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1

Measurement of the ZZ production cross section using the full CDF II data set  

Science Journals Connector (OSTI)

We present a measurement of the ZZ-boson pair-production cross section in 1.96 TeV center-of-mass energy pp¯ collisions. We reconstruct final states incorporating four charged leptons or two charged leptons and two neutrinos from the full data set collected by the Collider Detector experiment at the Fermilab Tevatron, corresponding to 9.7??fb?1 of integrated luminosity. Combining the results obtained from each final state, we measure a cross section of 1.04?0.25+0.32??pb, in good agreement with the standard model prediction at next-to-leading order in the strong-interaction coupling.

T. Aaltonen et al. (CDF Collaboration)

2014-06-03T23:59:59.000Z

2

Measurement of the ZZ production cross section using the full CDF II data set  

E-Print Network (OSTI)

We present a measurement of the ZZ boson-pair production cross section in 1.96 TeV center-of-mass energy ppbar collisions. We reconstruct final states incorporating four charged leptons or two charged leptons and two neutrinos from the full data set collected by the Collider Detector experiment at the Fermilab Tevatron, corresponding to 9.7 fb-1 of integrated luminosity. Combining the results obtained from each final state, we measure a cross section of 1.04(+0.32)(-0.25) pb, in good agreement with the standard model prediction at next-to-leading order in the strong-interaction coupling.

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

2014-03-10T23:59:59.000Z

3

Double-differential light-ion production cross sections  

Science Journals Connector (OSTI)

......deuteron breakup production cross sections...alpha fragmentation production cross sections, with hydrogen as the target, is...neutron and proton production cross sections...semi-classical geometric methods to describe the fragmentation......

T. M. Miller; L. W. Townsend

2004-08-01T23:59:59.000Z

4

Clean Energy Manufacturing Resources - Technology Full-Scale Production |  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Full-Scale Production Full-Scale Production Clean Energy Manufacturing Resources - Technology Full-Scale Production Clean Energy Manufacturing Resources - Technology Full-Scale Production Find resources to help you design a production and manufacturing process for a new clean energy technology or product. For full-scale production, other areas to consider include workforce development; R&D funding; and regional, state, and local resources. For more resources, see the Clean Energy Manufacturing Federal Resource Guide. Design Production and Manufacturing Process Advanced Research Projects Agency: Tech-to-Market Resources - general tech-to-market (T2M) resources. DOE Advanced Manufacturing Office: Manufacturing Demonstration Facility - a collaborative manufacturing community that works to provide real data to

5

Calculation of the cross section for top quark production  

SciTech Connect

The authors summarize calculations of the cross section for top quark production at hadron colliders within the context of perturbative quantum chromodynamics, including resummation of the effects of initial-state soft gluon radiation to all orders in the strong coupling strength. In their approach they resume the universal leading-logarithm contributions, and they restrict the calculation to the region of phase space that is demonstrably perturbative. They compare the approach with other methods. They present predictions of the physical cross section as a function of the top quark mass in proton-antiproton reactions at center-of-mass energies of 1.8 and 2.0 TeV, and they discuss estimated uncertainties.

Berger, E.L.; Contopanagos, H. [Argonne National Lab., IL (United States). High Energy Physics Div.

1996-06-21T23:59:59.000Z

6

Catalyst-Assisted Production of Olefins from Natural Gas Liquids: Prototype Development and Full-Scale Testing, April 2013  

Energy.gov (U.S. Department of Energy (DOE))

Catalyst-Assisted Production of Olefins from Natural Gas Liquids: Prototype Development and Full-Scale Testing

7

Systematics of isotopic production cross sections from interactions of relativistic 40Ca in hydrogen  

Science Journals Connector (OSTI)

The isotopic production cross sections for 40Ca projectiles at 357, 565, and 763 MeV/nucleon interacting in a liquid hydrogen target have been measured by the Transport Collaboration at the LBL HISS facility. The systematics of these cross sections are studied, and the results indicate that nuclear structure effects are present in the isotope production process during the relativistic collisions. The newly measured cross sections are also compared with those predicted by semiempirical and parametric formulas, but the predictions do not fully describe the systematics such as the energy dependence. The consequences of the cross section systematics in galactic cosmic ray studies are also discussed.

C.-X. Chen; S. Albergo; Z. Caccia; S. Costa; H. J. Crawford; M. Cronqvist; J. Engelage; L. Greiner; T. G. Guzik; A. Insolia; C. N. Knott; P. J. Lindstrom; M. McMahon; J. W. Mitchell; R. Potenza; G. V. Russo; A. Soutoul; O. Testard; C. E. Tull; C. Tuvé; C. J. Waddington; W. R. Webber; J. P. Wefel

1997-09-01T23:59:59.000Z

8

Modeling requirements for full-scope reactor simulators of fission-product transport during severe accidents  

SciTech Connect

This paper describes in the needs and requirements to properly and efficiently model fission product transport on full scope reactor simulators. Current LWR simulators can be easily adapted to model severe accident phenomena and the transport of radionuclides. Once adapted these simulators can be used as a training tool during operator training exercises for training on severe accident guidelines, for training on containment venting procedures, or as training tool during site wide emergency training exercises.

Ellison, P.G.; Monson, P.R. (Westinghouse Savannah River Co., Aiken, SC (United States)); Mitchell, H.A. (Concord Associates, Inc., Knoxville, TN (United States))

1990-01-01T23:59:59.000Z

9

Modeling requirements for full-scope reactor simulators of fission-product transport during severe accidents  

SciTech Connect

This paper describes in the needs and requirements to properly and efficiently model fission product transport on full scope reactor simulators. Current LWR simulators can be easily adapted to model severe accident phenomena and the transport of radionuclides. Once adapted these simulators can be used as a training tool during operator training exercises for training on severe accident guidelines, for training on containment venting procedures, or as training tool during site wide emergency training exercises.

Ellison, P.G.; Monson, P.R. [Westinghouse Savannah River Co., Aiken, SC (United States); Mitchell, H.A. [Concord Associates, Inc., Knoxville, TN (United States)

1990-12-31T23:59:59.000Z

10

Production cross section and topological decay branching fractions of the ? lepton  

E-Print Network (OSTI)

We report new measurements of the production cross section for the reaction e(+)e(?)??(+)?(?) at s?=29 GeV, as well as the topological decay branching fractions of the ? lepton. The data were taken with the High Resolution ...

Baringer, Philip S.

1989-08-01T23:59:59.000Z

11

Draft Guidance for Section 242 of the Energy Policy Act of 2005- Hydroelectric Production Incentive Program- July 2014  

Energy.gov (U.S. Department of Energy (DOE))

This document contains draft guidance for Section 242 of the Energy Policy Act of 2005, the "Hydroelectric Production Incentive Program"

12

Production cross sections of tritium in high energy nuclear reactions with 12 GeV protons  

Science Journals Connector (OSTI)

Production cross sections of tritium in high energy nuclear reactions with 12 GeV protons were measured for Al, Co, Cu, Nb, Ag, In, Sn, Au and Pb targets. Large production cross sections of > 500 (mb) were obtained for Au and Pb targets. From their atomic weight dependence, tritium cross sections (?) in mb can be expressed as a function of target atomic weight (A) by the following simple equation: ?(A) = 95 exp(A107), which should be useful for predicting unknown cross sections. Together with other existing data at different energies, the present data suggest that there is no energy dependence of tritium cross section at proton energies above several GeV.

Masaharu Noguchi; Taichi Miura; Kenjiro Kondo; Takenori Suzuki; Yuichi Oki; Minoru Takasaki; Kazuhiro H. Tanaka; Masaharu Ieiri

1991-01-01T23:59:59.000Z

13

Systematics of cross sections for target K-vacancy production in heavy ion collisions  

E-Print Network (OSTI)

-shell vacancy production by heavy ions. .......................................................................................... 9 2. Regions of validity for various approximation schemes as a function of the projectile-to-target nuclear charge ratio, Z1.... ........................................................................... 33 8. Photograph of the experimental setup for the measurement of x-ray production cross sections ......................................................................................... 34 9. Schematic view of the experimental setup...

Peng, Yong

2007-04-25T23:59:59.000Z

14

Measurements of the W production cross sections in association with jets with the ATLAS detector  

E-Print Network (OSTI)

This paper presents cross sections for the production of a W boson in association with jets, measured in proton--proton collisions at $\\sqrt{s}=7$ TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of $4.6 fb^{-1}$, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The measurements are compared to numerous QCD predictions including next-to-leading-order perturbative calculations, resummation calculations and Monte Carlo generators.

ATLAS Collaboration

2014-09-30T23:59:59.000Z

15

Interactions of relativistic neon to nickel projectiles in hydrogen, elemental production cross sections  

Science Journals Connector (OSTI)

This paper reports the elemental production cross sections for 17 projectile-energy combinations with energies between 338 and 894 MeV/nucleon interacting in a liquid hydrogen target. These results were obtained from two runs at the LBL Bevalac using projectiles ranging from Ne22 to Ni58. Cross sections were measured for all fragment elements with charges greater than or equal to half the charge of the projectile. The results show that, over the energy and ion range investigated, the general decrease in cross section with decreasing fragment charge is strongly modified by the isospin of the projectile ion. Significant additional modifications of the cross sections due to the internal structure of the nucleus have also been seen. These include both pairing and shell effects. Differences in the cross sections due to the differing energies of the projectile are also considerable. © 1996 The American Physical Society.

C. N. Knott et al.

1996-01-01T23:59:59.000Z

16

New Statistical Techniques in the Measurement of the inclusive Top Pair Production Cross Section  

E-Print Network (OSTI)

We present several different types of multivariate statistical techniques used in the measurement of the inclusive top pair production cross section in $p \\bar{p}$-collisions at $\\sqrt{s} = 1.96 \\text{TeV}$ employing the full RunII data ($9.7\\textrm{fb}^{-1}$) collected with the D0 detector at the Fermilab Tevatron Collider. We consider the final state of the top quark pair decays containing one electron or muon and at least two jets. We proceed various statistical homogeneity tests such as Anderson - Darling, Kolmogorov - Smirnov, and $\\varphi$-divergences tests to determine, which variables have good data-MC agreement, as well as a good separation power. We adjusted all tests for using weighted empirical distribution functions. Further we separate $t\\bar{t}$ signal from the background by the application of Generalized Linear Models, Gaussian Mixture Models), Neural Networks with Switching Units and confront them with familiar methods from ROOT TMVA package such as Boosted Decision Trees, and Multi-layer Per...

Franc, Ji?í; Št?pánek, Michal; K?s, Václav

2014-01-01T23:59:59.000Z

17

tt¯ production cross section in pp¯ collisions at s=1.8 TeV  

Science Journals Connector (OSTI)

Results are presented on a measurement of the tt¯ pair production cross section in pp¯ collisions at s=1.8 TeV from nine independent decay channels. The data were collected by the DØ experiment during the 1992–1996 run of the Fermilab Tevatron Collider. A total of 80 candidate events is observed with an expected background of 38.8±3.3 events. For a top quark mass of 172.1 GeV/c2, the measured cross section is 5.69±1.21(stat)±1.04(syst) pb.

V. M. Abazov et al. ((DØ Collaboration))

2003-01-15T23:59:59.000Z

18

Assessment of Fission Product Cross-Section Data for Burnup Credit Applications  

SciTech Connect

Past efforts by the Department of Energy (DOE), the Electric Power Research Institute (EPRI), the Nuclear Regulatory Commission (NRC), and others have provided sufficient technical information to enable the NRC to issue regulatory guidance for implementation of pressurized-water reactor (PWR) burnup credit; however, consideration of only the reactivity change due to the major actinides is recommended in the guidance. Moreover, DOE, NRC, and EPRI have noted the need for additional scientific and technical data to justify expanding PWR burnup credit to include fission product (FP) nuclides and enable burnup credit implementation for boiling-water reactor (BWR) spent nuclear fuel (SNF). The criticality safety assessment needed for burnup credit applications will utilize computational analyses of packages containing SNF with FP nuclides. Over the years, significant efforts have been devoted to the nuclear data evaluation of major isotopes pertinent to reactor applications (i.e., uranium, plutonium, etc.); however, efforts to evaluate FP cross-section data in the resonance region have been less thorough relative to actinide data. In particular, resonance region cross-section measurements with corresponding R-matrix resonance analyses have not been performed for FP nuclides. Therefore, the objective of this work is to assess the status and performance of existing FP cross-section and cross-section uncertainty data in the resonance region for use in burnup credit analyses. Recommendations for new cross-section measurements and/or evaluations are made based on the data assessment. The assessment focuses on seven primary FP isotopes (103Rh, 133Cs, 143Nd, 149Sm, 151Sm, 152Sm, and 155Gd) that impact reactivity analyses of transportation packages and two FP isotopes (153Eu and 155Eu) that impact prediction of 155Gd concentrations. Much of the assessment work was completed in 2005, and the assessment focused on the latest FP cross-section evaluations available in the international nuclear data community as of March 2005. The accuracy of the cross-section data was investigated by comparing existing cross-section evaluations against available measured cross-section data. When possible, benchmark calculations were also used to assess the performance of the latest FP cross-section data. Since March 2005, the U.S. and European data projects have released newer versions of their respective data files. Although there have been updates to the international data files and to some degree FP data, much of the updates have included nuclear cross-section modeling improvements at energies above the resonance region. The one exception is improved ENDF/B-VII cross-section uncertainty data or covariance data for gadolinium isotopes. In particular, ENDF/B-VII includes improved 155Gd resonance parameter covariance data, but they are based on previously measured resonance data. Although the new covariance data are available for 155Gd, the conclusions of the FP cross-section data assessment of this report still hold in lieu of the newer international cross-section data files. Based on the FP data assessment, there is judged to be a need for new total and capture cross-section measurements and corresponding cross-section evaluations, in a prioritized manner, for the nine FPs to provide the improved information and technical rigor needed for criticality safety analyses.

Leal, Luiz C [ORNL; Derrien, Herve [ORNL; Dunn, Michael E [ORNL; Mueller, Don [ORNL

2007-12-01T23:59:59.000Z

19

Characterization of radiolytically generated degradation products in the strip section of a TRUEX flowsheet  

SciTech Connect

This report presents a summary of the work performed to meet the FCRD level 2 milestone M3FT-13IN0302053, “Identification of TRUEX Strip Degradation.” The INL radiolysis test loop has been used to identify radiolytically generated degradation products in the strip section of the TRUEX flowsheet. These data were used to evaluate impact of the formation of radiolytic degradation products in the strip section upon the efficacy of the TRUEX flowsheet for the recovery of trivalent actinides and lanthanides from acidic solution. The nominal composition of the TRUEX solvent used in this study is 0.2 M CMPO and 1.4 M TBP dissolved in n-dodecane and the nominal composition of the TRUEX strip solution is 1.5 M lactic acid and 0.050 M diethylenetriaminepentaacetic acid. Gamma irradiation of a mixture of TRUEX process solvent and stripping solution in the test loop does not adversely impact flowsheet performance as measured by stripping americium ratios. The observed increase in americium stripping distribution ratios with increasing absorbed dose indicates the radiolytic production of organic soluble degradation compounds.

Dean R. Peterman; Lonnie G. Olson; Gary S. Groenewold; Rocklan G. McDowell; Richard D. Tillotson; Jack D. Law

2013-08-01T23:59:59.000Z

20

Neutral Scalar Higgs Masses and Production Cross Sections in an Extended Supersymmetric Standard Model  

E-Print Network (OSTI)

Upper bounds on the three neutral scalar Higgs masses are considered in the supersymmetric standard model with a gauge singlet Higgs field. When the lightest Higgs is singlet-dominated the second lightest Higgs is shown to lie near or below the theoretical upper bound on the lightest Higgs mass. We also consider detectability of these Higgs bosons at a future $e^+ e^-$ linear collider with $\\sqrt{s}\\sim 300 $ GeV and show that at least one of the neutral scalar Higgs has a production cross section larger than 0.04~pb.

Jun-ichi Kamoshita; Yasuhiro Okada; Minoru Tanaka

1994-02-14T23:59:59.000Z

Note: This page contains sample records for the topic "full section production" 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

Measurement of the differential dijet production cross section in proton–proton collisions at  

SciTech Connect

A measurement of the double-differential inclusive dijet production cross section in proton-proton collisions at sqrt(s)=7 TeV is presented as a function of the dijet invariant mass and jet rapidity. The data correspond to an integrated luminosity of 36 inverse picobarns, recorded with the CMS detector at the LHC. The measurement covers the dijet mass range 0.2 TeV to 3.5 TeV and jet rapidities up to |y|=2.5. It is found to be in good agreement with next-to-leading-order QCD predictions.

Chatrchyan, Serguei; et al.

2011-06-01T23:59:59.000Z

22

Title III section 313 release reporting guidance: Estimating chemical releases from rubber production and compounding  

SciTech Connect

Facilities engaged in rubber production and compounding may be required to report annually any releases to the environment of certain chemicals regulated under Section 313, Title III, of the Superfund Amendments and Reauthorization Act (SARA) of 1986. The document has been developed to assist those who produce rubber in the completion of Part III (Chemical Specific Information) of the Toxic Chemical Release Inventory Reporting Form. Included herein is general information on toxic chemicals used and process wastes generated, along with several examples to demonstrate the types of data needed and various methodologies available for estimating releases.

Not Available

1988-03-01T23:59:59.000Z

23

Top quark pair production cross section using the ATLAS detector at the LHC  

E-Print Network (OSTI)

Measurements of the inclusive top quark pair production cross sections in proton-proton collisions with the ATLAS detector at the Large Hadron Collider are presented. The measurements are performed requiring one or two electrons or muons in the final state. Various experimental techniques are compared. The most accurate result in obtained requiring opposite sign electrons and muons, achieves a precision of a few percent, and is in good agreement with a recent NNLO+NNLL QCD calculation. In addition, a di erential measurement of the top transverse momentum and kinematic properties of the top pair system are presented. This measurement requires one electron or muon in the final state and probes our understanding of top pair production in the TeV regime and is compared to recent Monte Carlo generators and theory calculations.

Theveneaux-Pelzer, Timothee; The ATLAS collaboration

2014-01-01T23:59:59.000Z

24

Enhanced production of full-length immunoglobulin G via the signal recognition particle (SRP)-dependent pathway in Escherichia coli  

Science Journals Connector (OSTI)

Abstract Because of the lack of post-translational glycosylation, Escherichia coli is not a preferable host for immunoglobulin G (IgG) production. However, recent successes in the developments of aglycosylated IgG variants that do not require glycosylation for effector functions have increased the likelihood of using E. coli for IgG production. Here, we have developed a new E. coli host–vector system for enhanced production of recombinant IgG using: (i) a combination of SRP/Sec-dependent pathways for the efficient secretion of heavy and light chains in the periplasm; (ii) co-expression of periplasmic foldase (DsbC) for efficient assembly of IgG in the periplasm; and (iii) co-expression of Ffh for enhancing the SRP machinery. Finally, with engineered host–vector system, fed-batch cultivations were conducted at four different conditions, and under an optimized condition, up to 62 mg/L of active full-length IgG was produced during a 28-h cultivation.

Yong Jae Lee; Hee Sung Kim; Ae Jin Ryu; Ki Jun Jeong

2013-01-01T23:59:59.000Z

25

New isotope 44Si and systematics of the production cross sections of the most neutron-rich nuclei  

E-Print Network (OSTI)

The results of measurements of the production of neutron-rich nuclei by the fragmentation of a 48Ca beam at 142 MeV/u are presented. Evidence was found for the production of a new isotope that is the most neutron-rich silicon nuclide, 44Si, in a net neutron pick-up process. A simple systematic framework was found to describe the production cross sections based on thermal evaporation from excited prefragments that allows extrapolation to other weak reaction products.

O. B. Tarasov; T. Baumann; A. M. Amthor; D. Bazin; C. M. Folden III; A. Gade; T. N. Ginter; M. Hausmann; M. Matos; D. J. Morrissey; A. Nettleton; M. Portillo; A. Schiller; B. M. Sherrill; A. Stolz; M. Thoennessen

2007-05-02T23:59:59.000Z

26

Fuel Cell Technologies Office Multi-Year Research, Development, and Demonstration Plan- Section 3.1 Hydrogen Production  

Energy.gov (U.S. Department of Energy (DOE))

Hydrogen Production technical plan section of the Fuel Cell Technologies Office Multi-Year Research, Development, and Demonstration Plan; updated October 2014. This plan includes goals, objectives, technical targets, tasks, and schedules for the Office of Energy Efficiency and Renewable Energy's contribution to the DOE Hydrogen and Fuel Cells Program.

27

ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data  

E-Print Network (OSTI)

testing of the ENDF/B-VII.1 library is provided for a variety of quantities: For nuclear criticalityENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Jozef Stefan Institute, Jamova 39, 1000 Ljubljana, Slovenia 11 Nuclear Research and Consultancy Group, P

Danon, Yaron

28

Measurement of differential production cross section for $Z/?^*$ bosons in association with jets in $p\\bar{p}$ collisions at $\\sqrt{s}=1.96$ TeV  

E-Print Network (OSTI)

Differential cross sections for the production of $Z$ bosons or off-shell photons $\\gamma^*$ in association with jets are measured in proton-antiproton collisions at center-of-mass energy $\\sqrt{s}=1.96$ TeV using the full data set collected with the Collider Detector at Fermilab in Tevatron Run II, and corresponding to 9.6 fb$^{-1}$ of integrated luminosity. Results include first measurements at CDF of differential cross sections in events with a $Z/\\gamma^*$ boson and three or more jets, the inclusive cross section for production of $Z/\\gamma^*$ and four or more jets, and cross sections as functions of various angular observables in lower jet-multiplicity final states. Measured cross sections are compared to several theoretical predictions.

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

2014-09-15T23:59:59.000Z

29

Top physics: measurement of the cross section for ttbar production in ppbar collisions using the kinematics of lepton + jets events  

SciTech Connect

We present a measurement of the top pair production cross section in p{bar p} collisions at {radical}s = 1.96 TeV. We collect a data sample with an integrated luminosity of 194 {+-} 11 pb{sup -1} with the CDF II detector at the Fermilab Tevatron. We use an artificial neural network technique to discriminate between top pair production and background processes in a sample of 519 lepton+jets events, which have one isolated energetic charged lepton, large missing transverse energy and at least three energetic jets. We measure the top pair production cross section to be {sigma}{sub t{bar t}} = 6.6 {+-} 1.1 {+-} 1.5 pb, where the first uncertainty is statistical and the second is systematic.

