad comparator and the LM324 op amp operation and ease of use has contributed to the wide range of applications for these devices. The LM392 FIGURE 1. 00749302 Q1, Q2, Q3 = 2N2369 Q4 = 2N2907 C1, A1 = LM392 amplifier-comparator dual *1% metal

Lanterman, Aaron

72

Second Quarter 2014 Volume 7, number 2  

E-Print Network [OSTI]

.5% in Q2, 4.1% in Q3, and 2.6% in Q4. March projections for annual average real GDP provided. The Bureau of Economic Analysis (BEA) reports U.S. real GDP expanded at an annual rate of 1.1% in Q1 2013, 2 coincides with positive signals from the market--accelerating GDP growth, employment gains, and rebounding

73

Measurement of high-Q2 neutral current deep inelastic e+p scattering cross sections with a longitudinally polarised positron beam at HERA  

E-Print Network [OSTI]

Measurements of neutral current cross sections for deep inelastic scattering in e+p collisions at HERA with a longitudinally polarised positron beam are presented. The single-differential cross-sections d(sigma)/dQ2, d(sigma)/dx and d(sigma)/dy and the reduced cross-section were measured in the kinematic region Q2 > 185 GeV2 and y energy of 318 GeV. The structure functions F3 and F3(gamma)Z were determined by combining the e+p results presented in this paper with previously published e-p neutral current results. The asymmetry parameter A+ is used to demonstrate the parity violation predicted in electroweak interactions. The measurements are well described by the predictions of the Standard Model.

ZEUS Collaboration; H. Abramowicz; I. Abt; L. Adamczyk; M. Adamus; R. Aggarwal; S. Antonelli; P. Antonioli; A. Antonov; M. Arneodo; O. Arslan; V. Aushev; Y. Aushev; O. Bachynska; A. Bamberger; A. N. Barakbaev; G. Barbagli; G. Bari; F. Barreiro; N. Bartosik; D. Bartsch; M. Basile; O. Behnke; J. Behr; U. Behrens; L. Bellagamba; A. Bertolin; S. Bhadra; M. Bindi; C. Blohm; V. Bokhonov; T. Bold; K. Bondarenko; E. G. Boos; K. Borras; D. Boscherini; D. Bot; I. Brock; E. Brownson; R. Brugnera; N. Brummer; A. Bruni; G. Bruni; B. Brzozowska; P. J. Bussey; B. Bylsma; A. Caldwell; M. Capua; R. Carlin; C. D. Catterall; S. Chekanov; J. Chwastowski; J. Ciborowski; R. Ciesielski; L. Cifarelli; F. Cindolo; A. Contin; A. M. Cooper-Sarkar; N. Coppola; M. Corradi; F. Corriveau; M. Costa; G. D'Agostini; F. Dal Corso; J. del Peso; R. K. Dementiev; S. De Pasquale; M. Derrick; R. C. E. Devenish; D. Dobur; B. A. Dolgoshein; G. Dolinska; A. T. Doyle; V. Drugakov; L. S. Durkin; S. Dusini; Y. Eisenberg; P. F. Ermolov; A. Eskreys; S. Fang; S. Fazio; J. Ferrando; M. I. Ferrero; J. Figiel; B. Foster; G. Gach; A. Galas; E. Gallo; A. Garfagnini; A. Geiser; I. Gialas; A. Gizhko; L. K. Gladilin; D. Gladkov; C. Glasman; O. Gogota; Yu. A. Golubkov; P. Gottlicher; I. Grabowska-Bold; J. Grebenyuk; I. Gregor; G. Grigorescu; G. Grzelak; O. Gueta; M. Guzik; C. Gwenlan; T. Haas; W. Hain; R. Hamatsu; J. C. Hart; H. Hartmann; G. Hartner; E. Hilger; D. Hochman; R. Hori; A. Huttmann; Z. A. Ibrahim; Y. Iga; R. Ingbir; M. Ishitsuka; H. -P. Jakob; F. Januschek; T. W. Jones; M. Jungst; I. Kadenko; B. Kahle; S. Kananov; T. Kanno; U. Karshon; F. Karstens; I. I. Katkov; M. Kaur; P. Kaur; A. Keramidas; L. A. Khein; J. Y. Kim; D. Kisielewska; S. Kitamura; R. Klanner; U. Klein; E. Koffeman; N. Kondrashova; O. Kononenko; P. Kooijman; Ie. Korol; I. A. Korzhavina; A. Kotanski; U. Kotz; H. Kowalski; O. Kuprash; M. Kuze; A. Lee; B. B. Levchenko; A. Levy; V. Libov; S. Limentani; T. Y. Ling; M. Lisovyi; E. Lobodzinska; W. Lohmann; B. Lohr; E. Lohrmann; K. R. Long; A. Longhin; D. Lontkovskyi; O. Yu. Lukina; J. Maeda; S. Magill; I. Makarenko; J. Malka; R. Mankel; A. Margotti; G. Marini; J. F. Martin; A. Mastroberardino; M. C. K. Mattingly; I. -A. Melzer-Pellmann; S. Mergelmeyer; S. Miglioranzi; F. Mohamad Idris; V. Monaco; A. Montanari; J. D. Morris; K. Mujkic; B. Musgrave; K. Nagano; T. Namsoo; R. Nania; A. Nigro; Y. Ning; T. Nobe; D. Notz; R. J. Nowak; A. E. Nuncio-Quiroz; B. Y. Oh; N. Okazaki; K. Olkiewicz; Yu. Onishchuk; K. Papageorgiu; A. Parenti; E. Paul; J. M. Pawlak; B. Pawlik; P. G. Pelfer; A. Pellegrino; W. Perlanski; H. Perrey; K. Piotrzkowski; P. Plucinski; N. S. Pokrovskiy; A. Polini; A. S. Proskuryakov; M. Przybycien; A. Raval; D. D. Reeder; B. Reisert; Z. Ren; J. Repond; Y. D. Ri; A. Robertson; P. Roloff; I. Rubinsky; M. Ruspa; R. Sacchi; U. Samson; G. Sartorelli; A. A. Savin; D. H. Saxon; M. Schioppa; S. Schlenstedt; P. Schleper; W. B. Schmidke; U. Schneekloth; V. Schonberg; T. Schorner-Sadenius; J. Schwartz; F. Sciulli; L. M. Shcheglova; R. Shehzadi; S. Shimizu; I. Singh; I. O. Skillicorn; W. Slominski; W. H. Smith; V. Sola; A. Solano; D. Son; V. Sosnovtsev; A. Spiridonov; H. Stadie; L. Stanco; N. Stefaniuk; A. Stern; T. P. Stewart; A. Stifutkin; P. Stopa; S. Suchkov; G. Susinno; L. Suszycki; J. Sztuk-Dambietz; D. Szuba; J. Szuba; A. D. Tapper; E. Tassi; J. Terron; T. Theedt; H. Tiecke; K. Tokushuku; J. Tomaszewska; V. Trusov; T. Tsurugai; M. Turcato; O. Turkot; T. Tymieniecka; M. Vazquez; A. Verbytskyi; O. Viazlo; N. N. Vlasov; R. Walczak; W. A. T. Wan Abdullah; J. J. Whitmore; K. Wichmann; L. Wiggers; M. Wing; M. Wlasenko; G. Wolf; H. Wolfe; K. Wrona; A. G. Yagues-Molina; S. Yamada; Y. Yamazaki; R. Yoshida; C. Youngman; O. Zabiegalov; A. F. . Zarnecki; L. Zawiejski; O. Zenaiev; W. Zeuner; B. O. Zhautykov; N. Zhmak; A. Zichichi; Z. Zolkapli; D. S. Zotkin

2014-05-12T23:59:59.000Z

74

Measurement of the Electric Form Factor of the Neutron at Q^2 = 0.3-0.8 (GeV/c)^2  

E-Print Network [OSTI]

The electric form factor of the neutron, G_En, has been measured at the Mainz Microtron by recoil polarimetry in the quasielastic D(e_pol,e'n_pol)p reaction. Three data points have been extracted at squared four-momentum transfers Q^2 = 0.3, 0.6 and 0.8 (GeV/c)^2. Corrections for nuclear binding effects have been applied.

D. I. Glazier; M. Seimetz; J. R. M. Annand; H. Arenhvel; M. Ases Antelo; C. Ayerbe; P. Bartsch; D. Baumann; J. Bermuth; R. Bhm; D. Bosnar; M. Ding; M. O. Distler; D. Elsner; J. Friedrich; S. Hedicke; P. Jennewein; G. Jover Maas; F. H. Klein; F. Klein; M. Kohl; K. W. Krygier; K. Livingston; I. J. D. MacGregor; M. Makek; H. Merkel; P. Merle; D. Middleton; U. Mller; R. Neuhausen; L. Nungesser; M. Ostrick; R. Prez Benito; J. Pochodzalla; Th. Pospischil; M. Potokar; A. Reiter; G. Rosner; J. Sanner; H. Schmieden; A. Sle; Th. Walcher; D. Watts; M. Weis

2004-10-18T23:59:59.000Z

75

Consistent threshold pi0 electro-production at Q^2=0.05, 0.10, and 0.15 GeV^2/c^2  

E-Print Network [OSTI]

New, accurate data are presented on the near threshold p(e,e'p)pi^0 reaction in the range of four-momentum transfers between Q^2=0.05 and 0.15GeV^2/c^2. The data were taken with the spectrometer setup of the A1 Collaboration at the Mainz Microtron MAMI. The complete center of mass solid angle was covered up to a center of mass energy of 4MeV above threshold. These results supersede the previous analysis based on three separate experiments, and are compared with calculations in Heavy Baryon Chiral Perturbation Theory and with phenomenological models.

H. Merkel; P. Achenbach; C. Ayerbe Gayoso; M. Ases Antelo; D. Baumann; A. M. Bernstein; R. Bhm; D. Bosnar; M. Ding; M. O. Distler; L. Doria; J. Garcia Llongo; D. W. Higinbotham; G. Jover Maas; M. Makek; U. Mller; R. Neuhausen; L. Nungesser; R. Prez Benito; J. Pochodzalla; M. Seimetz; S. Sirca; S. Stave; Th. Walcher; M. Weis

2011-09-23T23:59:59.000Z

76

A new measurement of the structure functions $P_{LL}-P_{TT}/epsilon$ and $P_{LT}$ in virtual Compton scattering at $Q^2=$ 0.33 (GeV/c)$^2$  

E-Print Network [OSTI]

The cross section of the $ep \\to e' p' \\gamma$ reaction has been measured at $Q^2 = 0.33$ (GeV/c)$^2$. The experiment was performed using the electron beam of the MAMI accelerator and the standard detector setup of the A1 Collaboration. The cross section is analyzed using the low-energy theorem for virtual Compton scattering, yielding a new determination of the two structure functions $P_LL}-P_{TT}/epsilon$ and $P_{LT}$ which are linear combinations of the generalized polarizabilities of the proton. We find somewhat larger values than in the previous investigation at the same $Q^2$. This difference, however, is purely due to our more refined analysis of the data. The results tend to confirm the non-trivial $Q^2$-evolution of the generalized polarizabilities and call for more measurements in the low-$Q^2$ region ($\\le$ 1 (GeV/c)$^2$).

The MAMI-A1 Collaboration; :; P. Janssens; L. Doria; P. Achenbach; C. Ayerbe Gayoso; D. Baumann; J. C. Bernauer; I. K. Bensafa; R. Bhm; D. Bosnar; E. Burtin; N. D'Hose; X. Defa; M. Ding; M. O. Distler; H. Fonvieille; J. Friedrich; J. M. Friedrich; G. Laveissire; M. Makek; J. Marroncle; H. Merkel; U. Mller; L. Nungesser; B. Pasquini; J. Pochodzalla; O. Postavaru; M. Potokar; D. Ryckbosch; S. Sanchez Majos; B. S. Schlimme; M. Seimetz; S. irca; G. Tamas; R. Van de Vyver; L. Van Hoorebeke; A. Van Overloop; Th. Walcher; M. Weinriefer

2008-03-06T23:59:59.000Z

77

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

E-Print Network [OSTI]

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

D. Karakhanyan; Sh. Khachatryan

2006-02-08T23:59:59.000Z

78

幻灯片 1  

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

Electric-Drive Vehicle Testing Electric-Drive Vehicle Testing at CAERI Hao Zhang China Automotive Engineering Research Institute 1. Overview 2. On-going Work 3. Future Work 4. Conclusion Contents Three-year Plan Full Hybrid BEV Plug-in REEV Mild Hybrid  Three year program in CAERI  Evaluating the performance of the EV, HEV and PHEV  Plan to benchmark more than 12 cars in three years ☆ Milestones 2011-Q2 2011-Q3 2011-Q4 2012-Q1 2012-Q2 2012-Q3 2012-Q4 Test Procedures Research and Preparation for cars Civic Hybrid Test and Analysis Nissan Leaf Test and Analysis MY2010 Prius Test and Analysis Fusion Hybrid Test and Analysis Volt Test and Analysis Plug-in Prius Test and Analysis 2011-2012 works Testing Approach  The vehicle testing activity and analysis approach has been defined:

79

LLQR-2012-Q2.pdf  

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

NEPA NEPA 1 June 2012 Second Quarter FY 2012 June 5, 2012; Issue No. 71 U.S. DepartmeNt oF eNergY QUarterlY report National environmental policy act LESSONS LEARNED LEARNED LESSONS N E P A How to Manage an EIS Schedule Successfully By: Brian Costner and Carrie Moeller, Office of NEPA Policy and Compliance Developing and maintaining the schedule for preparation of an environmental impact statement (EIS) is one of a NEPA Document Manager's most important responsibilities. The Office of NEPA Policy and Compliance recently asked several NEPA Compliance Officers (NCOs) and NEPA Document Managers to share their advice for completing an EIS on time. An EIS schedule goes through several stages, they observed. An initial schedule must be revised as data

80

LLQR-2000-Q2.pdf  

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

June 2000 June 2000 1 LESSONS LEARNED LEARNED LESSONS National Environmental Policy Act N E P A U.S. DEPARTMENT OF ENERGY QUARTERLY REPORT For Second Quarter FY 2000 June 1, 2000; Issue No. 23 NEPA Compliance Officers Celebrate 10 Years of Progress, Look to Future Los Alamos Site-wide EIS Analyzed Wildfire Impacts, Prompted Mitigation Actions continued on page 3 As DOE and the Los Alamos region cope with the effects of last month's devastating fire, the 1999 Los Alamos National Laboratory (LANL) Site- wide EIS has proved to be a valuable reference document. In fact, the NEPA process had earlier focused DOE attention on the risks of wildfire at LANL and prompted mitigation actions within the past year that reduced the severity of impacts of the fire. Moreover, the analyses in the Site-wide EIS

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81

Microsoft Word - Q4report.doc  

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

2009 to September 2009 2009 to September 2009 Heat Flow and Gas Hydrates on the Continental Margin of India: Building on Results from NGHP Expedition 01 Submitted by: College of Oceanic and Atmospheric Science Oregon State University Corvallis, OR 97331 Principal Investigator: Anne M. Trehu Prepared for: United States Department of Energy National Energy Technology Laboratory October 30, 2009 Oil & Natural Gas Technology 1 Progress Report July 2009 to September 2009 Heat flow and gas hydrates on the continental margin of India: Building on results from NGHP expedition 01 DE-NT0005669 Principal Investigator Anne Trehu (PI) Oregon State University Oct 30, 2009 2 Table of Contents: Executive Summary..................................................................................................3

82

LLQR-2012-Q4-r1.pdf  

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

2 2 December 3, 2012; Issue no. 73 NEPA Lessons Learned December 2012 1 Quality Assurance Integral to NEPA Implementation DOE senior leaders have repeatedly emphasized quality assurance as essential to a successful NEPA program. Secretarial Officers and Heads of Field Organizations have the responsibility to ensure the preparation of a NEPA quality assurance plan (DOE O 451.1B, NEPA Compliance Program, paragraph 5.a(3)). This provision was added in response to a June 1994 Secretarial NEPA policy statement. This requirement to prepare a plan signifies that a formal approach to quality assurance should be in place at the beginning of a NEPA review. Most recently, Secretary of Energy Steven Chu's June 2012 policy memorandum on integrating program and project management with NEPA expressed the

83

Microchannel Receiver Development- FY12 Q4  

Broader source: Energy.gov [DOE]

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

84

Determination of quadrupole strengths in the gamma*p-->Delta(1232) transition at Q2= 0.20 (GeV/c)2  

E-Print Network [OSTI]

We report new precise p$(\\vec{e},e^\\prime p)\\pi^0$ measurements at the peak of the $\\Delta^{+}(1232)$ resonance at $Q^2=\\unit[0.20](GeV/c)^2$ performed at the Mainz Microtron (MAMI). The new data are sensitive to both the electric quadrupole ($E2$) and the coulomb quadrupole ($C2$) amplitudes of the $\\gamma^* N\\to\\Delta$ transition. They yield precise quadrupole to dipole amplitude ratios CMR $= (-5.09 \\pm 0.28_{stat+sys}\\pm 0.30_{model})%$ and EMR $= (-1.96 \\pm 0.68_{stat+sys} \\pm 0.41_{model})%$ for $M^{3/2}_{1+} = (39.57 \\pm 0.75_{stat+sys}\\pm 0.40_{model})(10^{-3}/m_{\\pi^+})$. The new results are in disagreement with Constituent Quark Model predictions and in qualitative agreement with models that account for mesonic contributions, including recent Lattice calculations. They thus give further credence to the conjecture of deformation in hadronic systems favoring the attribution of the origin of deformation to the dominance of mesonic effects.

N. F. Sparveris; P. Achenbach; C. Ayerbe Gayoso; D. Baumann; J. Bernauer; A. M. Bernstein; R. Bohm; D. Bosnar; T. Botto; A. Christopoulou; D. Dale; M. Ding; M. O. Distler; L. Doria; J. Friedrich; A. Karabarbounis; M. Makek; H. Merkel; U. Muller; I. Nakagawa; R. Neuhausen; L. Nungesser; C. N. Papanicolas; A. Piegsa; J. Pochodzalla; M. Potokar; M. Seimetz; S. Sirca; S. Stave; S. Stiliaris; Th. Walcher; M. Weis

2006-11-20T23:59:59.000Z

85

Q1 1998 STEO Docs  

Gasoline and Diesel Fuel Update (EIA)

8 (Released January 12, 1998) 8 (Released January 12, 1998) Energy Information Administration DOE/EIA-0202(98/1Q) Distribution Category UC-950 Short-Term Energy Outlook Quarterly Projections First Quarter 1998 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 U.S. Department of Energy. The information contained herein should be attributed to the Energy Information Administration and should not be construed as advocating or reflecting any policy position of the Department of Energy or any other organization. Energy Information Administration/Short-Term Energy Outlook --January 1998

86

Microsoft PowerPoint - Proceedings Cover Sheets  

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

Monitoring, Mitigation, and Verification Monitoring, Mitigation, and Verification Measuring Surface and Shallow Gas Flux and Composition As a Prelude to Geologic Carbon Sequestration in Eastern Kentucky Thomas (Marty) Parris, Mike Solis, and Kathryn Takacs May 8-11, 2006 * Hilton Alexandria Mark Center * Alexandria, Virginia Organization & Schedule Organization & Schedule Phase I Task 1.0 Task 3.0 Task 4.0 Start 2005 2006 2007 End 07/15/05 Q3 Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 01/14/08 Phase II Phase III Task 2.0 Task 5.0 Task 6.0 Task 7.0 Task 8.0 Task 9.0 Task 10.0 Task 11.0 Task 12.0 Task 13.0 Phase II Phase II - - Tasks Tasks Task 5.0- Training, instrumentation, calibration, strategy Task 6.0- Surface & shallow measurements Task 7.0- Laboratory GC & isotope measurements Task 8.0- Evaluate surface data- anomalies & deep wells

87

Electroproduction of ppi+pi- off protons at 0.2<Q^2<0.6 GeV^2 and 1.3 < W < 1.57 GeV with CLAS.  

SciTech Connect (OSTI)

This paper reports on the most comprehensive data set obtained on differential and fully integrated cross sections for the process $e p \\rightarrow e' p \\pi^{+} \\pi^{-} $. The data were collected with the CLAS detector at Jefferson Laboratory. Measurements were carried out in the so-far unexplored kinematic region of photon virtuality 0.2 $<$ $Q^{2}$ $<$ 0.6 GeV$^{2}$ and invariant mass of the final hadron system $W$ from 1.3 to 1.57~GeV. For the first time, nine independent 1-fold differential cross sections were determined in each bin of $W$ and $Q^{2}$ covered by the measurements. A phenomenological analysis of the data allowed us to establish the most significant mechanisms contributing to the reaction. The non-resonant mechanisms account for a major part of cross-sections. However, we find sensitivity to s-channel excitations of low-mass nucleon resonances, especially to the $N(1440)P_{11}$ and $N(1520)D_{13}$ states in kinematical dependencies of the 1-fold

Fedotov, Gleb; Mokeev, Viktor; Burkert, Volker; Elouadrhiri, Latifa; Golovach, Evgeny; Ishkhanov, Boris; Isupov, Evgeny; Shvedunov, Nikolay

2009-01-01T23:59:59.000Z

88

Executive Branch Management Scorecard  

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

June 30, 2009 June 30, 2009 CURRENT STATUS (As of June 30,, 2009) PROGRESS Third Quarter FY 2009 COMMENTS REAL PROPERTY Agency Lead: Paul Bosco, Senior Real Property Officer Lead RMO Examiner: Cynthia Vallina Lead OFFM Analyst: Joseph Pika Asset management plan (AMP) X in place by Q1 2005 (Y) X consistent with Federal Real Property Council (FRPC) standards or expected equivalent by Q2 2005 (Y) X OMB-approved by Q2 2005 (Y) X 3 year timeline for meeting plan goals/objectives by Q3 2006 (G) X evidence that plan is being implemented to achieve improved real property mgmt by Q4 2006 (G) Accurate and current inventory X in place by Q3 2004 (Y) X consistent with FRPC standards or expected equivalent by Q3 2004 (Y) X provided to govt.-wide real property

89

Executive Branch Management Scorecard  

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

September 30, 2009 September 30, 2009 CURRENT STATUS (As of September 30, 2009) PROGRESS Fourth Quarter FY 2009 COMMENTS REAL PROPERTY Agency Lead: Paul Bosco, Senior Real Property Officer Lead RMO Examiner: Cynthia Vallina Lead OFFM Analyst: Joseph Pika Asset management plan (AMP) X in place by Q1 2005 (Y) X consistent with Federal Real Property Council (FRPC) standards or expected equivalent by Q2 2005 (Y) X OMB-approved by Q2 2005 (Y) X 3 year timeline for meeting plan goals/objectives by Q3 2006 (G) X evidence that plan is being implemented to achieve improved real property mgmt by Q4 2006 (G) Accurate and current inventory X in place by Q3 2004 (Y) X consistent with FRPC standards or expected equivalent by Q3 2004 (Y) X provided to govt.-wide real property

90

JGI - Statistics  

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

Statistics Statistics FY 2014 Overall Sequencing Progress, Updated Quarterly Quarter Total Bases (trillions) Operating Hours Goal Actual Total* Actual % of Goal Goal (hours)** Actual Total Actual % Goal Q1 2014 15,000 18.827 126% 2,164 2208 102% Q2 2014 17,000 2,117 Q3 2014 18,000 2,140 Q4 2014 18,000 2,164 FY 2014 Total 68,000 18.827 28% 8,585 2208 26% * Includes Illumina HiSeq, MiSeq and PacBio sequencing platforms. ** Operating Hour target is based on 98% of the total available hours. FY 2013 Overall Sequencing Progress, Updated Quarterly Quarter Total Bases (Billions) Operating Hours Goal Actual Total* Actual % of Goal Goal (hours)** Actual Total Actual % Goal Q1 2013 15,000 20,004 133% 2,164 2,208 102%

91

OFFICE OF THE CHIEF INFORMATION OFFICER (OCIO)  

Office of Environmental Management (EM)

Security. (FY 12 Q4 - FY 13 Q3) One GS-13 employee is participating in the NDU 14-week Advanced Management Program. (FY 12 Q4 - FY 13 Q1) The OCIO strives to ensure supervisors,...

92

Final Meeting Summary Page 1  

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

EIS (TC & WM EIS), Q4 * Draft Land Conveyance Environmental Assessment, Q2 * Natural Gas Pipeline Environmental Impact Statement (EIS), Q3 * 2014 Budget meetings (2015 & 2016...

93

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.

94

FOIA QUARTERLY REPORTS (Q2-2014)  

Broader source: Energy.gov [DOE]

The DOEs 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...

95

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 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 large refractive index, the FDTD simulation is sensitive to the treatment of particle edge. In this study, we have introduced an effective particle edge treatment to reduce the FDTD errors. Using this treatment for particles with large refractive index (e.g., 7.15 i + 2.92 i), the

96

PROCEEDINGS OF RIKEN BNL RESEARCH CENTER WORKSHOP ON RHIC SPIN PHYSICS III AND IV, POLARIZED PARTONS AT HIGH Q2 REGION, AUGUST 3, 2000 AT BNL, OCTOBER 14, 2000 AT KYOTO UNIVERSITY.  

SciTech Connect (OSTI)

International workshop on II Polarized Partons at High Q2 region 11 was held at the Yukawa Institute for Theoretical Physics, Kyoto University, Kyoto, Japan on October 13-14, 2000, as a satellite of the international conference ''SPIN 2000'' (Osaka, Japan, October 16-21,2000). This workshop was supported by RIKEN (The Institute of Physical and Chemical Research) and by Yukawa Institute. The scientific program was focused on the upcoming polarized collider RHIC. The workshop was also an annual meeting of RHIC Spin Collaboration (RSC). The number of participants was 55, including 28 foreign visitors and 8 foreign-resident Japanese participants, reflecting the international nature of the RHIC spin program. At the workshop there were 25 oral presentations in four sessions, (1) RHIC Spin Commissioning, (2) Polarized Partons, Present and Future, (3) New Ideas on Polarization Phenomena, (4) Strategy for the Coming Spin Running. In (1) the successful polarized proton commissioning and the readiness of the accelerator for the physics program impressed us. In (2) and (3) active discussions were made on the new structure function to be firstly measured at RHIC, and several new theoretical ideas were presented. In session (4) we have established a plan for the beam time requirement toward the first collision of polarized protons. These proceedings include the transparencies presented at the workshop. The discussion on ''Strategy for the Coming Spin Running'' was summarized by the chairman of the session, S. Vigdor and G. Bunce.

BUNCE, G.; VIGDOR, S.

2001-03-15T23:59:59.000Z

97

FOIA Quarterly Reports (Q1-2014)  

Broader source: Energy.gov [DOE]

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

98

Berechenbarkeitstheorie Ralf Schindler  

E-Print Network [OSTI]

endlicher Automat, A = (Q, #, #, q 0 , F ). Dann kann # auch durch eine Tafel (eine Matrix) der Gr? o?e n ? Ubergangsfunktion # : Q? # # Q durch folgende Tafel gegeben sein. 0 1 q 0 q 1 q 2 q 1 q 2 q 3 q 2 q 3 q 3 q 3 q 3 q

Schindler, Ralf

99

Berechenbarkeitstheorie Ralf Schindler  

E-Print Network [OSTI]

Tafel (eine Matrix) der Gr¨o?e n · m wiedergegeben werden, wobei n die Zahl der Element von Q und m die ¨Ubergangsfunktion : Q ? Q durch folgende Tafel gegeben sein. 0 1 q0 q1 q2 q1 q2 q3 q2 q3 q3 q3 q3 q3 Die

Schindler, Ralf

100

Microsoft Word - WAPA FY06_Q4_HCM.doc  

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

Western Area Power Administration Western Area Power Administration P.O. Box 281213 Lakewood, CO 80228-1213 9-12-06 MEMORANDUM FOR CLAUDIA A. CROSS, HR-1 DIRECTOR, OFFICE OF HUMAN CAPITAL MANAGEMENT FROM: FRANCES TELLES, A7200 HUMAN RESOURCES MANAGER WESTERN AREA POWER ADMINISTRATION SUBJECT: Fourth Quarter FY 2006 Internal President's Management Agenda Scorecard Report on Human Capital The Western Area Power Administration is pleased to submit our human capital management performance report for the fourth quarter of FY 2006. The report is structured to match the nine scorecard requirements. Western's Senior Managers are committed to supporting the President's Management Agenda and Department of Energy's (DOE) Human Capital Program. To achieve our vision of being a premier power marketing and transmission organization, we will need to recruit,

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


101

Microsoft Word - Issue FY2009 Q4 Draft 20090910.doc  

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

Do you remember as a Do you remember as a kid how much it hurt to walk barefoot on a paved road? Do you also remember that walking on the white shoulder stripes hurt less? The blacktop absorbed much more of the sun's energy than the white stripes. A conventional roof works the same way, making it a hot place in the summer. Recent advances in roofing design have given rise to the concept of a "cool roof." A cool roof efficiently reflects the sun's energy and emits absorbed solar radiation back into the atmosphere. Such a roof remains relatively cooler and less likely to transfer heat down through the other components of the roof system and into the building thereby reducing the facility cooling load. Two factors determine the degree of efficiency of

102

Supercritical Carbon Dioxide Turbo-Expander- FY12 Q4  

Broader source: Energy.gov [DOE]

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

103

Scattering Solar Thermal Concentrators- FY12 Q4  

Broader source: Energy.gov [DOE]

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

104

Advanced Manufacture of Reflectors- FY12 Q4  

Broader source: Energy.gov [DOE]

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

105

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

SciTech Connect (OSTI)

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 Connecticuts existing residential energy efficiency programs that are overseen by the ratepayer fund board and administered by CT utilities. N2Ns 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 N2Ns and DOEs short-term program goals, as well as the State of Connecticuts long-term energy, efficiency, and carbon reduction goals. However, despite the slow program start, N2N found evidence of increasing upgrade uptake rates over time, due to delayed customer action of one to two years from N2N introduction to completion of deeper household upgrades. Two main social/behavioral principles have contributed to driving deeper upgrades in CT: 1. Word of mouth, where people share their experience with others, which leads to others to take action; and 2. Self-herding, where people follow past behavior, which leads to deeper and deeper actions within individual households.

Donnelly, Kat A.

2014-01-10T23:59:59.000Z

106

J. theor. Biol. (1997) 189, 171174 00225193/97/220171 + 04 $25.00/0/jt970503 7 1997 Academic Press Limited  

E-Print Network [OSTI]

with regard to their statistical #12;p1 5' -- 3' -- C( ) q3 p2 -- -- C( ) q2 p3 -- -- C( ) q1 -- -- 3' 5' A

Michel, Christian

107

Office of Headquarters Security Operations: Questions and Answers on the  

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

Questions and Answers on the New Access Control System at DOE Headquarters Questions and Answers on the New Access Control System at DOE Headquarters Q1 Why is the current access control system to security areas being changed? Q2 How is the new access control system different from the existing one? Q3 Who is affected? Q4 When will the new proximity card readers be installed? Q5 How will affected personnel at DOE HQ be notified about the installation of the proximity card readers that will affect their access to the HQ facilities and security areas, and the actions they will be required to take to assure their HSPD-12 badge will operate in the new readers? Q6 What will DOE HQ "Q" and "L" badged employees need to do? Q7 Will all DOE HQ security areas be changed out to the new access control system at the same time?

108

22680  

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

QUARTERLY PROGRAM REPORT QUARTERLY PROGRAM REPORT State: __________________ Budget period: / / - / / Grant Number: __________________ I. GRANT OUTLAYS - FUNDS SUBJECT TO DOE PROGRAM RULES (rounded to the nearest dollar) DOE F 540.3 (08/05) OMB Control No. 1910-5127 Expiration Date: 6/30/08 A. OUTLAYS BY FUND SOURCE DOE Other funds included in grant budget, section A B. OUTLAYS BY FUNCTION Grantee Administration Subgrantee Administration Grantee T&TA Subgrantee T&TA Program Operations Total Health and Safety Vehicles and Equipment - Acquisition Cost* Liability Insurance Leveraging Financial Audits Vehicles and Equipment - Amortized Cost* Total Grant Outlays Total Grant Outlays Reporting Period Quarter / - / Q1 / - / Q2 / - / Q3 / - / Q4 Total To Date Notes: Total grant outlays must equal outlays reported on the Financial Status Report, line 10.d.

109

Physics 182 Equation Sheet for Exams Good Stuff from 181  

E-Print Network [OSTI]

QH = 1 - QC QH Carnot = 1 - TC TH Refrigerator: Win + QC = QH K = QC Win = QC QH -QC KCarnot = TC TH -TC 1 #12;· Chapter 25: Coulomb Law: |Fq1q2 | = K |q1||q2| r2 = 1 40 |q1||q2| r2 Charge in a Field: F = q E Field of a Point Charge q: E = K q r2 ^r = 1 40 q r2 ^r · Chapter 26: Dipole Moment: p = (qs

Alexander, Stephen G.

110

Carbon Fiber Technology Facility  

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

FY13Q4 * Forecast finish FY13Q2 * Currently in design phase * Barriers addressed - Cost - Inadequate supply base - Manufacturability * 34.77M Budget - No cost share * All...

111

E-Print Network 3.0 - antenatal corticosteroid therapy Sample...  

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

Genetics, National Institutes of Health Collection: Biology and Medicine 50 Uricase for gout treatment Chapter 5.1 Summary: ) + q 4 w (for 3 y) 0.20 mgkg; q 1 w (for 16 m)...

112

EV-Smart Grid Research & Interoperability Activities 2014 DOE...  

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

to establish interoperability centers - Q1, FY 2012 Official Argonne launch - Q4, FY 2013 2 Budget* FY2012 - 1180 K FY2013 - 2200 K FY2014 - 1550 K Barriers...

113

Microsoft Word - 2011Q2Report.doc  

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

1) 1) Mechanisms Leading to Co-Existence of Gas and Hydrate in Ocean Sediments Submitted by: The University of Texas at Austin 1 University Station C0300 Austin, TX 78712-0228 Prepared for: United States Department of Energy National Energy Technology Laboratory July 26, 2011 Office of Fossil Energy 1 MECHANISMS LEADING TO CO-EXISTENCE OF GAS AND HYDRATE IN OCEAN SEDIMENTS CONTRACT NO. DE-FC26-06NT43067 QUARTERLY PROGRESS REPORT Reporting Period: 1 Apr 11 - 30 Jun 11 Prepared by Steven L. Bryant Department of Petroleum and Geosystems Engineering The University of Texas at Austin 1 University Station C0300 Austin, TX 78712-0228 Phone: (512) 471 3250 Email: steven_bryant@mail.utexas.edu Ruben Juanes Department of Civil and Environmental Engineering

114

Microsoft Word - Q2 2010 DOE Report Aug 26.doc  

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

Half 2010 Half 2010 ConocoPhillips Gas Hydrate Production Test Submitted by: ConocoPhillips 700 G Street Anchorage, AK 99501 Principal Investigator: David Schoderbek Prepared for: United States Department of Energy National Energy Technology Laboratory August 26, 2010 Office of Fossil Energy Disclaimer This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or

115

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.

116

Hydrogen Tank Project Q2 Report - FY 11  

SciTech Connect (OSTI)

Quarterly report that represents PNNL's results of HDPE, LDPE, and industrial polymer materials testing. ASTM D638 type 3 samples were subjected to a high pressure hydrogen environment between 3000 and 4000 PSI. These samples were tested using an instron load frame and were analyzed using a proprietary set of excel macros to determine trends in data. The development of an in-situ high pressure hydrogen tensile testing apparatus is discussed as is the stress modeling of the carbon fiber tank exterior.

Johnson, Kenneth I.; Alvine, Kyle J.; Skorski, Daniel C.; Nguyen, Ba Nghiep; Kafentzis, Tyler A.; Dahl, Michael E.; Pitman, Stan G.

2011-05-15T23:59:59.000Z

117

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.

118

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.

119

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.

120

Measurements of the ?* p --> ?(1232) reaction at low Q2  

E-Print Network [OSTI]

We report new p$(\\vec{e},e^\\prime p)\\pi^\\circ$ measurements in the $\\Delta^{+}(1232)$ resonance at the low momentum transfer region utilizing the magnetic spectrometers of the A1 Collaboration at MAMI. The mesonic cloud dynamics are predicted to be dominant and appreciably changing in this region while the momentum transfer is sufficiently low to be able to test chiral effective calculations. The results disagree with predictions of constituent quark models and are in reasonable agreement with dynamical calculations with pion cloud effects, chiral effective field theory and lattice calculations. The reported measurements suggest that improvement is required to the theoretical calculations and provide valuable input that will allow their refinements.

N. Sparveris; S. Stave; P. Achenbach; C. Ayerbe Gayoso; D. Baumann; J. Bernauer; A. M. Bernstein; R. Bohm; D. Bosnar; T. Botto; A. Christopoulou; D. Dale; M. Ding; M. O. Distler; L. Doria; J. Friedrich; A. Karabarbounis; M. Makek; H. Merkel; U. Muller; I. Nakagawa; R. Neuhausen; L. Nungesser; C. N. Papanicolas; A. Piegsa; J. Pochodzalla; M. Potokar; M. Seimetz; S. Sirca; S. Stiliaris; Th. Walcher; M. Weis

2013-07-02T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


121

Integrated Solar Thermochemical Reaction System- FY13 Q2  

Broader source: Energy.gov [DOE]

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

122

Microsoft Word - Issue FY2010 Q1 Draft 20091228.doc  

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

On October 5, 2009, On October 5, 2009, President Obama signed Executive Order (EO) 13514, Federal Leadership in Environmental, Energy, and Economic Performance. 1 This order represents a transformative shift in the way the government will operate by establishing greenhouse gas emissions (GHGs) as the integrating metric for tracking progress toward federal sustainability. The new order does not replace EO 13423, Strengthening Federal Environmental, Energy, and Transportation Management. Like previous orders, the new order relies heavily on effective real property asset management practices to achieve its goals. It provides new direction in these areas: * Stormwater, potable, industrial and landscaping water * Waste including recycling and composting * Integrated planning

123

9 Science Service FeaturQ 1 IHY THE FIEATHER ?  

E-Print Network [OSTI]

increases the wind velocity indoors; Systems of re- frigeration lover the temperature of cars Or buildings n moisture, Air driers o r moisteners i n operation night and day are not Cotton mills prefer, "condition11 t h e i r air and keep the windows shut, Modern mills now Lsather, too, may be injured by lack

124

System Advisor Model Enhancements for CSP- FY13 Q1  

Broader source: Energy.gov [DOE]

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

125

Q1 Review Session Complex system fails for complex reasons!  

E-Print Network [OSTI]

interlocks -- protective circuits · Therac-25 · software shared code with Therac-20 · software interlock that, in practice, hardware interlocks are necessary for safety. · True. The authors discuss the need of radiation, contributed to the accidents. · True. Some of the accidents occurred when one part of the machine

126

NBB Enclosed Particle Receiver- FY13 Q1  

Broader source: Energy.gov [DOE]

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

127

Advanced Manufacture of Reflectors- FY13 Q1  

Broader source: Energy.gov [DOE]

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

128

Quarterly SSP Experiment Summary-Q1FY14 1  

National Nuclear Security Administration (NNSA)

fundamental properties of material, plasma, radiation, fusion ignition, and thermonuclear burn at temperatures and pressures relevant to those obtained in a nuclear weapon....

129

FY 2014 Metric Summary | Department of Energy  

Office of Environmental Management (EM)

4 Metric Summary FY 2014 Metric Summary FY 2014 Q1 Metric Summary.pdf FY 2014 Q2 Metric Summary.pdf FY 2014 Q3 Metric Summary.pdf More Documents & Publications FY 2014 Q3 Metric...

130

PowerPoint Presentation  

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

1, 2013 (NEW PROJECT) Planned end date: September 30, 2014 Key Milestones 1. 200g Dark Red Pigment, End Q1 2. Additional Pigments Identified, End Q2 3. 500g of 2 New Pigments,...

131

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

Broader source: Energy.gov [DOE]

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

132

TOTAL_ARRA_Homes_Weatherized_thru_Q4_2010_3.7.11.pdf | Department...  

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

TOTALARRAHomesWeatherizedthruQ420103.7.11.pdf TOTALARRAHomesWeatherizedthruQ420103.7.11.pdf TOTALARRAHomesWeatherizedthruQ420103.7.11.pdf More Documents &...

133

U.S. Residential Photovoltaic (PV) System Prices, Q4 2013 Benchmarks...  

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

by the top 10 installers in terms of installed capacity, based on data from the California Solar Initiative (CSI 2013). Focusing our analysis on large installers represents a...

134

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

Broader source: Energy.gov [DOE]

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

135

http://www.eh.doe.gov/nepa/process/ll/95q4.htm  

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

4TH 4TH QUARTER FY 1995 Office of NEPA Policy and Assistance U.S. Department of Energy December 1, 1995 INTRODUCTION To foster continuing improvement of the Department's National Environmental Policy Act (NEPA) compliance program, the Secretarial Policy Statement on NEPA, issued June 13, 1994, requires the Office of Environment, Safety and Health to solicit comments on lessons learned in the process of completing NEPA documents from the NEPA Document Manager, the NEPA Compliance Officer, and team members after completing each environmental impact statement (EIS) and environmental assessment (EA), and to distribute a quarterly summary to all NEPA Compliance Officers and NEPA Document Managers. This quarterly report summarizes the lessons learned for documents completed between July 1 and

136

On CORI Results Merging Ilya Markov1  

E-Print Network [OSTI]

a source R: snorm(d|q) = 1 + 0.4 · sMinMax (R|q) 1.4 · sMinMax (d|q), (1) P. Serdyukov et al. (Eds.): ECIR. Arampatzis, and F. Crestani where sMinMax (R|q) denotes the relevance of the source R to a query q and rewrite Eq. 1 as follows: snorm(d|q) = 1 + · sMinMax (R|q) 1 + · sMinMax (d|q). (2) Depending on , Eq. 2

Arampatzis, Avi

137

Frequently Asked Questions Form EIA-857  

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

Natural Gas Survey Forms FAQ Natural Gas Survey Forms FAQ EIA-857, "Monthly Report of Natural Gas Purchases and Deliveries to Consumers" You may always call Amy Sweeney for assistance at (202) 586-2627 or e-mail us at OOG.SURVEYS@eia.gov. Q1. How do I get a copy of the form and/or the instructions? Q2. What version of the form should I use? Q3. How do I submit the form? Q4. When is the form due? Q5. My company does not have the information required on the Form EIA-857 within 30 days after the end of the report month. Can we get an extension? Q6. Who should I inform of a change in the contact person in our company for Form EIA-857? Q7. Who should I inform if our company is sold, merged with another company, or buys another natural gas company? Q8. Why does my company always get selected to file Form EIA-857?

138

DOE FY10_Svc_Cont_Inv 122910 v2 MAX.xlsx  

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

Fixed Fixed Price Cost T&M/LH Other Competed Not Competed Blank Q1 Q2 Q3 Q4 B505 Cost Benefit Analyses $0 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% R406 Policy Review/Development Services $0 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% R407 Program Evaluation Services $6,598,775 0% 1% 0% 99% 0% 30% 5% 65% 5% 33% 32% 31% R408 Program Management/Support Services $311,028,791 1% 2% 67% 32% 0% 90% 4% 6% 26% 25% 13% 35% R409 Program Review/Development Services $49,991 0% 100% 0% 0% 0% 100% 0% 0% 0% 0% 0% 100% R413 Specifications Development Service $106,958 0% 0% 100% 0% 0% 100% 0% 0% 0% 100% 0% 0% R707 Management Services/Contract & Procurement Support $35,519,976 0% 3% 93% 4% 0% 0% 100% 0% 17% 1% 49% 32% R423 Intelligence Services $10,385,300 0% 2% 0% 98% 0% 57% 0% 43% 7% 39% 26% 29% R425 Engineering and Technical Services $315,519,561 1% 2% 58% 33% 7% 93% 6% 1% 10% 25% 23% 42% R414 Systems Engineering Services

139

Figure 7.1. Control of an alarm system. Figure 7.2. A simple memory element.  

E-Print Network [OSTI]

-digit BCD counter. Enable Q0 Q1 Q2 D0 D1 D2 Load Clock 1 0 0 0 Clock Q30 D3 Enable Q0 Q1 Q2 D0 D1 D2 Load Clock 0 0 0 Q30 D3 BCD0 BCD1 Clear Figure 7.30. Johnson counter. D Q Q Clock D Q Q D Q Q Q0 Q1 Qn 1 by CAD tools. Data Clock Latch #12;Figure 7.34. Timing simulation of storage elements. Figure 7.35. Code

Kalla, Priyank

140

On the determination of phosphorous via charged particle activation analysis  

E-Print Network [OSTI]

of Cyclotron Terminal . "or Activation Analysis Ql ? WATER INLET Q2 ? BNC CONNECTOR Q3 ? LUCITE Q4 ? CA RBON Figure 3. Four-leaved Carl. on Pea, -. Monitor 1. Ta COLLIMATOR 2. Cu HEAT SINK K MONITOR 4. SAMPLE 5. Cu BASE PLATE 6. WATER COOLING I 2... of Cyclotron Terminal . "or Activation Analysis Ql ? WATER INLET Q2 ? BNC CONNECTOR Q3 ? LUCITE Q4 ? CA RBON Figure 3. Four-leaved Carl. on Pea, -. Monitor 1. Ta COLLIMATOR 2. Cu HEAT SINK K MONITOR 4. SAMPLE 5. Cu BASE PLATE 6. WATER COOLING I 2...

Poland, John Edward

2012-06-07T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


141

Evaluation of the pseudo force method applied to large strain dynamic problems  

E-Print Network [OSTI]

) {F2+3 Fl) + Y[] ql q 25 [] + 25 [M] {23q -3q ) (4. 24) The velocities are obtained by rearranging Eq. (4. 23). 5 2 1 1 {q2)= 3Xt{q2)- ht(ql)+ 3ht{q, )- r(ql) The stability of the Park method is compared with 38 that of the Houbolt method... ) {F2+3 Fl) + Y[] ql q 25 [] + 25 [M] {23q -3q ) (4. 24) The velocities are obtained by rearranging Eq. (4. 23). 5 2 1 1 {q2)= 3Xt{q2)- ht(ql)+ 3ht{q, )- r(ql) The stability of the Park method is compared with 38 that of the Houbolt method...

Richardson, Edward Quentin

2012-06-07T23:59:59.000Z

142

113-0033 7-3-1 153-8505 4-6-1-Ee405  

E-Print Network [OSTI]

13, Q2 87.8% Q4 12 6. MR CG MR HMD #12; 13. [1] R. Azuma "A Survey] R. Azuma, Y. Baillot, R. Behringer, S. Feiner, S. Julier, and B. MacIntyre "Recent Advances. Vlahakis, N. Ioannidis, J. Karigiannis, M. Tsotros, M.l Gounaris, D. Stricker, T. Gleue, P. Daehne and L

Tokyo, University of

143

Vegetables, Fruit, and Lung Cancer in the Iowa Women's Health Study  

Science Journals Connector (OSTI)

...65-69, 70-74), total energy (quartile), education...ginger, kelp and seaweeds Dark green leafy vegetables...0-118.5 118.6 Dark green leafy vegetables...Q2 Q3 Q4 (high) Total energy, kcal Male (M) 2157...in Japan. Analysis of survey data on incidence in Aomori...

Kristi A. Steinmetz; John D. Potter; and Aaron R. Folsom

1993-02-01T23:59:59.000Z

144

BIMA ARRAY DETECTIONS OF HCN IN COMETS LINEAR (C/2002 T7) AND NEAT (C/2001 Q4)  

E-Print Network [OSTI]

al. 1997; Womack, Festou, & Stern 1997; Biver et al. 1999a), Comet Hale-Bopp (C/1995 O1) (e of the first interferometric observations of HCN in Comet Hale-Bopp. From the distribution and temporal). The deviations from the Haser model were explained by the existence of jets releasing HCN gas, a conclusion

Hogerheijde, Michiel

145

Slide 1  

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

Kassianov Kassianov Aerosol remote sensing under partly cloudy conditions: How well are we doing? Background Ground-based/airborne lidar observations: Raman Lidar (RL), Micropulse Lidar (MPL) High Spectral Resolution Lidar (HSRL) Can they be extended by other observations? Outline Q1: Why it is important? Q2: What issues do we have? Q3: How can we address them? Q1: IAE and Aerosol RF Simultaneous and coincident measurements of aerosol and cloud properties are desirable: Indirect Aerosol Effects (IAEs) Aerosol Radiative Forcing (RF) Ghan and Schwartz, BAMS, 2007 Myhre et al., ACP, 2009 Q1: Occurrence Partly cloudy sky: 30% (SGP), 40-80% (TWP) Credit: C. Long Q2: 3D Problem Examples of 3D Cloud Impacts: Positive Cloud Radiative Forcing (RF) Reflectance Enhancement Cloud Screening Q2: Positive Cloud RF

146

Microsoft Word - Q2 '09 DOE Report 28 Aug 09.doc  

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

Second Quarter 2009 Second Quarter 2009 ConocoPhillips Gas Hydrate Production Test Submitted by: ConocoPhillips 700 G Street Anchorage, AK 99501 Principle Investigator: David Schoderbek Prepared for: United States Department of Energy National Energy Technology Laboratory August 28, 2009 Office of Fossil Energy 2 Disclaimer This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or

147

Microsoft Word - Q2 2012 DOE Report 26 July 12.doc  

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

First Half 2012 First Half 2012 ConocoPhillips Gas Hydrate Production Test Submitted by: ConocoPhillips 700 G Street Anchorage, AK 99501 Principal Investigator: David Schoderbek Prepared for: United States Department of Energy National Energy Technology Laboratory July 31, 2012 Office of Fossil Energy Disclaimer This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or

148

http://www.eh.doe.gov/nepa/process/ll/95q2.htm  

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

2ND 2ND QUARTER FY 1995 Office of NEPA Policy and Assistance U.S. Department of Energy June 1, 1995 INTRODUCTION To foster continuing improvement of the Department's National Environmental Policy Act (NEPA) compliance program, the Secretarial Policy Statement on NEPA, issued June 13, 1994, requires the Office of Environment, Safety and Health to solicit comments from the NEPA Document Manager, the NEPA Compliance Officer, and team members after completing each environmental impact statement and environmental assessment on lessons learned in the process, and to distribute a quarterly summary to all NEPA Compliance Officers and NEPA Document Managers. This quarterly report summarizes the lessons learned for documents completed between January 1 and March 31, 1995. It is based primarily on responses to the revised questionnaire that was

149

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.

150

Probing New Physics with $q^2$ distributions in $\\bar{B} \\to D^{(*)} ?\\bar?$  

E-Print Network [OSTI]

Recent experimental results for the ratios of the branching fractions of the decays $\\bar{B} \\to D^{(*)} \\tau \\bar\

Yasuhito Sakaki; Minoru Tanaka; Andrey Tayduganov; Ryoutaro Watanabe

2014-12-11T23:59:59.000Z

151

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.

152

Flavor decomposition of the nucleon electromagnetic form factors at low $Q^2$  

E-Print Network [OSTI]

The spatial distribution of charge and magnetization within the proton is encoded in the elastic form factors. These have been precisely measured in elastic electron scattering, and the combination of proton and neutron form factors allows for the separation of the up- and down-quark contributions. In this work, we extract the proton and neutron form factors from world's data with an emphasis on precise new data covering the low-momentum region, which is sensitive to the large-scale structure of the nucleon. From these, we separate the up- and down-quark contributions to the proton form factors. We combine cross section and polarization measurements of elastic electron-proton scattering to separate the proton form factors and two-photon exchange (TPE) contributions. We combine the proton form factors with parameterization of the neutron form factor data and uncertainties to separate the up- and down-quark contributions to the proton's charge and magnetic form factors. The extracted TPE corrections are compare...

Qattan, I A; Alsaad, A

2015-01-01T23:59:59.000Z

153

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.

154

Assessment of SCaMPR and NEXRAD Q2 Precipitation Estimates Using Oklahoma Mesonet Observations  

Science Journals Connector (OSTI)

Although satellite precipitation estimates provide valuable information for weather and flood forecasts, infrared (IR) brightness temperature (BT)-based algorithms often produce large errors for precipitation detection and estimation during deep ...

Ronald Stenz; Xiquan Dong; Baike Xi; Robert J. Kuligowski

2014-12-01T23:59:59.000Z

155

TOTAL ARRA Homes Weatherized thru Q2 2010 8.19.10.xls  

Energy Savers [EERE]

Weatherization Assistance Program Homes Weatherized By State through 06302010 (Calendar Year) *State Number of Homes Weatherized in 2nd Quarter 2010 (Apr-Jun) Recovery Act...

156

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.

157

Microsoft Word - SAND2013-2448P - FY13Q2 Field Aged Cable Assesment...  

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

but could be confirmed at a later date) cable (bonded jacketinsulation) from the Zion Nuclear Power Station. Physical property testing was performed on the as received cables....

158

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.

159

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.

160

EE290Q-2 Spring 2009 1 Abstract--Wireless sensor networks (WSNs) have proven and  

E-Print Network [OSTI]

reserves, power scavenging), metrics, and tradeoffs affecting energy-aware routing strategies. The proposed production lines, solar power systems, building automation, medical devices, weather monitoring and many performance and thus, its connectivity/survivability. Although there are a number of metrics for routing

Sanders, Seth

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


161

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.

162

Application of Fibonacci oscillators in the Debye model  

E-Print Network [OSTI]

In this paper we study the thermodynamics of a crystalline solid by applying q-deformed algebra of Fibonacci oscillators through the generalized Fibonacci sequence of two real and independent deformation parameters q1 and q2. We find a (q1, q2)-deformed Hamiltonian and consequently the q-deformed thermodynamic quantities. The results led us to interpret the deformation parameters acting as disturbance or impurities factors modifying the characteristics of a crystal structure. More specifically, we found the possibility of adjusting the Fibonacci oscillators to describe the change of thermal conductivity of a given element as one inserts impurities.

Marinho, Andre A A; Chesman, C

2014-01-01T23:59:59.000Z

163

Joint Top-K Spatial Keyword Query Processing Dingming Wu, Man Lung Yiu, Gao Cong, and Christian S. Jensen, Fellow, IEEE  

E-Print Network [OSTI]

-8200 Aarhus, Denmark. E-mail: csj@cs.au.dk p1 q3 q1 {pizza, grill} {curry, sushi}{curry, seafood} Q p3 p2 q2 {sushi, soup, curry} {seafood, grill, sushi} {seafood, sushi} p4 {soup, steak} Q Fig. 1. Top1 prefers `curry' and `sushi,' user q2 prefers `seafood' and `sushi,' and user q3 prefers `curry

Yiu, Man Lung

164

Low-Cost Metal Hydride TES Systems- FY13 Q1  

Broader source: Energy.gov [DOE]

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

165

Table 1. Questions Q1, gender 1 = male, 2 = female. (3 occurences of "Not  

E-Print Network [OSTI]

on AoC compared to exercises in other courses" Likert scale where 1 = Strongly Agree, 2 = Somewhat Agree value 3). Q7, "AoC is more motivating than a traditional set of exercises" Likert scale as for Q5. Q9, "I perceive the learning effect by using AoC as good compared to traditional exercises Likert scale

Natvig, Lasse

166

Microsoft Word - fy09_annualtarget_climatemodeling1_Q1 _2_.doc  

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

WD, Bitz CM, Blackmon ML, Bonan GB, Bretherton CS, Carton JA, Chang P, Doney SC, Hack JJ,Henderson TB (2006) The Community Climate System Model Version 3 (CCSM3). Journal of...

167

Q1Report for CADWR Project: Desalination Using Carbon NAnotube Membranes  

SciTech Connect (OSTI)

In this research and development project, LLNL will leverage the process for fabrication of the membranes developed by our internally funded effort (LLNL Laboratory Directed Research and Development). LLNL will then employ chemical manipulations to modify charge at the ends of the nanotubes and make the membranes more selective to either positive or negative ions through a combination of size and charge selectivity. LLNL's goal is to demonstrate ion exclusion while preserving high permeabilities and low energy use. Success of this research and development project may warrant further developments in the fabrication of membranes.

Bakajin, O

2008-05-14T23:59:59.000Z

168

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

SciTech Connect (OSTI)

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

Tyler L. Westover

2014-04-01T23:59:59.000Z

169

High Efficiency Thermal Energy Storage System for CSP- FY13 Q1  

Broader source: Energy.gov [DOE]

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

170

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

Broader source: Energy.gov [DOE]

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

171

Low-Cost Heliostat for Modular Systems- FY13 Q1  

Broader source: Energy.gov [DOE]

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

172

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

Broader source: Energy.gov [DOE]

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

173

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

Broader source: Energy.gov [DOE]

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

174

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

Broader source: Energy.gov [DOE]

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

175

1Q1 Mathematics for Engineers and Scientists Lecturer: Professor Paul Glendinning  

E-Print Network [OSTI]

this as understood. #12;3.8 Integration by parts Stroud P15 Integrate the product formula of dierentiation: (uv)H = uHv + uvH to get Z (uv)Hdx = Z uHv dx + Z uvHdx Now, by the Fundamental Theorem of Calculus the left hand side is just [uv] so [uv] = Z uHv dx + Z uvHdx or Z uvHdx = [uv] Z uHv dx This is the formula

Glendinning, Paul

176

The neutron electric form factor to Q = 1.45 (GeV/c)  

E-Print Network [OSTI]

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

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

2004-01-01T23:59:59.000Z

177

FY14 Q1 Progress Report for SECA Core Technology Program  

SciTech Connect (OSTI)

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

Stevenson, Jeffry W.; Koeppel, Brian J.

2014-01-31T23:59:59.000Z

178

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

Gasoline and Diesel Fuel Update (EIA)

ministration (EIA), Office of Energy Markets and End Use, under the direc tion "of Wray Smith (202252-1617). General supervision is provided by W. Calvin Kilgore (202252-1130),...

179

Quarterly SSP Experiment Summary-FY13-1Q 1  

National Nuclear Security Administration (NNSA)

fundamental properties of material, plasma, radiation, fusion ignition, and thermonuclear burn at temperatures and pressures relevant to those obtained in a nuclear weapon....

180

Microsoft Word - DE-FE0010160 Q1 report.doc  

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

Oil & Natural Gas Technology Oil & Natural Gas Technology DOE Award No.: DE-FE0010160 Quarterly Research Performance Progress Report (Period ending 12/31/2012) Advanced Hydrate Reservoir Modeling Using Rock Physics Techniques 10/1/2012 - 9/30/2013 Submitted by: Principal Investigator: Dan McConnell Fugro GeoConsulting, Inc. DUNS #: 118972301 6100 Hillcroft Ave., 3 rd Floor Houston, TX 77081 e-mail: dmcconnell@fugro.com Phone number: (713) 778-6801 Prepared for: United States Department of Energy National Energy Technology Laboratory January 31, 2013 Executive Summary This research effort will focus on developing and refining techniques that integrate rock physics modeling, amplitude analysis, and spectral decomposition to characterize complex gas hydrate reservoirs. The

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


181

acs_cm_cm-2009-03769q 1..3  

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

pubs.acs.org/cm pubs.acs.org/cm Published on Web 02/16/2010 r 2010 American Chemical Society Chem. Mater. 2010, 22, 1943-1945 1943 DOI:10.1021/cm903769q Universal and Solution-Processable Precursor to Bismuth Chalcogenide Thermoelectrics Robert Y. Wang, † Joseph P. Feser, ‡ Xun Gu, § Kin Man Yu, † Rachel A. Segalman, †,§ Arun Majumdar, †,‡ Delia J. Milliron,* ,† and Jeffrey J. Urban* ,† † Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, ‡ Department of Mechanical Engineering, and § Department of Chemical Engineering, University of California, Berkeley, California 94720 Received December 15, 2009 Revised Manuscript Received February 7, 2010 Thermoelectric materials convert thermal power into electrical power and vice versa. In practice, thermoelectric coolers and power generators are made by alternately

182

MSSV FAQ 2013-14 Q1 How close is Murano to the University?  

E-Print Network [OSTI]

a kitchen with a cooker, fridge/freezer, microwave, toaster and kettle. Each large flat (10/12 persons) has a #12;kitchen with 2 cookers, 2 fridges and freezers, microwave, kettle, toaster. Ironing equipment

Glasgow, University of

183

Comparison of an exact analytic second born term with its asymptotic approximations  

E-Print Network [OSTI]

) If we use this wave to calculate the scattering amplitude, T ?(Q), for a transition to y we obtain T, ?(Q) = mp & y (r) ~e ' ' Vp(q) + ? dQ"e '( / I l' V (Q/2 ? Q") I 2(H ? e ) + 2k (Q" + Q/2) ? iI, e Vp(Q + Q/2)lxo(r) ) Here ke=vp ~ (6) Q=(Qs Qz... similar to (I+r) '=Q( ? *)' 1=0 Thus equation (19) becomes z &1. (20) 1 ( ? 2(H, ? 6) 2(6' ? e?) y 2k, (Q" y Q/2) ? iI' ~ (2(6 ? s?) + 2k, . (Q" + Q/2) ? fr) where the radius of convergence is not as clearly defined as in the above expansion...

Fitzpatrick, Mathew Jared

2012-06-07T23:59:59.000Z

184

The Optimal Design of Investments in Biodiversity Conservation  

E-Print Network [OSTI]

The Optimal Design of Investments in Biodiversity Conservation q1 p1 Area Price q2 p2 qd qc Paul R to terrestrial biodiversity and financial investment in habitat conservation efforts has become a cornerstone the needs of biodiversity leads to ineffective conservation programmes and may even risk conservation

Gray, Matthew

185

On abelian automorphism groups of Mumford curves  

Science Journals Connector (OSTI)

......P1,P2,Q1,Q2 be four distinct points on the boundary of Tk...by . Since the fixed point of in the boundary is...Let v1, v2 be two lifts of v1, v2 on the BruhatTits...have the same fixed points. Hence a lift of the edge e in TN......

Aristides Kontogeorgis; Victor Rotger

2008-06-01T23:59:59.000Z

186

Fluctuation theory of connectivities for subcritical random cluster models  

E-Print Network [OSTI]

Fluctuation theory of connectivities for subcritical random cluster models Massimo Campanino subcritical regime; the latter is known to be true, in any dimensions, when q = 1, q = 2, and when q. Campanino et al./Connectivities of subcritical random cluster models 2 variance principle, Ruelle operator

187

AN OPTIMAL ITERATIVE METHOD FOR THE TIME-DEPENDENT STOKES PROBLEM  

E-Print Network [OSTI]

well for the Mini element. Numerical experiments indicate that this preconditioner also works for the Q will propose a preconditioner which is uniform in " and h, where h is the grid size parameter. The system (2 at least the Mini element and seemingly the Q 2 Q 1 element possess. We notice that the " parameter only

188

Dualities and Topological Field Theories from Twisted Geometries  

E-Print Network [OSTI]

modes on the D2-brane and F1-strings for (a) Sectors 1 anda) A fundamental string (F1) bound to the D2-brane. The D2-12 q 13 ? q 1m SR q 23 F1 q 20 q 21 q 22 q 2m SR F1 q

Markov, Ruza

2012-01-01T23:59:59.000Z

189

Total Space Heating Water Heating Cook-  

Gasoline and Diesel Fuel Update (EIA)

Q Q Q Q Q Q Q Q Q Q Food Service ... Q Q Q Q Q Q Q Q Q Q Health Care ... 11 6 2 Q 2 5.6 3.3 0.8 Q 1.3 Inpatient...

190

Question and Answers Alternative Fuel Readiness Plans  

E-Print Network [OSTI]

Question and Answers Alternative Fuel Readiness Plans PON-13-603 September 3, 2013 Eligibility Q1 to readiness plans? A1 This solicitation is limited to readiness planning only for alternative fuels. Q2 In regards to PON-13-603 - Alternative Fuel Readiness Plans, is electricity used for transportation

191

On bounding the bandwidth of graphs with symmetry - Optimization ...  

E-Print Network [OSTI]

Hamming graph H(2,q) (also known as the lattice graph) has bandwidth equal to. (q+1)q. 2. ?1 .... 59. 10 3 120. 72. 75. 76. 90. Table 9: Bounds on the bandwidth of K(v,2) and K(v,3). v d meig .... Freeman, San Francisco, 1979. [19] Graham, A.

2013-08-08T23:59:59.000Z

192

Optimal control approach to termination of re-entry waves in cardiac electrophysiology  

E-Print Network [OSTI]

)Ie(t) - c2 (x)Ie(t) in Q (2) v t = · ¯i v + · ¯i u - Iion(v, w) + Itr(x, t) in Q (3) w t = G(v, w) in Q, (4 electrode. The Iion(v, w) is the current density flowing through the ionic channels and the function g(v, w

Kunisch, Karl

193

Weak solutions to a parabolic nonlinear system arising in biological dynamic in the soil  

E-Print Network [OSTI]

+ µ + r + , q2(u) = k u1 Ks + u2 , q3(u) = c1 u5 Km + u5 , q4(u) = c2 u5 Km + u5 , q5(u) = , q6(u) = 0, f1(u) = 0, f2(u) = u5 Km + u5 (c1u3 + c2u4) + u5 + µu1 2 , f3(u) = u5 + µu1 2 , f4(u) = 0, f5(u) = u

Frey, Pascal

194

HODGE-THEORETIC INVARIANTS FOR ALGEBRAIC CYCLES MARK GREEN AND PHILLIP GRIFFITHS  

E-Print Network [OSTI]

) Spreads; explanation of the idea (3) Construction of the filtration on CHp (X)Q (4) Interpretations, these conjectures would have the following implications for the Chow group CHP (X)Q: (I) There is a filtration CHp (X)Q = F0 CHp (X)Q F1 CHp (X)Q(1.1) · · · Fp CHp (X)Q Fp+1 CHp (X)Q = 0 whose successive

195

Fully differential heavy quark contributions to the photon structure functions $F_{2}^?(x,Q^2)$ and $F_{L}^?(x,Q^2)$ at next-to-leading order QCD  

E-Print Network [OSTI]

Fully differential heavy quark contributions to the photon structure functions in deeply inelastic scattering are computed in next-to-leading order QCD, including both the direct and resolved contributions. A variety of distributions are presented and discussed. Several of the distributions show marked differences between the resolved and direct cases due primarily to the presense of the gluon distribution in the former and lack thereof in the later.

B. W. Harris; J. F. Owens

1996-03-13T23:59:59.000Z

196

Elemental and structural analysis of silicon forms in herbal drugs using silicon-29 MAS NMR and WD-XRF spectroscopic methods  

Science Journals Connector (OSTI)

The objective of this work was to study concentration of silicon and its structural forms present in herbal drugs. Equisetum arvense and Urtica dioica L. from teapot bags, dietary supplements (tablets and capsules) containing those herbs, dry extract obtained from a teapot bag of E. arvense, and samples of the latter herb harvested in wild habitat over four months were studied using wavelength dispersive X-ray spectroscopy (WD-XRF) and high-resolution solid-state 29Si NMR. The highest concentration of Si, ca. 27mg/g, was found in the herbal material from the teapot bags containing E. arvense. The Si content in natural E. arvense (whole plants) increased from May to August by ca. 7mg/g, reaching value 26mg/g. Three different silicon forms were detected in the studied herbal samples: Si(OSi)4 (Q4), Si(OH)(OSi)3 (Q3) and Si(OH)2(OSi)2 (Q2). Those sites were populated in E. arvense in the following order: Q4?Q3>Q2. A dramatic, ca. 50-fold decrease of the Si concentration during the infusion process was observed. The infusion process and the subsequent drying procedure augmented population of the Q4 sites at the cost of the Q2 sites. The WD-XRF and 29Si NMR methods occurred useful and complementary in the study of herbal materials.

L. Pajchel; P. Nykiel; W. Kolodziejski

2011-01-01T23:59:59.000Z

197

Precision Measurements of the Nucleon Strange Form Factors at Q^2 ~ 0.1GeV^2  

SciTech Connect (OSTI)

We report new measurements of the parity-violating asymmetry A{sub PV} in elastic scattering of 3 GeV electrons off hydrogen and {sup 4}He targets with ({theta}{sub lab}) {approx} 6.0{sup o}. The {sup 4}He result is A{sub PV} = (+6.40 {+-} 0.23 (stat) {+-} 0.12 (syst)) x 10{sup -6}. The hydrogen result is A{sub PV} = (-1.58 {+-} 0.12 (stat) {+-} 0.04 (syst)) x 10{sup -6}. These results significantly improve constraints on the electric and magnetic strange form factors G{sub E}{sup s} and G{sub M}{sup s}. We extract G{sub E}{sup s} = 0.002 {+-} 0.014 {+-} 0.007 at (Q{sup 2}) = 0.077 GeV{sup 2}, and G{sub E}{sup s} + 0.09 G{sub M}{sup s} = 0.007 {+-} 0.011 {+-} 0.006 at (Q{sup 2}) = 0.109 GeV{sup 2}, providing new limits on the role of strange quarks in the nucleon charge and magnetization distributions.

Armando Acha Quimper; Konrad Aniol; David Armstrong; John Arrington; Todd Averett; Stephanie Bailey; James Barber; Arie Beck; Hachemi Benaoum; Jay Benesch; Pierre Bertin; Peter Bosted; Florentin Butaru; Etienne Burtin; Gordon Cates; Yu-Chiu Chao; Jian-Ping Chen; Eugene Chudakov; Evaristo Cisbani; Brandon Craver; Francesco Cusanno; Raffaele De Leo; Piotr Decowski; Alexandre Deur; Robert Feuerbach; John Finn; Salvatore Frullani; Sabine Fuchs; Kirsten Fuoti; Ronald Gilman; Lindsay Glesener; Klaus Grimm; Joseph Grames; Jens-ole Hansen; John Hansknecht; Douglas Higinbotham; Richard Holmes; Timothy Holmstrom; Hassan Ibrahim; Cornelis De Jager; Xiaodong Jiang; Joseph Katich; Lisa Kaufman; Aidan Kelleher; Paul King; Ameya Kolarkar; Stanley Kowalski; Elena Kuchina; Krishna Kumar; Luigi Lagamba; Peter Laviolette; John LeRose; Richard Lindgren; David Lhuillier; Nilanga Liyanage; Demetrius Margaziotis; Pete Markowitz; David Meekins; Zein-Eddine Meziani; Robert Michaels; Bryan Moffit; Sirish Nanda; Vladimir Nelyubin; Keith Otis; Kent Paschke; Sasha Philips; Benard Poelker; Roman Pomatsalyuk; Milan Potokar; Yelena Prok; Andrew Puckett; Y. Qian; Yi Qiang; Bodo Reitz; Julie Roche; Arunava Saha; Bradley Sawatzky; Jaideep Singh; Karl Slifer; Simon Sirca; Ryan Snyder; Patricia Solvignon; Paul Souder; Marcy Stutzman; Ramesh Subedi; Riad Suleiman; Vincent Sulkosky; William Tobias; Paul Ulmer; Guido Urciuoli; Kebin Wang; Richard Wilson; Bogdan Wojtsekhowski; Huan Yao; Yunxiu Ye; Xiaohui Zhan; Xiaochao Zheng; Shi-Lin Zhu; Vitaliy Ziskin

2006-09-11T23:59:59.000Z

198

Experimental study of exclusive $^2$H$(e,e^\\prime p)n$ reaction mechanisms at high $Q^2$  

SciTech Connect (OSTI)

The reaction {sup 2}H(e,e{prime} p)n has been studied with full kinematic coverage for photon virtuality 1.75 < 5.5 {approx} GeV{sup 2}. Comparisons of experimental data with theory indicate that for very low values of neutron recoil momentum (p{sub n} < 100 MeV/c) the neutron is primarily a spectator and the reaction can be described by the plane-wave impulse approximation. For 100 < 750 MeV/c proton-neutron rescattering dominates the cross section, while {Delta} production followed by the N{Delta} {yields} NN transition is the primary contribution at higher momenta.