Acosta, D.; The CDF Collaboration

2005-04-27T23:59:59.000Z

30

Process Optimization for Solid Extraction, Flavor Improvement and Fat Removal in the Production of Soymilk From Full Fat Soy Flakes  

SciTech Connect

Traditionally soymilk has been made with whole soybeans; however, there are other alternative raw ingredients for making soymilk, such as soy flour or full-fat soy flakes. US markets prefer soymilk with little or no beany flavor. modifying the process or using lipoxygenase-free soybeans can be used to achieve this. Unlike the dairy industry, fat reduction in soymilk has been done through formula modification instead of by conventional fat removal (skimming). This project reports the process optimization for solids and protein extraction, flavor improvement and fat removal in the production of 5, 8 and 12 {sup o}Brix soymilk from full fat soy flakes and whole soybeans using the Takai soymilk machine. Proximate analyses, and color measurement were conducted in 5, 8 and 12 {sup o}Brix soymilk. Descriptive analyses with trained panelists (n = 9) were conducted using 8 and 12 {sup o}Brix lipoxygenase-free and high protein blend soy flake soymilks. Rehydration of soy flakes is necessary to prevent agglomeration during processing and increase extractability. As the rehydration temperature increases from 15 to 50 to 85 C, the hexanal concentration was reduced. Enzyme inactivation in soy flakes milk production (measured by hexanal levels) is similar to previous reports with whole soybeans milk production; however, shorter rehydration times can be achieved with soy flakes (5 to 10 minutes) compared to whole beans (8 to 12 hours). Optimum rehydration conditions for a 5, 8 and 12 {sup o}Brix soymilk are 50 C for 5 minutes, 85 C for 5 minutes and 85 C for 10 minutes, respectively. In the flavor improvement study of soymilk, the hexanal date showed differences between undeodorized HPSF in contrast to triple null soymilk and no differences between deodorized HPSF in contrast to deodorized triple null. The panelists could not differentiate between the beany, cereal, and painty flavors. However, the panelists responded that the overall aroma of deodorized 8 {sup o}Brix triple null and HPSF soymilk are lower than the undeodorized triple null and HPSF soymilk. The triple null soymilk was perceived to be more bitter than the HPSF soymilk by the sensory panel due to oxidation on the triple null soy flakes. This oxidation may produce other aroma that was not analyzed using the GC but noticed by the panelists. The sensory evaluation results did show that the deodorizer was able to reduce the soymilk aroma in HPSF soymilk so it would be similar to triple null soymilk at 8 {sup o}Brix level. Regardless of skimming method and solids levels, the fat from the whole soybean milk was removed less efficiently than soy flake milk (7 to 30% fat extraction in contrast to 50 to 80% fat extraction respectively). In soy flake milk, less fat was removed as the % solid increases regardless of the processing method. In whole soybean milk, the fat was removed less efficiently at lower solids level milk using the commercial dairy skimmer and more efficient at lower solids level using the centrifuge-decant method. Based on the Hunter L, a, b measurement, the color of the reduced fat soy flake milk yielded a darker, greener and less yellow colored milk than whole soymilk ({alpha} < 0.05), whereas no differences were noticed in reduced fat soybean milk ({alpha} < 0.05). Color comparison of whole and skim cow's milk showed the same the same trend as in the soymilk.

Stanley Prawiradjaja

2003-05-31T23:59:59.000Z

31

Measurement of differential cross sections for the production of a pair of isolated photons in pp collisions at \\(\\sqrt{s}=7\\,\\text {TeV} \\)  

Science Journals Connector (OSTI)

A measurement of differential cross sections for the production of a pair of isolated photons in proton–proton collisions at $$\\sqrt{s...

S. Chatrchyan; V. Khachatryan; A. M. Sirunyan…

2014-11-01T23:59:59.000Z

32

Cross sections and energy loss for lepton pair production in muon transport  

E-Print Network (OSTI)

We reevaluate electron-positron pair production from electromagnetic interactions of muons in transit through materials. Our approach, through the use of structure functions for inelastic and elastic scattering and including hadronic recoil, make the formalism useful for tau pair production at high energies. Our results for electron-positron pair production agree well with prior evaluations. Tau pair production, has a significant contribution from inelastic scattering in addition to the usual coherent scattering with the nucleus and scattering with atomic electrons.

A. Bulmahn; M. H. Reno

2008-12-30T23:59:59.000Z

33

Measurement of the $WW+WZ$ Production Cross Section Using a Matrix Element Technique in Lepton + Jets Events  

SciTech Connect

We present a measurement of the WW + WZ production cross section observed in a final state consisting of an identified electron or muon, two jets, and missing transverse energy. The measurement is carried out in a data sample corresponding to up to 4.6 fb{sup -1} of integrated luminosity at {radical}s = 1.96 TeV collected by the CDF II detector. Matrix element calculations are used to separate the diboson signal from the large backgrounds. The WW + WZ cross section is measured to be 17.4 {+-} 3.3 pb, in agreement with standard model predictions. A fit to the dijet invariant mass spectrum yields a compatible cross section measurement.

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

2010-08-01T23:59:59.000Z

34

Measurement of the ZZ production cross section in p p? collisions at ?s=1.96 TeV  

The authors present a new measurement of the production cross section ?(pp? = ZZ) at a center-of-mass energy ?s = 1.96 TeV, obtained from the analysis of the four charged lepton final state ?+?-?`+?`- (?, ?` = e or ?). They observe ten candidate events with an expected background of 0.37 ± 0.13 events. The measured cross section ?(pp? =ZZ) = 1.26-0.37+0.47 (stat) ± 0.14 (syst) pb is in agreement with NLO QCD predictions. This result is combined with a previous result from the ZZ = ?+?- ??? channel resulting in a combined cross section of ?(pp? = ZZ) = 1.40-0.37+0.43 (stat) ±0.14 (syst) pb.

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

2011-07-06T23:59:59.000Z

35

Measurement of the ZZ production cross section in p p? collisions at ?s=1.96 TeV  

SciTech Connect

The authors present a new measurement of the production cross section ?(pp? = ZZ) at a center-of-mass energy ?s = 1.96 TeV, obtained from the analysis of the four charged lepton final state ?+?-?`+?`- (?, ?` = e or ?). They observe ten candidate events with an expected background of 0.37 ± 0.13 events. The measured cross section ?(pp? =ZZ) = 1.26-0.37+0.47 (stat) ± 0.14 (syst) pb is in agreement with NLO QCD predictions. This result is combined with a previous result from the ZZ = ?+?- ??? channel resulting in a combined cross section of ?(pp? = ZZ) = 1.40-0.37+0.43 (stat) ±0.14 (syst) pb.

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

2011-07-06T23:59:59.000Z

36

Improved measurement of the bb¯ production cross section in 920 GeV fixed-target proton-nucleus collisions  

Science Journals Connector (OSTI)

A new measurement of the bb¯ production cross section in 920 GeV proton-nucleus collisions is presented by the HERA-B Collaboration. The bb¯ production is tagged via inclusive bottom quark decays into J/? mesons by exploiting the longitudinal separation of J/??l+l- decay vertices from the primary proton-nucleus interaction point. Both e+e- and ?+?- channels are reconstructed for a total of 83±12 inclusive b?J/?X events found. The combined analysis yields a bb¯ to prompt J/? cross section ratio of ??(bb¯)??J/?=0.032±0.005stat±0.004sys measured in the xF acceptance (-0.35

I. Abt et al. (HERA-B Collaboration)

2006-03-10T23:59:59.000Z

37

Energy Dependence of Cross Sections near Threshold: One Neutral and Two Charged Reaction Products  

Science Journals Connector (OSTI)

The energy dependence near threshold of cross sections for reactions leading to the escape of one neutral and two charged particles is determined. The method is an extension of one developed previously for uncharged particles, and utilizes only general properties of solutions of the time-independent three-particle Schrödinger equation valid outside a reaction zone of finite extent. Electron detachment from H- by charged particle bombardment, and nuclear reactions of the type (n, np) are considered as examples.

Robert W. Hart; Ernest P. Gray; William H. Guier

1957-12-15T23:59:59.000Z

38

CROSS SECTION MEASUREMENTS IN THE MAIN INJECTOR PARTICLE PRODUCTION (FNAL-E907) EXPERIMENT AT 58 GEV ENERGY  

SciTech Connect

Cross-sections are presented for 58 GeV {pi}, K, and p on a wide range of nuclear targets. These cross-sections are essential for determining the neutrino flux in measurements of neutrino cross-sections and oscillations. The E907 Main Injector Particle Production (MIPP) experiment at Fermilab is a fixed target experiment for measuring hadronic particle production using primary 120 GeV/c protons and secondary {pi}, K, and p beams. The particle identification is made by dE/dx in a time projection chamber, and by time-of-flight, differential Cherenkov and ring imaging Cherenkov detectors, which together cover a wide range of momentum from 0.1 GeV/c up to 120 GeV/c. MIPP targets span the periodic table, from hydrogen to uranium, including beryllium and carbon. The MIPP has collected {approx} 0.26 x 10{sup 6} events of 58 GeV/c secondary particles produced by protons from the main injector striking a carbon target.

Gunaydin, Yusuf Oguzhan; /Iowa U.

2009-12-01T23:59:59.000Z

39

Section I  

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

Projectile and Target Z-scaling of Target K-vacancy Production Cross Sections at 10A MeV R. L. Watson, V. Horvat and K. E. Zaharakis Molecular Orbital Effects in Near-symmetric...

40

Calculating vibrational spectra with sum of product basis functions without storing full-dimensional vectors or matrices  

E-Print Network (OSTI)

We propose an iterative method for computing vibrational spectra that significantly reduces the memory cost of calculations. It uses a direct product primitive basis, but does not require storing vectors with as many components as there are product basis functions. Wavefunctions are represented in a basis each of whose functions is a sum of products (SOP) and the factorizable structure of the Hamiltonian is exploited. If the factors of the SOP basis functions are properly chosen, wavefunctions are linear combinations of a small number of SOP basis functions. The SOP basis functions are generated using a shifted block power method. The factors are refined with a rank reduction algorithm to cap the number of terms in a SOP basis function. The ideas are tested on a 20-D model Hamiltonian and a realistic CH$_3$CN (12 dimensional) potential. For the 20-D problem, to use a standard direct product iterative approach one would need to store vectors with about $10^{20}$ components and would hence require about $8 \\times 10^{11}$ GB. With the approach of this paper only 1 GB of memory is necessary. Results for CH$_3$CN agree well with those of a previous calculation on the same potential.

Arnaud Leclerc; Tucker Carrington

2014-05-12T23:59:59.000Z

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to obtain the most current and comprehensive results.


41

1989 annual book of ASTM standards. Section 5: Petroleum products, lubricants and fossil fuels  

SciTech Connect

This volume of standards pertains to petroleum products and lubricants and to catalysts. The standards presented include: Standard test method for estimation of net and gross heat of combustion of petroleum fuels; Standard guide for generation and dissipation of static electricity in petroleum fuel systems; and Standard test method for solidification point of petroleum wax.

Not Available

1989-01-01T23:59:59.000Z

42

Cross sections for production of closed superstrings at high energy colliders in brane world models  

E-Print Network (OSTI)

In brane world string models with large extra dimensions, there are processes where fermion and antifermion (or two gluons) can annihilate producing a light particle (e.g. gluon) carrying transverse momentum and a Kaluza-Klein graviton or an excited closed string that propagates in the extra dimensions. In high energy colliders, this process gives a missing momentum signature. We compute the total cross section for this process within the context of type II superstring theory in the presence of a D brane. This includes all missing energy sources for this string theory model up to s=8M_s^2, and it can be used to put new limits on the string scale M_s.

Diego Chialva; Roberto Iengo; Jorge G. Russo

2005-05-24T23:59:59.000Z

43

Measurement of the (n, H3) Cross Section in Nitrogen and Its Relationship to the Tritium Production in the Atmosphere  

Science Journals Connector (OSTI)

Nitrogen gas is irradiated by fast neutrons from a U235 fission plate and tritium is produced. The tritium is identified and counted by two different methods: (1) The gas is put into a cloud chamber where the H3 electrons are identified by their range and counted; (2) hydrogen is separated from nitrogen by its passage through palladium and is then counted in a Geiger counter. The average cross section for fission neutrons with energy sufficient to make the reaction proceed [4.4 Mev is (11±2)×10-27 cm2].This cross section combined with cosmic-ray neutron data gives an H3 production rate of between 0.10/cm2 sec and 0.20/cm2 sec averaged over the earth. Cosmic-ray stars eject H3 at a rate estimated between 0.30/cm2 sec and 0.70/cm2 sec. These two processes maintain a world reservoir of 50 to 110 million curies of H3. This H3 production leads to a mean escape time of He3 from the atmosphere of about 5 million years. This is consistent with a temperature at the base of the exosphere of 1500°K.

E. L. Fireman

1953-08-15T23:59:59.000Z

44

Measurements of fiducial and differential cross sections for Higgs boson production in the diphoton decay channel at ?s = 8 TeV with ATLAS  

E-Print Network (OSTI)

Measurements of fiducial and differential cross sections are presented for Higgs boson production in proton-proton collisions at a centre-of-mass energy of ?s = 8 TeV. The analysis is performed in the H ? ?? decay channel ...

Taylor, Frank E.

45

Measurement of K(+) production cross section by 8 GeV protons using high-energy neutrino interactions in the SciBooNE detector  

E-Print Network (OSTI)

The SciBooNE Collaboration reports K[superscript +] production cross section and rate measurements using high-energy daughter muon neutrino scattering data off the SciBar polystyrene (C[subscript 8]H[subscript 8]) target ...

Bugel, Leonard G.

46

Measurement of the t[bar over t] production cross section in pp collisions at ?s = 8 TeV in dilepton final states containing one ? lepton  

E-Print Network (OSTI)

The top-quark pair production cross section is measured in final states with one electron or muon and one hadronically decaying ? lepton from the process t[bar over t] ? (??[subscript ?])(??[subscript ?])b[bar over b], ...

Zhukova, Victoria

47

Biofiltration of asphalt emissions: Full-scale operation treating off-gases from polymer-modified asphalt production  

SciTech Connect

In response to complaints from nearby residents, a biofilter was designed, installed, and tested for treating odors in one of three odorous emission streams from an asphalt plant producing polymer-modified asphalt. Hydrogen sulfide (H{sub 2}S) was determined to be the most prevalent gaseous reduced sulfur compound and was detected in the emission stream only when polymer material was being added to raw asphalt. Emission stream H{sub 2}S concentrations were quite variable, ranging from 16 to approximately 30,000 ppm (v/v) and considered the likely compound contributing most to the plant's odor complaints. The biofilter was effective in controlling odor from the production process and removed an overall average of 65% of the H{sub 2}S during polymer addition, and for H{sub 2}S concentrations less than 400 ppmv, removal averaged 98%. These removal efficiencies reflect data from the biofilter operating at 2.5-minute empty bed residence time in 1996 and a 6.1-minute empty bed residence time in 1997. The biofilter's bed became increasingly acidified during the plant's 1997 operating season producing a pH gradient through the bed ranging from a high of 6.6 to a low of 3.1. The bed medium moisture content remained constant at about 60% (wet weight basis), but changes were observed in the water potential: no correlation to performance was determined. Changes in the microbial community reflected the bed acidification trend, with acidophiles becoming generally more numerous in the bed's deeper portions and in the mid to late season when the bed was most acidified. Bed acidification did not impact the biofilter's H{sub 2}S removal efficiency.

Cook, L.L.; Gostomski, P.A.; Apel, W.A.

1999-09-30T23:59:59.000Z

48

Biofiltration of Asphalt Emissions: Full-scale Operation Treating Off-gases from Polymer-modified Asphalt Production  

SciTech Connect

In response to complaints from nearby residents, a biofilter was designed, installed, and tested for treating odors in one of three odorous emission streams from an asphalt plant producing polymer-modified asphalt. Hydrogen sulfide (H2S) was determined to be the most prevalent gaseous reduced sulfur compound and was detected in the emission stream only when polymer material was being added to raw asphalt. Emission stream H2S concentrations we requite variable, ranging from 16 to approximately 30,000 ppm (v/v) and considered the likely compound contributing most to the plant's odor complaints. The biofilter was effective in controlling odor from the production process and removed an overall average of 65% of the H2S during polymer addition, and for H2S concentrations less than 400 ppmv, re m oval averaged 98%. These removal efficiencies reflect data from the biofilter operating at 2.5-minute empty bed residence time in 1996 and a 6.1-minute empty bed residence time in 1997. The biofilter's bed became increasingly acidified during the plant's 1997 operating season producing a pH gradient through the bed ranging from a high of 6.6 to a low of 3.1. The bed medium moisture content remained constant at about 60% (wet weight basis), but changes were observed in the water potential: no correlation to performance was determined. Changes in the microbial community reflected the bed acidification trend, with acidophiles becoming gene rally more numerous in the bed's deeper portions and in the mid to late season when the bed was most acidified. Bed acidification did not impact the biofilter's H2S removal efficiency. Nearby residents we resurveyed and roughly half of the respondents indicated that the odor conditions had improved, one-third felt odor conditions were unchanged and the remaining 15% felt odor conditions were worse despite the fact that only one of three of the plant's odorous emission streams were treated by the biofilter. Plans are to implement biofiltration for odor control at all of the facility's emission points.

Cook, Lawrence Leslie; Apel, William Arnold; Gostomski, P. A.

2004-04-01T23:59:59.000Z

49

FULL-COST ACCOUNTING  

Science Journals Connector (OSTI)

FULL-COST ACCOUNTING ... Environmental costs would be built into a product's cost, and consumers would be able to make informed purchases. ...

1993-01-11T23:59:59.000Z

50

Measurement of ?? and ?¯? induced neutral current single ?0 production cross sections on mineral oil at E??O (1 GeV)  

Science Journals Connector (OSTI)

MiniBooNE reports the first absolute cross sections for neutral current single ?0 production on CH2 induced by neutrino and antineutrino interactions measured from the largest sets of NC ?0 events collected to date. The principal result consists of differential cross sections measured as functions of ?0 momentum and ?0 angle averaged over the neutrino flux at MiniBooNE. We find total cross sections of (4.76±0.05stat±0.76sys)×10-40??cm2/nucleon at a mean energy of ?E??=808??MeV and (1.48±0.05stat±0.23sys)×10-40??cm2/nucleon at a mean energy of ?E??=664??MeV for ?? and ?¯? induced production, respectively. In addition, we have included measurements of the neutrino and antineutrino total cross sections for incoherent exclusive NC 1?0 production corrected for the effects of final state interactions to compare to prior results.

A. A. Aguilar-Arevalo et al. (The MiniBooNE Collaboration)

2010-01-26T23:59:59.000Z

51

Proton production cross sections for reactions by 300- and 392-MeV protons on carbon, aluminum, and niobium  

SciTech Connect

Proton productions from proton induced reactions have been investigated for target nuclei of {sup 12}C, {sup 27}Al, and {sup 93}Nb at 300 and 392 MeV. Proton inelastic continua over a broad energy range were measured at laboratory angles from 20 deg. to 105 deg. The differential cross sections were compared with two theoretical models, the quantum molecular dynamics (QMD) and the intranuclear cascade (INC) model in terms of the multistep direct process. We demonstrated that consistencies of these models can be improved using a realistic ground state of target nucleus, and that the INC model developed presently has a fairly good consistency and a higher predictive ability than the QMD.

Kin, Tadahiro; Saiho, Fuminobu; Hohara, Shinya; Ikeda, Katsuhiko; Ichikawa, Kiyohisa; Yamashita, Yusuke; Imamura, Minoru; Wakabayashi, Genichiro; Ikeda, Nobuo; Uozumi, Yusuke; Matabo, Masaru; Nakano, Masahiro; Koori, Norihiko [Department of Applied Quantum Physics and Nuclear Engineering, Kyushu University, Fukuoka 812-8581 (Japan); University of Occupational and Environmental Health, Kita-kyushu 807-8555 (Japan); Faculty of integrated Arts and Sciences, University of Tokushima, Tokushima 770-8502 (Japan)

2005-07-01T23:59:59.000Z

52

Pion Production Cross-section Measurements in p+C Collisions at the CERN SPS for Understanding Extensive Air Showers  

E-Print Network (OSTI)

An important approach to studying high-energy cosmic rays is the investigation of the properties of extensive air showers; however, the lateral distribution of particles in simulations of such showers strongly depends on the applied model of low-energy hadronic interactions. It has been shown that many constraints to be applied to these models can be obtained by studying identified-particle spectra from accelerator collisions, in the energy range of the CERN Super Proton Synchrotron. Here we present measurements of the pion production cross-section obtained by the NA61/SHINE experiment at the SPS, in proton-carbon collisions at the beam energy of 31 GeV from the year 2007. Further analyses of identified-particle yields in SHINE, in particular with a pion beam, are in preparation.

Marek Szuba; for the NA61/SHINE Collaboration

2010-09-16T23:59:59.000Z

53

First Measurements of the Differential Cross Sections of Higgs Boson Production and Decay in the Four Lepton Final State  

E-Print Network (OSTI)

The discovery of a new scalar particle in the search for the Higgs boson at the Large Hadron Collider (LHC) was a great success for the ATLAS and CMS collaborations. Additional measurements of this new particle present opportunities to both test the Standard Model (SM) predictions for the Higgs boson and to search for non-SM properties of this new particle. This thesis presents measurements of the mass, signal strength, and production cross sections of the Higgs boson in the $H \\rightarrow ZZ^{(*)} \\rightarrow \\ell\\ell\\ell'\\ell' $($\\ell,\\ell'=e,\\mu$) decay channel. The cross section measurements are performed using 20.3 fb$^{-1}$ of $pp$ collisions at center of mass energy $\\sqrt{s}=8$ TeV collected by the ATLAS detector and the mass and signal strength measurements are performed using an additional 4.5 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s}=7$ TeV. From the data in the $H \\rightarrow4\\ell$ channel, the best estimate of the mass is $124.51~\\pm~0.52~\\rm{(stat)}~\\pm 0.06~\\rm{(syst)}$ GeV. The signal str...

Stahlman, Jonathan Mark

54

A measurement of the top pair production cross-section in the dilepton channel using lepton plus track selection  

SciTech Connect

Using 1.1 fb{sup -1} of data collected by the Collider Detector at Fermilab (CDF) from Run II of the Fermilab Tevatron, they measure the t{bar t} production cross section in events with two leptons, significant missing transverse energy, and {ge} 2 jets. As the Run II dataset grows, more stringent tests of Standard Model predictions for the top quark sector are becoming possible. The dilepton channel, where both top quarks decay t {yields} Wb {yields} {ell}{nu}b, is of particular interest due to its high purity even in the absence of a b jet 'tagging' requirement. Use of an isolated track as the second lepton significant increases the dilepton acceptance, at the price of some increase in background, particular from W + jets events where one of the jets is identified as a lepton. With the amount of data available, it has been possible to improve the estimate of the contribution from that background, reflected in a reduced systematic uncertainty. Assuming a branching ratio of BR(W {yields} {ell}{nu}) = 10.8% and a top mass of m{sub t} = 175 GeV/c{sup 2}, the measured cross-section is {sigma}(p{bar p} {yields} t{bar t}) = 8.3 {+-} 1.3(stat.) {+-} 0.7(syst.) {+-} 0.5(lumi.) pb. The result is consistent with the Standard Model prediction of 6.7{sub -0.9}{sup +0.7} pb and represents a significant improvement in precision over previous results using this selection.

Mills, Corrinne Elaine; /UC, Santa Barbara

2007-06-01T23:59:59.000Z

55

New measurement of cross section of evaporation residues from $^{\\textrm{nat}}$Pr+$^{12}$C reaction: A comparative study on the production of $^{149}$Tb  

E-Print Network (OSTI)

Production cross sections of evaporation residues, $^{149}$Tb, $^{150}$Tb, $^{151}$Tb and $^{149}$Gd, have been measured using the stacked foil technique followed by off-line $\\gamma$-spectrometry in $^{12}$C induced reactions on naturally abundant mononuclidic praseodymium target in the 44-79 MeV incident energy range. Measured data have been interpreted comparing with previous measurements and theoretical prediction of nuclear reaction model code \\textsc{PACE4}. About 5% and 14% of the theoretical cross sections have been measured for $^{149}$Tb and $^{150}$Tb, respectively. The new cross sections of $^{149}$Tb complement those measured earlier by $\\alpha$-spectrometry. Cross sections of $^{151}$Tb are comparable to the theory. Cumulative cross section of $^{149}$Gd sheds light on the nuclear reaction mechanism. In addition, a discussion has been made to show the feasibility of producing $^{149}$Tb in $p$- and $\\alpha$-induced reactions on gadolinium isotopes.