Kim Egiyan; Gegham Asryan; Nerses Gevorgyan; Keith Griffioen; Jean Laget; Sebastian Kuhn; Gary Adams; Moscov Amaryan; Pawel Ambrozewicz; Marco Anghinolfi; Gerard Audit; Harutyun AVAKIAN; Harutyun Avakian; Hovhannes Baghdasaryan; Nathan Baillie; Jacques Ball; Nathan Baltzell; Steve Barrow; Vitaly Baturin; Marco Battaglieri; Ivan Bedlinski; Ivan Bedlinskiy; Mehmet Bektasoglu; Matthew Bellis; Nawal Benmouna; Barry Berman; Angela Biselli; Lukasz Blaszczyk; Sylvain Bouchigny; Sergey Boyarinov; Robert Bradford; Derek Branford; William Briscoe; William Brooks; Stephen Bueltmann; Volker Burkert; Cornel Butuceanu; John Calarco; Sharon Careccia; Daniel Carman; Antoine Cazes; Shifeng Chen; Philip Cole; Patrick Collins; Philip Coltharp; Dieter Cords; Pietro Corvisiero; Donald Crabb; Volker Crede; John Cummings; Natalya Dashyan; Rita De Masi; Raffaella De Vita; Enzo De Sanctis; Pavel Degtiarenko; Haluk Denizli; Lawrence Dennis; Alexandre Deur; Kahanawita Dharmawardane; Richard Dickson; Chaden Djalali; Gail Dodge; Joseph Donnelly; David Doughty; Michael Dugger; Steven Dytman; Oleksandr Dzyubak; Hovanes Egiyan; Lamiaa Elfassi; Latifa Elouadrhiri; Paul Eugenio; Renee Fatemi; Gleb Fedotov; Gerald Feldman; Robert Feuerbach; Robert Fersch; Michel Garcon; Gagik Gavalian; Gerard Gilfoyle; Kevin Giovanetti; Francois-Xavier Girod; John Goetz; Atilla Gonenc; Christopher Gordon; Ralf Gothe; Michel Guidal; Matthieu Guillo; Hayko Guler; Lei Guo; Vardan Gyurjyan; Cynthia Hadjidakis; Kawtar Hafidi; Hayk Hakobyan; Rafael Hakobyan; Charles Hanretty; John Hardie; F. Hersman; Kenneth Hicks; Ishaq Hleiqawi; Maurik Holtrop; Charles Hyde-Wright; Yordanka Ilieva; David Ireland; Boris Ishkhanov; Eugeny Isupov; Mark Ito; David Jenkins; Hyon-Suk Jo; Kyungseon Joo; Henry Juengst; Narbe Kalantarians; James Kellie; Mahbubul Khandaker; Wooyoung Kim; Andreas Klein; Franz Klein; Alexei Klimenko; Mikhail Kossov; Zebulun Krahn; Laird Kramer; V. Kubarovsky; Joachim Kuhn; Sergey Kuleshov; Jeff Lachniet; Jorn Langheinrich; David Lawrence; Ji Li; Kenneth Livingston; Haiyun Lu; Marion MacCormick; Claude Marchand; Nikolai Markov; Paul Mattione; Simeon McAleer; Bryan McKinnon; John McNabb; Bernhard Mecking; Surik Mehrabyan; Joseph Melone; Mac Mestayer; Curtis Meyer; Tsutomu Mibe; Konstantin Mikhaylov; Ralph Minehart; Marco Mirazita; Rory Miskimen; Viktor Mokeev; Kei Moriya; Steven Morrow; Maryam Moteabbed; James Mueller; Edwin Munevar Espitia; Gordon Mutchler; Pawel Nadel-Turonski; Rakhsha Nasseripour; Silvia Niccolai; Gabriel Niculescu; Maria-Ioana Niculescu; Bogdan Niczyporuk; Megh Niroula; Rustam Niyazov; Mina Nozar; Grant O'Rielly; Mikhail Osipenko; Alexander Ostrovidov; Kijun Park; Evgueni Pasyuk; Craig Paterson; Sergio Pereira; Joshua Pierce; Nikolay Pivnyuk; Dinko Pocanic; Oleg Pogorelko; Sergey Pozdnyakov; Barry Preedom; John Price; Yelena Prok; Dan Protopopescu; Brian Raue; Gregory Riccardi; Giovanni Ricco; Marco Ripani; Barry Ritchie; Federico Ronchetti; Guenther Rosner; Patrizia Rossi; Franck Sabatie; Julian Salamanca; Carlos Salgado; Joseph Santoro; Vladimir Sapunenko; Reinhard Schumacher; Vladimir Serov; Youri Sharabian; Nikolay Shvedunov; Alexander Skabelin; Elton Smith; Lee Smith; Daniel Sober; Daria Sokhan; Aleksey Stavinskiy; Samuel Stepanyan; Stepan Stepanyan; Burnham Stokes; Paul Stoler; Steffen Strauch; Mauro Taiuti; David Tedeschi; Ulrike Thoma; Avtandil Tkabladze; Svyatoslav Tkachenko; Luminita Todor; Clarisse Tur; Maurizio Ungaro; Michael Vineyard; Alexander Vlassov; Daniel Watts; Lawrence Weinstein; Dennis Weygand; M. Williams; Elliott Wolin; Michael Wood; Amrit Yegneswaran; Lorenzo Zana; Jixie Zhang; Bo Zhao; Zhiwen Zhao

2007-06-01T23:59:59.000Z

199

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.

200

Juraj Bracink, Hadron Structure, Modra, September 2007 Physics with eP collisions at highest Q2  

E-Print Network [OSTI]

) Solenoidal magnet Muon system Depleted uranium calorimeter #12;Juraj Braciník, Hadron Structure, Modra

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
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We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


201

SustSciTeam_ProgramSummary_051611.xlsx.5/16/11 1Q 2Q 3Q Summer  

E-Print Network [OSTI]

-month) Orientation and Team Building Year 1 Sustainability Science ESS280A (4units) Independent Research XXX299 (4 units) Independent Research XXX299 (4 units) Summer Salary Sustainability Science Course; Define Team Report; Progress mtgs. Sustainability Science Team - Summary Schedule Apply to Sustainability Science

Rose, Michael R.

202

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

SciTech Connect (OSTI)

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

Chase, J.

2000-05-12T23:59:59.000Z

203

The RecQ4 Orthologue Hrq1 Is Critical for DNA Interstrand Cross-Link Repair and Genome Stability in Fission Yeast  

Science Journals Connector (OSTI)

...Cross-Link Repair and Genome Stability in Fission Yeast Lynda...substrates, including bubbles but not blunt duplexes...mediators of genome stability include the RecQ family...cross-link repair and genome stability in fission yeast...substrates, including bubbles but not blunt duplexes...

Lynda M. Groocock; John Prudden; J. Jefferson P. Perry; Michael N. Boddy

2011-11-07T23:59:59.000Z

204

Microsoft PowerPoint - DOE Supplemental Instructions for OMB Section 1512 Reporting Contractors Q1 2010 [Compatibility Mode]  

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

Contractors Contractors 1 For Contractors Quarterly reporting through FederalReporting.gov April 2010 April 2010 Reporting Timeline Date Action Ongoing Registration open for FederalReporting.gov. Early registration is encouraged. April 1, 2010 Reporting Period Begins April 16, 2010 Reporting Period Ends - No new reports can be entered after 11:59 PM PDT on this date. NOTE: Reporting deadline was extended. April 17, 2010 Prime Recipient Review begins- Only corrections to existing reports can be made. April 19, 2010 Prime Recipient Review ends- No updates may be made after 11:59 PM PDT on this date without DOE Reviewer action. April 20, 2010 Federal review of data begins -Recipients may be contacted to answer 2 April 20, 2010 Federal review of data begins -Recipients may be contacted to answer

205

Microsoft PowerPoint - DOE Supplemental Instructions for OMB Section 1512 Reporting Grant and Loan Recipients Q1 2010 [Compati  

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

Grant and Loan Recipients Grant and Loan Recipients | 1 For Grant and Loan Recipients Quarterly reporting through FederalReporting.gov April 2010 April 2010 Reporting Timeline Date Action Ongoing Registration open for FederalReporting.gov. Early registration is encouraged. April 1, 2010 Reporting Period Begins April 16, 2010 Reporting Period Ends - No new reports can be entered after 11:59 PM PDT on this date. NOTE: Reporting deadline was extended. April 17, 2010 Prime Recipient Review begins- Only corrections to existing reports can be made. April 19, 2010 Prime Recipient Review ends- No updates may be made after 11:59 PM PDT on this date without DOE Reviewer action. For more information, contact DOE at: https://recoveryclearinghouse.energy.gov or 1-888-363-7289 or go to: http://www.FederalReporting.gov

206

Q1. Who is Healthyroads? Healthyroads is our wellness program provider. The university selected Healthyroads from a  

E-Print Network [OSTI]

.com to sign up. Q6. What's this about a wellness rebate? A. To encourage employees and their spouses're making it worth your time with a rebate of up to $600 for you, and $600 for your spouse, for a total of up to $1,200. #12;Q7. What does earning a rebate "up to $600" mean? How is it paid to us? The rebate

Pantaleone, Jim

207

Chemical Communications c2cc30957b Q1Hypergolic ionic liquids to mill, suspend, and ignite  

E-Print Network [OSTI]

of nanoscale additives to improve EIL properties, such as energetic density and heat of combustion, while to their practical use such as low density5 and relatively low heats of combustion6 when compared to the current

Anderson, Scott L.

208

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

E-Print Network [OSTI]

of Illinois at Urbana-Champaign, 265 Morrill Hall, 505 South Goodwin Avenue, Urbana, IL 61801, USA 10 g Center). We end this review by discussing the uniqueness of bi- 44carbonate's role in oxygenic photosynthesis and its role in the evolutionary development of O2-evolving PSII. This 45article is part of a Special

Govindjee

209

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

Broader source: Energy.gov [DOE]

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

210

IEIITIEIIT--CNRCNR 1 Introduction to Robustness and  

E-Print Network [OSTI]

of Mini-UAV - wingspan 1000 mm - maximum take-off weight 1500 g - DC motor - remote piloting For the Mini-UAV we set some specifications (system property) ExamplesExamples:: 1. Flight speed in the range Rectangle Q q1 q2 1.2 1.7 1.7 2.2 #12;IEIIT-CNR ©© IEIITIEIIT--CNRCNR 16 Grid Approach Suppose we follow

Tempo, Roberto

211

Name: Entry: Gp: 1 Indian Institute of Technology, Delhi  

E-Print Network [OSTI]

relation R #18; A#2;A is an equivalence. R = f (a; b) : f(a) = f(b) g Re exivity: for all a 2 S : (a; a) 2 Marks: 80 Q1 [8 Marks] Equivalences. Suppose f : A ! B is a total function. Prove that the following(c). By transitivity of equality, f(a) = f(c), whence (a; c) 2 R. Q2 [8+8 Marks] Partial Orders. In a partial order h

Prasad, Sanjiva

212

a5.xls  

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

4,859 4,859 2,586 948 810 261 147 74 26 8 Principal Building Activity Education .......................................... 386 162 56 60 48 39 16 5 Q Food Sales ....................................... 226 164 44 Q Q Q Q N N Food Service ..................................... 297 202 65 23 Q Q N Q N Health Care ....................................... 129 56 38 19 5 5 3 2 1 Inpatient .......................................... 8 N N Q Q Q Q 2 1 Outpatient ....................................... 121 56 38 19 Q 3 Q Q N Lodging ............................................. 142 38 21 38 23 11 7 4 Q Mercantile ......................................... 657 275 156 155 34 21 12 2 2 Retail (Other Than Mall) .................. 443 241 97 83 14 Q 4 Q Q Enclosed and Strip Malls ................ 213 Q 59 72 20 18 8 Q 2 Office ................................................

213

Virtual Compton Scattering and the Generalized Polarizabilities of the Proton at Q^2=0.92 and 1.76 GeV^2  

SciTech Connect (OSTI)

Virtual Compton Scattering (VCS) on the proton has been studied at Jefferson Lab using the exclusive photon electroproduction reaction (e p --> e p gamma). This paper gives a detailed account of the analysis which has led to the determination of the structure functions P{sub LL}-P{sub TT}/epsilon and P{sub LT}, and the electric and magnetic generalized polarizabilities (GPs) alpha{sub E}(Q{sup 2}) and beta{sub M}(Q{sup 2}) at values of the four-momentum transfer squared Q{sup 2} = 0.92 and 1.76 GeV{sup 2}. These data, together with the results of VCS experiments at lower momenta, help building a coherent picture of the electric and magnetic GPs of the proton over the full measured Q{sup 2}-range, and point to their non-trivial behavior.

Helene Fonvieille, Geraud Laveissiere, Natalie Degrande, Stephanie Jaminion, Christophe Jutier, Luminita Todor, L. Van Hoorebeke, Bryon Anderson, Konrad Aniol, Kathleen Arundell, Gerard Audit, Leonard Auerbach, F. Baker, Maud Baylac, J. Berthot, Pierre Bertin, William Bertozzi, Louis Bimbot, Werner Boeglin, Edward Brash, Vincent Breton, Herbert Breuer, Etienne Burtin, John Calarco, Lawrence Cardman, Christian Cavata, Jian-Ping Chen, Eugene Chudakov, Evaristo Cisbani, Daniel Dale, Cornelis De Jager, Raffaele De Leo, Alexandre Deur, Nicole D'Hose, Gail Dodge, John Domingo, Latifa Elouadrhiri, Martin Epstein, Lars Ewell, John Finn, Kevin Fissum, Guy Fournier, Bernhard Frois, Salvatore Frullani, Christophe Furget, Haiyan Gao, Juncai Gao, Franco Garibaldi, Ashot Gasparian, Shalev Gilad, Ronald Gilman, Oleksandr Glamazdin, Charles Glashausser, Javier Gomez, Viktor Gorbenko, Pierre Guichon, Jens-Ole Hansen, Richard Holmes, Maurik Holtrop, Calvin Howell, Garth Huber, Charles Hyde, Sebastien Incerti, Mauro Iodice, Johann Jardillier, Mark Jones, Seigo Kato, James Kelly, Armen Ketikyan, Mohammad Khayat, Kouichi Kino, Serge Kox, Laird Kramer, Krishna Kumar, Gerfried Kumbartzki, Michael Kuss, Antonio Leone, John LeRose, Richard Lindgren, Nilanga Liyanage, George Lolos, Kazushige Maeda, Sergey Malov, D. Manley, Claude Marchand, Dominique Marchand, Demetrius Margaziotis, Pete Markowitz, Jacques Marroncle, Jacques Martino, Kathy McCormick, James McIntyre, Surik Mehrabyan, Fernand Merchez, Zein-Eddine Meziani, Robert Michaels, Jean Mougey, Sirish Nanda, Amra Offermann, Zisis Papandreou, Charles Perdrisat, R. Perrino, Gerassimos Petratos, Stephane Platchkov, Roman Pomatsalyuk, David Prout, Vina Punjabi, Thierry Pussieux, Gilles Quemener, Ronald Ransome, Oliver Ravel, Jean-Sebastien Real, Yves Roblin, David Rowntree, Gary Rutledge, Paul Rutt, Arunava Saha, Teijiro Saito, Adam Sarty, Tim Smith, Paul Souder, Riad Suleiman, Jeffrey Templon, Tatsuo Terasawa, Raphael Tieulent, Egle Tomasi, Hiroaki Tsubota, Hiroaki Ueno, Paul Ulmer, Guido Urciuoli, Marc Vanderhaeghen, Rob van der Meer, R.Van De Vyver, Pascal Vernin, Branislav Vlahovic, Hakob Voskanyan, Eric Voutier, John Watson, Lawrence Weinstein, Krishni Wijesooriya, Richard Wilson, Bogdan Wojtsekhowski, Dan Zainea, Zilu Zhou, Rachele Di Salvo

2012-07-01T23:59:59.000Z

214

Search for an exotic S = -2, Q = -2 baryon resonance at a mass near 1862 MeV in quasi-real photoproduction  

E-Print Network [OSTI]

at the CERN Super Proton Synchroton. A narrow peak at a mass of about 1862 MeV in the - - invariant mass

215

Search for an exotic S = -2, Q = -2 baryon resonance at a mass near 1862 MeV in quasireal photoproduction  

E-Print Network [OSTI]

at the CERN Super Proton Synchroton. A narrow peak at a mass of about 1862 MeV in the # - # - invariant mass

216

Quiz # 7, STAT 383, Prof. Suman Sanyal, April 8, 2009 (Q2, Page 354) To decide whether the pipe welds in a nuclear power plant meet  

E-Print Network [OSTI]

welds in a nuclear power plant meet specifications, a random sample of welds is to be selected : µ nuclear power plants is to determine if welds

Sanyal, Suman

217

Measured Lifetimes of Selected Metastable Levels of Arq+ Ions (Q=2, 3, 9, and 10) Stored in an Electrostatic Ion-Trap  

E-Print Network [OSTI]

life- 'Present address: Advanced Photon Source, Argonne National Laboratory, Argonne, IL 60439-4814. ~Present address: Lawrence Berkeley Laboratory, Bldg. 88, Berkeley, CA 94720. times, numerous theoretical calculations of transition rates...

Yang, L. S.; Church, David A.; Tu, S. G.; Jin, J.

1994-01-01T23:59:59.000Z

218

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.

219

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

Broader source: Energy.gov [DOE]

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

220

Total Space Heating Water Heating Cook-  

Gasoline and Diesel Fuel Update (EIA)

28 28 198 18 Q 10 14.0 12.2 1.1 Q 0.6 Building Floorspace (Square Feet) 1,001 to 5,000 ........................... 34 32 Q (*) Q 56.9 52.2 Q (*) Q 5,001 to 10,000 .......................... 36 33 Q (*) Q 49.4 44.7 Q 0.1 Q 10,001 to 25,000 ........................ 28 25 1 (*) Q 26.7 23.8 1.4 0.1 Q 25,001 to 50,000 ........................ 17 16 Q (*) 1 19.1 17.8 Q (*) 0.6 50,001 to 100,000 ...................... 29 26 1 Q 1 15.6 14.1 0.7 Q 0.5 100,001 to 200,000 .................... 37 35 Q Q 1 12.5 11.5 Q Q 0.5 200,001 to 500,000 .................... 36 25 Q Q 2 10.5 7.4 2.4 Q 0.5 Over 500,000 ............................. 10 Q Q Q 2 2.1 Q Q Q 0.4 Principal Building Activity Education .................................. 47 45 2 Q Q 25.4 23.9 0.8 Q 0.3 Food Sales ................................ Q Q Q Q Q Q Q Q Q Q Food Service ............................. Q Q Q Q Q Q Q Q Q Q

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


221

Eltron Research & Development  

SciTech Connect (OSTI)

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

Evenson, Carl; Mackay, Richard; Faull, John

2014-03-01T23:59:59.000Z

222

A disease of swine caused by a chromobacterium species  

E-Print Network [OSTI]

\\j O O lAvO ?A O -tU M A lX S 'v O r -O 'H rC f\\ y5Pml6gQPa66I4jDI?Q?4s6w?QIw?I6I664jDw6I?Iw??I46 CM OJCMCMOJCVOJCVJOJOJOJCMOJCMCNJCVCNJCVCVCMCNJCM Oi O H C*-I?I wQS 0,2 5 M ? ? <,' ? S w u ?4 u Q , P6 Q ,'w 4g 68 0.2 5...library l i b rayy?hyI a? OQItj'Q4'4g68 nS (g??g'M y'AQ,8w, Q'1u'4, Q4g'? 5u?5...

Sippel, William Lawrence

2013-10-04T23:59:59.000Z

223

b4.pdf  

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

........... ........... 4,657 208 479 782 406 748 396 618 315 705 Building Floorspace (Square Feet) 1,001 to 5,000 .............................................. 2,348 99 206 390 230 368 189 360 155 351 5,001 to 10,000 ............................................ 1,110 41 128 200 72 194 80 139 80 175 10,001 to 25,000 .......................................... 708 38 92 122 66 105 87 69 39 91 25,001 to 50,000 .......................................... 257 14 25 32 17 43 25 25 25 52 50,001 to 100,000 ........................................ 145 10 16 22 13 24 9 16 12 23 100,001 to 200,000 ...................................... 59 3 7 11 5 11 4 6 4 8 200,001 to 500,000 ...................................... 23 1 4 5 2 4 1 2 Q 3 Over 500,000 ............................................... 7 Q 2 1 1 1 Q 1 Q 1 Principal Building Activity Education ....................................................

224

State of the campuS April 17, 2012  

E-Print Network [OSTI]

Ree YeaRS · 115 RiSe pRopoSalS fRom facultY StAte oF the CAMpUS 6 UC dAViS iS A ReSeaRch poweRhouSe #12RceNt iN fY 2011-12 StAte oF the CAMpUS 8 2012 Q1-Q2 ReSeaRch awaRdS ($m) UC dAViS iS A ReSeaRch poweRhouSe

California at Davis, University of

225

Non-Extensive Black Hole Thermodynamics Estimate for Power-Law Particle Spectra  

E-Print Network [OSTI]

We point out that by considering the Hawking-Bekenstein entropy of Schwarzschild black hole horizons as a non-extensive Tsallis entropy, its additive formal logarithm, coinciding with the Renyi entropy, generates an equation of state with positive heat capacity above a threshold energy. Based on this, the edge of stability is conjectured to be trans-Planckian, i.e. being in the quantum range. From this conjecture an estimate arises for the q-parameter in the Renyi entropy, (q=2/pi^2), also manifested in the canonical power-law distribution of high energy particles (q ~ 1.2 for quark matter).

Tamas S. Biro

2010-11-15T23:59:59.000Z

226

b28.xls  

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

4,645 4,645 3,982 1,258 1,999 282 63 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,552 2,100 699 955 171 Q 5,001 to 10,000 ................................. 889 782 233 409 58 Q 10,001 to 25,000 ............................... 738 659 211 372 32 Q 25,001 to 50,000 ............................... 241 225 63 140 8 9 50,001 to 100,000 ............................. 129 123 32 73 6 8 100,001 to 200,000 ........................... 65 62 15 33 Q 9 200,001 to 500,000 ........................... 25 24 5 13 Q 4 Over 500,000 .................................... 7 6 1 3 Q 2 Principal Building Activity Education .......................................... 386 382 141 172 14 24 Food Sales ....................................... 226 188 94 68 Q N Food Service ..................................... 297 282

227

Measurement of the Electric Charge of the Top Quark in $\\boldsymbol{t\\bar{t}}$ Events  

E-Print Network [OSTI]

We present a measurement of the electric charge of top quarks using $t\\bar{t}$ events produced in $p\\bar{p}$ collisions at the Tevatron. The analysis is based on fully reconstructed $t\\bar{t}$ pairs in lepton+jets final states. Using data corresponding to 5.3 $\\rm fb^{-1}$ of integrated luminosity, we exclude the hypothesis that the top quark has a charge of $Q=-4/3\\,e$ at a significance greater than 5 standard deviations. We also place an upper limit of 0.46 on the fraction of such quarks that can be present in an admixture with the standard model top quarks ($Q=+2/3\\,e$) at a 95\\% confidence level.

D0 Collaboration

2014-09-25T23:59:59.000Z

228

b4.xls  

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

East East South Central West South Central Mountain Pacific All Buildings* .................................. 4,645 233 493 696 571 874 348 553 299 580 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,552 127 237 369 356 457 215 294 165 333 5,001 to 10,000 ................................. 889 48 101 117 97 189 56 116 56 110 10,001 to 25,000 ............................... 738 37 90 122 75 139 51 88 54 81 25,001 to 50,000 ............................... 241 10 26 44 27 47 15 26 14 32 50,001 to 100,000 ............................. 129 7 21 24 10 21 10 18 5 13 100,001 to 200,000 ........................... 65 3 12 12 5 16 Q 8 Q 6 200,001 to 500,000 ........................... 25 Q 6 6 1 4 Q 2 1 3 Over 500,000 .................................... 7 Q 1 1 Q 1 Q Q Q 1 Principal Building Activity Education ..........................................

229

 

Gasoline and Diesel Fuel Update (EIA)

0. Fuel Oil Consumption (gallons) and Energy Intensities by End Use for 0. Fuel Oil Consumption (gallons) and Energy Intensities by End Use for Non-Mall Buildings, 2003 Total Fuel Oil Consumption (million gallons) Fuel Oil Energy Intensity (gallons/square foot) Total Space Heating Water Heating Cook- ing Other Total Space Heating Water Heating Cook- ing Other All Buildings* ........................ 1,602 1,397 125 Q 69 0.11 0.09 0.01 Q (*) Building Floorspace (Square Feet) 1,001 to 5,000 ......................... 249 228 Q (*) Q 0.41 0.38 Q (*) Q 5,001 to 10,000 ....................... 261 237 Q 1 Q 0.37 0.33 Q (*) Q 10,001 to 25,000 ..................... 196 177 10 (*) Q 0.20 0.18 0.01 (*) Q 25,001 to 50,000 ..................... 117 112 Q (*) 4 0.14 0.14 Q (*) (*)

230

The nexus between electricity consumption and economic growth in Bahrain  

Science Journals Connector (OSTI)

Abstract This paper explores the relationship between electricity consumption, foreign direct investment, capital and economic growth in the case of the Kingdom of Bahrain. The CobbDouglas production is used over the period of 1980Q12010Q4. We have applied the ARDL bounds testing approach and found that cointegration exists among the series. Electricity consumption, foreign direct investment and capital add in economic growth. The VECM Granger causality analysis has exposed the feedback effect between electricity consumption and economic growth and the same is true for foreign direct investment and electricity consumption. This study suggests government authorities to explore new sources of energy to achieve sustainable economic development for the long run.

Helmi Hamdi; Rashid Sbia; Muhammad Shahbaz

2014-01-01T23:59:59.000Z

231

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)

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.

Chase, J.

2000-10-24T23:59:59.000Z

232

Biochimtca et Biophyszva Acta. IlllO( 1992}I-bl ] 19q2 Elsevier Science Publishers B.V. All rights reserved O) ~-272~;/92/$ J5.0n  

E-Print Network [OSTI]

..~phaeroide~) Photosystcm I1 of oxygen-evolving organisms exhibits a bicarbonatc-revcrsiblc ff~rmatc effect on clcctron through the quinone electron accep- ters of Photosygtem 1I (PS 11) in oxygen-evolving organ- isms of the glutamate ligand to the iron atom in bacterial reaction centers? X. Wang a, j. Cao a, p. Mar6ti ", H

Govindjee

233

Beam-Target Double Spin Asymmetry A_LT in Charged Pion Production from Deep Inelastic Scattering on a Transversely Polarized He-3 Target at 1.4<Q^2<2.7 GeV^2  

E-Print Network [OSTI]

We report the first measurement of the double-spin asymmetry $A_{LT}$ for charged pion electroproduction in semi\

J. Huang; K. Allada; C. Dutta; J. Katich; X. Qian; Y. Wang; Y. Zhang; K. Aniol; J. R. M. Annand; T. Averett; F. Benmokhtar; W. Bertozzi; P. C. Bradshaw; P. Bosted; A. Camsonne; M. Canan; G. D. Cates; C. Chen; J. -P. Chen; W. Chen; K. Chirapatpimol; E. Chudakov; E. Cisbani; J. C. Cornejo; F. Cusanno; M. M. Dalton; W. Deconinck; C. W. de Jager; R. De Leo; X. Deng; A. Deur; H. Ding; P. A. M. Dolph; D. Dutta; L. El Fassi; S. Frullani; H. Gao; F. Garibaldi; D. Gaskell; S. Gilad; R. Gilman; O. Glamazdin; S. Golge; L. Guo; D. Hamilton; O. Hansen; D. W. Higinbotham; T. Holmstrom; M. Huang; H. F. Ibrahim; M. Iodice; X. Jiang; G. Jin; M. K. Jones; A. Kelleher; W. Kim; A. Kolarkar; W. Korsch; J. J. LeRose; X. Li; Y. Li; R. Lindgren; N. Liyanage; E. Long; H. -J. Lu; D. J. Margaziotis; P. Markowitz; S. Marrone; D. McNulty; Z. -E. Meziani; R. Michaels; B. Moffit; C. Muoz Camacho; S. Nanda; A. Narayan; V. Nelyubin; B. Norum; Y. Oh; M. Osipenko; D. Parno; J. C. Peng; S. K. Phillips; M. Posik; A. J. R. Puckett; Y. Qiang; A. Rakhman; R. D. Ransome; S. Riordan; A. Saha; B. Sawatzky; E. Schulte; A. Shahinyan; M. H. Shabestari; S. irca; S. Stepanyan; R. Subedi; V. Sulkosky; L. -G. Tang; A. Tobias; G. M. Urciuoli; I. Vilardi; K. Wang; B. Wojtsekhowski; X. Yan; H. Yao; Y. Ye; Z. Ye; L. Yuan; X. Zhan; Y. -W. Zhang; B. Zhao; X. Zheng; L. Zhu; X. Zhu; X. Zong; for the Jefferson Lab Hall A Collaboration

2012-02-10T23:59:59.000Z

234

Thermal conduction by dark matter with velocity and momentum-dependent cross-sections  

E-Print Network [OSTI]

We use the formalism of Gould and Raffelt to compute the dimensionless thermal conduction coefficients for scattering of dark matter particles with standard model nucleons via cross-sections that depend on the relative velocity or momentum exchanged between particles. Motivated by models invoked to reconcile various recent results in direct detection, we explicitly compute the conduction coefficients $\\alpha$ and $\\kappa$ for cross-sections that go as $v_{\\rm rel}^2$, $v_{\\rm rel}^4$, $v_{\\rm rel}^{-2}$, $q^2$, $q^4$ and $q^{-2}$, where $v_{\\rm rel}$ is the relative DM-nucleus velocity and $q$ is the momentum transferred in the collision. We find that a $v_{\\rm rel}^{-2}$ dependence can significantly enhance energy transport from the inner solar core to the outer core. The same can true for any $q$-dependent coupling, if the dark matter mass lies within some specific range for each coupling. This effect can complement direct searches for dark matter; combining these results with state-of-the-art Solar simulations should greatly increase sensitivity to certain DM models. It also seems possible that the so-called Solar Abundance Problem could be resolved by enhanced energy transport in the solar core due to such velocity- or momentum-dependent scatterings.

Aaron C. Vincent; Pat Scott

2013-11-08T23:59:59.000Z

235

Trends in U.S. Venture Capital Investments Related to Energy: 1980 through the Second Quarter of 2010  

SciTech Connect (OSTI)

This report documents trends in U.S. venture capital investments over the period 1980 through the second quarter of calendar year 2010 (2010Q1+Q2). Particular attention is given to U.S. venture capital investments in the energy/industrial sector over the period 1980-2010Q1+Q2 as well as in the more recently created cross-cutting category of CleanTech over the period 1995-2010Q1+Q2. During the early 1980s, U.S. venture capital investments in the energy/industrial sector accounted for more than 20% of all venture capital investments. However subsequent periods of low energy prices, the deregulation of large aspects of the energy industry, and the emergence of fast growing new industries like computers (both hardware and software), biotechnology and the Internet quickly reduced the priority accorded to energy/industrial investments. To wit, venture capital investments related to the energy/industrial sector accounted for only 1% of the $119 billion dollars invested in 2000 by the U.S. venture capital community. The significant increase in the real price of oil that began in 2003-2004 correlates with renewed interest and increased investment by the venture capital community in energy/industrial investment opportunities. Venture capital investments for 2009 for the energy/industrial sector accounted for $2.1 billion or slightly more than 13% of all venture capital invested that year. The total venture capital invested in energy/industrial during the first two quarters of 2010 is close to $1.8 billion accounting for 17% of all venture capital investments during the first two quarters of 2010. In 2009, the aggregate amount invested in CleanTech was $1.8 billion (30% of the total US venture capital invested in that lean year) and for the first two quarters of 2010 US venture capital investments in CleanTech have already exceeded $1.9 billion (19% of all US venture capital investments made during the first half of 2010). Between 2004 and 2009, U.S. venture capital investments in energy/industrial as well as CleanTech have more than quadrupled in real terms.

Dooley, James J.

2010-07-29T23:59:59.000Z

236

Symmetric Long Straight Section Lattices  

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

Symmetric Symmetric Long Straight Section Lattices for 2, 4, and 8 Sectors formerly AOP-TN-2009-007, Rev. 2 Michael Borland March 23, 2009 Accelerator Systems Division, Advanced Photon Source 1 Introduction Long straight sections [1] (LSS) are anticipated to be one of the significant changes to the accel- erator as part of the APS Renewal. Previously [2], we developed a lattice with eight LSS that, while workable, would have presented some operational challenges. In the present note, we show improved results for 8LSS, along with new solutions for 4LSS and 2LSS. As before, these lattices are developed by removing the Q2 quadrupoles and moving the Q1 back into its place, permitting a 7.7-m-long insertion device (as judged by the increase in face-to-face distance for the innermost powered quadrupoles). Further increases in length (perhaps 10%) might be possible by removing corrector magnets,

237

USDOE Technology Transfer, Frequently Asked Questions about Agreement for  

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

Frequently Asked Questions about ACT: Frequently Asked Questions about ACT: Q1: What is ACT (Agreement for Commercializing Technology)? A1: ACT is a pilot program under which businesses may partner with participating DOE laboratories for research and development that commercializes technology. Q2: Why is this pilot being introduced? A2: ACT is being piloted to address concerns about difficulties in partnering with the DOE laboratories that were raised in public responses to a DOE Request for Information on improving technology transfer. These concerns include requirements for advance payments, indemnification and government use rights in intellectual property. Q3: Who can partner with the laboratories under ACT? A3: ACT is available to a full range of sponsors, including start-ups, small and large businesses that provide private funding to

238

Microsoft PowerPoint - compliant sealing glass review 7,27,2010 rev1.pptx [Read-Only]  

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

Compliant glass seal development Compliant glass seal development Y-S Matt Chou, E. Thomsen, E. Mast, J-P Choi, W. Voldrich, and J. W. Stevenson Introduction and objectives Q1: Effect of differential pressure on thermal cycle stability 1 experimental 1. experimental 2. leak rates versus cycling (700-850 o C/1000h) Q2: thermal stability study in a duel environment 1. leak rates versus time (750-800 o C/1000h) 2. microstructure and interface characterization Q3: assess YSZ coating and other mat'l for spacer rings Q g p g Summary Future work Solid-State Energy Conversion Alliance Core Technology Programs Review, July 27-29, 2010, Pittsburgh, PA Compliant versus refractory sealing glass  = E T Compliant sealing glass 1.20E-02 YSO1 glass Refractory sealing glass Data provided by ORNL

239

Frequently Asked Questions - DOE O 420.1C  

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

Frequently Asked Questions Regarding DOE Order 420.1C, Facility Safety, and its supporting directives, DOE-STD-1020-2012, Natural Phenomena Hazards Analysis and Design Criteria for DOE Facilities, and DOE-STD-1066-2012, Fire Protection Q-1: For existing facilities how do I determine the list of applicable design codes and standards? A: For existing facilities the code of record (i.e. those codes and standards in effect at the time that the facility was designed) is the list of applicable design codes and standards. In the case of major modifications to existing facilities, the design codes and standards of O 420.1C apply. Q-2: I work at an existing facility. What changes in DOE O 420.1C do I have to be concerned about?

240

ESS 2012 Peer Review - Tehachapi Wind Energy Storage Project Using Li-Ion Batteries - Christopher Clarke, SCE  

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

Tehachapi Storage Project (TSP) Tehachapi Storage Project (TSP) American Recovery and Reinvestment Act Funded Project Christopher R. Clarke - Southern California Edison (SCE) christopher.r.clarke@sce.com Examples of Wind Generation in the Tehachapi Wind Resource Area August 2012 June 2012 May 2012 February 2012 April 2012 Progress To Date * Facility construction expected to complete in September 2012 * First Power Conversion System installed September 13, 2012 * A123 to ship initial battery equipment for delivery week of September 24, 2012 Future Major Milestones * September 2012 - Completion of BESS facility * October 2012 - Initial installation * November 2012 - Installation of second Power Conversion Subsystem * Q1 2013 - Install balance of equipment and commissioning * Q2 2013 - Start of 2 year M&V testing and reporting

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


241

b8.pdf  

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

4,657 4,657 419 499 763 665 774 846 690 Building Floorspace (Square Feet) 1,001 to 5,000 .............................................. 2,348 227 270 359 321 367 413 390 5,001 to 10,000 ............................................ 1,110 107 102 240 166 193 156 145 10,001 to 25,000 .......................................... 708 63 90 97 84 130 179 65 25,001 to 50,000 .......................................... 257 13 20 39 53 44 43 44 50,001 to 100,000 ........................................ 145 7 9 19 24 26 33 27 100,001 to 200,000 ...................................... 59 Q 5 5 12 8 15 12 200,001 to 500,000 ...................................... 23 Q 2 3 4 4 4 4 Over 500,000 ............................................... 7 Q 1 1 1 2 2 1 Principal Building Activity Education .................................................... 327

242

Heating Oil and Propane Update  

Gasoline and Diesel Fuel Update (EIA)

State Energy Offices State Energy Offices Q1: What price should be reported to EIA when submitting weekly data? EIA requests that you collect / report the residential credit price (keep-full prices being preferred) and that all prices exclude taxes for the Monday of each survey week, even if that Monday falls on a holiday. Prices should not include discounts for payment of cash or for payment made within a short period of time. However, if a company deals exclusively in cash, then this price should be reported and noted in the file sent to EIA. Q2: When is this data due to EIA each week? The EIA-877 "Winter Heating Fuels Telephone Survey" will begin the first Monday in October. Data should be submitted to EIA as soon as they are available but no later than noon on Tuesday of each week. Data collection

243

Deformed Statistics Formulation of the Information Bottleneck Method  

E-Print Network [OSTI]

A candidate variational principle for the information bottleneck (IB) method is formulated within the ambit of the generalized nonadditive statistics of Tsallis. Given a nonadditivity parameter $ q $, the role of the \\textit{additive duality} of nonadditive statistics ($ q^*=2-q $) in relating Tsallis entropies for ranges of the nonadditivity parameter $ q 1 $ is described. Defining $ X $, $ \\tilde X $, and $ Y $ to be the source alphabet, the compressed reproduction alphabet, and, the \\textit{relevance variable} respectively, it is demonstrated that minimization of a generalized IB Lagrangian defined in terms of the nonadditivity parameter $ q^* $ self-consistently yields the \\textit{nonadditive effective distortion measure} to be the \\textit{$ q $-deformed} generalized Kullback-Leibler divergence: $ D_{K-L}^{q}[p(Y|X)||p(Y|\\tilde X)] $. This result is achieved without enforcing any \\textit{a-priori} assumptions. Finally, it is proven that the nonadditive free energy of the system in $ q^* $ space is non-ne...

Venkatesan, R C

2008-01-01T23:59:59.000Z

244

Valuation Network Representation and Solution of Asymmetric Decision Problems  

E-Print Network [OSTI]

are subsets of X, suppose q i is a probability valuation for h, and suppose q j is a probability valuation for g. Then the combination Table 2 Probability valuations in the UCB problem X S r X fS;R 1 g q 1 X fS;R 1 ;R 2 g q 2 p 0.80 p n 1 1 p n 1 n 2 1 l 0.... The marginal of q for h {X}, denoted by q # h fXg , is a probability valuation for h {X} such that q # h X c Rfq c;x jx2W X 3 c;x 2X h g for all c2X h fXg . Suppose q is a probability valuation for r. We say q is a probability distribution for r...

Shenoy, Prakash P.

2000-03-16T23:59:59.000Z

245

b31.xls  

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

4,645 4,645 3,472 1,910 1,445 94 27 128 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,552 1,715 1,020 617 41 N 66 5,001 to 10,000 ................................. 889 725 386 307 Q Q 27 10,001 to 25,000 ............................... 738 607 301 285 16 Q 27 25,001 to 50,000 ............................... 241 217 110 114 Q Q Q 50,001 to 100,000 ............................. 129 119 53 70 Q 5 Q 100,001 to 200,000 ........................... 65 60 27 35 Q 5 Q 200,001 to 500,000 ........................... 25 23 9 14 Q 2 Q Over 500,000 .................................... 7 6 3 3 Q 1 N Principal Building Activity Education .......................................... 386 298 144 149 10 6 15 Food Sales ....................................... 226 186 109 68 Q N Q Food Service .....................................

246

Inclusive Jet Production in ?p and ?? Processes: Direct and Resolved Photon Cross Sections in Next-To-Leading Order QCD  

Science Journals Connector (OSTI)

The production of jets in low Q 2 ep scattering (photoproduction) and in low Q 2 ey + ey ? scatterin...

M. Klasen; T. Kleinwort; G. Kramer

2000-12-01T23:59:59.000Z

247

a3.xls  

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

4,859 252 509 728 577 926 360 587 316 603 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,586 134 240 372 356 474 217 294 166 333 5,001 to 10,000 ................................. 948 49 106 128 100 200 59 127 62 117 10,001 to 25,000 ............................... 810 46 92 133 78 151 54 103 61 91 25,001 to 50,000 ............................... 261 10 29 48 27 52 16 28 16 34 50,001 to 100,000 ............................. 147 8 23 25 10 26 11 21 7 15 100,001 to 200,000 ........................... 74 3 12 14 5 18 Q 10 3 7 200,001 to 500,000 ........................... 26 Q 6 6 1 4 Q 3 1 3 Over 500,000 .................................... 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 .......................................

248

Vol XXIV, Issue 7 In This Issue February 16, 2009  

E-Print Network [OSTI]

Enforcing Emissions Policies Pemex Seeks Bids for Gasoline Desulfurization Plants Canada's EnCana Q4

Nikolaou, Michael

249

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

Science Journals Connector (OSTI)

We present neutron scattering measurements of the phonon-roton (P-R) mode of superfluid 4He confined in 47 MCM-41 at T=0.5 K at wave vectors, Q, beyond the roton wave vector (QR=1.92?1). Measurements beyond the roton require access to high wave vectors (up to Q=4?1) with excellent energy resolution and high statistical precision. Only one previous measurement in porous media (in aerogel) with low statistical precision has been reported. At T=0.5 K, we find that the P-R mode in MCM-41 extends out to wave vector Q?3.6?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 0.01meV in MCM-41. This upper limit means the P-R mode decays to two rotons if 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=0.60meV is the energy of the roton-like minimum of the layer mode. Rather the P-R mode and the layer modes observed in porous media appear to be quite different modes with little interaction between them.

R. T. Azuah; S. O. Diallo; M. A. Adams; O. Kirichek; H. R. Glyde

2013-07-22T23:59:59.000Z

250

Phase behavior of colloidal superballs: Shape interpolation from spheres to cubes  

Science Journals Connector (OSTI)

The phase behavior of hard superballs is examined using molecular dynamics within a deformable periodic simulation box. A superballs interior is defined by the inequality |x|2q+|y|2q+|z|2q?1, which provides a versatile family of convex particles (q?0.5) with cubelike and octahedronlike shapes as well as concave particles (q<0.5) with octahedronlike shapes. Here, we consider the convex case with a deformation parameter q between the sphere point (q=1) and the cube (q=?). We find that the asphericity plays a significant role in the extent of cubatic ordering of both the liquid and crystal phases. Calculation of the first few virial coefficients shows that superballs that are visually similar to cubes can have low-density equations of state closer to spheres than to cubes. Dense liquids of superballs display cubatic orientational order that extends over several particle lengths only for large q. Along the ordered, high-density equation of state, superballs with 1q=4.0. The structures of the high-density phases are examined using certain order parameters, distribution functions, and orientational correlation functions. We also find that a fixed simulation cell induces artificial phase transitions that are out of equilibrium. Current fabrication techniques allow for the synthesis of colloidal superballs and thus the phase behavior of such systems can be investigated experimentally.

Robert D. Batten; Frank H. Stillinger; Salvatore Torquato

2010-06-02T23:59:59.000Z

251

Information media used by cotton farmers in producing cotton in a ten-county area of North Central Texas  

E-Print Network [OSTI]

~~/%M~(~ ~ . , gP'Z'1$'+19'f. . W~jF ' ' ~Q. , "f Q9&'1+~ , gp @P '~ 8p ~~AC/. 9g"55!, QP y'4~3'6~ @1+ $4~ Q4~ f~'. t$, QM~gg8Z Z$;, '3'TOKgQg ppj7 8&, ", ~ Otp gC Q2~ Slp89p&Q, ~Q C$ pRH@p%Q~~ 1 ': ' I I l '$ '~CP1&p 4' . ~", I t 'C Fi... ' . 4~$AJ"1~9"~3'i7~ . . KK W:~1ivjg' ~ ~gg:yg grq-'gg~g gg +'~ ~~ y? ~g gg~' ~0@ @gal g~ QlfCL@CQ @AQ, ~'ALVJQ9 ~, QQS g1'~gi~i+1 5$ a J+S $+QgfQq ~~7$+Vl:g ( 'Vx'pi~i~('f8 &M~ ~':~'g8CM 4O ~M~ ~ 4i 3s K~-;JAy A"w&i?8POV 88%. p R &~lC 4'W~ Wo RQL...

Anwarul Karim, A. M

2012-06-07T23:59:59.000Z

252

Attachment 1 - PIC Transcribed Flip Chart Notes Final Meeting...  

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

Plan | *** Q2 * 100 D-H Proposed Plan * Draft Land Conveyance EA | Q2 * Natural Gas Pipeline EIS | * Q2 * 2014 Budget Meetings (2015 & 2016 Budgets) | ** Q3 *...

253

TableHC4.13.xls  

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

.. .. 111.1 33.0 8.0 3.4 5.9 14.4 1.2 Indoor Lights Turned On During Summer Number of Lights Turned On Between 1 and 4 Hours per Day......................... 91.8 26.8 6.7 2.8 4.8 11.7 0.9 1........................................................................ 28.6 10.7 1.9 1.2 2.0 5.2 0.4 2........................................................................ 29.5 9.0 2.4 0.7 1.8 3.7 0.3 3........................................................................ 14.7 3.6 1.1 0.4 0.5 1.5 Q 4........................................................................ 9.3 2.0 0.7 0.3 Q 0.7 Q 5 or More........................................................... 9.7 1.5 0.5 Q 0.3 0.5 N Energy-Efficient Bulbs Used........................... 31.1 8.2 2.1 0.7 1.6 3.6 Q 1....................................................................

254

b8.xls  

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

4,645 4,645 330 527 562 579 731 707 876 334 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,552 174 315 331 298 350 438 481 165 5,001 to 10,000 ................................. 889 71 107 90 120 180 98 158 66 10,001 to 25,000 ............................... 738 55 64 90 95 122 103 151 58 25,001 to 50,000 ............................... 241 19 23 26 33 48 32 39 21 50,001 to 100,000 ............................. 129 7 9 14 22 16 20 28 13 100,001 to 200,000 ........................... 65 Q 5 8 8 10 10 15 8 200,001 to 500,000 ........................... 25 Q 4 2 3 4 4 4 2 Over 500,000 .................................... 7 Q 1 1 0 1 2 1 Q Principal Building Activity Education .......................................... 386 12 26 78 60 58 44 75 32 Food Sales ....................................... 226 Q Q Q Q Q 33 56 Q Food Service .....................................

255

doepresentation.dvi  

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

Oil Oil Shocks and U.S. External Adjustment Martin Bodenstein, Christopher Erceg, Luca Guerrieri Division of International Finance, Federal Reserve Board April 2008 Net Exports of Petroleum and Products and Goods Trade Balance (percent share of GDP, 1970q1-2007q4) 1970 1975 1980 1985 1990 1995 2000 2005 -7 -6 -5 -4 -3 -2 -1 0 1 Persian Gulf War Iran-Iraq War Iranian Revolution Arab- Israeli War Effects of An Oil Demand Shock that Drives the Price of Oil Up by 20% (Linear Estimator) 1 2 3 4 5 6 7 8 0 5 10 15 20 25 30 Real Oil Price Percent Quarters 1 2 3 4 5 6 7 8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 Overall Trade Balance (GDP share) Percentage Point Quarters Effects of An Oil Demand Shock that Drives the Price of Oil Up by 20% (Linear Estimator) 1 2 3 4 5 6 7 8 -0.2 0 0.2 0.4 0.6 0.8 1 1.2 Non-oil Trade Balance (GDP share) Quarters Percentage Point 1 2 3 4 5 6 7 8 -0.8 -0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 Oil Trade Balance (GDP share)

256

Total Space Heating Water Heating Cook-  

Gasoline and Diesel Fuel Update (EIA)

Buildings.............................. Buildings.............................. 1,644 1,429 131 Q 72 0.10 0.09 0.01 Q (*) Building Floorspace (Square Feet) 1,001 to 5,000 ........................... 249 228 Q (*) Q 0.41 0.38 Q (*) Q 5,001 to 10,000 .......................... 262 237 Q 1 Q 0.36 0.32 Q (*) Q 10,001 to 25,000 ........................ 201 179 11 (*) Q 0.19 0.17 0.01 (*) Q 25,001 to 50,000 ........................ 124 115 Q (*) 4 0.14 0.13 Q (*) (*) 50,001 to 100,000 ...................... 209 188 10 Q 7 0.11 0.10 0.01 Q (*) 100,001 to 200,000 .................... 270 250 Q Q 10 0.09 0.08 Q Q (*) 200,001 to 500,000 .................... 258 183 Q Q 11 0.08 0.05 0.02 Q (*) Over 500,000 ............................. 72 Q Q Q 15 0.02 Q Q Q (*) Principal Building Activity Education .................................. 342 322 11 Q Q 0.18 0.17 0.01 Q (*) Food Sales ................................

257

Mechanism of runaway electron beam formation during plasma disruptions in tokamaks  

E-Print Network [OSTI]

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

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

2015-01-01T23:59:59.000Z

258

Household energy consumption and its demand elasticity in Thailand  

Science Journals Connector (OSTI)

This study concentrates on the analysis of energy consumption, expenditure on oil and LPG use in cars and aims to examine the elasticity effect of various types of oil consumption. By using the Deaton's analysis framework, the cross-sectional data of Thai households economic survey 2009 were used. By defining energy goods in the scope of automobile fuel, the results reflect the low importance of high-quality automobile fuel on all income level households. Thai households tend to vary the quality rather than the quantity of thermal energy. All income groups have a tendency to switch to lower quality fuel. Middle and high-middle households (Q3 and Q4) are the income groups with the greatest tendency to switch to lower-quality fuel when a surge in the price of oil price occurs. The poorest households (Q1) are normally insensitive to a change of energy expenditure in terms of quality and quantity. This finding illustrates the LPG price subsidy policy favours middle and high-middle income households. The price elasticity of energy quantity demand is negative in all income levels. High to middle income families are the most sensitive to changes in the price of energy.

Montchai Pinitjitsamut

2012-01-01T23:59:59.000Z

259

 

Gasoline and Diesel Fuel Update (EIA)

A. Fuel Oil Consumption (gallons) and Energy Intensities by End Use for All Buildings, 2003 A. Fuel Oil Consumption (gallons) and Energy Intensities by End Use for All Buildings, 2003 Total Fuel Oil Consumption (million gallons) Fuel Oil Energy Intensity (gallons/square foot) Total Space Heating Water Heating Cook- ing Other Total Space Heating Water Heating Cook- ing Other All Buildings.......................... 1,644 1,429 131 Q 72 0.10 0.09 0.01 Q (*) Building Floorspace (Square Feet) 1,001 to 5,000 ......................... 249 228 Q (*) Q 0.41 0.38 Q (*) Q 5,001 to 10,000 ....................... 262 237 Q 1 Q 0.36 0.32 Q (*) Q 10,001 to 25,000 ..................... 201 179 11 (*) Q 0.19 0.17 0.01 (*) Q 25,001 to 50,000 ..................... 124 115 Q (*) 4 0.14 0.13 Q (*) (*) 50,001 to 100,000 ................... 209 188 10 Q 7 0.11 0.10 0.01 Q (*)

260

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)

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}.

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

2006-02-01T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


261

I  

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

BAECC: BAECC: I ni*al S ite L ayout AOS Instrument Field, radars, and containers Instrument F ield a nd C ontainers 6 0 m 9 0 m Met Twr T r e e H e i g h t ~ 2 0 M T r e e H e i g h t ~ 2 0 m Tree Height ~5m T r e e H e i g h t ~ 2 0 m K A Z R B S R W P P D M Rad Tables: mfrsr, TSI skyrad, SPN 10 M Scale M W A C R MWR mounted side by side with 1 m in between scan direction indicated by arrows MWR3C p w r P W R D r o p G P R W P A N T E Q 1 9 0 f t 6 4 f t E Q 2 u n d e r s a c r E Q 1 A N T Snow Fence Measurements a re c lose a pproximates. S ite w as l aid o ut D uring A ug S ite V isit Container P ad D etail AMF2 SACR OPS Van GP Van RWP Van 20' 90' 64' PWR 20' 20' mpl 2d VD MAERI BBSS cart WBRG VCEIL Instrument Field 10" 10' 10" 10" 10" SWACR Antenna EQ1 Van AMFX SACR 20' EQ2 under SACR Instrument F ield 1 1 2 3 2 3 Instrument F ield Looking S outh E ast Looking S outh Looking N orth E ast Looking N orth W---Band a nd K a---Band R adar

262

Temperature Tomography of the Soft X-Ray Corona: Measurements  

Science Journals Connector (OSTI)

We analyze long-exposure and off-pointing Yohkoh/SXT data of the solar corona observed on 1992 August 26. We develop a new (temperature) tomography method that is based on a forward-fitting method of a four-parameter model to the observed soft X-ray fluxes F1(h) and F2(h) of two SXT wavelength filters as a function of height h. The model is defined in terms of a differential emission measure (DEM) distribution dEM(h, T)/dT, which includes also a temperature dependence of density scale heights ?n(T) = q??T and allows us to quantify deviations (q? ? 1) from hydrostatic equilibrium (q? = 1). This parametrization facilitates a proper line-of-sight integration and relates the widely used filter ratio temperature TFR to the peak of the DEM distribution. A direct consequence of the multi-scale height atmosphere is that the filter ratio temperature TFR(h) is predicted to increase with height, even if all magnetic field lines are isothermal. Our model fitting reveals that coronal holes and quiet-Sun regions are in perfect hydrostatic equilibrium but that coronal streamers have a scale height that exceeds the hydrostatic scale height by a factor of up to q? 2.3, which underscores the dynamic nature of coronal streamers. Our density measurements in coronal holes are slightly lower than most of the white-light polarized brightness inversions and seem to come closer to the requirements of solar wind models. Our DEM model provides also a physical framework for the semiempirical Baumbach-Allen formula and quantifies the temperature ranges and degree of hydrostaticity of the K, L, and F coronae.

Markus J. Aschwanden; Loren W. Acton

2001-01-01T23:59:59.000Z

263

Total.................................................................  

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

49.2 49.2 15.1 15.6 11.1 7.0 5.2 8.0 Have Cooling Equipment............................... 93.3 31.3 15.1 15.6 11.1 7.0 5.2 8.0 Use Cooling Equipment................................ 91.4 30.4 14.6 15.4 11.1 6.9 5.2 7.9 Have Equipment But Do Not Use it............... 1.9 1.0 0.5 Q Q Q Q Q Do Not Have Cooling Equipment................... 17.8 17.8 N N N N N N Air-Conditioning Equipment 1, 2 Central System............................................. 65.9 3.9 15.1 15.6 11.1 7.0 5.2 8.0 Without a Heat Pump................................ 53.5 3.5 12.9 12.7 8.6 5.5 4.2 6.2 With a Heat Pump..................................... 12.3 0.4 2.2 2.9 2.5 1.5 1.0 1.8 Window/Wall Units........................................ 28.9 27.5 0.5 Q 0.3 Q Q Q 1 Unit......................................................... 14.5 13.5 0.3 Q Q Q N Q 2 Units.......................................................

264

b41.xls  

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

64,783 64,783 56,940 11,035 9,041 12,558 2,853 11,636 29,969 1,561 1,232 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 5,007 1,568 675 972 Q Q 1,957 179 Q 5,001 to 10,000 ................................. 6,585 5,408 1,523 563 1,012 Q Q 2,741 207 Q 10,001 to 25,000 ............................... 11,535 9,922 2,173 1,441 1,740 Q 456 5,260 378 Q 25,001 to 50,000 ............................... 8,668 7,776 1,683 1,155 2,301 240 729 4,264 Q Q 50,001 to 100,000 ............................. 9,057 8,331 1,388 1,440 1,958 332 1,722 4,732 Q Q 100,001 to 200,000 ........................... 9,064 8,339 993 1,158 2,259 793 2,366 4,504 Q Q 200,001 to 500,000 ........................... 7,176 6,565 1,136 1,273 1,223 495 3,023 3,834 Q Q Over 500,000 .................................... 5,908 5,591 569 1,334 1,095

265

 

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

1. Cooling Equipment, Floorspace for Non-Mall Buildings, 2003 1. Cooling Equipment, Floorspace for Non-Mall Buildings, 2003 Total Floorspace (million square feet) All Build- ings* Cooled Build- ings Cooling Equipment (more than one may apply) Resid- ential- Type Central Air Condi- tioners Heat Pumps Indiv- idual Air Condi- tioners District Chilled Water Central Chillers Pack- aged Air Condi- tioning Units Swamp Coolers Other All Buildings* ............................... 64,783 56,940 11,035 9,041 12,558 2,853 11,636 29,969 1,561 1,232 Building Floorspace (Square Feet) 1,001 to 5,000 ................................ 6,789 5,007 1,568 675 972 Q Q 1,957 179 Q 5,001 to 10,000 .............................. 6,585 5,408 1,523 563 1,012 Q Q 2,741 207 Q 10,001 to 25,000 ............................ 11,535 9,922 2,173 1,441 1,740 Q 456 5,260 378 Q

266

c35.xls  

Gasoline and Diesel Fuel Update (EIA)

65 65 170 104 63 6,080 2,832 4,122 2,123 0.21 0.06 0.03 Q Building Floorspace (Square Feet) 1,001 to 10,000 ............................... 381 Q Q Q 757 Q 255 Q 0.50 Q 0.10 Q 10,001 to 100,000 ........................... 375 63 Q Q 1,704 643 833 351 0.22 0.10 Q Q Over 100,000 .................................. 509 20 44 Q 3,618 1,983 3,034 1,673 0.14 0.01 0.01 Q Principal Building Activity Education ........................................ 282 Q Q Q 933 Q Q Q 0.30 Q Q Q Health Care...................................... Q Q 17 7 Q 492 786 262 Q Q 0.02 0.03 Office .............................................. 105 6 14 1 1,379 714 1,235 748 0.08 0.01 0.01 0.00 All Others ........................................ 837 Q 44 40 3,426 1,281 1,644 984 0.24 Q 0.03 Q Year Constructed 1945 or Before ................................ 555 Q Q Q 2,126 Q Q Q 0.26 Q Q Q 1946 to 1959 ...................................

267

A<ACD6B;GAQ=CD4Q  

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

AQ &#2;!' (*$!%), &", %!(#+, HIOKLMJPNMQ :8Q(%,1-Q .WAFTWbe?#Q 9TT@Xe (3* e.AO AW:K e&T[ O"Q- W:OY d  ]L *aA <[YI ^Ae) IWA= YTWe 0T: Oe 4WTF W:M Xe3C >Ae %RS[:Ke2:YITO:Ke+O_IWTONAOY:Ke5TKH=ce %

268

PERIOD ERROR ESTIMATION FOR THE KEPLER ECLIPSING BINARY CATALOG  

SciTech Connect (OSTI)

The Kepler Eclipsing Binary Catalog (KEBC) describes 2165 eclipsing binaries identified in the 115 deg{sup 2} Kepler Field based on observations from Kepler quarters Q0, Q1, and Q2. The periods in the KEBC are given in units of days out to six decimal places but no period errors are provided. We present the PEC (Period Error Calculator) algorithm, which can be used to estimate the period errors of strictly periodic variables observed by the Kepler Mission. The PEC algorithm is based on propagation of error theory and assumes that observation of every light curve peak/minimum in a long time-series observation can be unambiguously identified. The PEC algorithm can be efficiently programmed using just a few lines of C computer language code. The PEC algorithm was used to develop a simple model that provides period error estimates for eclipsing binaries in the KEBC with periods less than 62.5 days: log {sigma}{sub P} Almost-Equal-To - 5.8908 + 1.4425(1 + log P), where P is the period of an eclipsing binary in the KEBC in units of days. KEBC systems with periods {>=}62.5 days have KEBC period errors of {approx}0.0144 days. Periods and period errors of seven eclipsing binary systems in the KEBC were measured using the NASA Exoplanet Archive Periodogram Service and compared to period errors estimated using the PEC algorithm.

Mighell, Kenneth J. [National Optical Astronomy Observatory, 950 North Cherry Avenue, Tucson, AZ 85719 (United States); Plavchan, Peter [NASA Exoplanet Science Institute, California Institute of Technology, Pasadena, CA 91125 (United States)

2013-06-15T23:59:59.000Z

269

The Super HMS  

SciTech Connect (OSTI)

As a part of physics instrumentation development for TJNAF long range institution upgrade plan, a 12 GeV/c Super High Momentum Spectrometer (the Super HMS) has been proposed for high luminosity and high q2 physics in endstation Hall C. The fundamental configuration of Super HMS is QQDD. Two identical quadrupoles are the superconducting HMS Q1s with maximum gradient 8 Tesla/m. Two identical SLAC B202/B203 dipole magnets are considered for the use of dispersive elements with accumulative bending power 18.7 degree at 12 GeV/c while the central field is set to 2.05 Tesla. A sliding mechanism could guide the whole system, including the magnetic elements and detector house, moving forwards and backwards by +/- 100 cm. Under an assumed magnetic structure, the Super HMS optics performance has been studied by using TRANSPORT, TURTLE, and RAYTRACE codes and related reconstruction methods. The applicable solid angle can be adjusted between 1 msr and 2.3 msr. The maximum central momentum is 12 GeV/c. The reconstructed momentum resolution within full momentum range 20% is better than 10-3. The in-plane angle reconstruction accuracy is about 0.5 mr, mainly determined by the local multiple scattering from detector materials. This report also points out the strategy of super HMS optics adapting low rigidity quadrupoles for the use of high momentum operation, and the potential capability of very forward angle operations.

Chen Yan

1998-06-01T23:59:59.000Z

270

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

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

33.0 33.0 8.0 3.4 5.9 14.4 1.2 Cooking Appliances Frequency of Hot Meals Cooked 3 or More Times A Day................................................. 8.2 3.4 1.0 0.4 0.6 1.2 Q 2 Times A Day.............................................................. 24.6 8.6 2.3 1.0 1.6 3.5 0.2 Once a Day.................................................................. 42.3 10.1 2.3 1.1 2.1 4.3 0.4 A Few Times Each Week............................................. 27.2 7.8 2.0 0.7 1.3 3.6 Q About Once a Week..................................................... 3.9 1.1 Q Q Q 0.6 Q Less Than Once a Week.............................................. 4.1 1.4 Q Q Q 1.0 N No Hot Meals Cooked.................................................. 0.9 0.4 Q N Q 0.3 Q Conventional Oven Use an Oven................................................................

271

c35a.xls  

Gasoline and Diesel Fuel Update (EIA)

02 02 172 107 64 6,464 2,909 4,663 2,230 0.20 0.06 0.02 Q Building Floorspace (Square Feet) 1,001 to 10,000 ............................... 381 Q Q Q 763 Q 274 Q 0.50 Q 0.10 Q 10,001 to 100,000 ........................... 404 63 Q Q 1,806 648 985 351 0.22 0.10 Q Q Over 100,000 .................................. 517 21 45 Q 3,894 2,055 3,404 1,780 0.13 0.01 0.01 Q Principal Building Activity Education ........................................ 282 Q Q Q 933 Q Q Q 0.30 Q Q Q Health Care...................................... Q Q 17 7 Q 492 786 262 Q Q 0.02 0.03 Office .............................................. 105 6 14 1 1,379 714 1,235 748 0.08 0.01 0.01 0.00 All Others ........................................ 873 Q 47 40 3,810 1,358 2,186 1,091 0.23 Q 0.02 Q Year Constructed 1945 or Before ................................ 562 Q Q Q 2,162 Q Q Q 0.26 Q Q Q 1946 to 1959 ...................................

272

Mathematica and Fortran programs for various analytic QCD couplings  

E-Print Network [OSTI]

We outline here the motivation for the existence of analytic QCD models, i.e., QCD frameworks in which the running coupling $A(Q^2)$ has no Landau singularities. The analytic (holomorphic) coupling $A(Q^2)$ is the analog of the underlying pQCD coupling $a(Q^2) \\equiv \\alpha_s(Q^2)/\\pi$, and any such $A(Q^2)$ defines an analytic QCD model. We present the general construction procedure for the couplings $A_{\

Cesar Ayala; Gorazd Cvetic

2014-11-06T23:59:59.000Z

273

Mathematica and Fortran programs for various analytic QCD couplings  

E-Print Network [OSTI]

We outline here the motivation for the existence of analytic QCD models, i.e., QCD frameworks in which the running coupling $A(Q^2)$ has no Landau singularities. The analytic (holomorphic) coupling $A(Q^2)$ is the analog of the underlying pQCD coupling $a(Q^2) \\equiv \\alpha_s(Q^2)/\\pi$, and any such $A(Q^2)$ defines an analytic QCD model. We present the general construction procedure for the couplings $A_{\

Ayala, Cesar

2014-01-01T23:59:59.000Z

274

Advanced, Low/Zero Emission Boiler Design and Operation  

SciTech Connect (OSTI)

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.

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

2007-06-30T23:59:59.000Z

275

Professional Worker Career Experience Survey (PWCES) Data and Metadata  

E-Print Network [OSTI]

,Engineering/Architecture ,, Q4,,1,select,numeric,4,Life/Physical/Social Sciences ,, Q4,,1,select,numeric,5,Legal ,, Q4,,1,select,numeric,6,K-12 Education ,, Q4,,1,select,numeric,7,Higher Education,, Q4,,1,select,numeric,8,Health-Related ,, Q4,,1,select...Other,"If Other, please specify",1,text,text,,,, Q5,How long have you been in your current career field?,1,text,numeric,,,Work History,ITWF Q6,How many different jobs in your current career field have you held?,1,text,numeric,,,Work History,ITWF Q7...

Rosenbloom, Joshua L.; Ash, Ronald A.

2009-10-06T23:59:59.000Z

276

2008-2010 Bulletin Industrial Engineering Curriculum  

E-Print Network [OSTI]

2008-2010 Bulletin M171Q (4) MATH 181Q Industrial Engineering Curriculum FRESHMAN Fall Spring M172Q (4) MATH 182Q SOPHOMORE JUNIOR SENIOR M273Q (4) MATH 224Q Fall Spring M274 (4)* MATH 225 I&ME 364 * (3) Fall Spring I&ME 422 (3) Fall Spring I&ME 477 (3) I&ME 354 (3) I&ME 454 (3) I&ME 434 (3) PHYS 211

Dyer, Bill

277

2010-2012 Bulletin Industrial Engineering Curriculum  

E-Print Network [OSTI]

2010-2012 Bulletin M 171Q (4) MATH 181Q Industrial Engineering Curriculum FRESHMAN Fall Spring M 172Q (4) MATH 182Q SOPHOMORE JUNIOR SENIOR M 273Q (4) MATH 224Q Fall Spring M 274 (4)* MATH 225 EIND 364 (3)* I&ME 364 Fall Spring EIND 422 (3) I&ME 422 Fall Spring EIND 477 (3) I&ME 477 EIND 354 (3) I

Dyer, Bill

278

PARIS-JOURDAN SCIENCES ECONOMIQUES 48, BD JOURDAN E.N.S. 75014 PARIS  

E-Print Network [OSTI]

schemes: selected questions in analytical perspective Roger Guesnerie JEL Codes : D02, D6, D7, F18, Q4,Q5 of required attention. JEL : D02, D6, D7, F18, Q4,Q5 Institutional design, fossil fuels prices, ratchet e ect'elle mérite. JEL : D02, D6, D7, F18, Q4,Q5 Institutions, carburants fossiles, e et de cliquet, quantité contre

Paris-Sud XI, Université de

279

High-Temperature Solar Selective Coating Development for Power...  

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

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

280

The muon g-2: where we are, what does it tell us? Fred Jegerlehner  

E-Print Network [OSTI]

(p ) µ F1(q2 ) + i µq 2mµ F2(q2 ) u(p) F1(0) = 1 ; F2(0) = aµ aµ responsible for the Larmor precession

Röder, Beate

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


281

Phase I and Pharmacokinetic Study of CT-322 (BMS-844203), a Targeted Adnectin Inhibitor of VEGFR-2 Based on a Domain of Human Fibronectin  

Science Journals Connector (OSTI)

...Bristol-Myers Squibb, Princeton, New Jersey Note: Supplementary...or biweekly (q2w). Plasma samples were assayed for CT-322 concentrations, plasma VEGF-A concentrations...kg qw or q2w. CT-322 plasma concentrations increased...

Anthony W. Tolcher; Christopher J. Sweeney; Kyri Papadopoulos; Amita Patnaik; Elena G. Chiorean; Alain C. Mita; Kamalesh Sankhala; Eric Furfine; Jochem Gokemeijer; Lisa Iacono; Cheryl Eaton; Bruce A. Silver; and Monica Mita

2011-01-15T23:59:59.000Z

282

What Does a Scattering Pattern Tell US?  

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

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

283

NIF Calendar  

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

Calendar Note: Q4 schedule is being modified to reflect the new facility maintenance days on Friday Saturday. SSP* - Stockpile Stewardship Change Log...

284

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

National Nuclear Security Administration (NNSA)

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

285

Carbon Fiber Technology Facility  

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

FY13Q2 * Currently in equipment fabrication and installation * Barriers addressed - Cost - Inadequate supply base - Manufacturability Timeline * Interactions collaborations -...

286

The impact of uncertainty and risk measures  

E-Print Network [OSTI]

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

Jo, Soojin; Jo, Soojin

2012-01-01T23:59:59.000Z

287

Corrosion Studies in High-Temperature Molten Salt Systems for...  

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

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

288

High-Temperature Thermal Array for Next Generation Solar Thermal...  

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

3 Q1 High-Temperature Thermal Array for Next Generation Solar Thermal Power Production - FY13 Q1 This document summarizes the progress of this Los Alamos National Laboratory...