Moumita Maiti

2011-09-29T23:59:59.000Z

56

Development of an integrated fission product release and transport code for spatially resolved full-core calculations of V/HTRs  

Science Journals Connector (OSTI)

Abstract The computer codes FRESCO-I, FRESCO-II, PANAMA and SPATRA developed at Forschungszentrum Jülich in Germany in the early 1980s are essential tools to predict the fission product release from spherical fuel elements and the TRISO fuel performance, respectively, under given normal or accidental conditions. These codes are able to calculate a conservative estimation of the source term, i.e. quantity and duration of radionuclide release. Recently, these codes have been reversed engineered, modernized (FORTRAN 95/2003) and combined to form a consistent code named STACY (Source Term Analysis Code System). STACY will later become a module of the V/HTR Code Package (HCP). In addition, further improvements have been implemented to enable more detailed calculations. For example the distinct temperature profile along the pebble radius is now taken into account and coated particle failure rates can be calculated under normal operating conditions. In addition, the absolute fission product release of an V/HTR pebble bed core can be calculated by using the newly developed burnup code Topological Nuclide Transformation (TNT) replacing the former rudimentary approach. As a new functionality, spatially resolved fission product release calculations for normal operating conditions as well as accident conditions can be performed. In case of a full-core calculation, a large number of individual pebbles which follow a random path through the reactor core can be simulated. The history of the individual pebble is recorded, too. Main input data such as spatially resolved neutron fluxes and fluid dynamics data are provided by the VSOP code. Capabilities of the FRESCO-I and SPATRA code which allow for the simulation of the redistribution of fission products within the primary circuit and the deposition of fission products on graphitic and metallic surfaces are also available in STACY. In this paper, details of the STACY model and first results for its application to the 200 MW(th) HTR-Module are presented.

Andre Xhonneux; Hans-Josef Allelein

2014-01-01T23:59:59.000Z

57

TOTAL Full-TOTAL Full-  

E-Print Network (OSTI)

Conducting - Orchestral 6 . . 6 5 1 . 6 5 . . 5 Conducting - Wind Ensemble 3 . . 3 2 . . 2 . 1 . 1 Early- X TOTAL Full- Part- X TOTAL Alternative Energy 6 . . 6 11 . . 11 13 2 . 15 Biomedical Engineering 52 English 71 . 4 75 70 . 4 74 72 . 3 75 Geosciences 9 . 1 10 15 . . 15 19 . . 19 History 37 1 2 40 28 3 3 34

Portman, Douglas

58

Measurement of the tt-bar production cross section in pp-bar collisions at s?=1.96??TeV using secondary vertex b tagging  

E-Print Network (OSTI)

We report a new measurement of the tt-bar production cross section in pp-bar collisions at a center-of-mass energy of 1.96 TeV using events with one charged lepton (electron or muon), missing transverse energy, and jets. ...

Baringer, Philip S.; Bean, Alice; Coppage, Don; Gardner, J.; Moulik, Tania; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Abolins, M.; Acharya, B. S.; Adams, M.

2006-12-26T23:59:59.000Z

59

Measurement of the production cross-section of ?(2S) ? [J over ?](??[superscript +] ?[superscript ?]) ?[superscript +] ? [superscript ?] in pp collisions at ?s = 7 TeV at ATLAS  

E-Print Network (OSTI)

The prompt and non-prompt production cross-sections for ?(2S) mesons are measured using 2.1 fb[superscript ?1] of pp collision data at a centre-of-mass energy of 7 TeV recorded by the ATLAS experiment at the LHC. The ...

Taylor, Frank E.

60

Measurement of the t[line over t] production cross section in the dilepton channel in pp collisions at ?s = 8 TeV  

E-Print Network (OSTI)

The top-antitop quark (t[¯ over t]) production cross section is measured in proton-proton collisions at ?s = 8 TeV with the CMS experiment at the LHC, using a data sample corresponding to an integrated luminosity of 5.3 ...

Apyan, Aram

Note: This page contains sample records for the topic "full section production" from the National Library of EnergyBeta (NLEBeta).
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61

Measurement of inclusive differential cross sections for Upsilon(1S) production in p(p)over-bar collisions at root s=1.96 TeV  

E-Print Network (OSTI)

We present measurements of the inclusive production cross sections of the Upsilon(1S) bottomonium state in p (p) over bar collisions at root s=1.96 TeV. Using the Upsilon(1S)->mu(+)mu(-) decay mode for a data sample of 159 ...

Baringer, Philip S.; Bean, Alice; Christofek, L.; Coppage, Don; Gardner, J.; Hensel, Carsten; Jabeen, S.; Wilson, Graham Wallace

2005-06-01T23:59:59.000Z

62

Fiducial and differential cross sections of Higgs boson production measured in the four-lepton decay channel in pp collisions at ?s = 8 TeV with the ATLAS detector  

E-Print Network (OSTI)

Measurements of fiducial and differential cross sections of Higgs boson production in the H?ZZ*?4? decay channel are presented. The cross sections are determined within a fiducial phase space and corrected for detection ...

Taylor, Frank E.

63

Measurement of ??-induced charged-current neutral pion production cross sections on mineral oil at E??0.5–2.0??GeV  

Science Journals Connector (OSTI)

Using a custom 3-?erenkov ring fitter, we report cross sections for ??-induced charged-current single ?0 production on mineral oil (CH2) from a sample of 5810 candidate events with 57% signal purity over an energy range of 0.5–2.0 GeV. This includes measurements of the absolute total cross section as a function of neutrino energy, and flux-averaged differential cross sections measured in terms of Q2, ?- kinematics, and ?0 kinematics. The sample yields a flux-averaged total cross section of (9.2±0.3stat±1.5syst)×10-39??cm2/CH2 at mean neutrino energy of 0.965 GeV.

A. A. Aguilar-Arevalo et al. (MiniBooNE Collaboration)

2011-03-23T23:59:59.000Z

64

Neutron-induced gamma-ray production cross sections for the first excited-state transitions in Ne-20 and Ne-22  

E-Print Network (OSTI)

Background: Neutron-induced reactions are a significant concern for experiments that require extremely low levels of radioactive backgrounds. Measurements of gamma-ray production cross sections over a wide energy range will help to predict and identify neutron backgrounds in these experiments. Purpose: Determine partial gamma-ray production cross sections for neutron-induced reactions in natural neon. Methods: The broad-spectrum neutron beam at the Los Alamos Neutron Science Center (LANSCE) was used for the measurement. Gamma rays from neutron-induced reactions were detected using the GErmanium Array for Neutron Induced Excitations (GEANIE). Results: Partial gamma-ray cross sections were measured for the first excited-state transitions in Ne-20 and Ne-22. The measured cross sections were compared to the TALYS and CoH3 nuclear reaction codes. Conclusions: These are the first experimental data for (n,n') reactions in neon. In addition to providing data to aid in the prediction and identification of neutron backgrounds in low-background experiments, these new measurements will help refine cross-section predictions in a mass region where models are not well constrained.

S. MacMullin; M. Boswell; M. Devlin; S. R. Elliott; N. Fotiades; V. E. Guiseppe; R. Henning; T. Kawano; B. H. LaRoque; R. O. Nelson; J. M. O'Donnell

2012-10-03T23:59:59.000Z

65

Measurement of the t anti-t production cross-section at s**(1/2) = 1.96-TeV using lifetime tagging  

SciTech Connect

A measurement of the t{bar t} production cross section in the lepton+jets channels with the D0 detector at {radical}s = 1.96 TeV using the lifetime-tagging techniques is presented. The t{bar t} cross section is estimated from the combination of the e+jets and {mu}+jets channels. The obtained result {sigma}{sub t{bar t}} = 7.47{sub -1.14}{sup +1.22}(stat){sub -1.03}{sup +1.65}(syst) {+-} 0.49(lumi) pb is consistent with the Standard Model expectation.

Khanov, Alexander; /Rochester U.; ,

2004-07-01T23:59:59.000Z

66

Longitudinal double-spin asymmetry and cross section for inclusivejet production in polarized proton collisions at sqrt(s) = 200 GeV  

SciTech Connect

We report a measurement of the longitudinal double-spinasymmetry A_LL and the differential cross section for inclusivemidrapidity jet production in polarized proton collisions at sqrt(s)=200GeV. The cross section data cover transverse momenta 5

Abelev, B.I.; Adams, J.; Aggarwal, M.M.; Ahammed, Z.; Amonett,J.; Anderson, B.D.; Anderson, M.; Arkhipkin, D.; Averichev, G.S.; Bai,Y.; Balewski, J.; Barannikova, O.; Barnby, L.S.; Baudot, J.; Bekele, S.; Belaga, V.V.; Bellingeri-Laurikainen, A.; Bellwied, R.; Benedosso, F.; Bhardwaj, S.; Bhasin, A.; Bhati, A.K.; Bichsel, H.; Bielcik, J.; Bielcikova, J.; Bland, L.C.; Blyth, S.-L.; Bonner, B.E.; Botje, M.; Bouchet, J.; Brandin, A.V.; Bravar, A.; Bystersky, M.; Cadman, R.V.; Cai,X.Z.; Caines, H.; Calderon de la Barca Sanchez, M.; Castillo, J.; Catu,O.; Cebra, D.; Chajecki, Z.; Chaloupka, P.; Chattopadhyay, S.; Chen,H.F.; Chen, J.H.; Cheng, J.; Cherney, M.; Chikanian, A.; Christie, W.; Coffin, J.P.; Cormier, T.M.; Cosentino, M.R.; Cramer, J.G.; Crawford,H.J.; Das, D.; Das, S.; Daugherity, M.; de Moura, M.M.; Dedovich, T.G.; DePhillips, M.; Derevschikov, A.A.; Didenko, L.; Dietel, T.; Djawotho,P.; Dogra, S.M.; Dong, W.J.; Dong, X.; Draper, J.E.; Du, F.; Dunin, V.B.; Dunlop, J.C.; Dutta Mazumdar, M.R.; Eckardt, V.; Edwards, W.R.; Efimov,L.G.; Emelianov, V.; Engelage, J.; Eppley, G.; Erazmus, B.; Estienne, M.; Fachini, P.; Fatemi, R.; Fedorisin, J.; Filimonov, K.; Filip, P.; Finch,E.; Fine, V.; Fisyak, Y.; Fu, J.; Gagliardi, C.A.; Gaillard, L.; Ganti,M.S.; Ghazikhanian, V.; Ghosh, P.; Gonzalez, J.S.; Gorbunov, Y.G.; Gos,H.; Grebenyuk, O.; Grosnick, D.; Guertin, S.M.; Guimaraes, K.S.F.F.; Guo,Y.; Gupta, N.; Gutierrez, T.D.; Haag, B.; Hallman, T.J.; Hamed, A.; Harris, J.W.; He, W.; Heinz, M.; Henry, T.W.; Hepplemann, S.; Hippolyte,B.; Hirsch, A.; Hjort, E.; Hoffman, A.M.; Hoffmann, G.W.; Horner, M.J.; Huang, H.Z.; Huang, S.L.; Hughes, E.W.; Humanic, T.J.; Igo, G.; Jacobs,P.; Jacobs, W.W.; Jakl, P.; Jia, F.; Jiang, H.; Jones, P.G.; Judd, E.G.; Kabana, S.; Kang, K.; Kapitan, J.; Kaplan, M.; Keane, D.; Kechechyan, A.; Khodyrev, V.Yu.; Kim, B.C.; Kiryluk, J.; Kisiel, A.; Kislov, E.M.; Klein,S.R.; Kocoloski, A.; Koetke, D.D.; et al.

2006-08-10T23:59:59.000Z

67

Measurement of the t anti-t production cross section in p anti-p collisions at s**(1/2) = 1.96-TeV  

SciTech Connect

The direct observation of the top quark was first achieved at the Tevatron proton anti-proton collider at Fermilab. This discovery completed the third generation quark sector where the top quark is expected to accompany the bottom quark in the weak isospin doublet. This dissertation discusses the experimental verification of the production cross section as predicted by the Standard Model. A measurement of the t{bar t} production cross section using 107.9 pb{sup -1} of p{bar p} collisions at {radical}s = 1.96 TeV collected with the Collider Detector at Fermilab between March of 2003 and June of 2003 is presented. The measurement focuses on the t{bar t} production in the ''lepton plus jets'' final state in which one of the W bosons from the t{bar t} decay subsequently decays leptonically to an electron or a muon, and the other decays hadronically. The B-tagging technique which utilizes the precision silicon detector tracking is used to enhance the signal for t{bar t} events relative to the background through identification of the bottom quark from its measurable lifetime. The t{bar t} production cross section is measured to be {sigma}{sub t{bar t}} = 4.5 {+-} 1.4(stat) {+-} 0.8(sys) pb.

Ray, Heather Lynn; /Michigan U.

2004-02-01T23:59:59.000Z

68

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

69

Production cross section of At radionuclides from $^{7}$Li+$^{\\textrm{nat}}$Pb and $^{9}$Be+$^{\\textrm{nat}}$Tl reactions  

E-Print Network (OSTI)

Earlier we reported theoretical studies on the probable production of astatine radionuclides from $^{6,7}$Li and $^{9}$Be-induced reactions on natural lead and thalliun targets, respectively. For the first time, in this report, production of astatine radionuclides has been investigated experimentally with two heavy ion induced reactions: $^{9}$Be+$^{\\textrm{nat}}$Tl and $^{7}$Li+$^{\\textrm{nat}}$Pb. Formation cross sections of the evaporation residues, $^{207,208,209,210}$At, produced in (HI, xn) channel, have been measured by the stacked-foil technique followed by the off-line $\\gamma$-spectrometry at the low incident energies ($<$50 MeV). Measured excitation functions have been explained in terms of compound nuclear reaction mechanism using Weisskopf-Ewing and Hauser-Feshbach model. Absolute cross section values are lower than the respective theoretical predictions.

Moumita Maiti; Susanta Lahiri

2011-09-29T23:59:59.000Z

70

Measurement of the tt? production cross section in pp? collisions at ?s=1.96 TeV using events with large Missing ET and jets  

In this paper we report a measurement of the t{anti t} production cross section in pp? collisions at ?s = 1.96 TeV using data corresponding to an integrated luminosity of 2.2 fb-1 collected with the CDF II detector at the Tevatron accelerator. We select events with significant missing transverse energy and high jet multiplicity. This measurement vetoes the presence of explicitly identified electrons and muons, thus enhancing the tau contribution of ttMs; decays. Signal events are discriminated from the background using a neural network and heavy flavor jets are identified by a secondary-vertex tagging algorithm. We measure a tt? production cross section of 7.99 ± 0.55(stat) ± 0.76(syst) ± 0.46(lumi) pb, assuming a top mass mtop = 172.5 GeV/c2, in agreement with previous measurements and standard model predictions.

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

2011-08-09T23:59:59.000Z

71

Activation cross-sections of long lived products of deuteron induced nuclear reactions on dysprosium up to 50 MeV  

E-Print Network (OSTI)

Activation cross-sections for production of 162m,161,155Ho,165,159,157,155Dy and 161,160,156,155Tb radionuclides in deuteron induced nuclear reactions on elemental dysprosium were measured up to 50 MeV for practical application and the test of the predictive power of nuclear reaction model codes. A stacked-foil irradiation technique and off-line gamma-ray spectrometry were used to determine the activities. No earlier cross-section data were found in the literature. The experimental data are compared with the predictions of the ALICE-D, EMPIRE-D and TALYS codes. Integral production yields were calculated from the fitted experimental data.

F. Tárkányi; F. Ditrói; S. Takács; J. Csikai; A. Hermanne; A. V. Ignatyuk

2014-02-05T23:59:59.000Z

72

Section efficace de production individuelle partir de la fission de l'238U avec des neutrons rapides et ultra-rapides  

E-Print Network (OSTI)

'estimer, par calculs, la section efficace de production de noyaux issus de la réaction de fission de l'uranium (faisceau de deuton, convertisseur en graphite, cible en uranium). On parle alors de « spectre modélisé 14 MeV. De ces valeurs, et étant donné que le spectre de neutrons produits par conversion du deuton

Paris-Sud XI, Université de

73

Measurement of the t anti-t production cross section in p anti-p collisions at s**(1/2) = 1.96-TeV  

SciTech Connect

We present the measurement of the t{bar t} cross section in the lepton plus jets channel with {ge} 1 and {ge} 2 secondary vertex tags. We use the scalar sum of transverse energies of the event (H{sub T}) to discriminate t{bar t} from the other backgrounds. We also use the transverse mass of the leptonic W-boson (M{sub T}{sup W}) to further reduce the Non-W backgrounds. We use a combination of data and Monte Carlo to estimate the backgrounds from electroweak processes, single top, fake leptons, W+ Light Flavor fake tags, and real W+ Heavy Flavor production. We obtain a value of {sigma} {sub {ge}1} = 8.7{sub -0.9}{sup +0.9}(stat){sub -0.9}{sup +1.2}(sys) pb for the {ge}1 tag cross section, and {sigma}{sub {ge}2} = 8.7{sub -1.6}{sup +1.8}(stat){sub -1.3}{sup +1.9}(sys) pb for the {ge}2 tag cross section. The authors also present a measurement of the t{bar t} cross section by fitting the N{sub jet} spectrum. They combine the =1 and {ge}2 tag cross sections to obtain {sigma}{sub t{bar t}} = 8.9{sub -0.9}{sup +0.9}(stat){sub -1.3}{sup +1.4}(syst)pb.

Rappoccio, Salvatore Rocco; /Harvard U.

2005-08-01T23:59:59.000Z

74

Efficient calculation of a normal matrix-vector product for anisotropic full-matrix least-squares refinement of macromolecular structures  

Science Journals Connector (OSTI)

A new set of equations for a normal matrix-vector product for the case of anisotropic refinement is given. Significantly faster methods for the calculation of a preconditioner and the normal matrix-vector product are described in detail.

Strokopytov, B.V.

2009-11-07T23:59:59.000Z

75

Syngas production by plasma treatments of alcohols, bio-oils and wood This article has been downloaded from IOPscience. Please scroll down to see the full text article.  

E-Print Network (OSTI)

Syngas production by plasma treatments of alcohols, bio-oils and wood This article has been Contact us My IOPscience #12;Syngas production by plasma treatments of alcohols, bio-oils and wood K conversion of biomass provide a great variety of products: oils, alcohols and gases. After treatment

Paris-Sud XI, Université de

76

Measurement of the t-Channel Single Top Quark Production Cross Section in pp Collisions at sqrt[s]=7??TeV  

SciTech Connect

Electroweak production of the top quark is measured in pp collisions at sqrt(s) = 7 TeV, using a dataset collected with the CMS detector at the LHC and corresponding to an integrated luminosity of 36 inverse picobarns. With an event selection optimized for t-channel production, two complementary analyses are performed. The first one exploits the special angular properties of the signal, together with background estimates from data. The second approach uses a multivariate analysis technique to probe the compatibility with signal topology expected from electroweak top quark production. The combined measurement of the cross section is 83.6 +/- 29.8 (stat.+syst.) +/- 3.3 (lumi.) pb, consistent with the standard model expectation.

Chatrchyan, Serguei; et al.

2011-08-01T23:59:59.000Z

77

Behavior of the Cross Sections for Polonium Production in Nuclear Reactions of Ar40 with Dy104  

Science Journals Connector (OSTI)

Excitation functions are reported for the reactions of Dy164 with Ar40 to produce Po200 and Po199. The cross sections are much smaller than the calculated values and it is concluded that this is due to an angular momentum cutoff and to a large fission width. The reaction threshold at a laboratory energy of 4.2 MeV per nucleon indicates a low Coulomb barrier (r0=1.45 fm).

Y. Le Beyec; M. Lefort; A. Vigny

1971-03-01T23:59:59.000Z

78

Bound-free pair production cross section in heavy-ion colliders from the equivalent photon approach  

E-Print Network (OSTI)

Exact calculations of the electron-positron pair production by a single photon in the Coulomb field of a nucleus with simultaneous capture of the electron into the K-shell are discussed for different nuclear charges. Using the equivalent photon method of Weizsaecker and Williams, a simple expression for the bound-free production of electron-positron pairs by colliding very-high-energy fully stripped heavy ions is derived for nuclei of arbitrary charge.

Andreas Aste

2008-01-16T23:59:59.000Z

79

Full list of Portfolio Manager custom reporting metrics | ENERGY STAR  

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Full list of Portfolio Manager custom reporting metrics Full list of Portfolio Manager custom reporting metrics Secondary menu About us Press room Contact Us Portfolio Manager Login Facility owners and managers Existing buildings Commercial new construction Industrial energy management Small business Service providers Service and product providers Verify applications for ENERGY STAR certification Design commercial buildings Energy efficiency program administrators Commercial and industrial program sponsors Associations State and local governments Federal agencies Tools and resources Training In This Section Campaigns Commercial building design Communications resources Energy management guidance Financial resources Portfolio Manager Products and purchasing Recognition Research and reports Service and product provider (SPP) resources

80

Measurement of the ZZ production cross section and search for the standard model Higgs boson in the four lepton final state in pp¯ collisions  

Science Journals Connector (OSTI)

We present a measurement of Z boson pair production in pp¯ collisions at 1.96 TeV with 9.6 to 9.8??fb-1 of D0 data. We examine the final states eeee, ee??, and ????. Based on selected data, the measured cross section in the mass region M(Z/?*)>30??GeV is ?(pp¯?Z/?*Z/?*)=1.26-0.36+0.44(stat)-0.15+0.17(syst)±0.08(lumi)??pb; after correcting for the expected ratio of ?(pp¯?Z/?*Z/?*) to ?(pp¯?ZZ), we derive a cross section for pp¯?ZZ production of 1.05-0.30+0.37(stat)-0.12+0.14(syst)±0.06(lumi)??pb. This result is combined with a previous result from the ZZ??+?-??¯ channel resulting in a combined pp¯?ZZ cross section measurement of 1.32-0.25+0.29(stat)±0.12(syst)±0.04(lumi)??pb. These measurements are consistent with the standard model expectation of 1.43±0.10??pb. We extend this analysis to search for the standard model (SM) Higgs boson between 115 and 200 GeV. At a Higgs boson mass of 125 GeV, we expect to set a limit of 43 times the SM expectation at 95% C.L., and set a limit of 42 times the SM expectation at 95% C.L.

V. M. Abazov et al. (D0 Collaboration)

2013-08-15T23:59:59.000Z

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81

Full documents available at: http://www.epa.gov/otaq/climate/regulations.htm EPA's section of the Preamble for the Light-Duty GHG Rule (see pp. 388-396)  

E-Print Network (OSTI)

of the Preamble for the Light-Duty GHG Rule (see pp. 388-396) III.H. What are the Estimated Cost, Economic, and Other Impacts of the Program? In this section, EPA presents the costs and impacts of EPA's GHG program. It is important to note that NHTSA's CAFE standards and EPA's GHG standards will both be in effect, and each

Edwards, Paul N.