289

Fluctuation theory of connectivities for subcritical random cluster models  

E-Print Network [OSTI]

We develop a fluctuation theory of connectivities for subcritical random cluster models. The theory is based on a comprehensive nonperturbative probabilistic description of long connected clusters in terms of essentially one-dimensional chains of irreducible objects. Statistics of local observables, for example, displacement, over such chains obey classical limit laws, and our construction leads to an effective random walk representation of percolation clusters. The results include a derivation of a sharp Ornstein--Zernike type asymptotic formula for two point functions, a proof of analyticity and strict convexity of inverse correlation length and a proof of an invariance principle for connected clusters under diffusive scaling. In two dimensions duality considerations enable a reformulation of these results for supercritical nearest-neighbor random cluster measures, in particular, for nearest-neighbor Potts models in the phase transition regime. Accordingly, we prove that in two dimensions Potts equilibrium crystal shapes are always analytic and strictly convex and that the interfaces between different phases are always diffusive. Thus, no roughening transition is possible in the whole regime where our results apply. Our results hold under an assumption of exponential decay of finite volume wired connectivities [assumption (1.2) below] in rectangular domains that is conjectured to hold in the whole subcritical regime; the latter is known to be true, in any dimensions, when $q=1$, $q=2$, and when $q$ is sufficiently large. In two dimensions assumption (1.2) holds whenever there is an exponential decay of connectivities in the infinite volume measure. By duality, this includes all supercritical nearest-neighbor Potts models with positive surface tension between ordered phases.

Massimo Campanino; Dmitry Ioffe; Yvan Velenik

2008-08-26T23:59:59.000Z

290

A Variable flavor number scheme at NNLO.  

E-Print Network [OSTI]

.e. second order in ?S, there is much more complication f n f +1i (Q2) = ( ?S 4pi )2 ? i j (A2,0i j +A 2,1 i j ln(Q2/m2H)+A2,2i j ln2(Q2/m2H))? f n f j (Q2), Evolution of NNLO Fc2(x,Q2) -0.2 0 0.2 0.4 2 3 4 5 6 7 8 9 10 20Q2 Fc 2 (x, Q2 ) x=0.00003 x=0.001 x... =0.012 x=0.1 Evolution of NNLO F2(x,Q2) 0 0.5 1 1.5 2 2.5 2 3 4 5 6 7 8 9 10 20Q2 F 2 (x, Q2 ) x=0.00003 x=0.001 x=0.012 x=0.1 FIGURE 1. NNLO Fc2 (x,Q2) and F2(x,Q2) in zero-mass VFNS where A2,0i j is generally non-zero [2]. There is no longer a...

Thorne, Robert S

291

The structure of the nucleon Elastic and deep inelastic scattering from nucleons, 19561973  

E-Print Network [OSTI]

. The electromagnetic current for the proton involves two form factors, Jproton µ = u(pf) F1(q2 )µ + i qµ 2M F2(q2 ) u¯h/(2Mc). The form factors, F1(q2) and F2(q2), are the analogs of F(q2) in the discussion above, and F1(0) = F2(0) = 1. If the proton were a pointlike Dirac particle like the electron, we would have instead F1

Murayama, Hitoshi

292

Scaling study of the pion electroproduction cross sections and the pion form factor  

E-Print Network [OSTI]

The $^{1}$H($e,e^\\prime \\pi^+$)n cross section was measured for a range of four-momentum transfer up to $Q^2$=3.91 GeV$^2$ at values of the invariant mass, $W$, above the resonance region. The $Q^2$-dependence of the longitudinal component is consistent with the $Q^2$-scaling prediction for hard exclusive processes. This suggests that perturbative QCD concepts are applicable at rather low values of $Q^2$. Pion form factor results, while consistent with the $Q^2$-scaling prediction, are inconsistent in magnitude with perturbative QCD calculations. The extraction of Generalized Parton Distributions from hard exclusive processes assumes the dominance of the longitudinal term. However, transverse contributions to the cross section are still significant at $Q^2$=3.91 GeV$^2$.

T. Horn

2007-07-12T23:59:59.000Z

293

Nucleon form factors and static properties of baryons in a quark model  

Science Journals Connector (OSTI)

The nucleon electromagnetic form factors GEp(q2), GMp(q2), GMn(q2), and the axial-vector form factor GA(q2) are calculated in a simple independent-quark model based on the Dirac equation with a logarithmic confining potential of the form V?(r)=(1+?0)aln(rb). The respective rms radii associated with GEp(q2) and GA(q2) come out as (?r2?EP)12=0.938 fm and ?rA2?12=0.953 fm. The magnetic moments, charge radii, and axial-vector coupling-constant ratios for octet baryons are also calculated with the appropriate center-of-mass correction. The results so obtained are quite comparable to experimental data.

N. Barik, S. N. Jena, and D. P. Rath

1990-03-01T23:59:59.000Z

294

Strangeness production in Deep-Inelastic ep Scattering EPS Conference  

E-Print Network [OSTI]

Ruiz Tabasco CINVESTAV M´erida On behalf of H1 Collaboration · Introduction · Measurement of K0 s and · Measurement of K± · Summary Julia Ruiz Tabasco (DESY-CINVESTAV) Strangeness production EPS conference 1 / 15) e + (k') Q2 = -q2 = -(k - k )2, y = qP kP , xBj = Q2 2qP Julia Ruiz Tabasco (DESY

295

Notes on blowups  

E-Print Network [OSTI]

Now we can define the Zariski topology on \\pn by letting the open sets be the ..... Since g ? Q2 we have the following isomorphism letting A = S[{\

296

--No Title--  

Gasoline and Diesel Fuel Update (EIA)

188 98 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...

297

Probabilistic Performance Analysis of Fault Diagnosis Schemes  

E-Print Network [OSTI]

2.2.6 Common Probability Distributions 2.3 Reliability+ . This distribution is denoted ? ? Geo(q). 2.3 Reliability

Wheeler, Timothy Josh

2011-01-01T23:59:59.000Z

298

A Smoothing SQP Framework for a Class of Composite $L_q ...  

E-Print Network [OSTI]

Jul 28, 2014 ... Abstract: The composite $L_q$ (0<q<1) minimization problem over a general polyhedron has received various applications in machine...

Ya-Feng Liu

2014-07-28T23:59:59.000Z

299

E-Print Network 3.0 - ancillary service rate Sample Search Results  

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

Institute of Technology (MIT) Collection: Engineering ; Geosciences 15 MARCELLUS SHALE APRIL 2011 EDITION Summary: to 2011 Q1): 48,000 new hires within the Marcellus...

300

Analysis of residual spectra and the monopole spectrum for 3 K blackbody radiation by means of non-extensive thermostatistics  

E-Print Network [OSTI]

We analyze residual spectra of 3 K blackbody radiation (CMB) using non-extensive thermostatistics with a parameter q-1. The limits of |q-1|<1.2x10^{-5} and the temperature fluctuation |delta T|<(1.6-4.3)x10^{-5} are smaller than those by Tsallis et al. Moreover, analyzing the monopole spectrum by a formula including the chemical potential mu, we obtain the limits |q-1|<2.3x10^{-5} and |mu|<1.6x10^{-4}. |q-1| is comparable with the Sunyaev-Zeldovich effect y.

Minoru Biyajima; Takuya Mizoguchi

2012-10-22T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


301

Materials for Advanced Turbocharger Designs (Agreement ID:17257...  

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

for the U.S. Department of Energy Presentationname Milestones * FY2013, Q1 - complete neutron-scattering residual- stress measurements on wheelshaft assemblies with...

302

E-Print Network 3.0 - achras miller fosberg Sample Search Results  

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

Q WSU FOUNDATION Q 1 CRIMSON BENEFACTORS Summary: Corporation Steven and Janice Boots Cleve and Judith Borth +Louis and +Edythe Bosch +Edythe Miller Boucher... and Kathryn...

303

Fundamental Corrosion Studies in High-Temperature Molten Salt...  

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

Molten Salt Systems for CSP Applications - FY13 Q1 Advanced Ceramic Materials and Packaging Technologies for Realizing Sensors for Concentrating Solar Power Systems...

304

--No Title--  

Gasoline and Diesel Fuel Update (EIA)

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

305

What Does a Scattering Pattern Tell US?  

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

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

306

E-Print Network 3.0 - amr ph gl Sample Search Results  

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

Algorithm using Adaptive Mesh Refinement Summary: the complexity for constructing the AMR tree is Odtn1 ph 1 p 6dm1 qh 1 q . 4.2 Data Clustering. The stage... of the AMR...

307

Microsoft PowerPoint - 2009.10.27 Bridge Inspection Follow-up...  

Energy Savers [EERE]

Inspection Follow-up Microsoft PowerPoint - 2009.10.27 Bridge Inspection Follow-up More Documents & Publications Slide 1 Slide 1 Microsoft Word - Issue FY2009 Q4 Draft 20090910.doc...

308

Microsoft Word - Agenda F&I Update 090804.doc | Department of...  

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

Agenda F&I Update 090804.doc Microsoft Word - Agenda F&I Update 090804.doc More Documents & Publications Agenda Slide 1 Microsoft Word - Issue FY2009 Q4 Draft 20090910.doc...

309

Slide 1 | Department of Energy  

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

Slide 1 Slide 1 Slide 1 More Documents & Publications Microsoft Word - Agenda F&I Update 090804.doc Agenda Microsoft Word - Issue FY2009 Q4 Draft 20090910.doc...

310

KAPL-4756 UC-901  

Office of Scientific and Technical Information (OSTI)

E q . (4), however, is virtually,identical to the -47.9 f6.6 Jmol-K value found by Johnson and Baumanml for dissolution of freshly precipitated, amorphous Fe(OH),. As shown in...

311

The Differential Effects of Oil Demand and Supply Shocks on the Global Economy  

E-Print Network [OSTI]

We employ a set of sign restrictions on the generalized impulse responses of a Global VAR model, estimated for 38 countries/regions over the period 1979Q2.2011Q2, to discriminate between supply-driven and demand-driven oil-price shocks and to study...

Cashin, Paul; Mohaddes, Kamiar; Raissi, Maziar; Raissi, Mehdi

2012-11-01T23:59:59.000Z

312

DECIDABILITY OF SCOTT'S MODEL AS AN ORDERED Q-VECTORSPACE  

E-Print Network [OSTI]

in Scott's model, then they are provable constructively. In this paper let L = hi q2Q , whereDECIDABILITY OF SCOTT'S MODEL AS AN ORDERED Q-VECTORSPACE Mikl#19; os Erd#19; elyi-Szab#19; o Wesleyan University Abstract. Let L = hi q2Q where Q is the set of rational numbers and hq

Erdélyi-Szabó, Miklós

313

Implications of low and high energy measurements on SUSY models  

E-Print Network [OSTI]

= 2 , aµ muon anomaly (q) µ(p ) µ(p) = (-ie) ¯u(p ) µ F1(q2 ) + iµq 2mµ F2(q2 ) u(p) F1(0) = 1 ; F2

Röder, Beate

314

The muon g-2: where we are, what does it tell us? Fred Jegerlehner  

E-Print Network [OSTI]

(p ) µ(p) = (-ie) ¯u(p ) µ F1(q2 ) + i µq 2mµ F2(q2 ) u(p) F1(0) = 1 ; F2(0) = aµ aµ responsible

Röder, Beate

315

Muon g -2 Theory Fred Jegerlehner, DESY Zeuthen/Humboldt University Berlin  

E-Print Network [OSTI]

anomaly (q) µ(p ) µ(p) = (-ie) ¯u(p ) µ F1(q2 ) + i µq 2mµ F2(q2 ) u(p) F1(0) = 1 ; F2(0) = aµ aµ

Röder, Beate

316

Overview of the Standard-Model value of a -especially the hadronic contribution.  

E-Print Network [OSTI]

48: ge = 2 (1.00119 ± 0.00005) (q) µ(p ) µ(p) = (-i e) ¯u(p ) µ F1(q2 ) + i µq 2mµ F2(q2 ) u(p) F1

Röder, Beate

317

arXiv:1406.2962v1[hep-ph]11Jun2014 Reduction of the proton radius discrepancy by 3  

E-Print Network [OSTI]

. On the one hand, it enters the QED calculations of atomic energy splittings (electronic and muonic [1 of the electric and magnetic Sachs form factors GE(Q2 ) and GM (Q2 ), respectively, that depend on the invariant approach was car- ried out by Hill and Paz [4]. In contrast to their analysis, we do not constrain

318

Spin Dynamics in the Presence of Spin-orbit Interactions: from the Weak to the Strong Spin-orbit Coupling Regime  

E-Print Network [OSTI]

exponential decay rate, value approaches ?so(1 + qQ) where Q = 2m?1... q. (b) The nonzero normalized oscillatory frequency, =(i??) is always zero when q is around Q and increases linearly at large q. The slope is close to ?so? and the value approaches ?so(1? qQ) at large q where Q = 2m?1...

Liu, Xin

2012-10-19T23:59:59.000Z

319

SUPPLEMENTARY MATERIAL Supplementary Material to "High-Dimensional Structure Learning of Ising Models  

E-Print Network [OSTI]

SUPPLEMENTARY MATERIAL Supplementary Material to "High-Dimensional Structure Learning of Ising) (P, Q) := 1 2 P - Q 1 = 1 2 xX |P(x) - Q(x)|. 1.1. Analysis of Ising Models on Trees. We first derive simple expressions for Ising models Markov on trees. This will be later used upon reduction of general

Anandkumar, Animashree

320

Novel Atomic Coherence and Interference Effects in Quantum Optics and Atomic Physics  

E-Print Network [OSTI]

. . . . . . . . . . . . . . . . . . . . . . . . . 7 1. Probability Amplitude Method . . . . . . . . . . . . . . . 9 2. Density Matrix Approach . . . . . . . . . . . . . . . . . . 12 B. Maxwell-Schrodinger Equation . . . . . . . . . . . . . . . . . 14 C. Three-Level Atom.... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 27 8 Pulse shapes given by Eq.(3.17). (a) Pulse shapes with varying ? and c = 2, q = ?1, ab = 0. (b) Pulse shapes with varying c and ? = 2, q = ?1, ab = 0. . . . . . . . . . . . . . . . . . . . . . . . . . . 30 xii FIGURE Page 9 Pulse shapes...

Jha, Pankaj

2012-10-19T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


321

The effect of airflow cooling on a scramjet: a preliminary assessment  

Science Journals Connector (OSTI)

...4 as affected by the heat loss q1 through an initial...10). Figure 19. Heat added during combustion H as a multiple of h...H. For a typical hydrocarbon fuel, c would be ca...200 (h/H). The heat loss q1 due to the coolant...

1999-01-01T23:59:59.000Z

322

c36a.xls  

Gasoline and Diesel Fuel Update (EIA)

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

323

Energy Information Administration - Commercial Energy Consumption...  

Annual Energy Outlook 2013 [U.S. Energy Information Administration (EIA)]

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

324

--No Title--  

Annual Energy Outlook 2013 [U.S. Energy Information Administration (EIA)]

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

325

c36a.xls  

Gasoline and Diesel Fuel Update (EIA)

,437 ,437 178 130 82 1.10 1.04 1.21 1.28 0.22 0.06 0.03 Q Building Floorspace (Square Feet) 1,001 to 10,000 ................................. 460 Q Q Q 1.21 Q Q Q 0.60 Q Q Q 10,001 to 100,000 ............................. 444 70 Q Q 1.10 1.12 1.29 1.31 0.25 0.11 Q Q Over 100,000 .................................... 533 22 48 Q 1.03 1.06 1.08 1.26 0.14 0.01 0.01 Q Principal Building Activity Education .......................................... 293 Q Q Q 1.04 Q Q Q 0.31 Q Q Q Health Care........................................ Q Q 19 8 Q 1.06 1.08 1.16 Q Q 0.02 0.03 Office ................................................ 122 8 18 Q 1.16 1.32 1.26 1.44 0.09 0.01 0.01 0.00 All Others .......................................... 980 Q 64 50 1.12 1.02 1.34 1.26 0.26 0.10 0.03 Q Year Constructed 1945 or Before .................................. 620 Q Q Q 1.10 Q Q Q 0.29

326

c36.xls  

Gasoline and Diesel Fuel Update (EIA)

,393 ,393 176 125 81 1.10 1.03 1.21 1.28 0.23 0.06 0.03 Q Building Floorspace (Square Feet) 1,001 to 10,000 ................................. 460 Q Q Q 1.21 Q Q Q 0.61 Q Q Q 10,001 to 100,000 ............................. 408 70 Q Q 1.09 1.12 1.29 1.31 0.24 0.11 Q Q Over 100,000 .................................... 524 21 47 Q 1.03 1.05 1.07 1.26 0.14 0.01 0.02 Q Principal Building Activity Education .......................................... 293 Q Q Q 1.04 Q Q Q 0.31 Q Q Q Health Care........................................ Q Q 19 8 Q 1.06 1.08 1.16 Q Q 0.02 0.03 Office ................................................ 122 8 18 Q 1.16 1.32 1.26 1.44 0.09 0.01 0.01 0.00 All Others .......................................... 936 Q 59 50 1.12 1.01 1.34 1.26 0.27 0.11 0.04 Q Year Constructed 1945 or Before .................................. 612 Q Q Q 1.10 Q Q Q 0.29

327

Neutron electric form factor via recoil polarimetry  

SciTech Connect (OSTI)

The ratio of the electric to the magnetic form factor of the neutron, G_En/G_Mn, was measured via recoil polarimetry from the quasielastic d({pol-e},e'{pol-n)p reaction at three values of Q^2 [viz., 0.45, 1.15 and 1.47 (GeV/c)^2] in Hall C of the Thomas Jefferson National Accelerator Facility. Preliminary data indicate that G_En follows the Galster parameterization up to Q^2 = 1.15 (GeV/c)^2 and appears to rise above the Galster parameterization at Q^2 = 1.47 (GeV/c)^2.

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

2003-05-01T23:59:59.000Z

328

Constraints on MOND theory from radio tracking data of the Cassini spacecraft  

E-Print Network [OSTI]

The MOdified Newtonian Dynamics (MOND) is an attempt to modify the gravitation theory to solve the Dark Matter problem. This phenomenology is very successful at the galactic level. The main effect produced by MOND in the Solar System is called the External Field Effect parametrized by the parameter $Q_2$. We have used 9 years of Cassini range and Doppler measurements to constrain $Q_2$. Our estimate of this parameter based on Cassini data is given by $Q_2=(3 \\pm 3)\\times 10^{-27} \\ \\rm{s^{-2}}$ which shows no deviation from General Relativity and excludes a large part of the relativistic MOND theories.

Hees, A; Jacobson, R A; Park, R S

2014-01-01T23:59:59.000Z

329

Microsoft PowerPoint - C-Mod_quarterly_res_highlights_21.ppt  

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

Q4 Q4 23 October 2009 Developing the steady state, high-Z wall, high-field tokamak for ITER and beyond C-Mod Quarterly Review FY2009 Q4 * E. Marmar - Research Highlights * R. Granetz - FY09 research statistics; FY10 research plans * J. Irby - Operations and Diagnostics: FY09 highlights, FY10 plans * S. Wukitch - Advanced ICRF antenna and Fast Ferrite Tuner upgrades: status and plans * D. Whyte - FY09 Joint Facility Research Milestone: Hydrogenic Retention * B. Labombard - FY10 Joint Facility Research Milestone: Scrape-Off Layer Transport and Divertor Power Handling Agenda Recent Research Highlights * Many new and interesting results from FY2009 research operations (9.1 weeks) - Improved confinement "I-mode" - Neon and nitrogen seeded plasmas (all regimes) - H-mode pedestal physics (APS invited)

330

Molecular Pathways: Adipose Inflammation as a Mediator of Obesity-Associated Cancer  

Science Journals Connector (OSTI)

...receptors are subject to a constellation of structurally significant...S-lens and Q2 collision energy optimization for the TSQ...phosphorylation sites. Discussion The constellation of phosphorylated residues...understand how the various constellations of ERalpha phosphorylations...

Louise R. Howe; Kotha Subbaramaiah; Clifford A. Hudis; and Andrew J. Dannenberg

2013-11-15T23:59:59.000Z

331

E-Print Network 3.0 - aadu paist vitali Sample Search Results  

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

quoziente R dove e l'equivalenza di Vitali: r s r - s Q ; 2. Z1 f Source: Di Nasso, Mauro - Dipartimento di Matematica Applicata "U. Dini", Universit di Pisa Collection:...

332

Reconciling the analytic QCD with the ITEP operator product expansion philosophy  

E-Print Network [OSTI]

Analytic QCD models are those versions of QCD in which the running coupling parameter a(Q^2) has the same analytic properties as the spacelike physical quantities, i.e., no singularities in the complex Q^2 plane except on the timelike semiaxis. In such models, a(Q^2) usually differs from its perturbative analog by power terms ~(Lambda^2/Q^2)^k for large momenta, introducing thus nonperturbative terms in spacelike physical quantities whose origin is the UV regime. Consequently, it contradicts the ITEP-OPE philosophy which states that such terms can come only from the IR regimes. We investigate whether it is possible to construct analytic QCD models which respect the ITEP-OPE philosophy and, at the same time, reproduce not just the high-energy QCD observables, but also the low-energy ones, among them the well-measured semihadronic tau decay ratio.

Gorazd Cvetic; Reinhart Koegerler; Cristian Valenzuela

2010-06-22T23:59:59.000Z

333

NERSC-ScienceHighlightSlidesJune2011.pptx  

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

Accomplishments, Q2CY2011 2 Energy Resources NERSC users have explained the cause of LED droop; this may lead to less-expensive higher efficiency LED lighting. (Kioupakis Van...

334

E-Print Network 3.0 - acyl halides mediated Sample Search Results  

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

Summary: Acyl Coordination: Reactions of High-Spin Iron(I1) Alkyls with Carbon Monoxide and the Crystal... Structure of the Bidentate Acyl Fe(q2-COC6H2Me,)Br(CO) (dippe) Ann...

335

Effect of the Composition of Hydrocarbon Streams on HCCI Performance  

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

of hydrocarbon samples and can be treated as compositional variables which could describe bulk properties of the samples Sample fingerprint STEP 1: Data receiving Q(2d)RPR How...

336

Homework #1: Critical Reading Describe each of the elements of a System Engineering Design and Analysis (in the table below)  

E-Print Network [OSTI]

(rate equation) 4) Bi-valve reproduction and sustainability (not modeled) 5) Benthic growth/decay (complex biological processes modeled in VIMS) Q2: What is the context of the study? Q3: Who are the major

337

Measurement of the N --> Delta^+ (1232) Transition at High-Momentum Transfer by pi^0 Electroproduction  

SciTech Connect (OSTI)

We report a new measurement of the exclusive electroproduction reaction gamma*_p --> pi0_p to explore the evolution from soft nonperturbative physics to hard processes via the Q2 dependence of the magnetic (M1+), electric (E1+), and scalar (S1+) multipoles in the N --> Delta transition. 9000 differential cross section data points cover W from threshold to 1.4 GeV/c2, 4pi center-of-mass solid angle, and Q2 from 3 to 6 GeV2/c2, the highest yet achieved. It is found that the magnetic form factor G^*M decreases with Q2 more steeply than the proton magnetic form factor, the ratio E1+/M1+ is small and negative, indicating strong helicity nonconservation, and the ratio S1+/M1+ is negative, while its magnitude increases with Q2.

M. Ungaro; P. Stoler; I. Aznauryan; V. D. Burkert; K. Joo; L. C. Smith; G. Adams; M. Amarian; P. Ambrozewicz; M. Anghinolfi; G. Asryan; G. Audit; H. Avakian; H. Bagdasaryan; J. P. Ball; N. A. Baltzell; S. Barrow; V. Batourine; M. Battaglieri; I. Bedliski; M. Bektasoglu; M. Bellis; N. Benmouna; B. L. Berman; A. S. Biselli; B. E. Bonner; S. Bouchigny; S. Boiarinov; R. Bradford; D. Branford; W. J. Briscoe; W. K. Brooks; S. Bltmann; C. Butuceanu; J. R. Calarco; S. L. Careccia; D. S. Carman; A. Cazes; S. Chen; P. L. Cole; P. Coltharp; D. Cords; P. Corvisiero; D. Crabb; J. P. Cummings; E. De Sanctis; R. DeVita; P. V. Degtyarenko; H. Denizli; L. Dennis; A. Deur; K. V. Dharmawardane; C. Djalali; G. E. Dodge; J. Donnelly; D. Doughty; M. Dugger; S. Dytman; O. P. Dzyubak; H. Egiyan; K. S. Egiyan; L. Elouadrhiri; P. Eugenio; R. Fatemi; G. Fedotov; G. Feldman; R. J. Feuerbach; H. Funsten; M. Garon; G. Gavalian; G. P. Gilfoyle; K. L. Giovanetti; F. X. Girod; J. Goetz; C. I. O. Gordon; R. W. Gothe; K. A. Griffioen; M. Guidal; M. Guillo; N. Guler; L. Guo; V. Gyurjyan; C. Hadjidakis; R. S. Hakobyan; J. Hardie; D. Heddle; F. W. Hersman; I. Hleiqawi; M. Holtrop; K. Hicks; C. E. Hyde-Wright; Y. Ilieva; D. G. Ireland; B. S. Ishkhanov; M. M. Ito; D. Jenkins; H. S. Jo; H. G. Juengst; J. D. Kellie; M. Khandaker; W. Kim; A. Klein; F. J. Klein; A. V. Klimenko; M. Kossov; L. H. Kramer; V. Kubarovsky; J. Kuhn; S. E. Kuhn; J. Lachniet; J. M. Laget; J. Langheinrich; D. Lawrence; T. Lee; Ji Li; K. Livingston; C. Marchand; N. Markov; S. McAleer; B. McKinnon; J. W. C. McNabb; B. A. Mecking; S. Mehrabyan; J. J. Melone; M. D. Mestayer; C. A. Meyer; K. Mikhailov; R. Minehart; M. Mirazita; R. Miskimen; V. Mokeev; L. Morand; S. A. Morrow; J. Mueller; G. S. Mutchler; J. Napolitano; R. Nasseripour; S. Niccolai; G. Niculescu; I. Niculescu; B. B. Niczyporuk; M. Niroula; R. A. Niyazov; M. Nozar; G. V. O'Rielly; M. Osipenko; A. I. Ostrovidov; K. Park; E. Pasyuk; S. A. Philips; N. Pivnyuk; D. Pocanic; O. Pogorelko; E. Polli; S. Pozdniakov; B. M. Preedom; J. W. Price; Y. Prok; D. Protopopescu; L. M. Qin; B. A. Raue; G. Riccardi; G. Ricco; M. Ripani; B. G. Ritchie; F. Ronchetti; G. Rosner; P. Rossi; P. D. Rubin; F. Sabati; C. Salgado; J. P. Santoro; V. Sapunenko; R. A. Schumacher; V. S. Serov; Y. G. Sharabian; A. V. Skabelin; E. S. Smith; D. I. Sober; A. Stavinsky; S. S. Stepanyan; S. Stepanyan; B. E. Stokes; I. I. Strakovsky; S. Strauch; M. Taiuti; D. J. Tedeschi; U. Thoma; A. Tkabladze; L. Todor; S. Tkachenko; C. Tur; M. F. Vineyard; A. V. Vlassov; L. B. Weinstein; D. P. Weygand; M. Williams; E. Wolin; M. H. Wood; A. Yegneswaran; L. Zana; B. Zhang; J. Zhang; and B. Zhao

2006-09-01T23:59:59.000Z

338

E-Print Network 3.0 - a4 parity violation Sample Search Results  

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

Greg Landsberg Brown University (for... @ the Tevatron" 2 Outline l R-parity Phenomenology l Current Constraints on R-parity Violation l HERA High Q 2... Event Excess Saga l...

339

E-Print Network 3.0 - atomic parity nonconservation Sample Search...  

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

Greg Landsberg Brown University (for... @ the Tevatron" 2 Outline l R-parity Phenomenology l Current Constraints on R-parity Violation l HERA High Q 2... Event Excess Saga l...

340

Cyclone analysis for the abatement of grain sorghum emmissions in granaries  

E-Print Network [OSTI]

RE FE RENCE S APPENDIX Appendix A Appendix B Q4, Q4, 4, 7 58 62 62 77 77 85 IO4. 118 120 123 125 128 129 130 VITA TABIE OF CONTENTS (continued) Appendix C Appendix D Appendix E Appendix F Page 132 134 135 138 14O LIST... OF TABLE 4 CYCLONE SAMPLING ROUTINE 1D-1D CYCLONE--AVERAGE DUST PROPERTIES OF UPSTIKAM AND DOWNSTREAM ISOKINETIC SAMPLES 1D-2D CYCLONE--AVERAGE DUST PROPERTIES OF UPSTREAM AND DOWNSTREAM ISOKINETIC SAMPLES 2D-2D CYCLONE--AVERAGE DUST PROPERTIES...

Avant, Robert V

2012-06-07T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
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341

Hadronic Light-by-Light Scattering and the Muon Fred Jegerlehner  

E-Print Network [OSTI]

, f1, f1 OScalar exchanges: a0, f0, f0, · · · OLbL: Present & Future OTheory vs experiment: do we see(p ) µ F1(q2 ) + i µq 2mµ F2(q2 ) u(p) F1(0) = 1 ; F2(0) = aµ aµ responsible for the Larmor precession

Röder, Beate

342

How Good Are Slicing Floorplans? F.Y. Young and D.F. Wong  

E-Print Network [OSTI]

module area, = q2Amax rAtotal and r 2 is the shape exibility of each module. Our result shows oorplan F of these rectangles such that area(F) minf(1+ 1 bprc) 5 4 (1+ )gAtotal where = q2Amax r the areas are small comparing with the total area, e.g. when r = 2 and Amax = Atotal 100 , the percentage

Young, Evangeline Fun Yu

343

The axial N to Delta transition form factors from Lattice QCD  

E-Print Network [OSTI]

We evaluate the N to Delta axial transition form factors in lattice QCD in the quenched theory, with two degenerate flavors of dynamical Wilson fermions and using domain wall valence fermions with staggered sea quark configurations. We predict the ratio $C_5^A(q^2)/C_3^V(q^2)$ relevant to the parity violating asymmetry and check the validity of the off-diagonal Goldberger-Treiman relation.

C. Alexandrou; Th. Leontiou; J. W. Negele; A. Tsapalis

2006-07-20T23:59:59.000Z

344

EXISTENCE OF DICRITICAL DIVISORS Section 1: Introduction. The ...  

E-Print Network [OSTI]

Conversely, for any finite subset U of D(R)?, upon letting. ?R(U) = ? ... gives a bijection W ? W. In turn g ?? Sg gives a bijection W ? Q1(R) where. M(Sg)=(g...

2010-07-30T23:59:59.000Z

345

Agenda Compiled by VP Anna Josephson Page 1 of 3 Senate Meeting  

E-Print Network [OSTI]

://www.purdue.edu/newsroom/purduetoday/releases/2014/Q1/active- learning-center-open-forum-being-held-march-13.html III. Approval of Minutes IV Bruce bruce7@purdue.edu> Treasurer: Yang Liu #12;

Ginzel, Matthew

346

High-Temperature Solar Selective Coating Development for Power...  

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

progress of this Sandia National LaboratoriesNREL project, funded by SunShot, for the first quarter of fiscal year 2013. snlpachecofy13q1.pdf More Documents & Publications...

347

Experimental determination of dynamic Young's modulus and mechanical damping, and theoretical prediction of dislocation density for depleted uranium-0.75 wt% titanium using the PUCOT  

Science Journals Connector (OSTI)

Dynamic Young's modulus (E) and mechanical damping (Q ?1) measurements were made for three microstructures (?, ? + ?, and ??) of a depleted uranium-0.75 wt% titanium alloy. The...E and Q ...

K. H. Keene; A. Wolfenden; G. M. Ludtka

1988-08-01T23:59:59.000Z

348

ATF Video Frame Grabber Subsystems - Frequently Asked Questions  

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

III - Re-creating images from captured data (Q1) Using Matlab, how can I recreate an image from captured data (without using the ATF frame grabber program)? (A1) The easiest way is...

349

E-Print Network 3.0 - arterial pressure difference Sample Search...  

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

Collection: Mathematics 5 Bio390 Atherosclerosis and Resistance thanks to Dr. J.F. Anderson, Summary: the pressure difference required: P R * Q 1.52. In the overall...

350

E-Print Network 3.0 - acholeplasma laidlawii b Sample Search...  

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

Cedex, France. Email... lateral information is lost. b) CCD images are taken (using a Peltier-cooled camera, 12421152 pixels... by Rosenfeld (33, Eq. (6.8)): S-1 hd (q) 1 + 4...

351

What Can China Do? China's Best Alternative Outcome for Energy Efficiency and CO2 Emissions  

E-Print Network [OSTI]

Aizhu Chen. Chinas energy intensity rises 3.2 pct in Q1. Table 1 Energy Use, Energy Intensity, and GDP Data (2005-2 Table 2 Frozen 2005 Energy Intensity Baseline and Reported

G. Fridley, David

2010-01-01T23:59:59.000Z

352

The Greening of the Middle Kingdom: The Story of Energy Efficiency in China  

E-Print Network [OSTI]

China View. 2009. Chinas energy intensity down 2.9% in Q1:demand at constant energy intensity, 19802006. Source: NBS,percent reduction in energy intensity (defined as energy use

Zhou, Nan

2010-01-01T23:59:59.000Z

353

MATH 690 NOTES 1. August 22, 2007, Filtered rings As Paolo and ...  

E-Print Network [OSTI]

Aug 22, 2007 ... ?bi1 = ai1 + ?ci1, where ai1 ? R and ?ci1 ? Q1. ?R1. Then f = s. ? ...... ian local domains (R, m) for which the set G(R) of Goto numbers of...

1910-71-00T23:59:59.000Z

354

E-Print Network 3.0 - asymmetric mass distribution Sample Search...  

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

the potential energy landscape on the fission dynamics K. Mazurek1,2,a Summary: of the fis- sion valley (red dashed lines in the Fig. 1) is presented in Fig. 2 in the plane q1,...

355

Low-Cost, Lightweight Solar Concentrator | Department of Energy  

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

Documents & Publications Low-Cost, Lightweight Solar Concentrators - FY13 Q1 Low-Cost Light Weigh Thin Film Solar Concentrators Low-Cost, Lightweight Solar Concentrators FY13...

356

TOUGH+Hydrate v1.0 User's Manual: A Code for the Simulation of System Behavior in Hydrate-Bearing Geologic Media  

E-Print Network [OSTI]

of radiative heat transfer between the two grid blocks is: Q= 1: The heat exchange is activated (for grid blocks thatgrid blocks Optional; provides time-variable conditions at specific boundaries Optional; list of mass or heat

Moridis, George

2008-01-01T23:59:59.000Z

357

--No Title--  

Gasoline and Diesel Fuel Update (EIA)

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

358

A Study of Internal Friction, Electric Resistance and Shape Change in Cu-Zn and Cu-Zn-Al Alloys During Phase Transformation Use Simultaneous Measurement Method  

Science Journals Connector (OSTI)

The internal friction (Q-1), electric resistance (r), shape change (X),...-1...peaks are not due to the phase transformation but due to point defects. The electric resistance during thermoelastic martensite (TEM)...

Yuan-Ti Huang; Tian-Fei Wang; Yin Mei

1990-01-01T23:59:59.000Z

359

IKs channels open slowly because KCNE1 accessory subunits slow the movement of S4 voltage sensors in KCNQ1 pore-forming subunits  

Science Journals Connector (OSTI)

...41). Assuming nine elementary gating charges per Q1...smaller fraction of the electric field...Microelectrodes had a resistance of 0.3 M{omega}. SDF Recordings...fluorometric approach to local electric field measurements in...

Katarina J. Ruscic; Francesco Miceli; Carlos A. Villalba-Galea; Hui Dai; Yukiko Mishina; Francisco Bezanilla; Steve A. N. Goldstein

2013-01-01T23:59:59.000Z

360

264.ps  

E-Print Network [OSTI]

Jan 30, 2001 ... P.O.Box 5031, 2600 GA Delft, The Netherlands. zDepartment of ..... [10, page 4]); by taking = q 1, the de nition coincides. with (15). By using...