82

Measurement of the inclusive W and Z production cross sections in pp collisions at $ \\sqrt {s} = 7 $ TeV with the CMS experiment  

SciTech Connect

A measurement of inclusive W and Z production cross sections in pp collisions at sqrt(s)=7 TeV is presented. The electron and muon decay channels are analyzed in a data sample collected with the CMS detector at the LHC and corresponding to an integrated luminosity of 36 inverse picobarns. The measured inclusive cross sections are sigma(pp-> WX) B(W-> l nu) = 10.30 +/- 0.02 (stat.) +/- 0.10 (syst.) +/- 0.10 (th.) +/- 0.41 (lumi.) nb and sigma(pp -> ZX) B(Z-> l^+l^-) = 0.974 +/- 0.007 (stat.) +/- 0.007 (syst.) +/- 0.018 (th.) +/- 0.039 (lumi.) nb, limited to the dilepton invariant mass range 60 to 120 GeV. The luminosity-independent cross section ratios are [sigma(pp->WX) B(W-> l nu)]/[sigma(pp-> ZX) B(Z->l^+l^-)] = 10.54 +/- 0.07 (stat.) +/- 0.08 (syst.) +/- 0.16 (th.) and [sigma(pp->W^+X) B(W^+ -> l^+nu)] / [sigma(pp->W^- X) B(W^- -> l^- nu)] = 1.421 +/- 0.006 (stat.) +/- 0.014 (syst.) +/- 0.029 (th.). The measured values agree with next-to-next-to-leading order QCD cross section calculations based on recent parton distribution functions.

Chatrchyan, Serguei; et al.

2011-10-01T23:59:59.000Z

83

Measurement of the cross section for W-boson production in association with jets in pp¯ collisions at s=1.96??TeV  

Science Journals Connector (OSTI)

We present a measurement of the cross section for W-boson production in association with jets in pp¯ collisions at s=1.96??TeV. The analysis uses a data sample corresponding to an integrated luminosity of 320??pb-1 collected with the CDF II detector. W bosons are identified in their electron decay channel and jets are reconstructed using a cone algorithm. For each W+?n-jet sample (n=1-4) we measure the differential cross section d?(pp¯?W+?n-jet)/dETnth-jet×B(W?e?) with respect to the transverse energy ET of the nth-highest ET jet above 20 GeV, and the total cross section ?(pp¯?W+?n-jet;ETnth-jet>25??GeV)×B(W?e?), for a restricted W?e? decay phase space. The cross sections, corrected for all detector effects, can be directly compared to particle level W+jet(s) predictions. We present here comparisons to leading order and next-to-leading order predictions.

T. Aaltonen et al. (CDF Collaboration)

2008-01-31T23:59:59.000Z

84

Updated Measurement of the Single Top Quark Production Cross Section and $V{tb}$ in the Missing Transverse Energy Plus Jets Topology in $p\\bar{p}$ Collisions at $\\sqrt{s} = 1.96$ TeV  

E-Print Network (OSTI)

An updated measurement of the single top quark production cross section is presented using the full data set collected by the Collider Detector at Fermilab (CDF) and corresponding to 9.5 fb${}^{-1}$ of integrated luminosity from proton-antiproton collisions at 1.96 TeV center-of-mass energy. The events selected contain an imbalance in the total transverse energy, jets identified as originating from $b$ quarks, and no identified leptons. The sum of the $s$- and $t$-channel single top quark cross sections is measured to be $3.53_{-1.16}^{+1.25}$ pb and a lower limit on $V_{tb}$ of 0.63 is obtained at the 95% credibility level. These measurements are combined with previously reported CDF results obtained from events with an imbalance in total transverse energy, jets identified as originating from $b$ quarks, and exactly one identified lepton. The combined cross section is measured to be $3.02_{-0.48}^{+0.49}$ pb and a lower limit on $V{tb}$ of 0.84 is obtained at the 95% credibility level.

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

2014-10-21T23:59:59.000Z

85

Measurement of the Cross Section for Prompt Isolated Diphoton Production in $p\\bar{p}$ Collisions at \\sqrt s = 1.96 TeV  

SciTech Connect

This article reports a measurement of the cross section of prompt isolated photon pair production in p{bar p} collisions at a total energy {radical}s = 1.96 TeV using data of 5.36 fb{sup -1} integrated luminosity collected with the CDF II detector at the Fermilab Tevatron. The measured cross section, differential in basic kinematic variables, is compared with three perturbative QCD predictions, a leading order (LO) parton shower calculation and two next-to-leading order (NLO) calculations. The NLO calculations reproduce most aspects of the data. By including photon radiation from quarks before and after hard scattering, the parton shower prediction becomes competitive with the NLO predictions.

Vellidis, Costas; /Fermilab

2011-09-01T23:59:59.000Z

86

Measurement of the ZZ production cross section in p-pbar collisions at sqrt(s)=1.96 TeV  

E-Print Network (OSTI)

We present a new measurement of the production cross section $\\sigma(p\\bar{p} \\rightarrow ZZ)$ at a center-of-mass energy $\\sqrt{s}=1.96$ TeV, obtained from the analysis of the four charged lepton final state $\\ell^{+}\\ell^{-}\\ell^{'+} \\ell^{'-}$ ($\\ell$, $\\ell^{'}$ = $e$ or $\\mu$). We observe ten candidate events with an expected background of $0.37 \\pm 0.13$ events. The measured cross section $\\sigma(p\\bar{p} \\to ZZ)= 1.26^{+0.47}_{-0.37} \\mathrm{(stat)} \\pm 0.14 \\mathrm{(syst)}$ pb is in agreement with NLO QCD predictions. This result is combined with a previous result from the $ZZ\\to\\ell^{+}\\ell^{-}\

D0 Collaboration; V. Abazov

2011-04-15T23:59:59.000Z

87

Measurement of K+ production cross section by 8 GeV protons using high energy neutrino interactions in the SciBooNE detector  

SciTech Connect

The SciBooNE Collaboration reports K+ production cross section and rate measurements using high energy daughter muon neutrino scattering data off the SciBar polystyrene (C8H8) target in the SciBooNE detector. The K+ mesons are produced by 8 GeV protons striking a beryllium target in Fermilab Booster Neutrino Beam line (BNB). Using observed neutrino and antineutrino events in SciBooNE, we measure d2?/dpd? = (5.34 ±0.76) mb/(GeV/c x sr) for p + Be =K+ + X at mean K+ energy of 3.9 GeV and angle (with respect to the proton beam direction) of 3.7 degrees, corresponding to the selected K+ sample. Compared to Monte Carlo predictions using previous higher energy K+ production measurements, this measurement, which uses the NUANCE neutrino interaction generator, is consistent with a normalization factor of 0.85 ± 0.12. This agreement is evidence that the extrapolation of the higher energy K+ measurements to an 8 GeV beam energy using Feynman scaling is valid. This measurement reduces the error on the K+ production cross section from 40% to 14%.

Cheng, G [Columbia U.; Mariani, C [Columbia U.; Alcaraz-Aunion, J L [Barcelona, IFAE; Brice, S J [Fermilab; Bugel, L [MIT; Catala-Perez, J [Valencia U.; Conrad, J M [MIT; Djurcic, Z [Columbia U.; Dore, U [Banca di Roma; INFN, Rome; Finley, D A [Fermilab; Franke, A J [Columbia U.; Banca di Roma; INFN, Rome

2011-07-28T23:59:59.000Z

88

Measurement of the production cross section for Z/?* in association with jets in pp collisions at ?s=7??TeV with the ATLAS detector  

E-Print Network (OSTI)

Results are presented on the production of jets of particles in association with a Z/?* boson, in proton-proton collisions at ?s=7??TeV with the ATLAS detector. The analysis includes the full 2010 data set, collected with ...

Taylor, Frank E.

89

Performance des jets et mesure de la section efficace de production de paires t tbar dans le canal tout hadronique auprès du détecteur ATLAS  

E-Print Network (OSTI)

In this report, we summarise our research program within the ATLAS collaboration between 2005-2012. We summarise our contribution to the integration of two of the Inner Detector sub-detectors, the SCT and the TRT. We describe also our contribution to the optimisation and tuning of the jet reconstruction in the harsh ATLAS environment. We compare the performances of these different algorithms. Finally, with the data collected at a centre of mass energy of 7 TeV, we extract the top-anti-top production cross section in the challenging all-hadronic decay channel.

Ghodbane, N

90

Inclusive hadronic production cross sections measured in proton-nucleus collisions at. sqrt. s = 27. 4 GeV  

SciTech Connect

We present results on the production of hadrons in collisions of 400-GeV/c protons with beryllium, copper, and tungsten nuclei. The data cover the region from 5.6 to 8.0 GeV/c in the transverse momentum of the final-state hadron and from 73/sup 0/ to 102/sup 0/ in the proton-nucleon center-of-momentum frame production angle theta/sup */. The restriction of the data to values of x/sub T/ (x/sub T/ = 2p/sub T// ..sqrt..s ) greater than 0.4 enriches the sample with hard collisions of valence quarks. Asymmetries about theta/sup */ = 90/sup 0/ reflect the presence of neutrons in the target nuclei. The variation of the atomic-weight dependence parameter ..cap alpha.. with production angle is discussed in the context of the phenomenology of nucleonic structure within nuclei. We also extrapolate our measurements to a ''deuteron'' target to minimize nuclear effects and compare the result to QCD calculations.

Crittenden, J.A.; Hsiung, Y.B.; Kaplan, a.D.M.; Hubbard, J.R.; Mangeot, P.; Peisert, A.; Charpak, G.; Sauli, F.; Brown, C.N.; Childress, S.; and others

1986-11-01T23:59:59.000Z

91

Measurement of the top quark mass and top-antitop production cross section from dilepton events at the Collider Detector at Fermilab  

E-Print Network (OSTI)

We present an analysis of dilepton events originating from top-antitop production in proton-antiproton collisions at sqrt{s}=1.8 TeV at the Fermilab Tevatron Collider. The sample corresponds to an integrated luminosity of 109+-7 pb^{-1}. We observe 9 candidate events, with an estimated background of 2.4+-0.5 events. We determine the mass of the top quark to be M_top = 161+-17(stat.)+-10(syst.) GeV/c^2. In addition we measure a top-antitop production cross section of 8.2+4.4-3.4 pb (where M_top = 175 GeV/c^2 has been assumed for the acceptance estimate).

CDF collaboration

1998-02-18T23:59:59.000Z

92

Differential cross section measurements for the production of a W boson in association with jets in proton-proton collisions at sqrt(s) = 7 TeV  

E-Print Network (OSTI)

Measurements are reported of differential cross sections for the production of a W boson, which decays into a muon and a neutrino, in association with jets, as a function of several variables, including the transverse momenta and pseudorapidities of the four leading jets, the scalar sum of jet transverse momenta, and the difference in azimuthal angle between the directions of each jet and the muon. The data sample of pp collisions at a centre-of-mass energy of 7 TeV was collected with the CMS detector at the LHC and corresponds to an integrated luminosity of 5.0 inverse femtobarns. The measured cross sections are compared to predictions from Monte Carlo generators, MADGRAPH+PYTHIA and SHERPA, and to next-to-leading-order calculations from BLACKHAT+SHERPA. The differential cross sections are found to be in agreement with the predictions, apart from the pt distributions of the leading jets at high pt values, the distributions of the HT at high-HT and low jet multiplicity, and the distribution of the difference in azimuthal angle between the leading jet and the muon at low values.

CMS Collaboration

2014-06-29T23:59:59.000Z

93

Measurement of the gamma(1S) production cross-section in pp collisions at root s=7 TeV in ATLAS  

SciTech Connect

A measurement of the cross-section for {Gamma}(1S) {yields} {mu}{sup +}{mu}{sup -} production in proton-proton collisions at center of mass energy of 7 TeV is presented. The cross-section is measured as a function of the {Gamma}(1S) transverse momentum in two bins of rapidity, |y{sup {Gamma}(1S)}| < 1.2 and 1.2 < |y{sup {Gamma}(1S)}| < 2.4. The measurement requires that both muons have transverse momentum p{sub T}{sup {mu}} > 4 GeV and pseudorapidity |{eta}{sup {mu}}| < 2.5 in order to reduce theoretical uncertainties on the acceptance, which depend on the poorly known polarization. The results are based on an integrated luminosity of 1.13 pb{sup -1}, collected with the ATLAS detector at the Large Hadron Collider. The cross-section measurement is compared to theoretical predictions: it agrees to within a factor of two with a prediction based on the NRQCD model including color-singlet and color-octet matrix elements as implemented in Pythia while it disagrees by up to a factor of ten with the next-to-leading order prediction based on the color-singlet model.

Aad, G.; Abbott, B; Abdallah, J; Abdelalim, AA; Abdesselam, A; Abdinov, O; Abi, B; Abolins, M; Abramowicz, H; Abreu, H; Acerbi, E; Acharya, BS; Adams, DL; Addy, TN; Adelman, J; Aderholz, M; Adomeit, S; Adragna, P; Adye, T; Aefsky, S; Aguilar-Saavedra, JA

2011-11-03T23:59:59.000Z

94

Cross sections of the reaction Pa231(d,3n)U230 for the production of U230/Th226 for targeted ? therapy  

Science Journals Connector (OSTI)

U230 and its daughter nuclide Th226 are novel therapeutic nuclides for application in targeted ? therapy of cancer. We investigated the feasibility of producing U230/Th226 via deuteron irradiation of Pa231 according to the reaction Pa231(d,3n)U230. The experimental excitation function for a deuteron-induced reaction on Pa231 is reported for the first time. Cross sections were measured using thin targets of Pa231 prepared by electrodeposition and U230 yields were analysed using ? spectrometry. Beam energies were calculated from measured beam orbits and compared with the values obtained via monitor reactions on aluminium foils using high-resolution ? spectrometry and IAEA recommended cross sections. Beam intensities were determined using a beam current integrator. The experimental cross sections are in excellent agreement with model calculations allowing for deuteron breakup using the EMPIRE 3 code. According to thick-target yields calculated from the experimental excitation function, the reaction Pa231(d,3n)U230 allows the production of U230/Th226 at moderate levels.

A. Morgenstern; O. Lebeda; J. Stursa; R. Capote; M. Sin; F. Bruchertseifer; B. Zielinska; C. Apostolidis

2009-11-25T23:59:59.000Z

95

Measurement of the tt, WW and Z -> tautau Production Cross Sections in p anti-p collisions at s**(1/2) = 1.96 TeV  

SciTech Connect

In this thesis we present a new technique to analyze events containing two highly energetic leptons, as a probe of the Standard Model. The philosophy is to consider the data in a more global way, as opposed to the more traditional process dependent approach of extracting a given signal over the expected backgrounds by using various kinematical requirements. We use our global technique to simultaneously measure the cross sections of the main Standard Model processes; the t{bar t}, WW and Z {yields} {tau}{tau} production from p{bar p} collisions at {radical}s = 1.96 TeV in the CDF detector at Fermilab. We select events by requiring they contain two highly energetic leptons (e{mu}, ee, or {mu}{mu}), and make no other kinematic requirements, except for the ee and {mu}{mu} channels. We then use a likelihood fit of the data in the two-dimensional phase space defined by the missing transverse energy (E{sub T}) and the number of jets in the event (N{sub jet}), to the expected Standard Model distributions, to simultaneously extract the production cross-sections of the main process contributing to our dilepton sample.

Carron Montero, Sebastian Fernando; /Duke U.

2006-11-01T23:59:59.000Z

96

Status of cross-section data for gas production from vanadium and {sup 26}AL from silicon carbide in a D-T fusion reactor.  

SciTech Connect

Current designs of fusion-reactor systems seek to use radiation-resistant, low-activation materials that support long service lifetimes and minimize radioactive-waste problems after decommissioning. Reliable assessment of fusion materials performance requires accurate neutron-reaction cross sections and radioactive-decay constants. The problem areas usually involve cross sections since decay parameters tend to be better known. The present study was motivated by two specific questions: (i) Why are the {sup 51}V(n,np){sup 50}Ti cross section values in the ENDF/B-VI library so large (a gas production issue)? (ii) How well known are the cross sections associated with producing 7.4 x 10{sup 5} y {sup 26}Al in silicon carbide by the process {sup 28}Si(n,np+d){sup 27} Al(n,2n){sup 26}Al (a long-lived radioactivity issue)? The energy range 14-15 MeV of the D-T fusion neutrons is emphasized. Cross-section error bars are needed so that uncertainties in the gas and radioactivity generated over the lifetime of a reactor can be estimated. We address this issue by comparing values obtained from prominent evaluated cross-section libraries. Small differences between independent evaluations indicate that a physical quantity is well known while the opposite signals a problem. Hydrogen from {sup 51}V(n,p){sup 51}Ti and helium from {sup 51}V(n,{alpha}){sup 48}Sc are also important sources of gas in vanadium, so they too were examined. We conclude that {sup 51}V(n,p){sup 51}Ti is adequately known but {sup 51}V(n,np+d){sup 50}Ti is not. The status for helium generation data is quite good. Due to recent experimental work, {sup 27}Al(n,2n){sup 26}Al seems to be fairly well known. However, the situation for {sup 28}Si(n,np+d){sup 27}Al remains unsatisfactory.

Gomes, I. C.

1998-08-11T23:59:59.000Z

97

Activation cross sections of $\\alpha$-particle induced nuclear reactions on hafnium and deuteron induced nuclear reaction on tantalum: production of $^{178}$W/$^{178m}$Ta generator  

E-Print Network (OSTI)

In the frame of a systematic study of charged particle production routes of medically relevant radionuclei, the excitation function for indirect production of $^{178m}$Ta through $^{nat}$Hf($\\alpha$,xn)$^{178}$W-$^{178m}$Ta nuclear reaction was measured for the first time up to 40 MeV. In parallel, the side reactions $^{nat}$Hf($\\alpha$,x)$^{179,177,176,175}$W, $^{183,182,178g,177,176,175}$Ta, $^{179m,177m,175}$Hf were also assessed. Stacked foil irradiation technique and $\\gamma$-ray spectrometry were used. New experimental cross section data for the $^{nat}$Ta(d,xn)$^{178}$W reaction are also reported up to 40 MeV. The measured excitation functions are compared with the results of the ALICE-IPPE, and EMPIRE nuclear reaction model codes and with the TALYS 1.4 based data in the TENDL-2013 library. The thick target yields were deduced and compared with yields of other charged particle ((p,4n), (d,5n) and ($^3$He,x)) production routes for $^{178}$W.

Tárk'anyi, F; Ditrói, F; Hermanne, A; Ignatyuk, A V; Uddin, M S

2014-01-01T23:59:59.000Z

98

Proton-production double-differential cross sections for 300-MeV and 392-MeV proton-induced reactions  

SciTech Connect

We investigate proton-production double-differential cross sections (DDXs) for 300- and 392-MeV proton-induced reactions on O, V, Tb, Ta, Au, Pb, and Bi. Emitted proton energies are measured with stacked scintillator spectrometers by the {Delta}E-E technique. Experimental results are compared with the intranuclear cascade (INC) and quantum molecular dynamics models. Although both models can reproduce spectral DDXs, there is a difference at the most forward and backward angles. The cause of these differences is discussed in terms of the refraction caused by the nuclear potential. Angular distributions of the present data are well accounted for by the Kalbach systematics plus INC one-step calculations. The quasi-free-scattering contribution increases with decreasing target mass and increasing emission energy.

Iwamoto, Hiroki [Department of Applied Quantum Physics and Nuclear Engineering, Kyushu University, 744 Motooka, Nishi-ku, Fukuoka 819-0395 (Japan); Japan Atomic Energy Agency, Tokai-mura, Naka-gun, Ibaraki 319-1195 (Japan); Imamura, Minoru; Koba, Yusuke; Fukui, Yoshinori; Wakabayashi, Genichiro; Uozumi, Yusuke [Department of Applied Quantum Physics and Nuclear Engineering, Kyushu University, 744 Motooka, Nishi-ku, Fukuoka 819-0395 (Japan); Kin, Tadahiro; Iwamoto, Yosuke [Japan Atomic Energy Agency, Tokai-mura, Naka-gun, Ibaraki 319-1195 (Japan); Hohara, Shinya [Kinki University Atomic Energy Research Institute, Kowakae, Higashiosaka 577-8502 (Japan); Nakano, Masahiro [University of Occupational and Environmental Health, Kitakyushu 807-8555 (Japan)

2010-09-15T23:59:59.000Z

99

Measurement of ww + wz production cross section and study of the dijet mass spectrum in the lnu + jets final state at CDF  

SciTech Connect

We present the measurement of the WW and WZ production cross section in p{bar p} collisions at {radical}s = 1.96 TeV, in a final state consisting of an electron or muon, neutrino and jets. The data analyzed were collected by the CDF II detector at the Tevatron collider and correspond to 4.3 fb{sup -1} of integrated luminosity. The analysis uses a fit to the dijet mass distribution to extract the diboson contribution. We observe 1582 {+-} 275(stat.) {+-} 107(syst.) diboson candidate events and measure a cross section of {sigma}{sub WW/WZ} = 18.1 {+-} 3.3(stat.) {+-} 2.5(syst.) pb, consistent with the Standard Model prediction of 15.9 {+-} 0.9 pb. The best fit to the dijet mass of the known components shows a good agreement with the data except for the [120, 160] GeV/c{sup 2} mass range, where an excess is observed. We perform detailed checks of our background model and study the significance of the excess, assuming an additional gaussian component with a width compatible with the expected dijet mass resolution. A standard {Delta}{sub {chi}}{sup 2} test of the presence of the additional component, returns a p-value of 4.2 x 10{sup -4} when standard sources of systematics are considered, corresponding to a significance of 3.3{sigma}.

Cavaliere, Viviana; /Siena U.

2010-12-01T23:59:59.000Z

100

Measurement of the Cross Section for Production of Prompt Diphoton in proton anti-proton Collisions at s**(1/2) = 1.96-TeV  

SciTech Connect

This thesis presents the measurement of prompt diphoton production rate in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV using the upgraded Collider Detector at Fermilab (CDF II). This process deserves some attention for the following reasons. The H {yields} {gamma}{gamma} decay mode is an important channel for the Standard Model (SM) Higgs boson searches in the low mass region (M{sub H} < 130 GeV) at the forth coming LHC. In many models involving physics beyond the SM, cascade decays of heavy new particles generate a {gamma}{gamma} signature. Some examples are supersymmetry with a light gravitino, radiative decays to a higgsino-LSP and models with large symmetry groups. The QCD production of prompt photon pairs with large invariant mass is the irreducible background to these searches. The rate is huge and requires to be quantitatively evaluated prior to any of the possible discoveries. In a hadronic collider environment such as LHC, prompt photon signals are contaminated by the production of neutral mesons which decay to multiple collinear photons. The experience of classifying background of neutral meson is very important. The process can be used to test the Next-to-Leading Order (NLO) calculation of Quantum Chromodynamics (QCD). The 4-momentum of particles in the di-photon final state can be precisely determined due to the fine energy resolution of the electromagnetic calorimeters. The imbalance in the transverse momentum of the two photons reflects the transverse motion of the colliding partons. At collider energies, most of the transverse momentum of the incoming partons can be attributed to multiple soft gluon emissions prior to the collision, of which the effect to di-photon production can be resummed by Collins-Soper-Sterman (CSS) formalism. The Tevatron data can be used to test the resummation formalisms. They have used 207 pb{sup -1} of data collected by CDF II detector during the February 2002 to September 2003 running period to study the diphoton QCD production, and compared with next-to-leading order predictions. The background is subtracted using a statistical method based on the difference between the EM showers initiated by photons and by the backgrounds. The cross sections are measured as a function of diphoton mass, diphoton system transverse momentum and azimuthal angle between the two photons. The results are found to be consistent with perturbative QCD predictions.