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


361

Differential-und Integralrechnung III Losungen fur Woche 4  

E-Print Network [OSTI]

(i) = xi und g(j) = yj. Dann saft die H¨older-Ungleichung: n i=1 |xiyi| (|xi|p ) 1 p |yj|q () 1 q wo 1/p

Mitchener, Paul

362

strucfunfigrpp.dvi  

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

21 21 NOTE: THE FIGURES IN THIS SECTION ARE INTENDED TO SHOW THE REPRESENTATIVE DATA. THEY ARE NOT MEANT TO BE COMPLETE COMPILATIONS OF ALL THE WORLD'S RELIABLE DATA. Q 2 (GeV 2 ) F 2 (x,Q 2 ) * 2 i x H1+ZEUS BCDMS E665 NMC SLAC 10 -3 10 -2 10 -1 1 10 10 2 10 3 10 4 10 5 10 6 10 7 10 -1 1 10 10 2 10 3 10 4 10 5 10 6 Figure 18.8: The proton structure function F p 2 measured in electromagnetic scattering of electrons and positrons on protons (collider experiments H1 and ZEUS for Q 2 ≥ 2 GeV 2 ), in the kinematic domain of the HERA data (see Fig. 18.10 for data at smaller x and Q 2 ), and for electrons (SLAC) and muons (BCDMS, E665, NMC) on a fixed target. Statistical and systematic errors added in quadrature are shown. The data are plotted as a function of Q 2 in bins of fixed x. Some points have been slightly offset in Q 2 for clarity. The H1+ZEUS combined binning in x is used in this plot; all other data are rebinned to the x values of

363

radhyp-web.dvi  

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

RADIATIVE RADIATIVE HYPERON DECAYS Revised July 2011 by J.D. Jackson (LBNL). The weak radiative decays of spin-1/2 hyperons, B i → B f γ, yield information about matrix elements (form factors) similar to that gained from weak hadronic decays. For a polarized spin-1/2 hyperon decaying radiatively via a ∆Q = 0, ∆S = 1 transition, the angular distribution of the direction ˆ p of the final spin-1/2 baryon in the hyperon rest frame is dN dΩ = N 4π (1 + α γ P i · ˆ p) . (1) Here P i is the polarization of the decaying hyperon, and α γ is the asymmetry parameter. In terms of the form factors F 1 (q 2 ), F 2 (q 2 ), and G(q 2 ) of the effective hadronic weak electromagnetic vertex, F 1 (q 2 )γ λ + iF 2 (q 2 )σ λµ q µ + G(q 2 )γ λ γ 5 , α γ is α γ = 2 Re[G(0)F ∗ M (0)] |G(0)| 2 + |F M (0)| 2 , (2) where F M = (m i - m f )[F 2 - F 1 /(m i + m f )]. If the decaying hyperon is unpolarized, the decay baryon has a longitudinal polarization

364

The B->pi l nu and Bs->K l nu form factors and |Vub| from 2+1-flavor lattice QCD with domain-wall light quarks and relativistic heavy quarks  

E-Print Network [OSTI]

We calculate the form factors for B->pi l nu & Bs->K l nu decay in lattice QCD. We use the (2+1)-flavor RBC-UKQCD gauge field-ensembles generated with the domain-wall fermion and Iwasaki gauge actions. For the b quarks we use the anisotropic clover action with the relativistic heavy-quark interpretation. We analyze data at 2 lattice spacings a~0.11, 0.086 fm with pion masses as light as M_pi~290 MeV. We extrapolate our numerical results to the physical light-quark masses and to the continuum and interpolate in the pion/kaon energy using SU(2) "hard-pion" chiral perturbation theory. We provide complete systematic error budgets for the vector & scalar form factors f+(q^2) & f0(q2) for B->pi l nu & Bs ->K l nu at 3 momenta that span the q^2 range accessible in our numerical simulations. Next we extrapolate these results to q^2 = 0 using a model-independent z-parameterization based on analyticity & unitarity. We present our final results for f+(q^2) & f0(q^2) as the z coefficients and matr...

Flynn, J M; Kawanai, T; Lehner, C; Soni, A; Van de Water, R S; Witzel, O

2015-01-01T23:59:59.000Z

365

DELFT UNIVERSITY OF TECHNOLOGY REPORT 06-05  

E-Print Network [OSTI]

2 - P0), (P2+ - P1) elements and (P2+ - P1) grid 9 3 Taylor Hood family mini elements Q+ 1 - Q1], the incompressible Stokes and Navier Stokes problems are solved in a square and L-shaped domain with a varying grid. Different ordering techniques of the grid points and the unknowns are used to avoid breakdown of the LU de

Vuik, Kees

366

BIG IMPROVEMENTS OF THE WEIL BOUND FOR ARTIN-SCHREIER CURVES  

E-Print Network [OSTI]

gives the estimate |Nr(f) - qr | (d - 1)(q - 1)q r 2 . This bound can be sharp in general, for instance to a somewhat better bound: |Nr(f) - qr | (d - 1)(q - 1) 2 [2q r 2 ], where [x] denotes the integer part the estimate |Nr(f) - qr | Cd,rq r+1 2 , where Cd,r is the constant Cd,r = r a=0 |a - 1| d - 2 + r - a r - a d

Wan, Daqing

367

Table 5.8. U.S. Vehicle Fuel Consumption by Family Income, 1994  

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

17.0 16 or 17 Years ... 9.6 Q Q Q 1.4 1.6 2.4 3.3 Q 1.4 2.1 30.8 Households Without Children ... 50.2 1.1 2.8 3.9 10.1 7.7 10.2 14.5 2.9 4.3 7.9 11.2...

368

Spin waves in a persistent spin-current Fermi liquid  

Science Journals Connector (OSTI)

We report two theoretical results for transverse spin waves, which arise in a system with a persistent spin current. Using Fermi liquid theory, we introduce a spin current in the ground state of a polarized or unpolarized Fermi liquid, and we derive the resultant spin waves using the Landau kinetic equation. The resulting spin waves have a q1 and q1/2 dispersion to leading order for the polarized and unpolarized systems, respectively.

J. D. Feldmann and K. S. Bedell

2010-06-14T23:59:59.000Z

369

c17.xls  

Gasoline and Diesel Fuel Update (EIA)

32 32 116 153 2,942 9,867 11,373 10.8 11.7 13.5 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 4 9 20 345 652 908 12.7 13.8 22.0 5,001 to 10,000 ................................. 3 7 8 350 732 781 7.7 9.6 10.7 10,001 to 25,000 ............................... Q 16 20 Q 1,390 1,934 Q 11.2 10.5 25,001 to 50,000 ............................... Q 8 16 Q 944 1,534 Q 8.5 10.4 50,001 to 100,000 ............................. Q 15 21 Q 1,524 1,618 Q 10.2 12.9 100,001 to 200,000 ........................... Q 17 26 Q 1,703 1,671 Q 10.1 15.5 200,001 to 500,000 ........................... Q 22 24 Q 1,673 1,801 Q 13.1 13.1 Over 500,000 .................................... Q 22 18 Q 1,248 1,126 Q 17.3 16.4 Principal Building Activity Education .......................................... Q 12 16 Q 1,384 1,990 Q 8.4 7.9 Food Sales .......................................

370

Deutsche Telekom launches new integrated location-based services in selected markets across Europe  

E-Print Network [OSTI]

Deutsche Telekom launches new integrated location-based services in selected markets across Europe in Q4 last year, services will be available in 2010 in the Netherlands and other countries Deutsche and check the weather in the area. Deutsche Telekom's LBS service is truly for the mass market. From launch

Deutschmann, Rainer

371

Assessing the physical nature of near-Earth asteroids through their dynamical histories  

E-Print Network [OSTI]

We analyze a sample of 139 near-Earth asteroids (NEAs), defined as those that reach perihelion distances $q 4.8$ au), having Tisserand parameters $2 4.8$ au of cometary origin, but it could be even lower if the NEAs in unstable orbits listed before turn out to be {\\it bona fide} asteroids from the main belt.

Fernndez, Julio A; Gallardo, Tabar; Gutirrez, Jorge N

2014-01-01T23:59:59.000Z

372

Leverage vs. Feedback: Which Effect Drives the Oil Market? Sofiane Aboura  

E-Print Network [OSTI]

on the WTI crude oil spot price. An increase in the volatility subsequent to an increase in the oil price (i- and fund-managers. Keywords: WTI, Crude Oil Price, Implied Volatility, Leverage Effect, Feedback Effect. JEL Codes: C4, G1, Q4. 1 Introduction The rise of the US benchmark oil West Texas Intermediate (WTI

Paris-Sud XI, Université de

373

S()l.9(.....Mws\\.i ,,~-Io;;"(k'-t-v liw.ikJ rea.c;(i6<-.S IAk cevr;;Jtr ~ -two ~~oJrytQl/i; a-... ~ 1{u. r-r{i&/tJ w.eei, ~  

E-Print Network [OSTI]

..fI,A- 1~.{i!)oQ4ecl. -10::'/ (11 l.,':PNA. Cal,! wti-vt (/k~ b..l ] SetH f)Jo.' 7T ~a.\\ rS,-lMo b'4rk

Potsdam, Universität

374

KEY DASHBOARD INDICATORS OF PROGRESS TOWARD Goals Human Resources, FY 09-10  

E-Print Network [OSTI]

in alignment with our service approach, technical Progress Indication capability, and regulatory requirements 2Q 3Q 4Q measuring performance, and increasing transparency · Identify, review, and enhance the top plan to reduce energy costs Supports Strategic Directions 1, 5, & 7 #12;

New Mexico, University of

375

Page 1 of 7 Installation Name ____________________________________________________________  

E-Print Network [OSTI]

chlorine q liquid flow q ammonia (NH3) q other: _______________ q gas velocity q carbon dioxide (CO2) q other: _______________ q liquid velocity q carbon monoxide (CO) q other: _______________ b) Have any modular q loop q other:______________ #12;06/07/99 Page 3 of 7 c) The system is q 4-20 mA control wiring q

US Army Corps of Engineers

376

Optoelectronic Oscillators and Their Applications to 60-GHz Fiber-Fed  

E-Print Network [OSTI]

Optoelectronic Oscillators and Their Applications to 60-GHz Fiber-Fed Wireless Systems Kwang;Optoelectronic Oscillators and Their Applications to 60-GHz Fiber-Fed Wireless Systems by Kwang-Hyun Lee-1-2. Oscillator phase noise limited by resonator's Q.............................4 1-2. Optoelectronic oscillators

Choi, Woo-Young

377

User-Aware Location Management of Prosumed Micro-services  

Science Journals Connector (OSTI)

......around 30 min on average. This time...from their own home town have a...the service consumption (white colour...transport, office, home location, public...transport, home and others Q4...provision duration? Energy consumption/mugglet popularity......

Bernhard Klein; Diego Lpez-de-Ipia; Christian Guggenmos; Jorge Prez Velasco

2014-03-01T23:59:59.000Z

378

Characterization of Metallurgical Chars by Small Angle Neutron Scattering  

Science Journals Connector (OSTI)

Characterization of Metallurgical Chars by Small Angle Neutron Scattering ... Small angle scattering measures the intensity I(q) of scattered neutrons as a function of scattering angle ? from the input beam, or alternatively, as a function of the scattering vector q:? q = |q| = (4?/?) sin(?/2), where ? is the wavelength of the incident wave. ...

I. Snook; I. Yarovsky; H. J. M. Hanley; M. Y. Lin; D. Mainwaring; H. Rogers; P. Zulli

2002-08-06T23:59:59.000Z

379

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

E-Print Network [OSTI]

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

Boyer, Edmond

380

The Smith Normal Form of the Incidence Matrix of Skew Lines in PG(3, q)  

E-Print Network [OSTI]

The Smith Normal Form of the Incidence Matrix of Skew Lines in PG(3, q) Peter Sin, University. In our case D = q4I. #12;Smith normal forms A, L define endomorphisms of the free Z-module on lines. Cokernel of A is called the Smith group and the torsion subgroup of the cokernel of L is known

Sin, Peter

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


381

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

Science Journals Connector (OSTI)

We discuss the feasibility of a weak charged current experiment using a low energy electron beam. A first goal is to measure the Q2 dependence of the axial-vector form factor ga (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 ga (Q 2). If ga (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 ga between 0.01 statistical and point to point uncorrelated uncertainties on each point. Such an experiment may also allow to measure the free-neutron magnetic form factor G M n . The experiment employs the usual techniques of electron-nucleon scattering and presents no special difficulty. Higher energy extensions are possible. They could yield measurements of ga (Q 2) up to Q 2=3 GeV2 and the possibility to access other form factors such as the almost unknown pseudoscalar form factor gP . However the experiments become much more challenging as soon as beam energies pass the pion production threshold.

2013-01-01T23:59:59.000Z

382

Structure  

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

Structure Structure functions 1 NOTE: THE FIGURES IN THIS SECTION ARE INTENDED TO SHOW THE REPRESENTATIVE DATA. THEY ARE NOT MEANT TO BE COMPLETE COMPILATIONS OF ALL THE WORLD'S RELIABLE DATA. Q 2 (GeV 2 ) F 2 (x,Q 2 ) * 2 i x H1 ZEUS BCDMS E665 NMC SLAC 10 -3 10 -2 10 -1 1 10 10 2 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 -1 1 10 10 2 10 3 10 4 10 5 10 6 Figure 16.6: The proton structure function F p 2 measured in electromagnetic scattering of positrons on protons (collider experiments ZEUS and H1), in the kinematic domain of the HERA data, for x > 0.00006 (cf. Fig. 16.9 for data at smaller x and Q 2 ), and for electrons (SLAC) and muons (BCDMS, E665, NMC) on a fixed target. Statistical and systematic errors added in quadrature are shown. The data are plotted as a function of Q 2 in bins of fixed x. Some points have been slightly offset in Q 2 for clarity. The ZEUS binning in x is used in this plot; all other data are rebinned to the x values of

383

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

SciTech Connect (OSTI)

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

Deur, Alexandre P. [JLAB

2013-11-01T23:59:59.000Z

384

c27a.xls  

Gasoline and Diesel Fuel Update (EIA)

85 85 364 550 1,861 8,301 10,356 45.4 43.8 53.1 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... Q 42 69 Q 427 741 Q 98.4 92.9 5,001 to 10,000 ................................. Q 32 49 Q 518 743 Q 62.1 65.5 10,001 to 25,000 ............................... Q 47 102 Q 952 1,860 Q 49.7 54.6 25,001 to 50,000 ............................... Q 42 78 Q 900 1,567 Q 47.1 49.6 50,001 to 100,000 ............................. Q 49 77 Q 1,421 1,611 Q 34.4 47.7 100,001 to 200,000 ........................... Q 44 73 Q 1,531 1,454 Q 28.4 50.4 200,001 to 500,000 ........................... Q 55 58 Q 1,484 1,323 Q 37.3 43.5 Over 500,000 .................................... Q 52 45 Q 1,068 1,056 Q 48.6 43.0 Principal Building Activity Education .......................................... Q 49 99 Q 1,247 1,804 Q 39.5 54.6 Food Sales .......................................

385

The Draft of ASME PTC 19  

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

ASME0027 1 Copyright © 2006 Siemens Power Generation, Inc. ASME0027 1 Copyright © 2006 Siemens Power Generation, Inc. Proceedings of PWR2006 2006 Joint Conference of ASME Power and Electric Power May 2-4, 2006, Atlanta, GA, USA PWR2006-88112 TURNING NGCC INTO IGCC: CYCLE RETROFITTING ISSUES Juan Pablo Gutierrez, MSc. Siemens Power Generation 4400 Alafaya Trail Q2-286 Orlando, FL 32826 Juangutierrez@siemens.com Terry B. Sullivan, P.E. Siemens Power Generation 4400 Alafaya Trail Q2-286 Orlando, FL 32826 Terry.Sullivan@siemens.com Gerald J. Feller, Ph.D. Siemens Power Generation 4400 Alafaya Trail Q2-286 Orlando, FL 32826 Gerald.Feller@siemens.com ABSTRACT The increase in price of natural gas and the need for a cleaner technology to generate electricity has motivated the power industry to move towards Integrated

386

 

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

Proton Electromagnetic Form Factor Ratio at Low Q2 Proton Electromagnetic Form Factor Ratio at Low Q2 Ron Guy Tel Aviv ABSTRACT Electromagnetic form factors of the nucleon are model-independent observables which encode our ignorance of its complex internal structure. In recent years significant attention has been drawn to these observables due to the discovery of unexplained deviations from previously measured results. Recoil polarization measurements are allowing the electric to magnetic form factor ratios be determined with unprecedented precision. New results from MIT-BLAST and, more recently, from Hall A at Jefferson Lab indicate that there is an unexpected decrease in the proton form factor ratio atlo w Q2 . Even newer data is expected to come from MAINZ and JLab experiments in the near future.

387

A direct measurement of meson-baryon contributions to the electroexcitation of the $N(1675){\\frac{5}{2}}^-$ nucleon resonance  

E-Print Network [OSTI]

We report on the determination of the electrocouplings for the transition from the proton to the $N^+(1675){\\frac{5}{2}}^-$ resonance state using new differential cross section data on $e p \\rightarrow e\\pi^+ n$ by the CLAS collaboration at $1.8 \\le Q^2 1675){\\frac{5}{2}}^-$ helicity amplitudes show significant coupling through the $A^p_{1/2}$ amplitude for $Q^2 \\le 4$GeV$^2$, while $A^p_{3/2}$ drops much faster and at $Q^2 \\ge 1.8$GeV$^2$ is already much smaller than $A^p_{1/2}$. Both results are consistent with the meson-baryon contributions from the dynamical coupled-channel model.

Aznauryan, I G

2014-01-01T23:59:59.000Z

388

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

SciTech Connect (OSTI)

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.

Jimenez-Delgado, Pedro [Thomas Jefferson National Accelerator Facility, Newport News, VA (United States); Accardi, Alberto [Hampton University, Hampton, VA (United States); Thomas Jefferson National Accelerator Facility, Newport News, VA (United States); Melnitchouk, Wally [Thomas Jefferson National Accelerator Facility, Newport News, VA (United States)

2014-02-01T23:59:59.000Z

389

Running coupling and power corrections in nonlinear evolution at the high-energy limit.  

E-Print Network [OSTI]

ar X iv :h ep -p h/ 06 09 08 7v 1 8 S ep 2 00 6 CERN-PH-TH/2006-170 Cavendish-HEP-06/21 Running coupling and power corrections in nonlinear evolution at the highenergy limit Einan Gardi1,2, Janne Kuokkanen3, Kari Rummukainen3,4, and Heribert... ; and (2) Bjorken x := Q2/(2p q), which is inversely proportional to the total energy s = (p + q)2 in the collision: x ? Q2/s. At high energy, the rapidity Y is directly related to Bjorken x via Y = ln(1/x). The rapidity is the natural evolution variable...

Gardi, Einan; Kuokkanen, Janne; Rummukainen, Kari; Weigert, Heribert

390

Final-state interactions in inclusive deep-inelastic scattering from the deuteron  

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

We explore the role of final-state interactions (FSI) in inclusive deep-inelastic scattering from the deuteron. Relating the inclusive cross section to the deuteron forward virtual Compton scattering amplitude, a general formula for the FSI contribution is derived in the generalized eikonal approximation, utilizing the diffractive nature of the effective hadron-nucleon interaction. The calculation uses a factorized model with a basis of three resonances with mass W~ 0.6 and Q2 2 increasing in magnitude for lower Q2, but vanishing in the high-Q2 limit due to phase space constraints. The off-shell rescattering contributes at x ~> 0.8 and is taken as an uncertainty on the on-shell result.

Cosyn, Wim [FL Intl U.; Melnitchouk, Wally [JLAB; Sargsian, Misak M. [JLAB

2014-01-01T23:59:59.000Z

391

Precision Measurements with High Energy Neutrino Beams  

E-Print Network [OSTI]

Neutrino scattering measurements offer a unique tool to probe the electroweak and strong interactions as described by the Standard Model (SM). Electroweak measurements are accessible through the comparison of neutrino neutral- and charged-current scattering. These measurements are complimentary to other electroweak measurements due to differences in the radiative corrections both within and outside the SM. Neutrino scattering measurements also provide a precise method for measuring the F_2(x,Q^2) and xF_3(x,Q^2 structure functions. The predicted Q^2 evolution can be used to test perturbative Quantum Chromodynamics as well as to measure the strong coupling constant, alpha _s, and the valence, sea, and gluon parton distributions. In addition, neutrino charm production, which can be determined from the observed dimuon events, allows the strange-quark sea to be investigated along with measurements of the CKM matrix element |V_{cd}| and the charm quark mass.

Janet M. Conrad; Michael H. Shaevitz; Tim Bolton

1997-07-03T23:59:59.000Z

392

Simultaneous QCD analysis of diffractive and inclusive DIS data  

E-Print Network [OSTI]

We perform a NLO QCD analysis of deep-inelastic scattering data, in which we account for absorptive corrections. These corrections are determined from a simultaneous analysis of diffractive deep-inelastic data. The absorptive effects are found to enhance the size of the gluon distribution at small x, such that a negative input gluon distribution at Q^2 = 1 GeV^2 is no longer required. We discuss the problem that the gluon distribution is valence-like at low scales, whereas the sea quark distribution grows with decreasing x. Our study hints at the possible importance of power corrections for Q^2 \\simeq 1--2 GeV^2.

Martin, A D; Watt, G

2004-01-01T23:59:59.000Z

393

Nuclear medium effects in $?(\\bar?)$-nucleus deep inelastic scattering  

E-Print Network [OSTI]

We study the nuclear medium effects in the weak structure functions $F_2(x,Q^2)$ and $F_3(x,Q^2)$ in the deep inelastic neutrino/antineutrino reactions in nuclei. We use a theoretical model for the nuclear spectral functions which incorporates the conventional nuclear effects, such as Fermi motion, binding and nucleon correlations. We also consider the pion and rho meson cloud contributions calculated from a microscopic model for meson-nucleus self-energies. The calculations have been performed using relativistic nuclear spectral functions which include nucleon correlations. Our results are compared with the experimental data of NuTeV and CDHSW.

H. Haider; I. Ruiz Simo; M. Sajjad Athar; M. J. Vicente Vacas

2011-08-16T23:59:59.000Z

394

Parity-Violating Electron Deuteron Scattering and the Proton's Neutral Weak Axial Vector Form Factor  

SciTech Connect (OSTI)

We report on a new measurement of the parity-violating asymmetry in quasielastic electron scattering from the deuteron at backward angles at Q2 = 0.038 (GeV/c)2. This quantity provides a determination of the neutral weak axial vector form factor of the nucleon, which can potentially receive large electroweak corrections. The measured asymmetry A = z3.51±0.57 (stat)±0.58 (syst) ppm is consistent with theoretical predictions. We also report on updated results of the previous experiment at Q2 = 0.091 (GeV/c)2, which are also consistent with theoretical predictions.

Ito, Takeyasu; Averett, Todd; Barkhuff, David; Batigne, Guillaume; Beck, Douglas; Beise, Elizabeth; Blake, A.; Breuer, Herbert; Carr, Robert; Clasie, Benjamin; Covrig, Silviu; Danagoulian, Areg; Dodson, George; Dow, Karen; Dutta, Dipangkar; Farkhondeh, Manouchehr; Filippone, Bradley; FRANKLIN, W.; Furget, Christophe; Gao, Haiyan; Gao, Juncai; Gustafsson, Kenneth; Hannelius, Lars; Hasty, R.; Allen, Alice; Herda, M.C.; Jones, CE; King, Paul; Korsch, Wolfgang; Kowalski, Stanley; Kox, Serge; Kramer, Kevin; Lee, P.; Liu, Jinghua; Martin, Jeffery; McKeown, Robert; Mueller, B.; Pitt, Mark; Plaster, Bradley; Quemener, Gilles; Real, Jean-Sebastien; Ritter, J.; Roche, Julie; Savu, V.; Schiavilla, Rocco; Seely, Charles; Spayde, Damon; Suleiman, Riad; Taylor, S.; Tieulent, Raphael; Tipton, Bryan; Tsentalovich, E.; Wells, Steven; Yang, Bin; Yuan, Jing; Yun, Junho; Zwart, Townsend

2004-03-01T23:59:59.000Z

395

The muon g-2 in the light of two photon physics and first lessons from the LHC  

E-Print Network [OSTI]

hadronic LbL: setup and problems OPseudoscalar exchanges: 0 , , OAxial exchanges: a1, f1, f1 OScalar + aµ) Dirac: gµ = 2 , aµ = 2 + · · · muon anomaly (q) µ(p ) µ(p) = (-ie) ¯u(p ) µ F1(q2 ) + i µq 2mµ F2(q2 ) u(p) F1(0) = 1 ; F2(0) = aµ aµ responsible for the Larmor precession Electromagnetic Lepton

Röder, Beate

396

Deep inelastic cross-section measurements at large y with the ZEUS detector at HERA  

E-Print Network [OSTI]

The reduced cross sections for $e^{+}p$ deep inelastic scattering have been measured with the ZEUS detector at HERA at three different centre-of-mass energies, $318$, $251$ and $225$ GeV. The cross sections, measured double differentially in Bjorken $x$ and the virtuality, $Q^2$, were obtained in the region $0.13\\ \\leq\\ y\\ \\leq\\ 0.75$, where $y$ denotes the inelasticity and $5\\ \\leq\\ Q^2\\ \\leq\\ 110$ GeV$^2$. The proton structure functions $F_2$ and $F_L$ were extracted from the measured cross sections.

ZEUS Collaboration; H. Abramowicz; I. Abt; L. Adamczyk; M. Adamus; R. Aggarwal; S. Antonelli; O. Arslan; V. Aushev; Y. Aushev; O. Bachynska; A. N. Barakbaev; N. Bartosik; O. Behnke; J. Behr; U. Behrens; A. Bertolin; S. Bhadra; I. Bloch; V. Bokhonov; E. G. Boos; K. Borras; I. Brock; R. Brugnera; A. Bruni; B. Brzozowska; P. J. Bussey; A. Caldwell; M. Capua; C. D. Catterall; J. Chwastowski; J. Ciborowski; R. Ciesielski; A. M. Cooper-Sarkar; M. Corradi; F. Corriveau; G. D'Agostini; R. K. Dementiev; R. C. E. Devenish; G. Dolinska; V. Drugakov; S. Dusini; J. Ferrando; J. Figiel; B. Foster; G. Gach; A. Garfagnini; A. Geiser; A. Gizhko; L. K. Gladilin; O. Gogota; Yu. A. Golubkov; J. Grebenyuk; I. Gregor; G. Grzelak; O. Gueta; M. Guzik; W. Hain; G. Hartner; D. Hochman; R. Hori; Z. A. Ibrahim; Y. Iga; M. Ishitsuka; A. Iudin; F. Januschek; I. Kadenko; S. Kananov; T. Kanno; U. Karshon; M. Kaur; P. Kaur; L. A. Khein; D. Kisielewska; R. Klanner; U. Klein; N. Kondrashova; O. Kononenko; Ie. Korol; I. A. Korzhavina; A. Kotanski; U. Kotz; N. Kovalchuk; H. Kowalski; O. Kuprash; M. Kuze; B. B. Levchenko; A. Levy; V. Libov; S. Limentani; M. Lisovyi; E. Lobodzinska; W. Lohmann; B. Lohr; E. Lohrmann; A. Longhin; D. Lontkovskyi; O. Yu. Lukina; J. Maeda; I. Makarenko; J. Malka; J. F. Martin; S. Mergelmeyer; F. Mohamad Idris; K. Mujkic; V. Myronenko; K. Nagano; A. Nigro; T. Nobe; D. Notz; R. J. Nowak; K. Olkiewicz; Yu. Onishchuk; E. Paul; W. Perlanski; H. Perrey; N. S. Pokrovskiy; A. S. Proskuryakov; M. Przybycien; A. Raval; P. Roloff; I. Rubinsky; M. Ruspa; V. Samojlov; D. H. Saxon; M. Schioppa; W. B. Schmidke; U. Schneekloth; T. Schorner-Sadenius; J. Schwartz; L. M. Shcheglova; R. Shevchenko; O. Shkola; I. Singh; I. O. Skillicorn; W. Slominski; V. Sola; A. Solano; A. Spiridonov; L. Stanco; N. Stefaniuk; A. Stern; T. P. Stewart; P. Stopa; J. Sztuk-Dambietz; D. Szuba; J. Szuba; E. Tassi; T. Temiraliev; K. Tokushuku; J. Tomaszewska; A. Trofymov; V. Trusov; T. Tsurugai; M. Turcato; O. Turkot; T. Tymieniecka; A. Verbytskyi; O. Viazlo; R. Walczak; W. A. T. Wan Abdullah; K. Wichmann; M. Wing; G. Wolf; S. Yamada; Y. Yamazaki; N. Zakharchuk; A. F. Zarnecki; L. Zawiejski; O. Zenaiev; B. O. Zhautykov; N. Zhmak; D. S. Zotkin

2014-04-25T23:59:59.000Z

397

Valence quark and meson cloud contributions to the $?^\\ast N \\to N^\\ast(1520)$ form factors  

E-Print Network [OSTI]

The covariant spectator quark model is applied to the $\\gamma^\\ast N \\to N^\\ast(1520)$ reaction. The valence quark contributions to the electromagnetic form factors and helicity transition amplitudes are estimated from the covariant structure of the $N^\\ast(1520)$ wave function calibrated by the experimental data for large squared momentum transfer $Q^2$. The difference between the model results and the experimental data is then used to parameterize the low $Q^2$ behavior, where meson cloud effects are assumed to dominate. This parametrization can be very useful for future studies of the reaction, as well as for the extension of the transition form factors to the timelike region.

G. Ramalho; M. T. Pea

2014-05-20T23:59:59.000Z

398

Behavior of sigma(gamma p) at Large Coherence Lengths  

E-Print Network [OSTI]

Various parametrizations of sigma(gamma p) are tried out on the small-x fixed target and HERA data. A two-Pomeron type parametrization is found to give the best reproduction of the data. The data indicate that the value of lambda(eff) for parametrizations of the form sigma(gamma p)~l^lambda(eff) approaches a constant value at high Q^2. The extrapolated values of sigma(gamma p) to very long coherence lengths are found to cross in some parametrizations for l>10^7 fm, indicating the possibility that sigma(gamma p) becomes Q^2 independent at large values of the coherence length l.

Allen Caldwell

2008-02-06T23:59:59.000Z

399

Deep inelastic cross-section measurements at large y with the ZEUS detector at HERA  

E-Print Network [OSTI]

The reduced cross sections for $e^{+}p$ deep inelastic scattering have been measured with the ZEUS detector at HERA at three different centre-of-mass energies, $318$, $251$ and $225$ GeV. The cross sections, measured double differentially in Bjorken $x$ and the virtuality, $Q^2$, were obtained in the region $0.13\\ \\leq\\ y\\ \\leq\\ 0.75$, where $y$ denotes the inelasticity and $5\\ \\leq\\ Q^2\\ \\leq\\ 110$ GeV$^2$. The proton structure functions $F_2$ and $F_L$ were extracted from the measured cross sections.

Abramowicz, H; Adamczyk, L; Adamus, M; Aggarwal, R; Antonelli, S; Arslan, O; Aushev, V; Aushev, Y; Bachynska, O; Barakbaev, A N; Bartosik, N; Behnke, O; Behr, J; Behrens, U; Bertolin, A; Bhadra, S; Bloch, I; Bokhonov, V; Boos, E G; Borras, K; Brock, I; Brugnera, R; Bruni, A; Brzozowska, B; Bussey, P J; Caldwell, A; Capua, M; Catterall, C D; Chwastowski, J; Ciborowski, J; Ciesielski, R; Cooper-Sarkar, A M; Corradi, M; Corriveau, F; D'Agostini, G; Dementiev, R K; Devenish, R C E; Dolinska, G; Drugakov, V; Dusini, S; Ferrando, J; Figiel, J; Foster, B; Gach, G; Garfagnini, A; Geiser, A; Gizhko, A; Gladilin, L K; Gogota, O; Golubkov, Yu A; Grebenyuk, J; Gregor, I; Grzelak, G; Gueta, O; Guzik, M; Hain, W; Hartner, G; Hochman, D; Hori, R; Ibrahim, Z A; Iga, Y; Ishitsuka, M; Iudin, A; Januschek, F; Kadenko, I; Kananov, S; Kanno, T; Karshon, U; Kaur, M; Kaur, P; Khein, L A; Kisielewska, D; Klanner, R; Klein, U; Kondrashova, N; Kononenko, O; Korol, Ie; Korzhavina, I A; Kotanski, A; Kotz, U; Kovalchuk, N; Kowalski, H; Kuprash, O; Kuze, M; Levchenko, B B; Levy, A; Libov, V; Limentani, S; Lisovyi, M; Lobodzinska, E; Lohmann, W; Lohr, B; Lohrmann, E; Longhin, A; Lontkovskyi, D; Lukina, O Yu; Maeda, J; Makarenko, I; Malka, J; Martin, J F; Mergelmeyer, S; Idris, F Mohamad; Mujkic, K; Myronenko, V; Nagano, K; Nigro, A; Nobe, T; Notz, D; Nowak, R J; Olkiewicz, K; Onishchuk, Yu; Paul, E; Perlanski, W; Perrey, H; Pokrovskiy, N S; Proskuryakov, A S; Przybycien, M; Raval, A; Roloff, P; Rubinsky, I; Ruspa, M; Samojlov, V; Saxon, D H; Schioppa, M; Schmidke, W B; Schneekloth, U; Schorner-Sadenius, T; Schwartz, J; Shcheglova, L M; Shevchenko, R; Shkola, O; Singh, I; Skillicorn, I O; Slominski, W; Sola, V; Solano, A; Spiridonov, A; Stanco, L; Stefaniuk, N; Stern, A; Stewart, T P; Stopa, P; Sztuk-Dambietz, J; Szuba, D; Szuba, J; Tassi, E; Temiraliev, T; Tokushuku, K; Tomaszewska, J; Trofymov, A; Trusov, V; Tsurugai, T; Turcato, M; Turkot, O; Tymieniecka, T; Verbytskyi, A; Viazlo, O; Walczak, R; Abdullah, W A T Wan; Wichmann, K; Wing, M; Wolf, G; Yamada, S; Yamazaki, Y; Zakharchuk, N; Zarnecki, A F; Zawiejski, L; Zenaiev, O; Zhautykov, B O; Zhmak, N; Zotkin, D S

2014-01-01T23:59:59.000Z

400

Determination of mechanical properties of the high temperature ceramic superconductors YBa?Cu?O????x (where x[0.5)  

E-Print Network [OSTI]

). 2. M. K Wu, J. Ashburn, C. J. Torng, P. H. Hor, R. L. Meng, L. Gao, Z. J. Huang, Y. Q. Wang, and C. W. Chu, Phys. Rev. Lett. Vol. 58, p. 908 (1987). 3. S. Jin, T. H. Tiefel, R. C. Sherwood, G. W. Kammlott and S. M. Zahurak, Appl. Phys. Lett... mass of gauge crystal mj mass of component j mq mass of quartz spacer rod ms mass of specimen md+ mg mdgq mdgqs mt nld + nlg + nlq md+ mg+ mq+ms total mass N q -1 ideal transf'ormerratio of quartz mechanical damping of component j q -1...

Rahman, Saifur

2012-06-07T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


401

A study of a lime-free calcium arsenate and lime-free calcium arsenate mixed with organic insecticides for cotton insect control  

E-Print Network [OSTI]

between observations and the fitted line: v ( a ) = - s - W - = - E c m r ? -0 2 3 9 - E q ? ( 1 2 ) 18 a n d V ( b ) " [ J ^ " T 7 3 ^ 2 T = * 7 6 5 5 * E q * ( 1 3 ) But if chi-square indicates a significant degree of heterogeneity...) (7.U081;) = 3-5012. The portion of survivors q was substituted in equation (2a) when expected probits were greater than 5o0: y = ( Y / 2 ) - q ( i ) Eq. (2A)a F or y = 6.2812 - oBUYD (2.5700) = 5-2532. A weight value was found for each corrected...