Liu, Yan-wen; /Geneva U.; ,

2004-11-01T23:59:59.000Z

Note: This page contains sample records for the topic "full section production" 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
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101

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising. ...

1982-01-11T23:59:59.000Z

102

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising. ...

1984-03-19T23:59:59.000Z

103

A measurement of hadron production cross sections for the simulation of accelerator neutrino beams and a search for muon-neutrino to electron-neutrino oscillations in the delta m**2 about equals 1-eV**2 region  

SciTech Connect

A measurement of hadron production cross-sections for the simulation of accelerator neutrino beams and a search for muon neutrino to electron neutrino oscillations in the {Delta}m{sup 2} {approx} 1 eV{sup 2} region. This dissertation presents measurements from two different high energy physics experiments with a very strong connection: the Hadron Production (HARP) experiment located at CERN in Geneva, Switzerland, and the Mini Booster Neutrino Experiment (Mini-BooNE) located at Fermilab in Batavia, Illinois.

Schmitz, David W.; /Columbia U.

2008-01-01T23:59:59.000Z

104

Section J  

Office of Environmental Management (EM)

M-1 Section J Appendix M Key Design, Licensing and Site Management M&O Milestone Chart Activity Planned Date Develop and Submit CD-2 (25%-30%) 082009 Submission of Construction...

105

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... ACS MEMBER RATES "Situations wanted" advertisements will be classified by the chemical field designated by the member. ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 1599 Post Road East, P.O. ...

1993-11-01T23:59:59.000Z

106

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 25 Sylvan Rd. ...

1985-04-15T23:59:59.000Z

107

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 25 Sylvan Rd. ...

1985-07-22T23:59:59.000Z

108

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 25 Sylvan Rd. ...

1986-04-28T23:59:59.000Z

109

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 500 Post Road East, P.O. ...

1987-06-22T23:59:59.000Z

110

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 500 Post Road East, P.O. ...

1992-01-27T23:59:59.000Z

111

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 25 Sylvan Rd. ...

1983-02-14T23:59:59.000Z

112

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 1599 Post Road East, P.O. ...

1992-03-30T23:59:59.000Z

113

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 500 Post Road East, P.O. ...

1989-01-02T23:59:59.000Z

114

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 1599 Post Road East, P.O. ...

1992-03-02T23:59:59.000Z

115

SECTION J  

Office of Environmental Management (EM)

J-1 SECTION J APPENDIX J PERFORMANCE EVALUATION AND MEASUREMENT PLAN (TO BE NEGOTIATED AFTER CONTRACT AWARD) Contract No.: DE-RW0000005 QA:QA J-J-2 Page Blank...

116

SECTION E  

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

Attachment P Completion Definition Sheets for Incentive Fee C.1 Activity Milestone Completion Incentive WTP Contract Section J Contract No. DE-AC27-01RV14136 Conformed...

117

Measurement of the tt[over-bar] production cross section in pp[over-bar] collisions at [sqrt]s=1.96??TeV using events with large missing transverse energy and jets  

E-Print Network (OSTI)

In this paper we report a measurement of the tt[over-bar] production cross section in pp[over-bar] collisions at [sqrt]s=1.96??TeV using data corresponding to an integrated luminosity of 2.2??fb[superscript -1] collected ...

Bauer, Gerry P.

118

Measurement of the hadronic activity in events with a Z and two jets and extraction of the cross section for the electroweak production of a Z with two jets in pp collisions at ?s =7 TeV  

E-Print Network (OSTI)

The first measurement of the electroweak production cross section of a Z boson with two jets (Zjj) in pp collisions at ?s = 7 TeV is presented, based on a data sample recorded by the CMS experiment at the LHC with an ...

Apyan, Aram

119

Production  

Science Journals Connector (OSTI)

Production is obtained from proved reserves but the determinants of the scale of production in the industry and country components of the world total are many and complex with some unique to the individual com...

D. C. Ion

1980-01-01T23:59:59.000Z

120

Measurement of neutrino-induced charged-current charged pion production cross sections on mineral oil at E??1??GeV  

Science Journals Connector (OSTI)

Using a high-statistics, high-purity sample of ??-induced charged current, charged pion events in mineral oil (CH2), MiniBooNE reports a collection of interaction cross sections for this process. This includes measurements of the CC?+ cross section as a function of neutrino energy, as well as flux-averaged single- and double-differential cross sections of the energy and direction of both the final-state muon and pion. In addition, each of the single-differential cross sections are extracted as a function of neutrino energy to decouple the shape of the MiniBooNE energy spectrum from the results. In many cases, these cross sections are the first time such quantities have been measured on a nuclear target and in the 1 GeV energy range.

A. A. Aguilar-Arevalo et al. (MiniBooNE Collaboration)

2011-03-23T23:59:59.000Z

Note: This page contains sample records for the topic "full section production" 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.
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121

Full SPP Partnership Requirements  

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

Partnership Requirements: Partnership Requirements: ENERGY STAR Partnership for Commercial & Industrial Service and Product Providers (SPP) Eligible Organizations Companies providing energy efficiency services and products to commercial buildings and industrial manufacturing facilities/plants are eligible for the Service and Product Provider (SPP) partnership, but must meet certain requirements as specified below. Types of eligible companies include: architecture, distributor, energy consultant/energy management services, energy improvement contractor, energy information services, energy services company (ESCO), engineering, equipment manufacturer, financial services, on-site energy production services, unregulated energy retailer and marketer, or other supplier of standard energy-efficient products and/or services for commercial buildings and/or

122

16O Cross Section  

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

p, X) (Incomplete) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1973MC12 16O(p, ): threshold - 7.7 X4 10172012 1981DY03 16O(p, p): for production of...

123

20Ne Cross Section  

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

p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1981DY03 20Ne(p, p'): for production of -rays threshold - 23 1.63-MeV -rays...

124

Section J  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

L-1 L-1 Section J Appendix L MEMORANDUM FROM DAVID R. HILL, GENERAL COUNSEL, DATED NOVEMBER 30, 2006, SUBJECT: ONGOING LICENSING SUPPORT NETWORK ("LSN") OBLIGATIONS Contract No.: DE-RW0000005 QA:QA J-L-2 Contract No.: DE-RW0000005 QA:QA J-L-3 Contract No.: DE-RW0000005

125

Advertising Section  

Science Journals Connector (OSTI)

Advertising Section ... "Situations wanted" advertisements placed by employed ACS members and student affiliates are accepted at 50 cents per word per insertion, no minimum charge. ... State ACS membership status and mail advertisements to CHEMICAL AND ENGINEERING NEWS, Classified Advertising, 25 Sylvan Rd. ...

1980-08-11T23:59:59.000Z

126

Production  

Energy.gov (U.S. Department of Energy (DOE))

Algae production R&D focuses on exploring resource use and availability, algal biomass development and improvements, characterizing algal biomass components, and the ecology and engineering of...

127

Measurement of the triple-differential cross section for photon + jets production in proton-proton collisions at s? = 7 TeV  

E-Print Network (OSTI)

A measurement of the triple-differential cross section, d[superscript 3]?/(dp[superscript ?]Td?[superscript ?]d?[superscript jet]) , in photon + jets final states using a data sample from proton-proton collisions at s? = ...

Apyan, Aram

128

Fox findings in full  

Science Journals Connector (OSTI)

... to reduce it involve matters of national security and international relations which are beyond the ambit of the Inquiry. We suggest that the questions involved are of such importance that ... recognition of the hazards, dangers and problems of and associated with the production of nuclear energy, and should therefore seek to limit or restrict expansion of that production.

1976-12-23T23:59:59.000Z

129

BlackboardSectioningTool Course Sectioning The Sectioning Tool  

E-Print Network (OSTI)

sectioning tool: Consult the online help provided within the sectioning tool Call the OIT Help Desk at (609 by those preferences, select Enable/Configure Student Preference Tool. Need help using the BlackboardBlackboardSectioningTool Course Sectioning 1 The Sectioning Tool The Sectioning Tool is a course

Bou-Zeid, Elie

130

Section 66  

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

CFCl CFCl 3 ) (CF 2 Cl 2 ) (CHFCl 2 ) CF 4 CCl 4 (CFCl 3 ) (CF 2 Cl 2 ) (CHFCl 2 ) SF 6 CF 4 CCl 4 Session Papers 277 Figure 1. Spectral absorption cross-sections of CF 4 between 1281 and 1284 cm . The experimental -1 conditions correspond to the surface, 5-km, and 19-km levels of the U.S. Standard Atmosphere. Figure 2. Spectral absorption cross-sections of CCl 4 between 755 and 810 cm . The experimental conditions -1 correspond to the surface, 5-km, and 19-km levels of the U.S. Standard Atmosphere. Laboratory Spectroscopy in Support of the Atmospheric Radiation Measurement Program P. Varanasi Institute for Terrestrial and Planetary Atmospheres The University at Stony Brook Stony Brook, New York There is considerable world-wide interest in the remote sensing of chlorofluorocarbons (CFCs), especially CFC-11

131

Cross-section  

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

Cross-section Cross-section formulae for specific processes 1 39. CROSS-SECTION FORMULAE FOR SPECIFIC PROCESSES Revised September 2005 by R.N. Cahn (LBNL). Setting aside leptoproduction (for which, see Sec. 16), the cross sections of primary interest are those with light incident particles, e + e - , γγ, qq, gq , gg, etc., where g and q represent gluons and light quarks. The produced particles include both light particles and heavy ones - t, W , Z, and the Higgs boson H. We provide the production cross sections calculated within the Standard Model for several such processes. 39.1. Resonance Formation Resonant cross sections are generally described by the Breit-Wigner formula (Sec. 16 of this Review). σ(E) = 2J + 1 (2S 1 + 1)(2S 2 + 1) 4π k 2 Γ 2 /4 (E - E 0 ) 2 + Γ 2 /4 B in B out , (39.1) where E is the c.m. energy, J is the spin of the resonance, and the number of polarization states of the two incident particles

132

Production  

Energy.gov (U.S. Department of Energy (DOE))

Algae production R&D focuses on exploring resource use and availability, algal biomass development and improvements, characterizing algal biomass components, and the ecology and engineering of cultivation systems.

133

Measurement of the t anti-t production cross section in p anti-p collisions at s**(1/2) = 1.96-TeV using missing E(T) + jets events with secondary vertex b-tagging  

SciTech Connect

The authors present a measurement of the t{bar t} production cross section in p{bar p} collisions at {radical}s = 1.96 TeV which uses events with an inclusive signature of significant missing transverse energy and jets. This is the first measurement which makes no explicit lepton identification requirements, so that sensitivity to W {yields} {tau}{nu} decays is maintained. Heavy flavor jets from top quark decay are identified with a secondary vertex tagging algorithm. From 311 pb{sup -1} of data collected by the Collider Detector at Fermilab they measure a production cross section of 5.8 {+-} 1.2(stat.){sub -0.7}{sup +0.9}(syst.) pb for a top quark mass of 178 GeV/c{sup 2}, in agreement with previous determinations and standard model predictions.

Abulencia, A.; Acosta, D.; Adelman, Jahred A.; Affolder, T.; Akimoto, T.; Albrow, M.G.; Ambrose, D.; Amerio, S.; Amidei, D.; Anastassov, A.; Anikeev, K.; /Taiwan, Inst.

2006-03-01T23:59:59.000Z

134

A Measurement of the t anti-t Production Cross Section in p anti-p Collisions at s**(1/2) = 1.96-TeV using Soft Muon Tagging  

SciTech Connect

I present a measurement of the t{bar t} production cross section at {radical}s = 1.96 TeV using 2034 pb{sup -1} of CDF Run II data using events with a high transverse momentum electron or muon, three or more jets, and missing transverse energy. The measurement assumes a t {yields} Wb branching fraction of 100 percent. Events consistent with t{bar t} decay are found by identifying jets containing heavy-flavor semileptonic decays to muons. The dominant backgrounds are evaluated directly from the data. Based on 248 candidate events and an expected background of 86.8 {+-} 5.6 events, I measure a production cross section of 8.7 {+-} 1.1{sub -0.8}{sup +0.9} {+-} 0.6 pb, in agreement with the Standard Model.

Grundler, Ulysses A.; /Illinois U., Urbana

2008-05-01T23:59:59.000Z

135

Full page fax print  

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

is the equivalent of 5,700 canisters of liquid waste currently stored in underground tanks at the Savannah River Site, a production rate of 81 canisters per year will complete...

136

SECTION J  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

J-F-1 SECTION J APPENDIX F CRITICAL STAFF Subject Matter Expert Subject Matter Canister Transfer Machine Engineering Waste Package Transfer Trolley Engineering Transport and Emplacement Vehicle Engineering Cask Transfer Trolley Engineering Criticality and Nuclear Engineering Subsurface Thermal Management Engineering Pre-closure Safety Analysis Specialist Waste Package and Drip Shields Engineering Waste Package Closure System Engineering NOG-1 Cranes Engineering Subsurface Design Engineering Structural Seismic Design Engineering Transport, Aging, and Disposal (TAD) interface with repository systems Note: The Contractor shall identify names of at least one individual which shall function in each of the subject matter areas identified above. Qualification requirements for these individuals are

137

SECTION J  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

D-1 D-1 SECTION J APPENDIX D KEY PERSONNEL Name Position Doug Cooper General Manager John Donnell Repository Licensing Lead Al Ebner, PE, PhD Repository Design Lead Steve Piccolo Deputy General Manager Steve White Quality & Performance Assurance Lead George Clare Project Management & Integration Lead Mike Hitchler Preclosure Safety Analysis Lead Contract No.: DE-RW0000005 QA:QA J-D-2 POSITION DESCRIPTIONS OCRWM SPECIFIED KEY PERSONNEL 1. General Manager: Requires 10 years experience as a Senior Manager, responsible for the licensing and/or design and/or operation of a large complex nuclear facility. Must have experience as a

138

SECTION D  

Science Journals Connector (OSTI)

...machinery provided for its operation seem to be well adapted...electrical equipment, (2) operation and product of the furnace...general theory from the fundamental differential equation...in fact per-fectly safe which beam theory would...When possible plans for boiler settings are re-viewed...

G. W. Bissell

1913-04-11T23:59:59.000Z

139

Full bridge converter Transformers and isolated converters  

E-Print Network (OSTI)

parts of the B-H curve are used. Include: push-pull, half-bridge, full-bridge (explained belowFull bridge converter Transformers and isolated converters Most DC power supplies have) cross section of a transformer. (b) Ideal B-H characteristics of the core. (c) B-H characteristics

Knobloch,Jürgen

140

Full Text Glossary  

Energy.gov (U.S. Department of Energy (DOE))

The full-text glossary includes terms used throughout the website and in Biomass Program publications. Terms are listed alphabetically for easy reference. The term index lists all of the terms defined in the glossary.

Note: This page contains sample records for the topic "full section production" 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

Section 19  

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

Observations and Applications of Data Taken with the Observations and Applications of Data Taken with the Cloud Profiling Radar System J. M. Firda, S. M. Sekelsky, S. P. Lohmeier, R. E. McIntosh Microwave Remote Sensing Laboratory, University of Massachusetts Amherst, Massachusetts Introduction During the past year, the University of Massachusetts' Cloud Profiling Radar System (CPRS) team has been active in collecting and processing data. Participation in several field campaigns has produced new and interesting data sets. A classification software was also developed using rule-based techniques and neural networks to identify cloud particles. This paper describes the activities of CPRS from March of 1995 to March of 1996. In the first section, involvement in field experiments is briefly described. This is followed by a

142

Section Number:  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

QA:QA J-E-1 SECTION J APPENDIX E LIST OF APPLICABLE DIRECTIVES Pursuant to the contract clause entitled, "Laws, Regulations, and DOE Directives," the following list of directives is applicable to this contract. List A Pursuant to the contract clause entitled, "Laws, Regulations, and DOE Directives," the Contractor shall comply with the requirements of applicable Federal, State, and local laws and regulations, unless relief has been granted in writing by the appropriate regulatory agency. Omission of any applicable law or regulation from this list does not affect the obligation of the contractor to comply with such law or regulation. Laws & Regulations Title 10 CFR Part 2 Rules of Practice for Domestic Licensing Proceedings and Issuance of Orders

143

SECTION J  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

H-1 H-1 SECTION J APPENDIX H CONTRACT GUIDANCE FOR PREPARATION OF DIVERSITY PLAN This Guidance is to assist the Contractor in understanding the information being sought by the Department for each of the Diversity elements and where these issues may already be addressed in the contract. To the extent these issues are already addressed in the contract, the Contractor need only cross reference the location. Contractor's Workforce The Department's contracts contain clauses on Equal Employment Opportunity (EEO) and Affirmative Action (AA). The Plan may discuss how the contractor has or plans to establish and maintain result-oriented EEO and AA programs in accordance with the requirements of these clauses, and how the contractor's organization includes

144

Section J  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

M-1 M-1 Section J Appendix M Key Design, Licensing and Site Management M&O Milestone Chart Activity Planned Date Develop and Submit CD-2 (25%-30%) 08/2009 Submission of Construction Performance Specifications - Balance of Plant Support Facilities (OCRWM Start of Construction 3/2012) TBD Submission of Construction Performance Specifications - Initial Handling Facility (IHF) (OCRWM Start of Construction for IHF: 9/2013) TBD Submission of Construction Performance Specifications - Wet Handling Facility (WHF) (OCRWM Start of Construction for WHF: 12/2012) TBD Submission of Construction Performance Specifications - Canister Receipt and Closure Facility (CRCF) (OCRWM Start of Construction for CRCF-1: 10/2011) TBD Submission of Construction Performance Specifications - Panel 1

145

Section 64  

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

Do Clouds Mitigate the Biological Effects of Ozone Do Clouds Mitigate the Biological Effects of Ozone Depletion in the Antarctic? P. Ricchiazzi, C. Gautier, and S. Yang Institute for Computational Earth System Science University of California, Santa Barbara Introduction Method Recent studies have shown that biological production in the To distinguish the cloud effect from the strong modulating maritime Antarctic is affected by the ratio of irradiance in the effects of the total ozone, we developed a retrieval technique UVB band to that in the UVA or PAR radiation bands (Smith which simultaneously retrieves column ozone and cloud and Cullen 1995). This result is consistent with the idea that opacity. The retrieval technique is based on the idea that the overall productivity is determined by how well the atmospheric transmission for pass-bands in the UVA and

146

Measurement of the cross section and angular correlations for associated production of a Z boson with b hadrons in pp collisions at s? = 7 TeV  

E-Print Network (OSTI)

corrections to Zbb¯ production with massive bottom quarks at the Fermilab Tevatron, Phys. Rev. D 78 (2008) 074014 [arXiv:0806.0808] [INSPIRE]. [13] F. Febres Cordero, L. Reina and D. Wackeroth, W- and Z-boson production with a massive bottom-quark pair... at the Large Hadron Collider, Phys. Rev. D 80 (2009) 034015 [arXiv:0906.1923] [INSPIRE]. [14] R. Frederix et al., W and Z/?? boson production in association with a bottom-antibottom pair, JHEP 09 (2011) 061 [arXiv:1106.6019] [INSPIRE]. [15] S. Frixione and B...

Baringer, Philip S.; Bean, Alice; Benelli, Gabriele; Kenney, R. P. III; Murray, Michael J.; Noonan, Danny; Sanders, Stephen J.; Stringer, Robert W.; Wood, Jeffrey Scott; Chatrchyan, S.; Khachatryan, V.; Sirunyan, A. M.; Tumasyan, A.; Adam, W.

2013-12-06T23:59:59.000Z

147

State Energy Production Data  

Gasoline and Diesel Fuel Update (EIA)

State Energy Data System State Energy Data System Production Estimates Technical Notes For 1960-2011 Estimates Table of Contents Section 1. Introduction ................................................................................................................... 1 Section 2. Coal ............................................................................................................................... 5 Section 3. Crude Oil ....................................................................................................................... 7 Section 4. Natural Gas (Marketed Production) .............................................................................. 9 Section 5. Renewable Energy and Nuclear Energy ..................................................................... 13

148

Report to the DOE nuclear data committee. [EV RANGE 10-100; CROSS SECTIONS; PHOTONEUTRONS; NEUTRONS; GAMMA RADIATION; COUPLED CHANNEL THEORY; DIFFERENTIAL CROSS SECTIONS; MEV RANGE 01-10; ; CAPTURE; GAMMA SPECTRA; THERMAL NEUTRONS; COMPUTER CALCULATIONS; DECAY; FISSION PRODUCTS; FISSION YIELD; SHELL MODELS; NUCLEAR DATA COLLECTIONS  

SciTech Connect

Topics covered include: studies of (n, charged particle) reactions with 14 to 15 MeV neutrons; photoneutron cross sections for /sup 15/N; neutron radiative capture; Lane-model analysis of (p,p) and (n,n) scattering on the even tin isotopes; neutron scattering cross sections for /sup 181/Ta, /sup 197/Au, /sup 209/Bi, /sup 232/Th, and /sup 238/U inferred from proton scattering and charge exchange cross sections; neutron-induced fission cross sections of /sup 245/Cm and /sup 242/Am; fission neutron multiplicities for /sup 245/Cm and /sup 242/Am; the transport of 14 MeV neutrons through heavy materials 150 < A < 208; /sup 249/Cm energy levels from measurement of thermal neutron capture gamma rays; /sup 231/Th energy levels from neutron capture gamma ray and conversion electron spectroscopy; new measurements of conversion electron binding energies in berkelium and californium; nuclear level densities; relative importance of statistical vs. valence neutron capture in the mass-90 region; determination of properties of short-lived fission products; fission yield of /sup 87/Br and /sup 137/I from 15 nuclei ranging from /sup 232/Th to /sup 249/Cf; evaluation of charged particle data for the ECPL library; evaluation of secondary charged-particle energy and angular distributions for ENDL; and evaluated nuclear structure libraries derived from the table of isotopes. (GHT)

Struble, G.L.; Haight, R.C.

1981-03-01T23:59:59.000Z

149

Measurement of Cross Sections for b Jet Production in Events with a Z Boson in p-anti-p Collisions at s**(1/2) = 1.96-TeV  

SciTech Connect

A measurement of the b jet production cross section is presented for events containing a Z boson produced in p{bar p} collisions at {radical}s = 1.96 TeV, using data corresponding to an integrated luminosity of 2 fb{sup -1} collected by the CDF II detector at the Tevatron. Z bosons are selected in the electron and muon decay modes. Jets are considered with transverse energy E{sub T} > 20 GeV and pseudorapidity |{eta}| < 1.5 and are identified as b jets using a secondary vertex algorithm. The ratio of the integrated Z+b jet cross section to the inclusive Z production cross section is measured to be 3.32 {+-} 0.53(stat:) {+-} 0.42(syst:) x 10{sup -3}. This ratio is also measured differentially in jet E{sub T}, jet {eta}, Z-boson transverse momentum, number of jets, and number of b jets. The predictions from leading order Monte Carlo generators and next-to-leading-order QCD calculations are found to be consistent with the measurements within experimental and theoretical uncertainties.