Roussel, John Severin

2013-10-04T23:59:59.000Z

402

Bayesian multiuser detection for CDMA with nonlinear modulation  

E-Print Network [OSTI]

. The probability density Welsh code l Walsh code 2 0 C g, (') ?, (& ck &(1) Spread Walsh code l Spread Welsh code 2 Fig. 1. Result of spreading on Walsh codes for q = 1, z = 4. 'r'n& Cbm. . l W( & x (m) Welsh pnooder In(ra&eever $ Random Spreader 2.... The probability density Welsh code l Walsh code 2 0 C g, (') ?, (& ck &(1) Spread Walsh code l Spread Welsh code 2 Fig. 1. Result of spreading on Walsh codes for q = 1, z = 4. 'r'n& Cbm. . l W( & x (m) Welsh pnooder In(ra&eever $ Random Spreader 2...

Phan, Van Dao

2012-06-07T23:59:59.000Z

403

Effect of unsteady wake passing frequency on boundary layer transition on the concave surface of a curved plate  

E-Print Network [OSTI]

for Q= 0. 0 (O-rods), 1. 033 (3-rods), 1. 725 (5-rods), 3A43 (10-rods), 5. 166 (15-rods). . 82 Figure 23. Ensemble-averaged velocity traces for Q = 1. 003 at different s/s. with t/r as parameter Figure 24. Ensemble-averaged velocity traces for Q = 1.... 725 at different s/s, with t/r as parameter Figure 25. Ensemble-averaged velocity traces for Q = 3. 443 at different s/s, with t/~ Page 83 89 as parameter Figure 26. Ensemble-averaged velocity traces for Q = 5. 166 at different s/s, with t/r...

Read, Robert Kevin

2012-06-07T23:59:59.000Z

404

Microsoft PowerPoint - RPS_Comp_Summary_1 CO2 IGTI 2007  

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

Ramgen Proprietary Material Ramgen Proprietary Material 0900-01217 Shock Compression Technology Applied to CCS Applications Ramgen Power Systems, Inc. Bellevue, WA 2 Ramgen Proprietary Material 0900-01217 Typical System Performance Requirements - CCS * IGCC & PC retrofits (geologic carbon sequestration) - PR ~ 100:1 (suction pressure ~ 15 psia) - Two comparably loaded stages - Stage efficiency ~ 85% - Mass flow range ~ 30% Property Summary by Station - 3,000 hp Q . 4 Intercooler CO 2 In Q . Aftercooler Electric Motor LP 1 HP 3 LP BL Control HP BL Control 5 2 CO 2 Out Q . Q . 4 Intercooler CO 2 In Q . Q . Aftercooler Electric Motor LP 1 HP 3 LP BL Control HP BL Control 5 2 CO 2 Out 4 Intercooler CO 2 In Q . Q . Aftercooler Electric Motor LP 1 HP 3 HP BL Control HP BL Control 5 2 CO 2 Out Q . Q . Single Pinion Configuration Dual Pinion Configuration Property Station

405

Questions of Indigeneity and the (Re)-Emergent Ch'orti' Maya of Honduras  

E-Print Network [OSTI]

). Conversely, some argue that states such as Mexico and El Salvador have created more inclusive definitions of indigenousQ4 to manage potentially unruly, impoverished populations (Hale 2005, 2006b; Speed 2005; Mart?nez Novo 2006; Tilley 2006). A strict social... their natural resources; and representation in Congress (Anderson 2007:393394). Thus, while the state was accepting international investments for indigenous and eco-tourism, including support for the multinational Ruta Maya (Mayan Trail) project, it found...

Metz, Brent

2010-01-01T23:59:59.000Z

406

JDJ.DVI  

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

4 4 19 October 1993 E ect of a Form Factor on dE=dx from Close Collisions J. D. Jackson Lawrence Berkeley Laboratory, Berkeley, CA 94720 Point 1: Close collisions and distant collisions contribute approximately equally to dE=dx. A form factor is possibly relevant only for the close collision half. We consider these close collisions in the \free electron" approximation. Point 2: We parameterize the pion-electron interaction with a form factor showing a -meson propagator: F Q 2 = m 2 m 2 + Q 2 ; where m = 0:77 GeV : Calculation: s = m 2 + m 2 e + 2m e E (lab) Q 2 max = s 2 m 2 + m 2 e + m 2 m 2 e 2 s T max = Q 2 max =2m e (maximum kinetic energy transfer) The form factor multiplies the cross section given by Rossi 1], p. 16, Eq. 2.3.6, which in the notation we are using then reads d dT = A T 2 1 2 T T max F (2m e T) 2 Upon multiplication by T and integration over T, we obtain the equivalent of Rossi's

407

strucfunfig.dvi  

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

NOTE: NOTE: THE FIGURES IN THIS SECTION ARE INTENDED TO SHOW THE REPRESENTATIVE DATA. THEY ARE NOT MEANT TO BE COMPLETE COMPILATIONS OF ALL THE WORLD'S RELIABLE DATA. Figure 0.8: The proton structure function F p 2 measured in electromagnetic scattering of electrons and positrons on protons (collider experiments H1 and ZEUS for Q 2 ≥ 2 GeV 2 ), in the kinematic domain of the HERA data (see Fig. 0.10 for data at smaller x and Q 2 ), and for electrons (SLAC) and muons (BCDMS, E665, NMC) on a fixed target. Statistical and systematic errors added in quadrature are shown. The data are plotted as a function of Q 2 in bins of fixed x. Some points have been slightly offset in Q 2 for clarity. The H1+ZEUS combined binning in x is used in this plot; all other data are rebinned to the x values of these data. For the purpose of plotting, F p 2 has been multiplied by 2 i x , where i x is the number of the x bin, ranging from i x = 1 (x =

408

bardecay-web.dvi  

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

BARYON BARYON DECAY PARAMETERS Written 1996 by E.D. Commins (University of California, Berke- ley). Baryon semileptonic decays The typical spin-1/2 baryon semileptonic decay is described by a matrix element, the hadronic part of which may be written as: B f f 1 (q 2 )γ λ + i f 2 (q 2 )σ λµ q µ + g 1 (q 2 )γ λ γ 5 + g 3 (q 2 )γ 5 q λ B i . (1) Here B i and B f are spinors describing the initial and final baryons, and q = p i - p f , while the terms in f 1 , f 2 , g 1 , and g 3 account for vector, induced tensor ("weak magnetism"), axial vector, and induced pseudoscalar contributions [1]. Second- class current contributions are ignored here. In the limit of zero momentum transfer, f 1 reduces to the vector coupling constant g V , and g 1 reduces to the axial-vector coupling constant g A . The latter coefficients are related by Cabibbo's theory [2], gen- eralized to six quarks (and three mixing angles) by Kobayashi

409

strucfunfigrpp.dvi  

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

1 1 NOTE: THE FIGURES IN THIS SECTION ARE INTENDED TO SHOW THE REPRESENTATIVE DATA. THEY ARE NOT MEANT TO BE COMPLETE COMPILATIONS OF ALL THE WORLD'S RELIABLE DATA. Figure 18.8: The proton structure function F p 2 measured in electromagnetic scattering of electrons and positrons on protons (collider experiments H1 and ZEUS for Q 2 ≥ 2 GeV 2 ), in the kinematic domain of the HERA data (see Fig. 18.10 for data at smaller x and Q 2 ), and for electrons (SLAC) and muons (BCDMS, E665, NMC) on a fixed target. Statistical and systematic errors added in quadrature are shown. The data are plotted as a function of Q 2 in bins of fixed x. Some points have been slightly offset in Q 2 for clarity. The H1+ZEUS combined binning in x is used in this plot; all other data are rebinned to the x values of these data. For the purpose of plotting, F p 2 has been multiplied by 2 i x , where i x is the number of the x bin, ranging from i x = 1

410

Nonlinear Oscillators Vacuum Squeezing  

E-Print Network [OSTI]

A e eAA i i DD = = DD AA =^ #12;Drive is amplified at resonance by factor Q ( ) ( )( ) 2 1 222 /1 of thermal photons in the cavity Wallraff et. al, NATURE, 2004 #12;Atom ­ Cavity detuning 1:detuning - zeptogram mass · MEMs gyroscopes, accelerometers · Gas sensors, Electronic Nose · LASER cavities

Haviland, David

411

Induced polarization of Lambda(1116) in kaon electroproduction  

SciTech Connect (OSTI)

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.

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.

2014-09-01T23:59:59.000Z

412

Random even graphs and the Ising model Geo#rey Grimmett # , Svante Janson +  

E-Print Network [OSTI]

Random even graphs and the Ising model Geo#rey Grimmett # , Svante Janson + September 19, 2007 Abstract We explore the relationship between the Ising model with inverse temperature #, the q = 2 random. For a planar graph G, the boundary edges of the + clusters of the Ising model on the planar dual of G forms

Janson, Svante

413

Muon-Nucleon Inelastic Interactions at High Energy  

Science Journals Connector (OSTI)

The inelastic interactions of 10.1-GeV/c positive and 15.8-GeV/c negative muons produced at the Brookhaven alternating gradient synchrotron have been studied in nuclear emulsions. Secondary particles produced in these interactions have been identified; their energy spectrum and angular distribution (in the c.m. system) are given for pions, kaons, and protons along with their partial cross sections. The inclusive pion-production reaction is studied and the relative shapes of the pt2 (squared transverse momentum) and pl (longitudinal momentum) distributions are discussed and compared with ?p, ?p, and pp reactions. The partial and integral cross sections have been measured for both beams along with the energy dependence of their total cross sections and are compared with theory by using the first, second, and fourth powers of 1(1+q2m?2) for ?exp(q2,?), the quantity commonly called the "virtual-photon-nucleon total cross section." The values of the structural function ?W2 are calculated for 0.025~10. The present data are compared with the previous muon data of Perl at low q2 values, and various theoretical models are considered to test scaling at low q2 values.

P. L. Jain, R. D. Malucci, M. J. Potoczak, and N. J. Wixon

1973-06-01T23:59:59.000Z

414

Appendix: Some elements of Indian Astronomy  

E-Print Network [OSTI]

. Z Z' N S P' P O W E Q Q' 2 #12;Appendix: Some elements of Indian Astronomy to two pointsChapter 1 Appendix: Some elements of Indian Astronomy 1.1 Generalities The sky is considered) perpendicular to the Celestial axis. Let us imagine an observer (O) on Earth. Since the Earth and thus the point

Paris-Sud XI, Université de

415

Multidimensional Hybrid Modulations for Ultrahigh-Speed Optical Transport  

E-Print Network [OSTI]

average symbol energy, we can increase the Euclidean distance between signal constellation points compared, in D-dimensional space ðD 9 2?, for the same average symbol energy, we can increase the Euclidean distance between signal constellation points compared with the conventional in-phase (I)/quadrature (Q) 2-D

Djordjevic, Ivan B.

416

Axisymmetric trawl cod-ends made from netting of a generalized mesh shape  

Science Journals Connector (OSTI)

......Section 4.2. The fourth region (that is, where all the circumferential mesh bars are slack) can be taken into account if we rede " ne equations (4.4) to (4.7) as follows: B D (q. 2 b Nb/2 ^0. 2 o y ^0 a Na ^0 j Nj/ 2 if o y = N min. a......

FG O'Neill

1999-06-01T23:59:59.000Z

417

Measurement of the Nucleon Structure Function in Iron Using 215- and 93-GeV Muons  

Science Journals Connector (OSTI)

This Letter presents measurements of the nucleon structure function F2(x,Q2) based on the deep-inelastic scattering of 215- and 93-GeV muons in the iron multimuon spectrometer at Fermilab. With use of a lowest-order QCD calculation, a value of ?LO=23040(stat.)80(syst.) MeV/c is found.

A. R. Clark; K. J. Johnson; L. T. Kerth; S. C. Loken; T. W. Markiewicz; P. D. Meyers; W. H. Smith; M. Strovink; W. A. Wenzel; R. P. Johnson; C. Moore; M. Mugge; R. E. Shafer; G. D. Gollin; F. C. Shoemaker; P. Surko

1983-11-14T23:59:59.000Z

418

Effect of quantum confinement on exciton-phonon interactions  

E-Print Network [OSTI]

We investigate the homogeneous linewidth of localized type-I excitons in type-II GaAs/AlAs superlattices. These localizing centers represent the intermediate case between quasi-two-dimensional (Q2D) and quasi-zero-dimensional ...

Zhao, Hui; Wachter, Sven; Kalt, Heinz

2002-08-01T23:59:59.000Z

419

Virtual Compton scattering and neutral pion electroproduction in the resonance region up to the deep inelastic region at backward angles  

SciTech Connect (OSTI)

We have made the first measurements of the virtual Compton scattering (VCS) process via the H(e,e'p)? exclusive reaction in the nucleon resonance region, at backward angles. Results are presented for the W-dependence at fixed Q2=1 GeV2, and for the Q2-dependence at fixed W near 1.5 GeV. The VCS data show resonant structures in the first and second resonance regions. The observed Q2-dependence is smooth. The measured ratio of H(e,e'p)? to H(e,e'p)?0 cross sections emphasizes the different sensitivity of these two reactions to the various nucleon resonances. Finally, when compared to Real Compton Scattering (RCS) at high energy and large angles, our VCS data at the highest W (1.8-1.9 GeV) show a striking Q2-independence, which may suggest a transition to a perturbative scattering mechanism at the quark level.

Laveissiere, Geraud; Degrande, Natalie; Jaminion, Stephanie; Jutier, Christophe; Todor, Luminita; Di Salvo, Rachele; Van Hoorebeke, L.; Alexa, L.C.; Anderson, Brian; Aniol, Konrad; Arundell, Kathleen; Audit, Gerard; Auerbach, Leonard; Baker, F.; Baylac, Maud; Berthot, J.; Bertin, Pierre; Bertozzi, William; Bimbot, Louis; Boeglin, Werner; Brash, Edward; Breton, Vincent; Breuer, Herbert; Burtin, Etienne; Calarco, John; Cardman, Lawrence; Cavata, Christian; Chang, C.; Chang, C.C.; Chang, C.; Chang, C.C.; Chang, C.; Chang, C.C.; Chang, C.; Chang, C.C.; Chen, Jian-Ping; Chudakov, Eugene; Cisbani, Evaristo; Dale, Daniel; De Jager, Cornelis; De Leo, Raffaele; Deur, Alexandre; D'Hose, Nicole; Dodge, Gail; Domingo, John; Elouadrhiri, Latifa; Epstein, Martin; Ewell, Lars; Finn, John; Fissum, Kevin; Fonvieille, Helene; Fournier, Guy; Frois, Bernard; Frullani, Salvatore; Furget, Christophe; Gao, Haiyan; Gao, Juncai; Garibaldi, Franco; Gasparian, Ashot; Gilad, Shalev; Gilman, Ronald; Glamazdin, Oleksandr; Glashausser, Charles; Gomez, Javier; Gorbenko, Viktor; Grenier, Philippe; Guichon, Pierre; Hansen, Jens-Ole; Holmes, Richard; Holtrop, Maurik; Howell, Calvin; Huber, Garth; Hyde, Charles; Incerti, Sebastien; Iodice, Mauro; Jardillier, Johann; Jones, Mark; Kahl, William; Kamalov, Sabit; Kato, Seigo; Katramatou, A.T.; Kelly, James; Kerhoas, Sophie; Ketikyan, Armen; Khayat, Mohammad; Kino, Kouichi; Kox, Serge; Kramer, Laird; Kumar, Krishna; Kumbartzki, Gerfried; Kuss, Michael; Leone, Antonio; LeRose, John; Liang, Meihua; Lindgren, Richard; Liyanage, Nilanga; Lolos, George; Lourie, Robert; Madey, Richard; Maeda, Kazushige; Malov, Sergey; Manley, D.; Marchand, Claude; Marchand, Dominique; Margaziotis, Demetrius; Markowitz, Pete; Marroncle, Jacques; Martino, Jacques; McCormick, Kathy; McIntyre, Justin; Mehrabyan, Surik; Merchez, Fernand; Meziani, Zein-Eddine; Michaels, Robert; Miller, Gerald; Mougey, Jean; Nanda, Sirish; Neyret, Damien; Offermann, Edmond; Papandreou, Zisis; Perdrisat, Charles; Perrino, R.; Petratos, Gerassimos; Platchkov, Stephane; Pomatsalyuk, Roman; Prout, David; Punjabi, Vina; Pussieux, Thierry; Quemener, Gilles; Ransome, Ronald; Ravel, Oliver; Real, Jean-Sebastien; Renard, F.; Roblin, Yves; Rowntree, David; Rutledge, Gary; Rutt, Paul; Saha, Arunava; Saito, Teijiro; Sarty, Adam; Serdarevic, A.; Smith, T.; Smirnov, G.; Soldi, K.; Sorokin, Pavel; Souder, Paul; Suleiman, Riad; Templon, Jeffrey; Terasawa, Tatsuo; Tiator, Lothar; Tieulent, Raphael; Tomasi-Gustaffson, E.; Tsubota, Hiroaki; Ueno, Hiroaki; Ulmer, Paul; Urciuoli, Guido; Van De Vyver, R.; van der Meer, Rob; Vernin, Pascal; Vlahovic, B.; Voskanyan, Hakob; Voutier, Eric; Watson, J.W.; Weinstein, Lawrence; Wijesooriya, Krishni; Wilson, R.; Wojtsekhowski, Bogdan; Zainea, Dan; Zhang, Wei-Ming; Zhao, Jie; Zhou, Z.-L.

2009-01-01T23:59:59.000Z

420

Influence of Iron and Aeration on Staphylococcus aureus Growth, Metabolism, and Transcription  

Science Journals Connector (OSTI)

...aureus strain SA564 were examined by using nuclear magnetic resonance (NMR) metabolomics...To assess the extent of the fitness cost of iron and oxygen limitation on growth...Tropsha. 2002. Beware of q2! J. Mol. Graph. Model. 20 :269-276. doi: 10.1016...

Nagender Ledala; Bo Zhang; Javier Seravalli; Robert Powers; Greg A. Somerville

2014-04-04T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


421

Study of quasielastic scattering using charged-current nu_mu-iron interactions in the MINOS Near Detector  

E-Print Network [OSTI]

Kinematic distributions from an inclusive sample of 1.41 x 10^6 charged-current nu_mu 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 used to guide the selection of a subsample enriched in quasielastic nu_mu Fe interactions, containing an estimated 123,000 quasielastic events of incident energies 1 = 2.79 GeV. Four additional subsamples representing topological and kinematic sideband regions to quasielastic scattering are also selected for the purpose of evaluating backgrounds. Comparisons using subsample distributions in four-momentum transfer Q^2 show the Monte Carlo model to be inadequate at low Q^2. Its shortcomings are remedied via inclusion of a Q^2-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 Q^2 distribution for the quasielastic-enriched sample is carried out with the axial-vector mass M_A of the dipole axial-vector form factor of the neutron as a free parameter. The effective M_A which best describes the data is 1.23 +0.13/-0.09 (fit) +0.12/-0.15 (syst.) GeV.

P. Adamson; I. Anghel; A. Aurisano; G. Barr; M. Bishai; A. Blake; G. J. Bock; D. Bogert; S. V. Cao; C. M. Castromonte; S. Childress; J. A. B. Coelho; L. Corwin; D. Cronin-Hennessy; J. K. de Jong; A. V. Devan; N. E. Devenish; M. V. Diwan; C. O. Escobar; J. J. Evans; E. Falk; G. J. Feldman; M. V. Frohne; H. R. Gallagher; R. A. Gomes; M. C. Goodman; P. Gouffon; N. Graf; R. Gran; K. Grzelak; A. Habig; S. R. Hahn; J. Hartnell; R. Hatcher; A. Holin; J. Huang; J. Hylen; G. M. Irwin; Z. Isvan; C. James; D. Jensen; T. Kafka; S. M. S. Kasahara; G. Koizumi; M. Kordosky; A. Kreymer; K. Lang; J. Ling; P. J. Litchfield; P. Lucas; W. A. Mann; M. L. Marshak; N. Mayer; C. McGivern; M. M. Medeiros; R. Mehdiyev; J. R. Meier; M. D. Messier; W. H. Miller; S. R. Mishra; S. Moed Sher; C. D. Moore; L. Mualem; J. Musser; D. Naples; J. K. Nelson; H. B. Newman; R. J. Nichol; J. A. Nowak; J. O Connor; M. Orchanian; R. B. Pahlka; J. Paley; R. B. Patterson; G. Pawloski; A. Perch; M. Pfutzner; S. Phan-Budd; R. K. Plunkett; N. Poonthottathil; X. Qiu; A. Radovic; B. Rebel; C. Rosenfeld; H. A. Rubin; M. C. Sanchez; J. Schneps; A. Schreckenberger; P. Schreiner; R. Sharma; A. Sousa; N. Tagg; R. L. Talaga; J. Thomas; M. A. Thomson; X. Tian; A. Timmons; S. C. Tognini; R. Toner; D. Torretta; J. Urheim; P. Vahle; B. Viren; J. J. Walding; A. Weber; R. C. Webb; C. White; L. Whitehead; L. H. Whitehead; S. G. Wojcicki; R. Zwaska

2014-10-31T23:59:59.000Z

422

Quantum Certificate Complexity Scott Aaronson  

E-Print Network [OSTI]

(f) R0 (f), and that QE (f) D (f). If f is partial (i.e. Dom (f) = {0, 1}n ), then Q2 (f) canQuantum Certificate Complexity Scott Aaronson Computer Science Division University of California for all i S then f (Y ) = f (X). Then CX (f) is the mini- mum size of a certificate for X, and C (f

Aaronson, Scott

423

Structure of the Virtual Photon at Neil Scott Macdonald  

E-Print Network [OSTI]

Structure of the Virtual Photon at HERA Neil Scott Macdonald Department of Physics & Astronomy , and on the scale of the probing jets, is investigated by measuring the reaction e + p ! e + + jet + jet + X as a function of Q 2 and the square of the transverse energy of the jets, E 2 T , where x obs is an estimator

Glasgow, University of

424

Quantum Certificate Complexity Scott Aaronson #  

E-Print Network [OSTI]

, that Q 0 (f) # R 0 (f), and that Q E (f) # D (f). If f is partial (i.e. Dom (f) #= {0, 1} n ), then Q 2Quantum Certificate Complexity Scott Aaronson # Computer Science Division University of California . Then the deterministic query complexity D (f) is the minimum number of queries to the y i 's needed to evaluate f , if Y

Aaronson, Scott

425

1.TIF  

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

Nuclide Table rem. Organ rem Disposal Nuclide 200 East Area Wastes Single-Shell Tanks TankResiduals Q.2 3 x 105 Thyroid 1 z 10 "3 5,100 1291 Q.6 1 x 10 S Thyroid 1 x 10-5...

426

Nuclear Effects in Deep Inelastic Scattering of Charged-Current Neutrino off Nuclear  

E-Print Network [OSTI]

Nuclear effect in the neutrino-nucleus charged-Current inelastic scattering process is studied by analyzing the CCFR and NuTeV data. Structure functions $F_2(x,Q^2)$ and $xF_3(x,Q^2)$ as well as differential cross sections are calculated by using CTEQ parton distribution functions and EKRS and HKN nuclear parton distribution functions, and compared with the CCFR and NuTeV data. It is found that the corrections of nuclear effect to the differential cross section for the charged-current anti-neutrino scattering on nucleus are negligible, the EMC effect exists in the neutrino structure function $F_2(x,Q^2)$ in the large $x$ region, the shadowing and anti-shadowing effect occurs in the distribution functions of valence quarks in the small and medium $x$ region,respectively. It is also found that shadowing effects on $F_2(x,Q^2)$ in the small $x$ region in the neutrino-nucleus and the charged-lepton-nucleus deep inelastic scattering processes are different. It is clear that the neutrino-nucleus deep inelastic scattering data should further be employed in restricting nuclear parton distributions.

Duan ChunGui; Li GuangLie; Shen PengNian

2006-04-18T23:59:59.000Z

427

--No Title--  

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

12,231 5,244 6,370 617 2,126 606 577 944 Heating Equipment (more than one may apply) Heat Pumps ... 8,814 6,502 3,362 3,117 Q 2,312 Q 216...

428

Test of QED to fourth order by study of four-lepton final states in e(+)e(?) interactions at 29 GeV with the HRS detector  

E-Print Network [OSTI]

Data taken with the High Resolution Spectrometer detector at the SLAC storage ring PEP were used to test QED to fourth order in the coupling constant ?. The experiment studied four-lepton final states produced at high Q(2) in e(+)e(?) interactions...

Baringer, Philip S.

1990-10-01T23:59:59.000Z

429

Questions, Answers and Clarifications Commercial Scale Advanced Biofuels Production Facilities Solicitation  

E-Print Network [OSTI]

Questions, Answers and Clarifications Commercial Scale Advanced Biofuels Production Facilities biofuels production facility? A.1 An existing biofuels facility is an existing facility that, as of the application due date of PON-13-601, produces (or did produce) biofuels in California. Q.2 Must an eligible

430

K9/9J)$&95LL"4-5&&  

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

J>J%)-).&F--"%19& 4BC7*)"D+%&)9*CE)")% 74"%-&J-4>F%J4E-"&F-99&9"F19& &&&&&&M-J>J-F"99O& Q W-"F)9"&"("&""-.)"9&M9E3&H"XO&& Q 2"("&9J)9&%*&J%-)1"9&...

431

ARITHMETIC OF THE OSCILLATOR REPRESENTATION Michael Harris  

E-Print Network [OSTI]

ARITHMETIC OF THE OSCILLATOR REPRESENTATION Michael Harris §1. Moduli 1.1. Let V = Q2g , and let schemes g N : Ag N [N] - (N-1 T/T)Mg N . Typeset by AMS-TEX 1 #12;2 MICHAEL HARRIS 1.3. Let : Ag N Mg N

Harris, Michael - Institut de Mathématiques de Jussieu, Université Paris 7

432

Variable flavor number schemes versus fixed order perturbation theory for charm quark electroproduction  

E-Print Network [OSTI]

Data for D*(2010) meson electroproduction in the range 10 1 GeV^2 to test whether one can distinguish between different theoretical schemes for charm quark electroproduction. We find that up to the largest Q2 measured, it is not possible to make such a differentiation. Then we point out the regions where differences between the various schemes arise.

A. Chuvakin; J. Smith; B. W. Harris

2000-10-31T23:59:59.000Z

433

Recent ZEUS Results Uwe Schneekloth  

E-Print Network [OSTI]

Experiment Structure of the Proton Structure function Neutral and Charged Current Scattering Electroweak polarization 92% (transverse) Build-up time 40min at HERA (Ee =27.5GeV) In practice, polarization is reduced, HERA CM energy equivalent to Ee = 54 TeV) · At high Q2, probe validity of QCD at smallest distance

434

The Qweak experimentThe Qweak experiment 1. Physics motivation/ what is QQweakweak  

E-Print Network [OSTI]

The Proton's Weak ChargeThe Proton's Weak Charge measures Qp ­ proton's electric charge measures Qp weak ­ proton's weak charge MEM MNC As Q2 0 At tree level in the SM (neglecting the radiative corrections) : A sensitive, low-energy extraction of the weak mixing angle. Well constraint from world data: HAPPEX, G0, A4

Martin, Jeff

435

DOI 10.1140/epja/i2005-10185-0 Eur. Phys. J. A 26, 421428 (2005)  

E-Print Network [OSTI]

total and differential cross-sections have been measured at two excess energies, Q = 2.6 MeV and 7.7 Me concerned heavier nu- clei (A > 11) but direct searches for them in the cases of lithium, carbon, oxygen-section are restricted to small excess energies (Q

Magiera, Andrzej

436

Bestimmung des ep{Wirkungsquerschnittes von Beauty-Quarks  

E-Print Network [OSTI]

Bestimmung des ep{Wirkungsquerschnittes von Beauty-Quarks durch ihren semileptonischen Zerfall in Myonen mit dem H1-Detektor bei HERA Determination of the ep Cross Section for Beauty Quarks via werden die sichtbaren ep-Wirkungsquerschnitte fur schwere Quarks in dem kinematischen Bereich Q2

437

JAROSLAW NOWAK  

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

CC1 + events CC1 + Resonant 81 CC1 + Coherent 5.9 CCQE 5.3 Multi-pion 3.8 CC1 0 1.5 No muon mass in dynamics in CC + 52209 2 J. Nowak - NuInt09 The Q 2 distribution has been...

438

Optical disk resonators with micro-wave free spectral range for optoelectronic oscillator  

E-Print Network [OSTI]

Optical disk resonators with micro-wave free spectral range for optoelectronic oscillator Herv to the resonator relaxation time = Q/ [2]. The optoelectronic delayed feed- back loop can thus oscillate at all. frequency selective resonator (e.g with a high Q factor). The detailed architecture is an optoelectronic

Paris-Sud XI, Université de

439

Energy Flow Energy Flow Energy Flow A.Ukleja, T.Tymieniecka, I.Skillicorn 1 Azimuthal asymmetry  

E-Print Network [OSTI]

Energy Flow Energy Flow Energy Flow A.Ukleja, T.Tymieniecka, I.Skillicorn 1 Azimuthal asymmetry using energy flow method Azimuthal angle distribution at Q2 >100 GeV2 Energy flow method.Ukleja on behalf of the ZEUS Collaboration #12; Energy Flow Energy Flow Energy Flow A.Ukleja, T.Tymieniecka, I

440

Michel et al Juin 2000 1 PERCOLATION IN A MODEL TRANSIENT NETWORK  

E-Print Network [OSTI]

. Usually this mode is overdamped due to the viscosity of the liquid solvent: it has a q2 dependence measurements are perfomed to characterize the dynamic behavior of an o/w droplet microemulsion into which 2000 2 R and S are of the same order, they both vanishes at the percolation threshold according

Boyer, Edmond

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


441

Cremona special sets of points in products of projective spaces  

E-Print Network [OSTI]

by the Coxeter graph of type Tp,q,r. We will be interested in the cases when the group Wp,q,r is infinite, if q = 2, the group of automorphisms of the blow-up surface becomes iso- morphic to a subgroup

Dolgachev, Igor V.

442

Jet Measurements and Extraction of the Strong Coupling Constant at HERA  

E-Print Network [OSTI]

Results on jet measurements in neutral current deep inelastic scattering at HERA are presented. The low-$x_{Bj}$ and low-$Q^2$ region is explicitly investigated using forward jet production and the azimuthal asymmetry between jets in dijet production. Recent results on the determination of the strong coupling constant, $\\alpha_s(M_Z)$, are discussed.

A. A. Savin

2005-05-22T23:59:59.000Z

443

" Million U.S. Housing Units"  

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

"Non-Hispanic Descent",96.3,17.3,24.7,35.8,18.4 "Race of Householder2, 3" "White",79.1,14.7,21,27.4,16 "Hispanic",5,0.8,"Q",2.1,2.1 "Non-Hispanic",74.1,13.9,20.9,25.4,...

444

DESY14083 Measurement of beauty and charm production  

E-Print Network [OSTI]

as a function of Q2, Bjorken x, jet transverse energy and pseudorapidity were measured and compared with next,e, V. Sola13, A. Solano29, A. Spiridonov10,k, L. Stanco23, N. Stefaniuk10, A. Stern27, T.P. Stewart

445

DISCRETE AND CONTINUOUS Website: www.AIMSciences.org DYNAMICAL SYSTEMS  

E-Print Network [OSTI]

is the generalized Swift-Hohenberg equation u t = ru - 2 x + q2 c 2 u + f(u) , - b3u3 - b5u5 , or f(u) = f23 c2u2 - c3u3 . Here b5, c3 > 0 provide large amplitude stabilization

Knobloch, Edgar

446

Fields of uinvariant 2 r + 1 November 21, 2006  

E-Print Network [OSTI]

assign so­called generic discrete in­ variant GDI(Q) ­ see [14], which is defined as the collection of subrings GDI(Q, i) := image(CH # (G(Q, i))/2 # CH # (G(Q, i)| k )/2), for all 0 6 i 6 d := [dim(Q)/2

447

University of Idaho 2009 GRADUATING SENIOR SURVEY  

E-Print Network [OSTI]

1 University of Idaho 2009 GRADUATING SENIOR SURVEY Class of 2008-09 Number of respondents n = 1370 are you with the quality of the education you received at the University of Idaho? 1 2 62 35 Q-2 effectively 4 20 45 31 Communicate well orally 5 20 45 30 Apply scientific principles and methods 9 24 36 30

O'Laughlin, Jay

448

"Coarse" Notes Population Genetics SELECTION & THE SINGLE DIALLELIC DIPLOID LOCUS. 1  

E-Print Network [OSTI]

selection (but before reproduction) · denoted by * · PAA * = number of AA parents surviving total number is the population mean fitness. · Similarly, PAa * = 2 pq wAa w , Paa * = q 2 waa w . ­ Allele frequencies after selection and reproduction · If surviving parents mate randomly, then p = p * = PAA * + 1 2 PAa * = p 2 w

Gomulkiewicz, Richard

449

A scaler-based data acquisition system for measuring parity violation asymmetry in deep inelastic scattering  

E-Print Network [OSTI]

An experiment that measured the parity violating (PV) asymmetry Ad in e- 2H deep inelastic scattering (DIS) at Q2 ~ 1.10 and 1.90 (GeV/c) 2 and XB ~ 0.3 was completed in experimental Hall A at the Thomas Jefferson National ...

Pan, Kai, S.M. Massachusetts Institute of Technology

2013-01-01T23:59:59.000Z

450

Diffractive Electroproduction of rho and phi Mesons at HERA  

E-Print Network [OSTI]

Diffractive electroproduction of rho and phi mesons is measured at HERA with the H1 detector in the elastic and proton dissociative channels. The data correspond to an integrated luminosity of 51 pb^-1. About 10500 rho and 2000 phi events are analysed in the kinematic range of squared photon virtuality 2.5 < Q^2 < 60 GeV^2, photon-proton centre of mass energy 35 < W < 180 GeV and squared four-momentum transfer to the proton |t| < 3 GeV^2. The total, longitudinal and transverse cross sections are measured as a function of Q^2, W and |t|. The measurements show a transition to a dominantly "hard" behaviour, typical of high gluon densities and small q\\bar{q} dipoles, for Q^2 larger than 10 to 20 GeV^2. They support flavour independence of the diffractive exchange, expressed in terms of the scaling variable (Q^2 + M_V^2)/4, and proton vertex factorisation. The spin density matrix elements are measured as a function of kinematic variables. The ratio of the longitudinal to transverse cross sections, t...