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

2008-12-01T23:59:59.000Z

150

Section 117  

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

Validation of GOES-7 to a Radiation Budget for April and Validation of GOES-7 to a Radiation Budget for April and July 1994 ARM/IOP Using ScaRaB/Meteor-3/7 Data A. Trishchenko and Z. Li Canada Centre for Remote Sensing Ottawa, Ontario, Canada Abstract Data from the ScaRaB radiometer flown on board the Meteor- 3/7 satellite were employed for validating a TOA Earth radiation budget product generated from GOES-7 for the Atmospheric Radiation Measurement (ARM) Program. Com- parisons were made between coincident and collocated short- wave and long-wave radiative quantities derived from ScaRaB and GOES sensors over the Southern Great Plains (SGP) Cloud and Radiation Testbed (CART) site in Oklahoma, U.S.A., during April and July 1994. Calibrations for both visible and infrared window channels appear to be adequate, but narrow- to broad-band conversion of short-wave measure-

151

A Measurement of the production cross section of top-antitop pairs in proton-antiproton collisions at a center of mass of 1.96 TeV using secondary vertex b-tagging.  

SciTech Connect

A measurement of the t{bar t} pair production cross section is presented using 162 pb{sup -1} of data collected by the CDF experiment during Run II at the Tevatron. t{bar t} events in the lepton+jets channel are isolated by identifying electrons and muons, reconstructing jets and transverse missing energy, and identifying b jets with a secondary vertex tagging algorithm. The efficiency of the algorithm is measured in a control sample using a novel technique that is less dependent on the simulation. For a top quark mass of 175 GeV/c{sup 2}, a cross section of {sigma}{sub t{bar t}} = 5.6{sub -1.1}{sup +1.2}(stat.){sub -0.6}{sup +0.9}(syst.)pb is measured.

Bachacou, Henri; /UC, Berkeley; ,

2004-12-01T23:59:59.000Z

152

Differential production cross section of Z bosons as a function of transverse momentum at root s=1.8 TeV  

E-Print Network (OSTI)

of California, Irvine, California 92697 24 University of California, Riverside, California 92521 25 Florida State University, Tallahassee, Florida 32306 26 University of Hawaii, Honolulu, Hawaii 96822 27 Fermi National Accelerator Laboratory, Batavia, Illinois... b )byexpH208512S H20849b,Q H20850H20852. fications required by changes in selection criteria. The 2794 max NP PACS numbers: 14.70.Hp, 13.38.Dg, 13.85.Qk We report a new measurement [1,2] of the inclusive differential cross section of the Z boson...

Baringer, Philip S.

2000-03-01T23:59:59.000Z

153

Office Buildings - Full Report  

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

Office Buildings - Full Report Office Buildings - Full Report file:///C|/mydocs/CBECS2003/PBA%20report/office%20report/office_pdf.html[9/24/2010 3:33:25 PM] Although no one building type dominates the commercial buildings sector, office buildings are the most common and account for more than 800,000 buildings or 17 percent of total commercial buildings. Offices comprised more than 12 billion square feet of floorspace, 17 percent of total commercial floorspace, the most of any building type. Types of Office Buildings The 2003 CBECS Detailed Tables present data for office buildings along with other principal building activities (see Detailed Tables B13 and B14, for example). Since office buildings comprise a wide range of office-related activities, survey respondents were presented with a

154

Full Hybrid: Overview  

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

highlighted Stop/Start button banner graphic: blue bar highlighted Stop/Start button banner graphic: blue bar subbanner graphic: gray bar Overview Button highlighted Starting button Low Speed button Cruising button Passing button Braking button Stopped button OVERVIEW Full hybrids use a gasoline engine as the primary source of power, and an electric motor provides additional power when needed. In addition, full hybrids can use the electric motor as the sole source of propulsion for low-speed, low-acceleration driving, such as in stop-and-go traffic or for backing up. This electric-only driving mode can further increase fuel efficiency under some driving conditions. stage graphic: vertical blue rule Main stage: See through car with battery, engine, generator, power split device, and electric motor visible. The car is stopped at an intersection.

155

Full Hybrid: Overview  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

highlighted Starting button Low Speed button Cruising button Passing button Braking button Stopped button highlighted Starting button Low Speed button Cruising button Passing button Braking button Stopped button OVERVIEW Full hybrids use a gasoline engine as the primary source of power, and an electric motor provides additional power when needed. In addition, full hybrids can use the electric motor as the sole source of propulsion for low-speed, low-acceleration driving, such as in stop-and-go traffic or for backing up. This electric-only driving mode can further increase fuel efficiency under some driving conditions. stage graphic: vertical blue rule Main stage: See through car with battery, engine, generator, power split device, and electric motor visible. The car is stopped at an intersection. Main stage: See through car with battery, engine, generator, power split device, and electric motor visible. The car is stopped at an intersection.

156

Mesure de la section efficace de production de paires de quarks top dans l'etat final di-electron avec les donnees collectees par l'experience D0 au RunIIa  

SciTech Connect

The top quark has been discovered in 1995 by CDF and D0 collaborations in proton-antiproton collisions at the Tevatron. The amount of data recorded by both experiments makes it possible to accurately measure the properties of this very massive quark. This thesis is devoted to the measurement of the top pair production cross-section via the strong interaction, in a final state composed of two electrons, two particle jets and missing transverse energy. It is based on a 1 fb{sup -1} data set collected by the D0 experiment between 2002 and 2006. The reconstruction and identification of electrons and jets is of major importance in this analysis, and have been studied in events where a Z boson is produced together with one or more jets. The Z+jets process is indeed the dominant physics background to top pair production in the dielectron final state. The primary goal of this cross-section measurement is to verify Standard Model predictions. In this document, this result is also interpreted to indirectly extract the top quark mass. Moreover, the cross-section measurement is sensitive to new physics such as the existence of a charged Higgs boson. The selection established for the cross-section analysis has been used to search for a H{sup +} boson lighter than the top quark, where the latter can decay into a W{sup +} or H{sup +} boson and a b quark. The model that has been studied makes the assumption that the H{sup +} boson can only decay into a tau lepton and a neutrino.

Martin Dit Latour, Bertrand; /LPSC, Grenoble

2008-09-01T23:59:59.000Z

157

Measurement of the Single Top Quark Production Cross Section and |V[subscript tb]| in Events with One Charged Lepton, Large Missing Transverse Energy, and Jets at CDF  

E-Print Network (OSTI)

We report a measurement of single top quark production in proton-antiproton collisions at a center-of-mass energy of ?s = 1.96??TeV using a data set corresponding to 7.5??fb[superscript -1] of integrated luminosity collected ...

Aaltonen, T.

158

Section 36  

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

7 7 Cloud and Aerosol Height Distribution Retrieval and Analysis Employing Continuous Operation Lidar Data J. D. Spinhirne, D. L. Hlavka and V. S. Scott NASA/Goddard Space Flight Center Greenbelt, Maryland A. E. Galbraith and J. A. Reagan University of Arizona Tucson, Arizona Introduction Instrument New technology now permits ground-based lidar to operate The basis of the MPL design is the use of lasers with high full time and profile all significant aerosol and cloud structure pulse repetition frequencies (PRF) and low pulse energies. of the atmosphere up to the limit of signal attenuation. Such When highly efficient optics, filters, and detectors are used, it systems are in operation at U.S. Department of Energy (DOE) is possible to obtain profiling of all significant cloud and aero-

159

Improved half-life measurement of 224Pa and its 209Bi(18O,3n)224Pa production cross section  

Science Journals Connector (OSTI)

224Pa was produced via the 209Bi(18O,3n) reaction at the Lawrence Berkeley National Laboratory 88-Inch Cyclotron and the half-life was determined to be 850±20 ms by measuring its alpha decay using our rotating wheel system. Our value is consistent with a previously reported half-life of 950±150 ms for 224Pa produced via the 205Tl(22Ne,3n) reaction, but its much more precise. The cross section for the 209Bi(18O,3n)224Pa reaction was measured to be 0.5±0.1 mb for 87–89 MeV 18O5+ projectiles incident on the target.

P. A. Wilk; K. E. Gregorich; M. B. Hendricks; M. R. Lane; D. M. Lee; C. A. McGrath; D. A. Shaughnessy; D. A. Strellis; E. R. Sylwester; D. C. Hoffman

1997-09-01T23:59:59.000Z

160

Measurement of the Single Top Quark Production Cross Section and |Vtb| in Events with One Charged Lepton, Large Missing Transverse Energy, and Jets at CDF  

E-Print Network (OSTI)

We report a measurement of single top quark production in proton-antiproton collisions at a center-of-mass energy of \\sqrt{s} = 1.96 TeV using a data set corresponding to 7.5 fb-1 of integrated luminosity collected by the Collider Detector at Fermilab. We select events consistent with the single top quark decay process t \\to Wb \\to l{\

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

2014-07-15T23:59:59.000Z

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161

Measurement of the Single Top Quark Production Cross Section and |Vtb| in Events with One Charged Lepton, Large Missing Transverse Energy, and Jets at CDF  

E-Print Network (OSTI)

We report a measurement of single top quark production in proton-antiproton collisions at a center-of-mass energy of \\sqrt{s} = 1.96 TeV using a data set corresponding to 7.5 fb-1 of integrated luminosity collected by the Collider Detector at Fermilab. We select events consistent with the single top quark decay process t \\to Wb \\to l{\

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

2015-01-25T23:59:59.000Z

162

t anti-t production cross section measurement using soft electron tagging in p anti-p collisions at s**(1/2) = 1.96-TeV  

SciTech Connect

We measure the production cross section of t{bar t} events in p{bar p} collisions at {radical}s = 1.96 TeV. The data was collected by the CDF experiment in Run 2 of the Tevatron accelerator at the Fermi National Accelerator Laboratory between 2002 and 2007. 1.7 fb{sup -1} of data was recorded during this time period. We reconstruct t{bar t} events in the lepton+jets channel, whereby one W boson - resulting from the decay of the top quark pairs - decays leptonically and the other hadronically. The dominant background to this process is the production of W bosons in association with multiple jets. To distinguish t{bar t} from background, we identify soft electrons from the semileptonic decay of heavy flavor jets produced in t{bar t} events. We measure a cross section of {sigma}{sub p{bar p}} = 7.8 {+-} 2.4(stat) {+-} 1.6(syst) {+-} 0.5(lumi).

Chou, John Paul; /Harvard U.

2008-09-01T23:59:59.000Z

163

Full Hybrid: Starting  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

highlighted Low Speed button Cruising button Passing button Braking button Stopped button highlighted Low Speed button Cruising button Passing button Braking button Stopped button STARTING When a full hybrid vehicle is initially started, the battery typically powers all accessories. The gasoline engine only starts if the battery needs to be charged or the accessories require more power than available from the battery. stage graphic: vertical blue rule Main stage: See through car with battery, engine, generator, power split device, and electric motor visible. the car is stopped at an intersection. Main stage: See through car with battery, engine, generator, power split device, and electric motor visible. the car is stopped at an intersection. Battery (highlighted): The battery stores energy generated from the gasoline engine or, during regenerative braking, from the electric motor. Since the battery powers the vehicle at low speeds, it is larger and holds much more energy than batteries used to start conventional vehicles. Main stage: See through car with battery, engine, generator, power split device, and electric motor visible. the car is stopped at an intersection. Main stage: See through car with battery, engine, generator, power split device, and electric motor visible. the car is stopped at an intersection.

164

Preparations for Measurement of Electroweak Boson Production Cross-Sections using the Electron Decay Modes, with the Compact Muon Solenoid Detector  

E-Print Network (OSTI)

The Compact Muon Solenoid was designed to make discoveries at the TeV scale : to elucidate the nature of electroweak symmetry breaking and to search for physics beyond the Standard Model. For any such discovery to be credible, it must first be demonstrated that the CMS detector is understood. One mechanism to make this demonstration is to measure “standard candle” processes, such as W and Z production. This thesis describes preparations undertaken to make these measurements using the electron decay modes, with an integrated luminosity of 10 inverse picobarns of collision data. The energy resolution of the electromagnetic calorimeter was measured in test beam data. An improved method of deriving the optimised weights necessary for amplitude reconstruction is described. The measurement of electron charge using tracks is impaired by the electron showering in the tracker material. A novel charge measurement technique that is complementary to the existing method was assessed. Missing transverse energy is a pow...

Wardrope, D R

2009-01-01T23:59:59.000Z

165

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Variation in cross- sectional area A with tide is ignored (thereby neglecting ... neap variations in tidal energy and atmospheric forcing None- theless, over a time ...

166

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mary production since we would expect ... average oxygen production was the same as in the upper zones. ... rubber ball closures that eliminate malfunc-.

1999-12-19T23:59:59.000Z

167

Determination of the top-quark pole mass and strong coupling constant from the t t-bar production cross section in pp collisions at sqrt(s) = 7 TeV  

E-Print Network (OSTI)

The inclusive cross section for top-quark pair production measured by the CMS experiment in proton-proton collisions at a center-of-mass energy of 7 TeV is compared to the QCD prediction at next-to-next-to-leading order with various parton distribution functions to determine the top-quark pole mass, mtpole, or the strong coupling constant, alphaS. With the parton distribution function set NNPDF2.3, a pole mass of 176.7 +3.0 -2.8 GeV is obtained when constraining alphaS at the scale of the Z boson mass, mZ, to the current world average. Alternatively, by constraining mtpole to the latest average from direct mass measurements, a value of alphaS(mZ) = 0.1151 +0.0028 -0.0027 is extracted. This is the first determination of alphaS using events from top-quark production.

CMS Collaboration

2014-08-20T23:59:59.000Z

168

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Production of the compounds ... leased. The rates of CHBr3 and C2H2Br2 production were neg- ... with PTFE-coated butyl rubber seals were equilibrated in the.

1999-07-01T23:59:59.000Z

169

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methanogenesis was the predominant CH4 production pathway. Methods. Sampling ...... hydrogen from paddy field rice roots and soil bacterial enrichments

2009-02-23T23:59:59.000Z

170

Measurement of the top - anti-top Production Cross Section at s**(/1/2) = 1.96-TeV in the e + jets Final State of proton anti-proton Collisions at the Tevatron  

SciTech Connect

We discuss the measurement of the cross section for t{bar t} production in p{bar p} collisions at {radical}s = 1.96 TeV in e+jets final states observed at the D0 experiment at the Fermilab Tevatron. Our result is based on data collected from the June 2002 to September 2003 period of Run II of the p{bar p} Collider. In the Standard Model, the top quark is expected to decay mainly into a W boson and a b quark. The W boson can decay subsequently into a lepton and its neutrino or a q{bar q} quark-antiquark pair. In this thesis, we focus on the e{sup +} {nu}{sub e} or e{sup -} {bar {nu}}{sub e} decays of one of the W bosons and the q{bar q} decays of the other W boson in t{bar t} final states. The b, q and q' quarks appear as jets of particles in the detector, thereby defining the e+jets final state. We present two methods used for performing this measurement. The first method is based on a Random Grid Search (RGS) that minimizes the uncertainty on the extracted cross section. The variables used in the search take advantage of differences between expected background and signal processes to obtain the yield of t{bar t} events. The second method uses a Neural Network (NN) procedure that discriminates signal from background through the application of a NN trained on simulated t{bar t} signal and W+jets background events. The preliminary results presented in this thesis for inclusive t{bar t} production are {sigma}{sub p{bar p} {yields} t{bar t} + x} of 7.9{sub -2.4}{sup +2.6}(stat) {sub -2.3}{sup +2.2}(syst) {+-} 0.5 (L) pb for the NN analysis, where the uncertainties correspond to contributions from statistical and systematic sources and from the uncertainty on luminosity. Our measurements are consistent with each other, and are within error of the value of 6.77 {+-} 0.42 pb expected in the Standard Model.

Cho, DooKee; /Rochester U.; ,

2005-02-01T23:59:59.000Z

171

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directly from municipal wastewater outfalls and pulp mills. The total flux of organic ... of summer wind storms could have increased primary production. Applying ...

2013-12-23T23:59:59.000Z

172

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... seawater with cium phosphates such as apatites and phos- calcium phosphates in two regions of the phorites; an ion product which in its. North Pacific Ocean.

2000-01-13T23:59:59.000Z

173

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recycling can perpetuate nitrogen deficiency in highly-productive reservoirs .... and internal recycling (RCYC) through biological organic ...... wastewater. 21st ed

2014-10-20T23:59:59.000Z

174

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Influence of salinity and temperature on the growth and production of a freshwater .... sonal gradient of salinity and a seasonal gradient of temper- ature.

2001-04-16T23:59:59.000Z

175

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Based on floating-sediment-trap data, export production to the aphotic zone was about 12–20% of the GPP; the rest accumulated as dissolved organic carbon ...

2008-07-31T23:59:59.000Z

176

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the holdfast to the floating productive region where blades are buoyed at the water surface by air bladders (Lobban. 1978; Kain 1982; Koehl and Alberte 1988

2001-04-16T23:59:59.000Z

177

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Meiofauna versus macrofauna: Secondary production of invertebrates in a .... regressions and conversion factors (see Web Appendix, Table ..... Ph.D. thesis.

2009-02-23T23:59:59.000Z

178

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production of L. quudripunctata from its maximum in July 1956 was prolonged and extended ..... factors and thp, life his- tory of Limnoria lignorum at St. Andrcws

179

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Experimental test of bacteria–phytoplankton coupling in the Southern Ocean ... generate a gradient of phytoplankton biomass and production in order to test the

2005-10-25T23:59:59.000Z

180

Technical Data to Justify Full Burnup Credit in Criticality Safety Licensing Analysis  

SciTech Connect

Enercon Services, Inc. (ENERCON) was requested under Task Order No.2 to identify scientific and technical data needed to benchmark and justify Full Burnup Credit, which adds 16 fission products and 4 minor actinides1 to Actinide-Only burnup credit. The historical perspective for Full Burnup Credit is discussed, and interviews of organizations participating in burnup credit activities are summarized as a basis for identifying additional data needs and making recommendation. Input from burnup credit participants representing two segments of the commercial nuclear industry is provided. First, the Electric Power Research Institute (EPRI) has been very active in the development of Full Burnup Credit, representing the interests of nuclear utilities in achieving capacity gains for storage and transport casks. EPRI and its utility customers are interested in a swift resolution of the validation issues that are delaying the implementation of Full Burnup Credit [EPRI 2010b]. Second, used nuclear fuel storage and transportation Cask Vendors favor improving burnup credit beyond Actinide-Only burnup credit, although their discussion of specific burnup credit achievements and data needs was limited citing business sensitive and technical proprietary concerns. While Cask Vendor proprietary items are not specifically identified in this report, the needs of all nuclear industry participants are reflected in the conclusions and recommendations of this report. In addition, Oak Ridge National Laboratory (ORNL) and Sandia National Laboratory (SNL) were interviewed for their input into additional data needs to achieve Full Burnup Credit. ORNL was very open to discussions of Full Burnup Credit, with several telecoms and a visit by ENERCON to ORNL. For many years, ORNL has provided extensive support to the NRC regarding burnup credit in all of its forms. Discussions with ORNL focused on potential resolutions to the validation issues for the use of fission products. SNL was helpful in ENERCON's understanding of the difficult issues related to obtaining and analyzing additional cross section test data to support Full Burnup Credit. A PIRT (Phenomena Identification and Ranking Table) analysis was performed by ENERCON to evaluate the costs and benefits of acquiring different types of nuclear data in support of Full Burnup Credit. A PIRT exercise is a formal expert elicitation process with the final output being the ranking tables. The PIRT analysis (Table 7-4: Results of PIRT Evaluation) showed that the acquisition of additional Actinide-Only experimental data, although beneficial, was associated with high cost and is not necessarily needed. The conclusion was that the existing Radiochemical Assay (RCA) data plus the French Haut Taux de Combustion (HTC)2 and handbook Laboratory Critical Experiment (LCE) data provide adequate benchmark validation for Actinide-Only Burnup Credit. The PIRT analysis indicated that the costs and schedule to obtain sufficient additional experimental data to support the addition of 16 fission products to Actinide-Only Burnup Credit to produce Full Burnup Credit are quite substantial. ENERCON estimates the cost to be $50M to $100M with a schedule of five or more years. The PIRT analysis highlights another option for fission product burnup credit, which is the application of computer-based uncertainty analyses (S/U - Sensitivity/Uncertainty methodologies), confirmed by the limited experimental data that is already available. S/U analyses essentially transform cross section uncertainty information contained in the cross section libraries into a reactivity bias and uncertainty. Recent work by ORNL and EPRI has shown that a methodology to support Full Burnup Credit is possible using a combination of traditional RCA and LCE validation plus S/U validation for fission product isotopics and cross sections. Further, the most recent cross section data (ENDF/B-VII) can be incorporated into the burnup credit codes at a reasonable cost compared to the acquisition of equivalent experimental data. ENERCON concludes that even with the cos

Enercon Services, Inc.

2011-03-14T23:59:59.000Z

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181

Section 49 - Business  

Science Journals Connector (OSTI)

The category entitled Business includes milestones involving companies and other business organizations with energy-related activities, and also business ventures in energy by individual entrepreneurs. This subject area is closely related to the preceding section Economics. The first significant energy business involved the mining, transportation, and sale of coal. The coal industry originated in Great Britain, especially in the Newcastle area of northern England. (This became the source of the expression “carrying coals to Newcastle” to describe a needless activity, since coal already could be found there in such abundance.) The U.S. coal business began in the mid 1700s, and was located mainly in the Appalachian region, where it still exists as a major industry today. The next major energy business to emerge in the U.S. was water power, in New Jersey in the late 1700s. This was followed by the gas lighting industry, which had begun in Britain in 1812 and then developed in the U.S. shortly afterward. Another notable energy business of this time was the whale oil industry, in which whales were hunted for use of their oil as a lighting fuel. This had a remarkable career arc as a business. It came of age in New England in the 1820s, peaked in the 1840s, and was virtually defunct by the end of the 1860s. Other fuel sources had replaced whale oil, chiefly kerosene, a cheaper and more easily obtainable product. The oil business had its formal beginnings in the 1850s in the U.S. and Romania. The year 1870 then saw a significant milestone in the business with the creation of the Standard Oil Company by John D. Rockefeller and colleagues. Three years later, the brothers Robert and Ludwig Nobel (siblings of the inventor Alfred) set up a company to exploit the oil riches of Baku, Azerbaijan. Baku’s oil industry would become the largest in the world in the late nineteenth century. Also in the 1850s, the first commercial natural gas company was formed in Fredonia, New York. The 1870s marked the beginning of another huge energy business, the commercial supply of electric power. The founding of Thomas Edison’s Edison Electric Light Company (1879) was the seminal event in this respect. Thus by the end of the 1870s, the four large energy supply industries of the U.S.—coal, oil, gas, and electricity—were all in full operation. The general availability of energy supply from oil and electricity led to the development of a huge energy-related business, the automobile industry. This began in the 1890s, with the founding of Daimler Motors in Germany being the most significant event. Electric car companies would enjoy success from this early period of the 1890s up until the early 1920s, when gasoline-powered cars eclipsed their sale. The first step in the demise of electric streetcar companies also came in the early 1920s when the General Motors Company began a campaign to replace street cars with gasoline-powered vehicles. A major development in the energy business in the 20th century was the effort to produce and market oil from Middle Eastern sources. This began in earnest in the 1930s when Western oil companies were granted concessions to begin oil prospecting in Saudi Arabia and Kuwait. Eventually, these two nations would take over their oil industry and control its revenue themselves, as would various other oil-exporting nations (e.g., Venezuela, Nigeria). The influence of Western oil companies was at its peak in the mid 1970s when the popular media referred to the “Seven Sisters” that then dominated the business: Exxon, Mobil, Socal (Chevron), Texaco, Gulf, British Petroleum, and Royal Dutch/Shell. These companies controlled about 85 percent of the world’s oil reserves. Their influence on the global market would soon diminish due to the importance of OPEC and the existence of various state-owned oil companies as noted above. Nevertheless, a contemporary list of the ten largest global companies still includes all of the Seven Sisters, either as independent companies or as part of a merger with another of this group. The

Cutler J. Cleveland; Christopher Morris

2014-01-01T23:59:59.000Z

182

Contract Mapper Full Symbology List  

E-Print Network (OSTI)

Contract Mapper Full Symbology List Colour symbology Operational Support Unit 15th October 2007 Main Road Management Area Other Fell Thin Compartments Sub-Compartments Contract Buffer Order

183

Contract Mapper Full Symbology List  

E-Print Network (OSTI)

Contract Mapper Full Symbology List Black & White symbology Operational Support Unit 15th October Compartments Sub-Compartments # # ## Management Area Fell Thin Contract Buffer Other #12;

184

Hypernuclear Production in High-Energy Nuclear Collisions  

Science Journals Connector (OSTI)

......Fermi motion on the production cross sections...Fermi-average method as shown in Eq. (A7). The primary production cross sections...functions of a hydrogen-like atom in...Table IV. s- atom production cross sections......