Aaron, FD; Alexa, C; Andreev, V; Antunovic, B; Asmone, A; Backovic, S; Baghdasaryan, A; Barrelet, E; Bartel, W; Begzsuren, K; Belousov, A; Bizot, J C; Boudry, V; Bozovic-Jelisavcic, I; Bracinik, J; Brandt, G; Brinkmann, M; Brisson, V; Bruncko, D; Bunyatyan, A; Buschhorn, G; Bystritskaya, L; Campbell, A J; Cantun Avila, K B; Cassol-Brunner, F; Cerny, K; Cerny, V; Chekelian, V; Cholewa, A; Contreras, J G; Coughlan, J A; Cozzika, G; Cvach, J; Dainton, J B; Daum, K; Deak, M; de Boer, Y; Delcourt, B; Del Degan, M; Delvax, J; De Wolf, E A; Diaconu, C; Dodonov, V; Dossanov, A; Dubak, A; Eckerlin, G; Efremenko, V; Egli, S; Eliseev, A; Elsen, E; Falkiewicz, A; Favart, L; Fedotov, A; Felst, R; Feltesse, J; Ferencei, J; Fischer, D J; Fleischer, M; Fomenko, A; Gabathuler, E; Gayler, J; Ghazaryan, S; Glazov, A; Glushkov, I; Goerlich, L; Gogitidze, N; Gouzevitch, M; Grab, C; Greenshaw, T; Grell, B R; Grindhammer, G; Habib, S; Haidt, D; Helebrant, C; Henderson, R C W; Hennekemper, E; Henschel, H; Herbst, M; Herrera, G; Hildebrandt, M; Hiller, K H; Hoffmann, D; Horisberger, R; Hreus, T; Jacquet, M; Janssen, M E; Janssen, X; Jonsson, L; Jung, A W; Jung, H; Kapichine, M; Katzy, J; Kenyon, I R; Kiesling, C; Klein, M; Kleinwort, C; Kluge, T; Knutsson, A; Kogler, R; Kostka, P; Kraemer, M; Krastev, K; Kretzschmar, J; Kropivnitskaya, A; Kruger, K; Kutak, K; Landon, M P J; Lange, W; Lastovicka-Medin, G; Laycock, P; Lebedev, A; Leibenguth, G; Lendermann, V; Levonian, S; Li, G; Lipka, K; Liptaj, A; List, B; List, J; Loktionova, N; Lopez-Fernandez, R; Lubimov, V; Lytkin, L; Makankine, A; Malinovski, E; Marage, P; Marti, Ll; Martyn, H U; Maxfield, S J; Mehta, A; Meyer, A B; Meyer, H; Meyer, H; Meyer, J; Michels, V; Mikocki, S; Milcewicz-Mika, I; Moreau, F; Morozov, A; Morris, J V; Mozer, M U; Mudrinic, M; Muller, K; Murin, P; Naumann, Th; Newman, P R; Niebuhr, C; Nikiforov, A; Nowak, G; Nowak, K; Nozicka, M; Olivier, B; Olsson, J E; Osman, S; Ozerov, D; Palichik, V; Panagoulias, I; Pandurovic, M; Papadopoulou, Th; Pascaud, C; Patel, G D; Pejchal, O; Perez, E; Petrukhin, A; Picuric, I; Piec, S; Pitzl, D; Placakyte, R; Pokorny, B; Polifka, R; Povh, B; Preda, T; Radescu, V; Rahmat, A J; Raicevic, N; Raspiareza, A; Ravdandorj, T; Reimer, P; Rizvi, E; Robmann, P; Roland, B; Roosen, R; Rostovtsev, A; Rotaru, M; Ruiz Tabasco, J E; Rurikova, Z; Rusakov, S; Salek, D; Sankey, D P C; Sauter, M; Sauvan, E; Schmitt, S; Schoeffel, L; Schoning, A; Schultz-Coulon, H C; Sefkow, F; Shaw-West, R N; Shtarkov, L N; Shushkevich, S; Sloan, T; Smiljanic, I; Soloviev, Y; Sopicki, P; South, D; Spaskov, V; Specka, A; Staykova, Z; Steder, M; Stella, B; Stoicea, G; Straumann, U; Sunar, D; Sykora, T; Tchoulakov, V; Thompson, G; Thompson, P D; Toll, T; Tomasz, F; Tran, T H; Traynor, D; Trinh, T N; Truol, P; Tsakov, I; Tseepeldorj, B; Turnau, J; Urban, K; Valkarova, A; Vallee, C; Van Mechelen, P; Vargas Trevino, A; Vazdik, Y; Vinokurova, S; Volchinski, V; von den Driesch, M; Wegener, D; Wissing, Ch; Wunsch, E; Zacek, J; Zalesak, J; Zhang, Z; Zhokin, A; Zimmermann, T; Zohrabyan, H; Zomer, F; Zus, R

2010-01-01T23:59:59.000Z

451

Separated Response Functions in Exclusive, Forward $?^{\\pm}$ Electroproduction on Deuterium  

E-Print Network [OSTI]

Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, $Q^2$, 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 $\\pi^-$ and $\\pi^+$ electroproduction are particularly informative. The 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: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central $Q^2$ values of 0.6, 1.0, 1.6 GeV$^2$ at W=1.95 GeV, and $Q^2$=2.45 GeV$^2$ at W=2.22 GeV. There was significant coverage in $\\phi$ and $\\epsilon$, which allowed separation of $\\sigma_{L,T,LT,TT}$. Results: $\\sigma_L$ shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, $\\sigma_T$ is much flatter versus t. The longitudinal/transverse ratios evolve with $Q^2$ and t, and at the highest $Q^2$=2.45 GeV$^2$ show a slight enhancement for $\\pi^-$ production compared to $\\pi^+$. The $\\pi^-/\\pi^+$ ratio for transverse photons exhibits only a small $Q^2$-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 $\\sigma_{TT}/\\sigma_T$ ratio also drops rapidly with $Q^2$, qualitatively consistent with s-channel helicity conservation. The $\\pi^-/\\pi^+$ 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.

G. M. Huber; H. P. Blok; C. Butuceanu; D. Gaskell; T. Horn; D. J. Mack; D. Abbott; K. Aniol; H. Anklin; C. Armstrong; J. Arrington; K. Assamagan; S. Avery; O. K. Baker; B. Barrett; E. J. Beise; C. Bochna; W. Boeglin; E. J. Brash; H. Breuer; C. C. Chang; N. Chant; M. E. Christy; J. Dunne; T. Eden; R. Ent; H. Fenker; E. F. Gibson; R. Gilman; K. Gustafsson; W. Hinton; R. J. Holt; H. Jackson; S. Jin; M. K. Jones; C. E. Keppel; P. H. Kim; W. Kim; P. M. King; A. Klein; D. Koltenuk; V. Kovaltchouk; M. Liang; J. Liu; G. J. Lolos; A. Lung; D. J. Margaziotis; P. Markowitz; A. Matsumura; D. McKee; D. Meekins; J. Mitchell; T. Miyoshi; H. Mkrtchyan; B. Mueller; G. Niculescu; I. Niculescu; Y. Okayasu; L. Pentchev; C. Perdrisat; D. Pitz; D. Potterveld; V. Punjabi; L. M. Qin; P. E. Reimer; J. Reinhold; J. Roche; P. G. Roos; A. Sarty; I. K. Shin; G. R. Smith; S. Stepanyan; L. G. Tang; V. Tadevosyan; V. Tvaskis; R. L. J. van der Meer; K. Vansyoc; D. Van Westrum; S. Vidakovic; J. Volmer; W. Vulcan; G. Warren; S. A. Wood; C. Xu; C. Yan; W. -X. Zhao; X. Zheng; B. Zihlmann; The Jefferson Lab Fpi Collaboration

2014-12-16T23:59:59.000Z

452

Separated Response Functions in Exclusive, Forward pi Electroproduction on Deuterium  

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

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 ?? And ?+ electroproduction are particularly informative. The 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: 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 ? And ?, which allowed separation of ?L,T,LT,TT. Results: ?L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, ?T 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 ?? Production compared to ?+. The ??/?+ 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 ?TT/?T ratio also drops rapidly with Q2, qualitatively consistent with s-channel helicity conservation. The ??/?+ 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.

Huber, G. M.; Blok, H. P.; Butuceanu, C.; Gaskell, D.; Horn, T.; Mack, D. J.; Abbott, D.; Aniol, K.; Anklin, H.; Armstrong, C.; Arrington, J.; Assamagan, K.; Avery, S.; Baker, O. K.; Barrett, B.; Beise, E. J.; Bochna, C.; Boeglin, W.; Brash, E. J.; Breuer, H.; Chang, C. C.; Chant, N.; Christy, M. E.; Dunne, J.; Eden, T.; Ent, R.; Fenker, H.; Gibson, E. F.; Gilman, R.; Gustafsson, K.; Hinton, W.; Holt, R. J.; Jackson, H.; Jin, S.; Jones, M. K.; Keppel, C. E.; Kim, P. H.; Kim, W.; King, P. M.; Klein, A.; Koltenuk, D.; Kovaltchouk, V.; Liang, M.; Liu, J.; Lolos, G. J.; Lung, A.; Margaziotis, D. J.; Markowitz, P.; Matsumura, A.; McKee, D.; Meekins, D.; Mitchell, J.; Miyoshi, T.; Mkrtchyan, H.; Mueller, B.; Niculescu, G.; Niculescu, I.; Okayasu, Y.; Pentchev, L.; Perdrisat, C.; Pitz, D.; Potterveld, D.; Punjabi, V.; Qin, L. M.; Reimer, P. E.; Reinhold, J.; Roche, J.; Roos, P. G.; Sarty, A.; Shin, I. K.; Smith, G. R.; Stepanyan, S.; Tang, L. G.; Tadevosyan, V.; Tvaskis, V.; van der Meer, R. L.; Vansyoc, K.; Van Westrum, D.; Vidakovic, S.; Volmer, J.; Vulcan, W.; Warren, G.; Wood, S. A.; Xu, C.; Yan, C.; Zhao, W.-X.; Zheng, X.; Zihlmann, B.

2014-01-01T23:59:59.000Z

453

c27.xls  

Gasoline and Diesel Fuel Update (EIA)

73 73 343 512 1,465 7,716 9,570 49.5 44.4 53.5 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... Q 41 68 Q 417 729 Q 99.5 93.6 5,001 to 10,000 ................................. Q 31 43 Q 482 654 Q 64.8 66.0 10,001 to 25,000 ............................... Q 45 90 Q 931 1,681 Q 47.9 53.6 25,001 to 50,000 ............................... Q 39 70 Q 829 1,422 Q 47.4 49.5 50,001 to 100,000 ............................. Q 43 73 Q 1,263 1,554 Q 34.1 47.2 100,001 to 200,000 ........................... Q 41 67 Q 1,445 1,264 Q 28.3 52.7 200,001 to 500,000 ........................... Q 55 56 Q 1,484 1,277 Q 37.3 44.1 Over 500,000 .................................... Q 47 44 Q 865 989 Q 54.0 44.4 Principal Building Activity Education .......................................... Q 49 99 Q 1,247 1,804 Q 39.5 54.6 Food Sales .......................................

454

SHARP THRESHOLDS FOR THE RANDOM-CLUSTER AND ISING MODELS  

E-Print Network [OSTI]

SHARP THRESHOLDS FOR THE RANDOM-CLUSTER AND ISING MODELS BENJAMIN GRAHAM AND GEOFFREY GRIMMETT. The models in question are the random-cluster model near the self-dual point psd(q) = q/(1 + q), the Ising in statistical physics, namely those of the random-cluster model and the Ising model. In each case, the event

Grimmett, Geoffrey

455

b11.pdf  

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

11,774 Q Q Q Q 1,100 2,426 8,086 Other Electronic Equipment (more than one may apply) Laser Printers ... 46,567 3,246 3,323 5,128 8,881...

456

Nonextensive effects on the relativistic nuclear equation of state  

E-Print Network [OSTI]

The Walecka many-body field theory is investigated in the context of quantum nonextensive statistical mechanics, characterized by a dimensionless parameter $q$. We consider nuclear matter described statistically by a power-law distribution which generalizes the standard Fermi-Dirac distribution ($q = 1$). We show that the scalar and vector meson fields become more intense due to the nonextensive effects ($q \

F. I. M. Pereira; R. SIlva; J. S. Alcaniz

2007-05-02T23:59:59.000Z

457

A Mutant Form of the Neisseria gonorrhoeae Pilus Secretin Protein PilQ Allows Increased Entry of Heme and Antimicrobial Compounds  

Science Journals Connector (OSTI)

...grids were used to lift cells directly from...solidified GC agar. Four filter paper disks...of them carried a point mutation in hpuB...precisely the same point mutation in one...FA7186H19. The other four hgbX mutants had the...preservation of the pilQ1 point mutation. The necessity...

Ching-ju Chen; Deborah M. Tobiason; Christopher E. Thomas; William M. Shafer; H. Steven Seifert; P. Frederick Sparling

2004-02-01T23:59:59.000Z

458

Quarter 1, 2012 Page 1 of 2  

E-Print Network [OSTI]

incompatible chemicals? 16. Are incompatible chemicals segregated according to SU storage scheme? 17. Is lab-level contact. (Return roster with completed Q1-12 Self-Inspection checklist to department) 22. Our lab has. Make sure that ALL rooms listed for your PI have been included as part of this quarter's self

Ford, James

459

rsif.royalsocietypublishing.org Cite this article: Menguc Y, Rohrig M,  

E-Print Network [OSTI]

Institute of Technology (KIT), 76344 Eggenstein-Leopoldshafen, Germany The exceptionally adhesive foot¨lscher H, Sitti M. 2014 Staying sticky: contact self-cleaning of gecko-inspired adhesives. J. R. Soc 2014 Subject Areas: biomimetics Keywords: adhesion, gecko, self-cleaning, contactQ1 , micro

Sitti, Metin

460

Alpha-particle physics in tokamaks  

Science Journals Connector (OSTI)

...achieving ignition or high fusion gain regimes (Q 1) in a tokamak...as an example. Keywords: fusion; tokamak; energetic -particles...Self-sustained ignition of a thermonuclear plasma in a tokamak reactor...4 He ions) produced from fusion reactions. The -particles...

1999-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q2" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
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We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


461

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

E-Print Network [OSTI]

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

Hu, Qinhong "Max"

462

ITC-12/APFA'01 December 10-14, 2001  

E-Print Network [OSTI]

) Electricity Generation Equivalent Q > 1 ~ Advanced Tokamak Study Reactor Technologies Core Program/NIFSUniversities/NIFS STASTA JAERI/Nat. Labs.JAERI/Nat. Labs. MEXTMEXT Ministry of Education,Ministry of Education, CultureMagneto-- electric/Magnetelectric/Magnet System/SafetySystem/Safety ICFICF Structural MaterialsStructural Materials

463

--No Title--  

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

2,711 1,916 1,197 2,649 942 1,565 973 1,638 Heating Equipment (more than one may apply) Heat Pumps ... 8,814 Q 1,019 719 339 3,677 542 722 333...

464

Energy Information Administration - Commercial Energy Consumption...  

Annual Energy Outlook 2013 [U.S. Energy Information Administration (EIA)]

Q 375 261 764 2,711 1,916 161.3 138.2 136.1 Heating Equipment (more than one may apply) Heat Pumps ... Q 141 68 Q 1,019 719 Q 137.9 94.1 Packaged...

465

--No Title--  

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

386 276 Q Q 68 3,210 1,767 Q Q 1,068 Heating Equipment (more than one may apply) Heat Pumps ... 476 N 37 61 378 8,814 N 670 1,497 6,647...

466

b34.xls  

Gasoline and Diesel Fuel Update (EIA)

386 276 Q Q 68 3,210 1,767 Q Q 1,068 Heating Equipment (more than one may apply) Heat Pumps ... 476 N 37 61 378 8,814 N 670 1,497 6,647...

467

--No Title--  

Gasoline and Diesel Fuel Update (EIA)

29 24 28 1,177 931 1,401 24.4 26.0 19.8 Heating Equipment (more than one may apply) Heat Pumps ... 12 Q 17 722 Q 1,268 16.2 Q 13.4 Packaged...

468

--No Title--  

Annual Energy Outlook 2013 [U.S. Energy Information Administration (EIA)]

58 134 75 1,284 3,076 1,551 45.5 43.5 48.6 Heating Equipment (more than one may apply) Heat Pumps ... Q 66 17 Q 1,947 373 Q 33.8 45.1 Packaged...

469

Dynamics of plasma formation during quasicontinuous laser irradiation of metals in high-pressure nitrogen atmospheres  

Science Journals Connector (OSTI)

This is a study of target destruction and the dynamics of surface plasma formation during the interaction of quasicontinuous laser...q = 17 MW/cm2..., ? ? 1.5 msec) with D16T duraluminum and bismuth in nitrogen

V. I. Nasonov; Yu. A. Chivel

2009-11-01T23:59:59.000Z

470

Contemporary Mathematics Algebraic Multigrid and Schur Complement Strategies  

E-Print Network [OSTI]

form: ut + g = F(1.1) t + · [(h + )u] = Q(1.2) where u = (u, v) is the velocity vector, is the sea acceleration, h is the resting depth of the fluid, Q is a mass source/sink term. The vector F = (fx , fy, viscous dissipation, and wind forcing. For simplicity, we assume no-slip boundary conditions. The shallow

Douglas, Craig C.

471

A Combinatorial Model for the Macdonald Polynomials Department of Mathematics  

E-Print Network [OSTI]

A Combinatorial Model for the Macdonald Polynomials J. Haglund Department of Mathematics University that ? C µ [Z; q, t] is none other than the modified Macdonald polynomial ? H µ [Z; q, t]. We further partition, set ? K #,µ (q, t) = t #(µ) K #,µ (q, 1/t), where K #,µ (q, t) is Macdonald's q, t

Haglund, Jim

472

A Combinatorial Model for the Macdonald Polynomials Department of Mathematics  

E-Print Network [OSTI]

A Combinatorial Model for the Macdonald Polynomials J. Haglund Department of Mathematics University, t] is none other than the modified Macdonald polynomial ~Hµ[Z; q, t]. We further introduce a general,µ(q, t) = t(µ)K,µ(q, 1/t), where K,µ(q, t) is Macdonald's q, t-Kostka polynomial [Mac95, p.354]. We call

Haglund, Jim

473

ukasiewicz Logic: From Proof Systems To Logic Programming  

Science Journals Connector (OSTI)

......n, n ? n)}, a contradiction. The next step is to show that all valid atomic (and hence also irreducible) queries suc- ceed in GDL. To this end we introduce a translation from irreducible queries containing propositional variables q1, . . . , qn into......

George Metcalfe; Nicola Olivetti; Dov Gabbay

2005-09-01T23:59:59.000Z

474

National Institutes of Health Q&A Transcript  

E-Print Network [OSTI]

how different parts of the brain work! Below is a description of the brain's lobes and their primary functions, followed by 12 questions and answers. The four brain lobes and their primary functions are. It also affects brain functions such as memory and emotion. Q1. Which part of the brain enables you

Baker, Chris I.

475

BY STEVEN P. LANZA Connecticut's 7,000-job addition  

E-Print Network [OSTI]

BY STEVEN P. LANZA Connecticut's 7,000-job addition in 2012-Q1 was opportune, as the Bureau the historical relationship between U.S. GDP and Connecticut job growth, and taking into account the state economy's recent dynamics, Connecticut can expect to add jobs at a rate of about 2,900 quarterly or nearly

Holsinger, Kent

476

Solutions to the non-autonomous ABS lattice equations: Casoratians and bilinearization  

E-Print Network [OSTI]

In the paper non-autonomous H1, H2, H3$_\\delta$ and Q1$_\\delta$ equations in the ABS list are bilinearized. Their solutions are derived in Casoratian form. We also list out some Casoratian shift formulae which are used to verify Casoratian solutions.

Ying Shi; Da-jun Zhang; Song-lin Zhao

2012-01-31T23:59:59.000Z

477

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

E-Print Network [OSTI]

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

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

478

CAT: Correct Answers of Continuous Queries Using Triggers  

E-Print Network [OSTI]

down the speed between 4:30PM and 9:30PM. Tr1 enters that segment after 4:30PM, and its future portion, issued the query Q1, we have to re-evaluate the answer. Research partially supported by NSF grant EIA-000

Scheuermann, Peter

479

Machine Learning as an Objective Approach to Understanding Musical Origin  

E-Print Network [OSTI]

Machine Learning as an Objective Approach to Understanding Musical Origin Claire Q1 and Ross King2 1 Aberystwyth University, UK, ceq08@aber.ac.uk 2 Manchester University, UK, ross of pieces of music. We collected 1,142 pieces of music from 73 countries, and described them using 2

Malerba, Donato

480

BIO321-Lec10 The cell...  

E-Print Network [OSTI]

-lectins #12;Protein export/secretion is essential for life #12;Q1:How do proteins cross lipid bilayers;...composed of phopholipids in out H20 H20 Lipid #12;...that form a dynamic bilayer H2O H2O headgroups headgroups Hydrocarbon chains Lipid bilayer in out H20 H20 Lipid #12;Bird's eye view of a sea of lipids

Economou, Tassos

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481

ELEC3028 Digital Transmission Overview & Information Theory S Chen Revision of Lecture 2  

E-Print Network [OSTI]

(symbols/s) information rate: R = Rs · H (bits/s) · Code each symbol by log2 q bits (BCD), then data rate Rs · log2 q > R, unless source is equal probable pi = 1/q, 1 i q · How to code symbols is coded ­ For example, samples of speech waveform are correlated; redundancy in samples is first removed

Chen, Sheng

482

INSTITUTE OF PHYSICS PUBLISHING PLASMA PHYSICS AND CONTROLLED FUSION Plasma Phys. Control. Fusion 47 (2005) 13671377 doi:10.1088/0741-3335/47/9/001  

E-Print Network [OSTI]

. They develop in the presence of a value of the safety factor q = 1: the nested magnetic flux surfaces]. Magnetic islands either accompany sawtooth activity [4] or are in the form of persistent (`snake proved very successful in describing temperature oscillations in several situations [4,14,15], it cannot

Zonca, Fulvio

483

SC  

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

ROW * Wastesites 1221 Other Set-Asides r:;c::J Areas B Hydric Soils D Three Rivers Landfill N A o o 660 Meters * CompartQ1enLJJ o 330 o 0 o o "0 ro o a: ..c:: O CO Soil...

484

A Cross-Flow Ceramic Heat Recuperator for Industrial Heat Recovery  

E-Print Network [OSTI]

recuperators currently available suffer from problems of creep, corrosion and oxidation, particularly at high temperatures. The Department of Energy and GTE Products corporation have pursued a jointly funded venture, Contract No. EX-76-C-Q1-2162, to establish...

Gonzalez, J. M.; Cleveland, J. J.; Kohnken, K. H.; Rebello, W. J.

1980-01-01T23:59:59.000Z

485

b14.xls  

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

64,783 64,783 12,208 3,939 1,090 3,754 4,050 10,078 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 1,382 336 122 416 1,034 895 5,001 to 10,000 ................................. 6,585 938 518 Q 744 722 868 10,001 to 25,000 ............................... 11,535 1,887 1,077 Q 1,235 1,021 2,064 25,001 to 50,000 ............................... 8,668 1,506 301 Q 930 560 1,043 50,001 to 100,000 ............................. 9,057 1,209 474 Q Q Q 1,494 100,001 to 200,000 ........................... 9,064 1,428 868 Q Q Q 1,162 200,001 to 500,000 ........................... 7,176 1,493 Q Q Q Q 1,322 Over 500,000 .................................... 5,908 2,365 Q Q N Q Q Year Constructed Before 1920 ...................................... 3,769 749 323 Q 586 Q 254 1920 to 1945 .....................................

486

An inverse scheme for sensitivity and uncertainty analysis in basin modeling: the resolution limits of Easy%Ro  

E-Print Network [OSTI]

, Mona-1 , Sten-1 and Q-1 wells located in the Danish Central Trough, in the North Sea. A range of geothermal gradients are investigated using the model. As a quantitative measure of mismatch between modeled and measured values, the mean squared residual...

Huvaz, Ozkan

2012-06-07T23:59:59.000Z

487

Download Full-text PDF  

Science Journals Connector (OSTI)

tracer of terrigenous dissolved organic carbon in river-influenced ocean margins ..... values: M 5 median, Q1 5 first quartile, Q3 5 third quartile, and whiskers are set at 6 1.53 ..... Leanne Powers and the crews of the R/V Cape Hatteras and the.

2012-08-06T23:59:59.000Z

488

New Results on Nucleon Spin Structure  

E-Print Network [OSTI]

Recent precision spin structure data from Jefferson Lab have significantly advanced our knowledge of nucleon structure in the valence quark (high-$x$) region and improved our understanding of higher-twist effects, spin sum rules and quark-hadron duality. First, results of a precision measurement of the neutron spin asymmetry, $A_1^n$, in the high-$x$ region are discussed. The new data shows that $A_1^n$ becomes positive at high $x$. They provide crucial input for the global fits to world data to extract polarized parton distribution functions. The up and down quark spin distributions in the nucleon were extracted. The results for $\\Delta d/d$ disagree with the leading-order pQCD prediction assuming hadron helicity conservation. Then, results of a precision measurement of the $g_2^n$ structure function to study higher-twist effects are presented. The data show a clear deviation from the lead-twist contribution. The second moment of the spin structure functions and the twist-3 matrix element $d_2^n$ results were extracted at a high $Q2$ of 5 GeV$^2$. Results for $d_2^n$ at low-to-intermediate $Q2$ from 0.1 to 0.9 GeV$^2$ were also extracted from the JLab data. In the same $Q2$ range, the $Q2$ dependence of the moments of the nucleon spin structure functions was measured, providing a unique bridge linking the quark-gluon picture of the nucleon and the coherent hadronic picture. Sum rules and generalized forward spin polarizabilities were extracted. Finally, preliminary results were presented on the resonance spin structure functions in the $Q2$ range from 1 to 4 GeV$^2$ to study the quark-hadron duality.

Jian-ping Chen

2005-11-21T23:59:59.000Z

489

All General Counsel Reports | Department of Energy  

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

5, 2010 5, 2010 Electrolux: ENERGY STAR Referral (GAH105Q2T1) 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. October 5, 2010 Department of Energy Data Access and Privacy Issues Related To Smart Grid Technologies This report by the Department of Energy (DOE) complements DOE's companion report, Informing Federal Smart Grid Policy: The Communications Requirements of Electric Utilities. Both reports are also components of the federal government's much broader efforts to facilitate the adoption and deployment of various Smart Grid technologies. October 5, 2010 Communications Requirements of Smart Grid Technologies This report sets forth the findings of the U.S. Department of Energy (DOE)

490

Page not found | Department of Energy  

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

401 - 22410 of 28,905 results. 401 - 22410 of 28,905 results. Article New Zealand Joins International Carbon Storage Group The Carbon Sequestration Leadership Forum today announced that New Zealand has become the newest member of the international carbon storage body. http://energy.gov/fe/articles/new-zealand-joins-international-carbon-storage-group Download FOIA Quarterly Reports (Q2 2013) 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... http://energy.gov/management/downloads/foia-quarterly-reports-q2-2013 Article Bolton Community Leaders' Institute Conference The Bolton Community Leaders Institute (CLI) held a conference on February 22 and 23 at the Southeastern Community College in Whiteville, North

491

FORMERLY UTILIZED SITES REMEDIAL ACTION PROGRAM ELIMINATION REPORT  

Office of Legacy Management (LM)

fi.q 2, fi.q 2, I: * FORMERLY UTILIZED SITES REMEDIAL ACTION PROGRAM ELIMINATION REPORT FOR WESTINGHOUSE ATOMIC POWER DEVELOPMENT PLANT EAST PITTSBURGH PLANT FOREST HILLS PITTSBURGH, PENNSYLVANIA Department of Energy Office of Nuclear Energy Office of Remedial Action and Waste Technology Division of Facility and Site Decommissioning Projects INTRODUCTION BACKGROUND CONTENTS Site Function Site Description Radiological History and Status ELIMINATION ANALYSIS REFERENCES Page 1 4 iii ELIMINATION REPORT WESTINGHOUSE ATOMIC POWER DEVELOPMENT PLANT EAST PITTSBURGH PLANT FOREST HILLS PITTSBURGH, PENNSYLVANIA INTRODUCTION The Department of Energy (DOE), Office of Nuclear Energy, Office of Remedial Action and Waste Technology, Division of Facility and Site Decormnissioning Projects (and/or predecessor agencies, offices and

492

b12.pdf  

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

4,657 4,657 4,135 2,801 1,099 236 521 63 83 375 Building Floorspace (Square Feet) 1,001 to 5,000 .............................................. 2,348 2,131 1,433 548 151 216 Q Q 175 5,001 to 10,000 ............................................ 1,110 1,006 693 250 Q 104 Q Q 70 10,001 to 25,000 .......................................... 708 618 431 172 15 91 Q 14 64 25,001 to 50,000 .......................................... 257 202 129 68 Q 55 Q 19 33 50,001 to 100,000 ........................................ 145 109 69 39 Q 36 Q 11 21 100,001 to 200,000 ...................................... 59 47 29 17 Q 13 2 3 8 200,001 to 500,000 ...................................... 23 18 13 4 Q 5 Q 2 3 Over 500,000 ............................................... 7 5 5 1 Q 2 1 Q Q Principal Building Activity Education ....................................................

493

United States Government Department of Energy  

Office of Legacy Management (LM)

;;Klisv; /l/IS , [ q -2 ;;Klisv; /l/IS , [ q -2 United States Government Department of Energy memorandum I q79Ll per, i, ' ) ' " Z? DATE: - - - j , ? REPLY TO ATTN OF: EM-421 (W. A. Williams, 903-8149) SUBJECT: Elimination of the Sites from the Formerly Utilized Program TO: The File I have reviewed the attached site summaries and elimination recommendations for the following sites: l Mitts & Merrel Co., Saginaw, Michigan l North Carolina State University, Raleigh, North Carolina l National Smelt & Refining, Cleveland, Ohio l Sutton, Steele & Steele, Dallas, Texas l Norfolk Naval Station, Virginia In each case, the potential for radiological contamination above applicable guidelines is small. In each case the amounts of radioactive materials handled was small. Based on these considerations, these sites

494

Alternative Fuels Data Center: Maps and Data  

Alternative Fuels and Advanced Vehicles Data Center [Office of Energy Efficiency and Renewable Energy (EERE)]

Trends Trends All Categories Vehicles AFVs and HEVs Fuel Consumption and Efficiency Vehicle Market Driving Patterns Fuels & Infrastructure Fuel Trends Emissions Alternative Fueling Stations Idle Reduction Transportation Infrastructure Biofuels Production Laws & Incentives Regulated Fleets Federal Fleets State & Alt Fuel Providers Clean Cities Vehicles Petroleum Use Reduction Program OR Go Sort by: Category Most Recent Most Popular 9 results Generated_thumb20131212-30432-1q2ycmx Average Retail Fuel Prices in the U.S. Generated_thumb20131212-30432-1q2ycmx Trend of alternative and traditional motor fuel prices from 2000-2013 Last update December 2013 View Graph Graph Download Data Generated_thumb20130810-31804-eaiva6 Consumption of Natural Gas in the U.S. Generated_thumb20130810-31804-eaiva6

495

Radioactive contamination of BaF2 crystal scintillator  

E-Print Network [OSTI]

Barium fluoride (BaF$_2$) crystal scintillators are promising detectors to search for double beta decay processes in $^{130}$Ba ($Q_{2{\\beta}}$ = 2619(3) keV) and $^{132}$Ba ($Q_{2{\\beta}}$ = 844(1) keV). The $^{130}$Ba isotope is of particular interest because of the indications on 2${\\beta}$ decay found in two geochemical experiments. The radioactive contamination of BaF$_2$ scintillation crystal with mass of 1.714 kg was measured over 113.4 hours in a low-background DAMA/R&D set-up deep underground (3600 m w.e.) at the Gran Sasso National Laboratories of INFN (LNGS, Italy). The half-life of $^{212}$Po (present in the crystal scintillator due to contamination by radium) was estimated as $T_{1/2}$ = 298.8 $\\pm$ 0.8(stat.) $\\pm$ 1.4(syst.) ns by analysis of the events pulse profiles.

Polischuk, O G; Bernabei, R; Cappella, F; Caracciolo, V; Cerulli, R; Di Marco, A; Danevich, F A; Incicchitti, A; Poda, D V; Tretyak, V I

2013-01-01T23:59:59.000Z

496

Neutron structure effects in the deuteron and one neutron halos  

E-Print Network [OSTI]

Although the neutron (n) does not carry a total electric charge, its charge and magnetization distributions represented in momentum space by the electromagnetic form factors, $F_1^{(n)} (q^2)$ and $F_2^{(n)} (q^2)$, lead to an electromagnetic potential of the neutron. Using this fact, we calculate the electromagnetic corrections to the binding energy, $B_d$, of the deuteron and a one neutron halo nucleus (11Be), by evaluating the neutron-proton and the neutron-charged core (10Be) potential, respectively. The correction to $B_d$ (~9 keV) is comparable to that arising due to the inclusion of the $\\Delta$-isobar component in the deuteron wave function. In the case of the more loosely bound halo nucleus, 11Be, the correction is close to about 2 keV.

M. Nowakowski; N. G. Kelkar; T. Mart

2005-11-28T23:59:59.000Z

497

Neutron structure effects in the deuteron and one neutron halos  

Science Journals Connector (OSTI)

Although the neutron (n) does not carry a total electric charge, its charge and magnetization distributions represented in momentum space by the electromagnetic form factors, F1(n)(q2) and F2(n)(q2), lead to an electromagnetic potential of the neutron. Using this fact, we calculate the electromagnetic corrections to the binding energy, Bd, of the deuteron and a one-neutron halo nucleus (Be11) by evaluating the neutron-proton and the neutron-charged core (Be10) potential, respectively. The correction to Bd (?9 keV) is comparable to that arising due to the inclusion of the ?-isobar component in the deuteron wave function. In the case of the more loosely bound halo nucleus, Be11, the correction is close to about 2 keV.

M. Nowakowski; N. G. Kelkar; T. Mart

2006-08-28T23:59:59.000Z

498

The electric and magnetic form factors of the proton  

E-Print Network [OSTI]

The paper describes a precise measurement of electron scattering off the proton at momentum transfers of $0.003 \\lesssim Q^2 \\lesssim 1$\\ GeV$^2$. The average point-to-point error of the cross sections in this experiment is $\\sim$ 0.37%. These data are used for a coherent new analysis together with all world data of unpolarized and polarized electron scattering from the very smallest to the highest momentum transfers so far measured. The extracted electric and magnetic form factors provide new insight into their exact shape, deviating from the classical dipole form, and of structure on top of this gross shape. The data reaching very low $Q^2$ values are used for a new determination of the electric and magnetic radii. An empirical determination of the Two-Photon-Exchange (TPE) correction is presented. The implications of this correction on the radii and the question of a directly visible signal of the pion cloud are addressed.

A1 Collaboration; J. C. Bernauer; M. O. Distler; J. Friedrich; Th. Walcher; P. Achenbach C. Ayerbe Gayoso; R. Bhm; L. Debenjak; L. Doria; A. Esser; H. Fonvieille; M. Gmez Rodrgues de la Paz; J. M. Friedrich; M. Makek; H. Merkel; D. G. Middleton; U. Mller; L. Nungesser; J. Pochodzalla; M. Potokar; S. Snchez Majos; B. S. Schlimme; S. irca; M. Weinriefer

2014-07-29T23:59:59.000Z

499

Precise measurement of neutrino and antineutrino differential cross sections  

Science Journals Connector (OSTI)

The NuTeV experiment at Fermilab has obtained a unique high-statistics sample of neutrino and antineutrino interactions using its high-energy sign-selected beam. We present a measurement of the differential cross section for charged-current neutrino and antineutrino scattering from iron. We determine the relative ? to ? cross section, r=??/??, at high energy with errors a factor of 2 smaller than the previous world average. Structure functions, F2(x,Q2) and xF3(x,Q2), are determined by fitting the inelasticity, y, dependence of the cross sections. This measurement has significantly improved systematic precision as a consequence of more precise understanding of hadron and muon energy scales.

M. Tzanov et al.

2006-07-28T23:59:59.000Z

500

Comparative study of nuclear effects in polarized electron scattering from 3He  

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

We present a detailed analysis of nuclear effects in inclusive electron scattering from polarized 3He nuclei for polarization asymmetries, structure functions and their moments, both in the nucleon resonance and deep-inelastic regions. We compare the results of calculations within the weak binding approximation at finite Q2 with the effective polarization ansatz often used in experimental data analyses, and explore the impact of ? components in the nuclear wave function and nucleon off-shell corrections on extractions of the free neutron structure. Using the same framework we also make predictions for the Q2 dependence of quasielastic scattering from polarized 3He, data on which can be used to constrain the spin-dependent nuclear smearing functions in 3He.

Ethier, Jacob James; Melnitchouk, Wally [JLAB

2013-11-01T23:59:59.000Z