Mitsuo Sano; Masamichi Wakai

1994-03-01T23:59:59.000Z

185

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Further, hydrogen peroxide photoproduction from UDOM ... photo-Fenton chemistry could not explain the increase in hydrogen peroxide production quantum yields (Qhp) .... Methods. Sample collection and handling—Water samples used in.

2008-12-10T23:59:59.000Z

186

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Gross and net O2 production between May 1996 and February 1999 was determined in bottle incubation exper- iments with ... of these methods is their inability to measure the rate of O2 .... hypolimnion (mostly hydrogen sulfide and ammonia).

2001-12-26T23:59:59.000Z

187

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erating organic-bound nutrients to fuel primary production .... portant pathway, accounting for up to 90% of the total car- .... by flow injection/diffusion cell analysis with conductivity ...... Spectrophotometric determination of hydrogen sul-.

2004-10-08T23:59:59.000Z

188

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benthic primary production challenge this assumption. Ca- hoon and Cooke ...... time-integrated isotopic signatures of the diet that are re- corded in the ... Sustainable development in the. Seto Inland Sea ... Differences in energy flow through ...

2002-04-18T23:59:59.000Z

189

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The spring, with its rapidly increasing temperature, is an important period for the ... productive rates and resource supply but also to increased feeding rates from ...... Phytoplankton control by grazing zooplankton: A study on the spring ...

2007-02-06T23:59:59.000Z

190

e00053-12.full.pdf  

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

10.1128/mBio.00053-12. 10.1128/mBio.00053-12. 3(2): . mBio . Temperature-Dependent Product Formation Engineering a Hyperthermophilic Archaeon for 2012. Mirko Basen, Junsong Sun and Michael W. W. Adams Product Formation Archaeon for Temperature-Dependent Engineering a Hyperthermophilic http://mbio.asm.org/content/3/2/e00053-12.full.html Updated information and services can be found at: REFERENCES http://mbio.asm.org/content/3/2/e00053-12.full.html#ref-list-1 This article cites 28 articles, 13 of which can be accessed free at: CONTENT ALERTS more>> article), Receive: RSS Feeds, eTOCs, free email alerts (when new articles cite this http://journals.asm.org/subscriptions/ To subscribe to another ASM Journal go to: http://mbio.asm.org/misc/contentdelivery.xhtml Information about Print on Demand and other content delivery options:

191

EPAct Section 242 Comments and DOE Responses | Department of...  

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

242 Program Draft Guidance for Section 242 of the Energy Policy Act of 2005 - Hydroelectric Production Incentive Program - July 2014 2014 Water Power Program Peer Review...

192

Full Rank Rational Demand Systems  

E-Print Network (OSTI)

as a nominal income full rank QES. R EFERENCES (A.84)S. G. Donald. “Inferring the Rank of a Matrix. ” Journal of97-102. . “A Demand System Rank Theorem. ” Econometrica 57 (

LaFrance, Jeffrey T; Pope, Rulon D.

2006-01-01T23:59:59.000Z

193

Section 42: Monitoring  

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

using techniques that do not jeopardize the containment of waste in the disposal system. Ten monitoring parameters were identified in an analysis performed to fulfill the section...

194

Full Circle Developments Inc | Open Energy Information  

Open Energy Info (EERE)

Full Circle Developments Inc Full Circle Developments Inc Jump to: navigation, search Name Full Circle Developments Inc Place Plymouth, Michigan Zip 48170 Sector Renewable Energy Product Private Michigan-based clean energy project developer, with focus on brownfield site biofuel projects that are powered by renewable energy. Coordinates 43.75681°, -87.984809° 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":43.75681,"lon":-87.984809,"alt":0,"address":"","icon":"","group":"","inlineLabel":"","visitedicon":""}]}

195

Cross-Section Measurement near 50 Bev  

Science Journals Connector (OSTI)

An experiment to measure the cross section for high-energy cosmic-ray protons and neutrons to interact with the Fe nucleus has been carried out at 3250 m elevation. The detector had a relatively good energy resolution, and was designed to select nucleons in the vicinity of 50 Bev. The purpose was to obtain a single interaction cross section with good accuracy in order to compare it with results obtained with accelerators in the 1- to 5-Bev region. This comparison yields a value for the elementary meson-production cross section [the average of ?(pp) and ?(np)] near 50 Bev. The Fe results are: neutrons, ?Fe=0.61±0.03 barn; protons, ?Fe=0.61±0.04 barn. The corresponding average nucleon-nucleon "inelastic" (presumably meson production) cross section is ?nucleon=21±4 millibarns.

A. E. Brenner and Robert W. Williams

1957-06-01T23:59:59.000Z

196

Measuring the top anti-t Production Cross-Section in the Electron + Jets Channel in Proton - Anti-proton Collisions at s**(1/2) = 1.96-TeV with the D0 Detector at the Tevatron: A Monte Carlo Study  

SciTech Connect

The measurement of the t{bar t} production cross section at {radical}s = 1.96 TeV using the final state with an electron and jets is studied with Monte Carlo event samples. All methods used in the real data analysis to measure efficiencies and to estimate the background contributions are examined. The studies focus on measuring the electron reconstruction efficiencies as well as on improving the electron identification and background suppression. With a generated input cross section of 7 pb the following result is obtained: {sigma}{sub t{bar t}} = (7 {+-} 1.63(stat){sub -1.14}{sup +0.94} (syst)) pb.

Park, Su-Jung; /Bonn U.

2004-02-01T23:59:59.000Z

197

14655 Section I  

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

with the same force and effect as if they were given in full text. Upon request, the Contracting Officer will make their full text available. Also, the full text of a clause may be...

198

Section I: Contract Clause  

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

with the same force and effect as if they were given in full text. Upon request, the Contracting Officer will make their full text available. Also, the full text of a clause may be...

199

17O Cross Section  

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

p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 2010SE11 17O(p, ): nuclear excitation function 0 - 0.7 1 06222011 1973RO03...

200

EMPLOYMENT Advertising Section  

Science Journals Connector (OSTI)

EMPLOYMENT Advertising Section ... "Situations wanted" advertisements will be classified by type of chemistry (analytical, biochemistry, etc.). ... State ACS membership status and mail advertisements to Chemical & Engineering News, Classified Advertising, 25 Sylvan Rd. ...

1981-09-14T23:59:59.000Z

Note: This page contains sample records for the topic "full section production" from the National Library of EnergyBeta (NLEBeta).
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201

11B Cross Section  

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p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 2004RO27, 2004SP03 11B(p, ): deduced , S-factor Ecm 0 - 1 X4 11072012...

202

18O Cross Section  

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

, X) (Current as of 05142012) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 2003DA19 18O(, ): deduced resonance strengths 470 - 770 keV X4 02132012...

203

12C Cross Section  

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

, X) (Current as of 05142012) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 2009MA70 12C(, 0): 0 - 2.27 X4 05012012 1997KU18 12C(, ): analyzed...

204

7Li Cross Section  

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

, X) (Current as of 05142012) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 2004GY02 7Li(, ): deduced absolute resonance strengths 810 - 820 keV X4 02...

205

7Li Cross Section  

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

p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1997GO13 7Li(pol. p, ): total , S-factor for capture to third-excited state 0 -...

206

4He Cross Section  

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

4He(, X) (Current as of 05142012) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 1978HI04 4He(, ): elastic scattering excitation function 32.6 - 35.4 ...

207

15N Cross Section  

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

, X) (Current as of 05142012) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 2002WI18 15N( ): 461 - 2642 keV X4 09122011 1997WI12 15N( ): 0.65...

208

6Li Cross Section  

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

, X) (Current as of 01212015) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 1985NE05 6Li(, ): thick target yield resonance X4 02152012 1966FO05...

209

19F Cross Section  

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

, X) (Current as of 01212015) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 2008UG01 19F(, p): yield curves, 792 - 1993 keV X4 09142011 2005UG04...

210

9Be Cross Section  

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

, X) (Current as of 01212015) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 1994WR01 9Be(, n): , thick target yield, deduced S-factor Ecm 0.16 - 1.87...

211

11B Cross Section  

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

, X) (Current as of 01212015) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 1991WA02 11B(, n): thick-target yield of E 411, 605 and 606 keV resonance...

212

20Ne Cross Section  

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

, X) (Current as of 01212015) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 1983SC17 20Ne(, ): deduced S-factor of capture 0.55 - 3.2 X4 09152011...

213

10B Cross Section  

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

, X) (Current as of 01212015) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 1992MC03 10B(, ): relative to Rutherford scattering 1 - 3.3 X4 05022012...

214

3He Cross Section  

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

, X) (Current as of 05142012) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 1982KR05 3He(, ): Ecm 107 - 1266 keV X4 01052012 1969NA24 3He(, ):...

215

14N Cross Section  

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

4N(, X) (Current as of 05142012) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 1971CO27 14N(, ): thick target yield 0.5 - 1.2 1 08042011 2000GO43...

216

Cross-Section Measurement  

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

Cross-Section Measurement of 2 H(n,np)n at 16 MeV in Symmetric Constant Relative Energy Configurations Alexander Hoff Couture A dissertation submitted to the faculty of the...

217

NNLO W Pair Production at the LHC: Status Report  

E-Print Network (OSTI)

We discuss the result with full mass dependence for the virtual NNLO QCD corrections to the W boson pair production in the quark-anti-quark annihilation channel. We also report on our progress regarding the treatment of the double-real radiative corrections which, along with the virtual-real corrections, are the other two necessary ingredients for a theoretical prediction of the total cross section for W+ W- production to NNLO accuracy.

Grigorios Chachamis

2013-12-16T23:59:59.000Z

218

Section 999 Program Library | Department of Energy  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Science & Innovation » Oil & Gas » Offshore Drilling » Section Science & Innovation » Oil & Gas » Offshore Drilling » Section 999 Program Library Section 999 Program Library Cost-Shared Program Publications October 2, 2013 URTAC Meeting - October 2013 October 2, 2013 UDAC Meeting - October 2013 September 10, 2013 Draft 2014 Annual Plan More Ultra-Deepwater Advisory Committee (UDAC) Activities and Products November 27, 2013 UDAC Meeting - December 2013 November 20, 2013 UDAC Meeting - December 2013 November 18, 2013 UDAC Meeting - September 2013 More Unconventional Resources Technology Advisory Committee (URTAC) Activities and Products November 27, 2013 URTAC Meeting - December 2013 November 18, 2013 URTAC Meeting - December 2013 November 18, 2013 URTAC Meeting - December 2013 More Stay Connected Fossil Energy on Facebook Fossil Energy on Twitter Sign up for NewsAlerts Fossil Energy RSS Feeds

219

POLICY SECTIONS POLICY OFFICE  

E-Print Network (OSTI)

POLICY SECTIONS POLICY OFFICE POLICIES FORMS PROCEDURES UNIVERSITY POLICY #12;guide to WRITING POLICIES Administrative policies align opera- tions, set behavior expectations across the University system and communicate policy roles and responsibilities. You, as the policy owner or writer, have the important task

Minnesota, University of

220

16O Cross Section  

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

6O(, X) (Current as of 05142012) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 1971TO06 16O(, ): 0.85 - 1.8 X4 09152011 1953CA44 16O(, ): 0.94...

Note: This page contains sample records for the topic "full section production" from the National Library of EnergyBeta (NLEBeta).
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221

14C Cross Section  

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

4C(p, X) (Incomplete) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1969SI04 14C(p, ): -rays yield for 230 - 690 keV E 2.8 MeV 08152013 1990GO25 14C(p,...

222

6Li Cross Section  

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

6Li(p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 2004TU02 6Li(p, ): coincidence yields, deduced S-factors low 1, S-factors from...

223

9Be Cross Section  

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

p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1997ZA06 9Be(p, ), (p, d): S-factor 16 - 390 keV X4 01232013 1973SI27 9Be(p,...

224

18O Cross Section  

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

p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 2008LA06 18O(p, ): deduced S-factor Ecm 0 - 1.5 46 12032012 1990CH32...

225

15N Cross Section  

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

p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1990WA10 15N(p, n): < 30 X4 04262012 1982RE06 15N(p, ): 78 - 810 keV X4...

226

11C Cross Section  

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

C(p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 2003LI51 11C(p, ): deduced S-factor low X4 09122011 2003TA02 11C(p, ):...

227

19F Cross Section  

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

p, X) (Incomplete) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1990WA10 19F(p, n): < 30 X4 04262012 2008CO03 19F(p, ): Ecm 200 - 700 keV X4 0514...

228

4He Cross Section  

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

p, X) (Incomplete) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1974KR07 4He(p, p): 0.5 - 3 X4 10232014 2004PU02 4He(p, p): ( 128.7) 1.2 - 5.2 X4 10...

229

3He Cross Section  

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

p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1980BE06 3He(pol. p, p): 0.3 - 1.0 X4 10302014 1964IM03 3He(p, ): deduced ...

230

17O Cross Section  

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

, X) (Current as of 05142012) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 1973BA10 17O(, n): neutron yields with target thickness 0.9 - 5.3 2.5 keV, 6...

231

3H Cross Section  

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

H(, X) (Current as of 05142012) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 2001TO07 3H(, ): deduced S-factor Ecm 0.05 - 0.8 X4 01092012 1994BR25...

232

14N Cross Section  

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

p, X) (Incomplete) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 2003MU12 14N(p, ): deduced astrophysical S-factors < 600 keV X4 05062013 1990WA10 14N(p, n):...

233

12C Cross Section  

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

p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 2001NE15 12C(p, ): , deduced S(E) ratio < 160 keV X4 10282014 1993CH02 12C(p,...

234

10B Cross Section  

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

p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 2010LA11 10B(p, ): deduced S(E) E(cm) 0 - 0.15 1 11302011 1993AN06 10B(p, ):...

235

10Be Cross Section  

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

Be(p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1970GO04 10Be(p, 0): 0.6 - 6.3 0, 90 06052012 1987ERZY...

236

13C Cross Section  

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

p, X) (Current as of 05152012) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 2001NE15 13C(p, ): , deduced S(E) ratio < 160 keV X4 09122011 1994KI02 13C(p,...

237

13C Cross Section  

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

3C(, X) (Current as of 01212015) NSR Reaction E (MeV) Cross Section File X4 Dataset Date Added 2006JO11 13C(, n): deduced S(E) 0 - 1 from (1993BR17), from (1993DR08) X4...

238

Full Circle Fuels | Open Energy Information  

Open Energy Info (EERE)

Fuels Fuels Jump to: navigation, search Name Full Circle Fuels Place Oberlin, Ohio Zip 44074 Sector Biofuels Product Alternative fuels center dedicated to increasing awareness and use of biofuels in northeast Ohio. Coordinates 41.292925°, -82.217354° 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":41.292925,"lon":-82.217354,"alt":0,"address":"","icon":"","group":"","inlineLabel":"","visitedicon":""}]}

239

Large Pt processes in ppbar collisions at 2 TeV: measurement of ttbar production cross section in ppbar collisions at s**(1/2) = 1.96 TeV in the dielectron final states at the D0 experiment  

SciTech Connect

The measurement of the top-antitop pair production cross section in p{bar p} collisions at {radical}s = 1.96 TeV in the dielectron decay channel using 384 pb{sup -1} of D0 data yields a t{bar t} production cross-section of {sigma}{sub t{bar t}} = 7.9{sub -3.8}{sup +5.2}(stat){sub -1.0}{sup +1.3}(syst) {+-} 0.5 (lumi) pb. This measurement [98] is based on 5 observed events with a prediction of 1.04 background events. The cross-section corresponds to the top mass of 175 GeV, and is in good agreement with the Standard Model expectation of 6.77 {+-} 0.42 pb based on next-to-next-leading-order (NNLO) perturbative QCD calculations [78]. This analysis shows significant improvement from our previous cross-section measurement in this channel [93] with 230 pb{sup -1} dataset in terms of significantly better signal to background ratio and uncertainties on the measured cross-section. Combination of all the dilepton final states [98] yields a yields a t{bar t} cross-section of {sigma}{sub t{bar t}} = 8.6{sub -2.0}{sup +2.3}(stat){sub -1.0}{sup +1.2}(syst) {+-} 0.6(lumi) pb, which again is in good agreement with theoretical predictions and with measurements in other final states. Hence, these results show no discernible deviation from the Standard Model. Fig. 6.1 shows the summary of cross-section measurements in different final states by the D0 in Run II. This measurement of cross-section in the dilepton channels is the best dilepton result from D0 till date. Previous D0 result based on analysis of 230 pb{sup -1} of data (currently under publication in Physics Letters B) is {sigma}{sub t{bar t}} = 8.6{sub -2.7}{sup +3.2}(stat){sub -1.1}{sup +1.1}(syst) {+-} 0.6(lumi) pb. It can be seen that the present cross-section suffers from less statistical uncertainty. This result is also quite consistent with CDF collaboration's result of {sigma}{sub t{bar t}} = 8.6{sub -2.4}{sup +2.5}(stat){sub -1.1}{sup +1.1}(syst) pb. These results have been presented as D0's preliminary results in the high energy physics conferences in the Summer of 2005 (Hadron Collider Physics Symposium, European Physical Society Conference, etc.). The uncertainty on the cross-section is still dominated by statistics due to the small number of observed events. It can be seen that we are at a level where statistical uncertainties are becoming closer to the systematic ones. Future measurements of the cross section will benefit from considerably more integrated luminosity, leading to a smaller statistical error. Thus the next generation of measurements will be limited by systematic uncertainties. Monte Carlo samples with higher statistics are also being generated in order to decrease the uncertainty on the background estimation. In addition, as the jet energy scale, the electron energy scale, the detector resolutions, and the luminosity measurement are fine-tuned, the systematic uncertainties will continue to decrease.

Kumar, Ashish; /Delhi U.

2005-10-01T23:59:59.000Z

240

American Bar Association Section on Environment | Open Energy Information  

Open Energy Info (EERE)

Bar Association Section on Environment Bar Association Section on Environment Jump to: navigation, search Name American Bar Association Section on Environment Place Chicago, Illinois Zip 60610 Product The Section of Environment, Energy, and Resources is the premier forum for lawyers working in areas related to environment law, natural resources law, and energy law. References American Bar Association Section on Environment[1] LinkedIn Connections CrunchBase Profile No CrunchBase profile. Create one now! This article is a stub. You can help OpenEI by expanding it. American Bar Association Section on Environment is a company located in Chicago, Illinois . References ↑ "American Bar Association Section on Environment" Retrieved from "http://en.openei.org/w/index.php?title=American_Bar_Association_Section_on_Environment&oldid=342108

Note: This page contains sample records for the topic "full section production" from the National Library of EnergyBeta (NLEBeta).
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We encourage you to perform a real-time search of NLEBeta
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241

This Week's Section  

Science Journals Connector (OSTI)

...supported by the United Nations to promote investments in sustainable tech- nologies and products. The school is also asking...Shen spent most of his career, and particularly on real estate devel- opment in Shanxi's capital, Taiyuan. Published...

2014-04-18T23:59:59.000Z

242

Covariance Evaluation Methodology for Neutron Cross Sections  

SciTech Connect

We present the NNDC-BNL methodology for estimating neutron cross section covariances in thermal, resolved resonance, unresolved resonance and fast neutron regions. The three key elements of the methodology are Atlas of Neutron Resonances, nuclear reaction code EMPIRE, and the Bayesian code implementing Kalman filter concept. The covariance data processing, visualization and distribution capabilities are integral components of the NNDC methodology. We illustrate its application on examples including relatively detailed evaluation of covariances for two individual nuclei and massive production of simple covariance estimates for 307 materials. Certain peculiarities regarding evaluation of covariances for resolved resonances and the consistency between resonance parameter uncertainties and thermal cross section uncertainties are also discussed.

Herman,M.; Arcilla, R.; Mattoon, C.M.; Mughabghab, S.F.; Oblozinsky, P.; Pigni, M.; Pritychenko, b.; Songzoni, A.A.

2008-09-01T23:59:59.000Z

243

Top quark pair cross section prospects in ATLAS  

E-Print Network (OSTI)

The observation of the top quark will be an important milestone in ATLAS. This talk reviews methods that ATLAS plans to use to observe the top quark pair production process and measure its cross section.

Andrei Gaponenko; for the ATLAS Collaboration

2009-10-20T23:59:59.000Z

244

Part III - Section J  

National Nuclear Security Administration (NNSA)

H H DIVERSITY PLAN GUIDANCE To Be Updated during Transition With regard to the Contract Section I Clause entitled "Diversity Plan", this Appendix provides guidance to assist the Contractor in understanding the information being sought by the Department for each of the clause's Diversity elements. If the Contractor's current policy or procedure already addresses the following elements, the Contractor need only provide a copy of the policy or procedure to the Contracting Officer and identify the applicable policy or procedure and applicable page number(s). Work Force This Contract includes clauses on Equal Employment Opportunity (EEO) and Affirmative Action (AA). The Contractor's Diversity Plan should describe the means by which the

245

Investigation of distortional buckling of cold-formed steel sections  

E-Print Network (OSTI)

Investigation of distortional buckling of cold-formed steel sections Researcher: Chong Ren Supervisors: Dr Long-yuan Li Dr Jian Yang Aims and Objectives Thin-walled, cold-formed steel sections considered to be the most popular products and account for a substantial proportion of cold-formed steel

Birmingham, University of

246

Electronic Full-text STI | Scientific and Technical Information Program  

Office of Scientific and Technical Information (OSTI)

Electronic Full-text STI Electronic Full-text STI Print page Print page Email page Email page STI products should be provided to OSTI in electronic format, preferably in Portable Document Format (PDF) Searchable; however, certain other electronic formats are acceptable: Hypertext Markup Language (HTML) for site-hosted STI only Microsoft Word (Versions 5.0 or greater) for AN 241.3 submittals only PDF Searchable PDF Non-Searchable As technologies evolve, the list of acceptable electronic formats will be revised and updated. The following table lists the acceptable electronic formats and usage guidance. If the originating site is going to host the product on a publicly accessible server, a unique URL must be provided to OSTI with a direct link to the product. The STI product should not be encrypted or

247

LLNL Section I Clauses/Prescriptions  

National Nuclear Security Administration (NNSA)

AC52-06NA27344 LLNL AC52-06NA27344 LLNL Section I, Page 56 Part II - Contract Clauses Section I I-1 CONTRACT CLAUSES Unless conditionally "Noted", all contract clauses are hereby incorporated by full text. The references cited herein are from the Federal Acquisition Regulation (FAR) (48 CFR Chapter 1) and the Department of Energy Acquisition Regulation (DEAR) (48 CFR Chapter 9). Note: The titles and page locations of the clauses are as follows: CLAUSE TITLE PAGE I001 FAR 52.202-1 DEFINITIONS (JUL 2004) (DEVIATION) ..............................62 I002 FAR 52.203-3 GRATUTIES (APR 1984) ..........................................................63

248

Section A Introduction to Review Section A Introduction to Review  

E-Print Network (OSTI)

with Review. Separate user guides for e-Recruitment Plan and Recruit are available on the AP On-Line UserSection A Introduction to Review A-1 Section A ­ Introduction to Review This section includes: · About AP On-Line (this page) · Accessing Review (this page) · Assignment of roles in Review (page A-2

Tsien, Roger Y.

249

A measurement of the t anti-t production cross-section in proton anti-proton collisions at s**(1/2) = 1.96-TeV with the D0 detector at the Tevatron using final states with a muon and jets  

SciTech Connect

A preliminary measurement of the t{bar t} production cross section at {radical}s = 1.96 TeV is presented. The {mu}-plus-jets final state is analyzed in a data sample of 94 pb{sup -1} and a total of 14 events are selected with a background expectation of 11.7 {+-} 1.9 events. The measurement yields: {sigma}{sub p{bar p} {yields} t{bar t} + X} = 2.4{sub -3.5}{sup +4.2}(stat.){sub -2.6}{sup +2.5}(syst.) {+-} 0.3(lumi.) pb. The analysis, being part of a larger effort to re-observe the top quark in Tevatron Run II data and to measure the production cross section, is combined with results from all available analyses channels. The combined result yields: {sigma}{sub p{bar p}} {yields} t{bar t} + X = 8.1{sub -2.0}{sup +2.2}(stat.){sub -1.4}{sup +1.6}(syst.) {+-} 0.8(lumi.) pb.

Klute, Markus; /Bonn U.

2004-02-01T23:59:59.000Z

250

Draft Guidance for Section 242 of the Energy Policy Act of 2005...  

Energy Savers (EERE)

Draft Guidance for Section 242 of the Energy Policy Act of 2005 - Hydroelectric Production Incentive Program - July 2014 Draft Guidance for Section 242 of the Energy Policy Act of...

251

Section 180(c)  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

: : Questions for Discussion * Funding Allocation Method: - Formula or needs-based? Does either choice impact a set-aside? * Eligibility: - What happens if a Tribe has no emergency response or law enforcement capability? Can they be eligible for Section 180(c) funds? Funding Allocation Method * What we've heard: - Population is not an appropriate measure for funds - Funding should protect all aboriginal lands - Don't use the ½ mile of a route measure used in the EIS - Consider a set-aside of funds for Tribes, higher than the 3% used by DOT's HMEP assistance program. Funding Allocation Method * Formula Approach - Factors in a formula should measure risk and need - What factors might be appropriate? - How can a formula account for varying levels of tribal authority over a route? For example,

252

Search for Single Top Quark Production at HERA  

E-Print Network (OSTI)

A search for single top quark production is performed in the full ep data sample collected by the H1 experiment at HERA, corresponding to an integrated luminosity of 474 pb^-1. Decays of top quarks into a b quark and a W boson with subsequent leptonic or hadronic decay of the W are investigated. A multivariate analysis is performed to discriminate top quark production from Standard Model background processes. An upper limit on the top quark production cross section via flavour changing neutral current processes sigma (ep -> etX) < 0.25 pb is established at 95% CL. Limits on the anomalous coupling kappa_{tu gamma} are derived.

Aaron, F D; Alexa, C; 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; 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, Andreas Werner; 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, Matthias Ulrich; 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; Schmitz, C; 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, 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; 10.1016/j.physletb.2009.06.057

2009-01-01T23:59:59.000Z

253

SECTION A: STUDENT INFORMATION ______________________________________________________________________ 93#____________________________________  

E-Print Network (OSTI)

SECTION A: STUDENT INFORMATION # __________________@_________________________ (______)______________ ________/________/_________ Email Address Phone # Effective Date of this Request SECTION B: ADDITIONAL INFORMATION The items listed below are designated as "Directory Information" and may be released for any purpose at the discretion

Swaddle, John

254

2010 EMPLOYMENT REPORT RICE MBA FULL TIME  

E-Print Network (OSTI)

Associate HP Karthik Narayanan Product Manager HSBC Koby West Relationship Manager J.P. Morgan Jan Goetgeluk

255

FULL FUEL CYCLE ASSESSMENT WELL TO WHEELS ENERGY INPUTS,  

E-Print Network (OSTI)

, greenhouse gas (GHG) emissions, criteria pollutant emissions, air toxics emissions, and multimedia impacts on a full fuel cycle basis for alternative-fueled vehicles is important when assessing the overall control, and assumptions regarding feedstock sources and fuel production conversion efficiency

256

Full Permit Application Handbook | Open Energy Information  

Open Energy Info (EERE)

Full Permit Application Handbook Jump to: navigation, search OpenEI Reference LibraryAdd to library Legal Document- OtherOther: Full Permit Application HandbookLegal Abstract...

257

Section XI -- 25 years of development  

SciTech Connect

The original concept of nuclear power plant designers was that the higher standards of design and fabrication would make inservice inspections unnecessary, and little attention was given to provisions for access. By 1966 the Atomic Energy Commission recognized that a planned program of periodic inservice inspections would be needed. They began development of criteria, and encouraged industry code-writing organizations to do likewise. These groups joined forces in 1968, and their product was published by ASME in 1970 as part of the Boiler and Pressure Code, Section XI, Rules for Inservice Inspection of Nuclear Reactor Coolant Systems. Section XI, 24 pages in 1970, is now 723 pages. While it originally covered only light water reactor Class 1 components and piping, it now includes Class 2, 3, and containment, and liquid metal cooled reactor plants. Along the way, rules have been developed for gas-cooled and low pressure heavy water reactor plants. The growth in size of Section XI from its modest beginning has been largely because of recognition that the rules governing plant inspection/operation need to be considerably different from the rules provided for the component designer/manufacturer. Rules have been developed in the areas of repair/replacement technology, NDE methodology, NDE acceptance standards, and analytical evaluation methods in the absence of appropriate rules in Section III.

Hedden, O.F. [ABB Combustion Engineering Nuclear Operations, Windsor, CT (United States)

1996-12-01T23:59:59.000Z

258

Assistant, Associate, or Full Professor Classification Information  

E-Print Network (OSTI)

400060 Working Title Assistant, Associate, or Full Professor Advertised Employing Department Statistics of Months Employed Per Year 9 Summary of Duties and Responsibilities The Department of Statistics at Iowa Appointment Type Faculty - Tenure-Eligible Base of Employment B - Faculty (9 Months) Full or Part Time Full

Carriquiry, Alicia

259

SECTION J - TABLE OF CONTENTS  

National Nuclear Security Administration (NNSA)

Arrangement Appendix Q Minimum Standards for Contractors' COI Plans (Replaced Mod 002) Appendix R RESERVED Appendix S Contracting Officer's Representative(s) Section J Page i...

260

2013 INTERNSHIP REPORT RICE MBA FULL TIME  

E-Print Network (OSTI)

Mackey Finance & Operations Intern Amazon Samarth Jain Sr.Product Manager Intern American Airlines Intern,Valves & Measurement Wolfgang von der Rosen Intern,Valves & Measurement CBM Enterprise Solutions Haldar Summer Associate Enterprise Products, LP Alex Weaver Commercial Analyst Ernst & Young Emily

Richards-Kortum, Rebecca

Note: This page contains sample records for the topic "full section production" 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

Inclusive jet cross section at CDF  

SciTech Connect

This contribution reports on preliminary measurements of the inclusive jet production cross section in p{bar p} collisions at {radical}s = 1.96 TeV using data collected with CDF corresponding to an integrated luminosity of 385 pb{sup -1}. Two analyzes are presented: one uses the longitudinally invariant k{sub T} algorithm to reconstruct the jets, the other uses the midpoint algorithm. Both are limited to jets with rapidity in the range 0.1 < |y{sup jet}| < 0.7. The measured cross sections are in good agreement with next-to-leading order perturbative QCD predictions after including the non-perturbative corrections necessary to account for underlying event and hadronization effects.

Lefevre, R.; Martinez, M.; /Barcelona, IFAE

2005-01-01T23:59:59.000Z

262

TABLE OF CONTENTS SECTION A: PREINTERVIEW OBSERVATION  

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

TABLE OF CONTENTS TABLE OF CONTENTS SECTION A: PREINTERVIEW OBSERVATION . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1 SECTION B: HOUSING TYPE . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2 SECTION C: HOME HEATING . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8 SECTION D: AIR CONDITIONING . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 16 SECTION E: WATER HEATING . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21 SECTION F: LIGHTS . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25 SECTION G: APPLIANCES . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 27 Cooking . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 27 Refrigerators and Freezers . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .

263

Section 44 - Environment  

Science Journals Connector (OSTI)

The category entitled Environment refers to the impact on the natural world of energy use in all forms. This section is complemented by two others, Ecology and Health and Safety, both of which focus on effects on organismal life rather than the physical environment. Ecology deals with energy effects on nonhuman organisms and Health and Safety covers effects on humans. Energy use did affect the environment to some extent in the preindustrial era through the clearing of forests for wood fuel, and through the urban air pollution resulting from burning of this fuel for processes such as ironmaking and brewing. However, it was not until the Industrial Revolution created an intensive demand for fuel to power engines and machines that the natural world was greatly impacted by energy use. This realization of human impact on the environment was associated with the Industrial Revolution because prior to that the concept of “Nature” as an entity distinct from civilization was not fully developed. When the landscape of Europe and North America began to be transformed on a large scale by industry in the 1800s, this created public awareness that the natural world was being degraded and diminished. The English novelist Charles Dickens wrote in 1840 that in the London of a half century earlier, “Nature was not so far removed, or hard to get at, as in these days.” In addition to the fundamental idea of Nature as an entity in itself, the 19th century saw the establishment of various other concepts of modern environmental science, such as the heat island effect, the phenomenon of acid rain, the fact of anthropomorphic influence on the physical landscape, and the role of carbon dioxide as a greenhouse gas. Also occurring during this period were the first study of environmental problems, the first formal pollution control measures, the beginnings of the practice of recycling, and the founding of the first environmental advocacy organization (Sierra Club). The development of motor vehicle transportation in the twentieth century brought with it major environmental impacts through air pollution from engine exhaust. This came to a crisis point in the postwar era with major smog events in urban areas such as London and Los Angeles. Disposal of nuclear wastes also became an issue during this time, and remains so today. The 1960s saw the first major commercial oil spill, one of numerous such events to occur since the industry began to use huge supertankers to transport oil from distant sites. Coal mining, always associated with environmental impact since the beginning of the Industrial Revolution, became even more significant in this respect in the late twentieth century, through the controversial practice of mountaintop removal mining. In today’s world fossil fuel sources that involve relatively little intrusion on the environment have been depleted, and the energy industry has been required to turn to other resources that are more difficult to extract and thus require more intrusive techniques; e.g., the use of fracking (hydraulic fracturing) to remove natural gas from rock formations far below the Earth’s surface. Increased use of alternative energy sources will reduce the environmental impact associated with fossil fuels, but the challenge is how to maintain a balance between supplying society’s vast energy needs and maintaining the quality of the natural environment.

Cutler J. Cleveland; Christopher Morris

2014-01-01T23:59:59.000Z

264

Section 5 - Coal  

Science Journals Connector (OSTI)

Coal has the longest history of use among the fossil fuels, with use as a fuel dating to 3000 BC in China and Wales. Marco Polo’s “Description of the World” (1298) comments on many novel customs and practices of China, including the use of “stones that burn like logs” (coal). By the thirteenth century the mining of coal was widespread in England in regions such as Durham, Nottinghamshire, Derbyshire, Staffordshire, and North and South Wales. By the early seventeenth century nearly half of England’s maritime trade consisted of coal exports. Coal was the fuel that launched the Industrial Revolution in Europe and then the United States. By the late 1890s, the U.S. assumed the lead in world coal production. Britain now ranked second, after having been the world leader since the beginnings of the formal industry in the 1500s. Germany was third, an indication of its growing industrial power relative to continental rival France. Coal’s leading role in energy use peaked in the early twentieth century, after which it was supplanted by oil and natural gas. By the late twentieth century China’s rapid economic expansion, surging demand for electricity, and prodigious coal resources combined to propel it to become the world leader in production. Continuous improvements in coal mining technology have produced lower costs, improved safety, and greater labor productivity. John Buddle introduced the first air pump to ventilate coal mines (1803), followed shortly by the miner’s safety lamps that were developed independently by Sir Humphry Davy, William Clanny, and George Stephenson (1813-1816). Coal mining underwent a rapid transition in the 1880s to mechanical coal cutting in mines in the United Kingdom, the United States, and Russia. The St. Joseph Lead Company of Missouri (1900) invented the first underground mine roof bolts that became a key safety feature in underground coal mines. The first commercially successful bucket wheel excavator was used at the Luise Mine in Braunkohlemwerke, Germany (1925), followed by the first successful continuous miners in U.S. underground coal mining (1948). The first mechanized U.S. longwall mining system appeared in 1951, and was followed by the self-advancing hydraulic longwall support system that provided greater support for the roof of the mine. LeTourneau Technologies, Inc. of Texas manufactured the largest rubber tired front-end wheel loader in the world, the L-2350, which would play an important role in loading coal in Wyoming’s large surface mines (2005). Coal mining has always been a very hazardous occupation, and has produced some of history’s worst industrial disasters. The Courrières mine disaster, Europe's worst mining accident, caused the death of 1,099 miners in Northern France (1906). An explosion in a coal mine in Liaoning province in northeastern China killed more than 1,500 Chinese miners (1942), as did other major accidents in Ky?sh?, Japan (1914), Wankie, Rhodesia (1972), Wales (1913), Bihar, India (1965), and West Virginia, U.S. (1907), to name just a few. Legislation such as the Federal Coal Mine Health and Safety Act in the U.S. (1969) improved working conditions in many nations. The Great Smog of London (1952) occurred after an exceptionally cold winter forced homes and factories to burn large quantities of coal. A temperature inversion formed, trapping pollutants above the ground. More than 4,000 people died from respiratory ailments within the following week. The use of coal has been impacted by legislation to control the environmental impacts associated with its mining and combustion. The first known environmental regulation of coal dates to 1306 when King Edward II of England prohibited burning sea coal while Parliament was in session because of its offensive smoke. Sulfur dioxide from coal combustion was tied to acid rain in the 1960s, and carbon dioxide emissions became a concern beginning in the 1980s when climate change emerged as a critical environmental issue.

Cutler J. Cleveland; Christopher Morris

2014-01-01T23:59:59.000Z

265

Comment on the $?^+$-production at high energy  

E-Print Network (OSTI)

We show that the cross sections of the $\\Theta^+$-pentaquark production in different processes decrease with energy faster than the cross sections of production of the conventional three-quark hyperons. Therefore, the threshold region with the initial energy of a few GeV or less seemsto be more favorable for the production and experimental study of $\\Theta^+$-pentaquark.

A. I. Titov; A. Hosaka; S. Date'; Y. Ohashi

2004-09-15T23:59:59.000Z

266

Cross sections for nuclide production in a Fe56 target irradiated by 300, 500, 750, 1000, 1500, and 2600 MeV protons compared with data on a hydrogen target irradiated by 300, 500, 750, 1000, and 1500 MeV/nucleon Fe56 ions  

Science Journals Connector (OSTI)

This work presents the cross sections for radioactive nuclide production in Fe56(p,x) reactions determined in six experiments using 300, 500, 750, 1000, 1500, and 2600 MeV protons of the external beam from the ITEP U-10 proton accelerator. In total, 221 independent and cumulative yields of radioactive residuals of half-lives from 6.6 min to 312 d have been obtained. The radioactive product nuclide yields were determined by direct ?-spectrometry. The measured data have been compared with the experimental data obtained elsewhere by the direct and inverse kinematics methods and with calculation results of 15 different codes that simulated hadron-nucleus interactions: MCNPX (INCL, CEM2K, BERTINI, ISABEL), LAHET (BERTINI, ISABEL), CEM03 (.01, .G1, .S1), LAQGSM03 (.01, .G1, .S1), CASCADE-2004, LAHETO, and BRIEFF. Most of the data obtained here are in a good agreement with the inverse kinematics results and disprove the results of some earlier activation measurements that were quite different from the inverse kinematics measurements. The most significant calculation-to-experiment differences are observed in the yields of the Aproducts.

Yu. E. Titarenko; V. F. Batyaev; A. Yu. Titarenko; M. A. Butko; K. V. Pavlov; S. N. Florya; R. S. Tikhonov; S. G. Mashnik; A. V. Ignatyuk; N. N. Titarenko; W. Gudowski; M. T?šínský; C.-M. L. Persson; H. Ait Abderrahim; H. Kumawat; H. Duarte

2008-09-30T23:59:59.000Z

267

,"Full Service Providers",,,,,"Other Providers",,  

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

Illinois" ,"Full Service Providers",,,,,"Other Providers",, "Item","Investor Owned","Public","Federal","Cooperative","Non-Utility","Energy","Delivery","Total" "Number of...

268

,"Full Service Providers",,,,,"Other Providers",,  

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

Connecticut" ,"Full Service Providers",,,,,"Other Providers",, "Item","Investor Owned","Public","Federal","Cooperative","Non-Utility","Energy","Delivery","Total" "Number of...

269

Biochemistry as a Programming Language Full Presentation  

E-Print Network (OSTI)

. One such objective is the biological production of useful chemicals. Target chemicals include biofuels or part of this work for personal or classroom use is granted without fee provided that copies

Seshia, Sanjit A.

270

Photoproduction models for total cross section and shower development  

E-Print Network (OSTI)

A model for the total photoproduction cross section based on the ansatz that resummation of infrared gluons limits the rise induced by QCD minijets in all the total cross-sections, is used to simulate extended air showers initiated by cosmic rays with the AIRES simulation program. The impact on common shower observables, especially those related with muon production, is analysed and compared with the corresponding results obtained with previous photoproduction models.

Fernando Cornet; Carlos Garcia Canal; Agnes Grau; Giulia Pancheri; Sergio Sciutto

2014-11-19T23:59:59.000Z

271

Cross section for nuclear fusion  

Science Journals Connector (OSTI)

... gamma rays. In recent years there have been many studies of the cross section for nuclear fusion, and some features of the process are now understood (Nature, 256, 261; ... velocities fusion cannot take place at all.

P. E. Hodgson

1976-05-20T23:59:59.000Z

272

Section 25: Future State Assumptions  

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

the Compliance Certification Application (CCA), Chapter 6.0, Section 6.2 and Appendices SCR and MASS (U.S. DOE 1996). Many of these future state assumptions were derived from the...

273

SBIR Full Application Preparation and Submission Information  

Office of Energy Efficiency and Renewable Energy (EERE)

An LOI is required and must be submitted by the small business concern. Only those applicants that submit an LOI by the due date are eligible to submit a full application.

274

Afghanistan Geospatial Toolkit - Full Data | OpenEI  

Open Energy Info (EERE)

Full Data Full Data Dataset Summary Description (Abstract): This Geospatial Toolkit contains the full (with high resolution data) version of the GsT interfaced to HOMER for Afghanistan. (Purpose): The products contained on this web site were developed by the U.S. National Renewable Energy Laboratory (NREL) for the U.S. Agency for International Development's (USAID) South Asia Regional Initiative for Energy Cooperation (SARI/E). (Supplemental Information): The GsT allows the user to examine the resource data in a geospatial context along with other key information relevant to renewable energy development, such as transportation networks, transmission corridors, existing power facilities, load centers, terrain conditions, and land use. Working within the GsT, the user can also incorporate location-specific data directly into NREL's Micropower Optimization Model, HOMER, to design least-cost hybrid renewable power systems to meet electric-load requirements at the village level.

275

Pakistan Geospatial Toolkit - Full Data | OpenEI  

Open Energy Info (EERE)

Full Data Full Data Dataset Summary Description (Abstract): This Geospatial Toolkit contains the full (with high resolution data) version of the GsT interfaced to HOMER for Pakistan. (Purpose): The products contained on this web site were developed by the U.S. National Renewable Energy Laboratory (NREL) for the U.S. Agency for International Development's (USAID) South Asia Regional Initiative for Energy Cooperation (SARI/E). (Supplemental Information): The GsT allows the user to examine the resource data in a geospatial context along with other key information relevant to renewable energy development, such as transportation networks, transmission corridors, existing power facilities, load centers, terrain conditions, and land use. Working within the GsT, the user can also incorporate location-specific data directly into NREL's Micropower Optimization Model, HOMER, to design least-cost hybrid renewable power systems to meet electric-load requirements at the village level.

276

Public Meeting and Availability of Statement of Policy for Adopting Full-Fuel-Cycle Analyses Into Energy Conservation Standards Program  

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

10 Aug 19, 2010 10 Aug 19, 2010 Jkt 220001 PO 00000 Frm 00001 Fmt 4702 Sfmt 4702 E:\FR\FM\20AUP1.SGM 20AUP1 jdjones on DSK8KYBLC1PROD with PROPOSALS-1 51423 Federal Register Proposed Rules Vol. 75, No. 161 Friday, August 20, 2010 This section of the FEDERAL REGISTER contains notices to the public of the proposed issuance of rules and regulations. The purpose of these notices is to give interested persons an opportunity to participate in the rule making prior to the adoption of the final rules. DEPARTMENT OF ENERGY 10 CFR Part 431 [Docket No (EERE-2010-BT-NOA-0028)] RIN 1904-AC24 Energy Conservation Program for Consumer Products and Certain Commercial and Industrial Equipment: Public Meeting and Availability of Statement of Policy for Adopting Full- Fuel-Cycle Analyses Into Energy

277

Overview of Commercial Buildings, 2003 - Full Report  

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

Full Report Full Report Energy Information Administration > Commercial Buildings Energy Consumption Survey > Overview of Commercial Buildings Overview of Commercial Buildings, 2003 Introduction The Energy Information Administration conducts the Commercial Buildings Energy Consumption Survey (CBECS) to collect information on energy-related building characteristics and types and amounts of energy consumed in commercial buildings in the United States. In 2003, CBECS reports that commercial buildings: ● total nearly 4.9 million buildings ● comprise more than 71.6 billion square feet of floorspace ● consumed more than 6,500 trillion Btu of energy, with electricity accounting for 55 percent and natural gas 32 percent (Figure 1) ●

278

L-shell x-ray cross sections for Cl-Ar and Ar-Ar collisions  

Science Journals Connector (OSTI)

Measurements of total x-ray production cross sections for Ar+ -Ar and Cl+ -Ar collisions for incident energies between 200 keV and 1.5 MeV are reported. For Cl+ -Ar collisions, separate argon and chlorine x-ray production cross sections are extracted. The cross sections exhibit steep increases as bombarding energy is increased. Using existing measurements of Auger cross sections, values for the mean fluorescence yields as a function of bombarding energy are deduced. The increases in the x-ray production cross sections are shown to be due primarily to changes in the mean fluorescence yields. A qualitative explanation for the observations is proposed.

H. Oona, J. D. Garcia, and R. J. Fortner

1977-08-01T23:59:59.000Z

279

Connected obstructions to full graph homomorphisms  

Science Journals Connector (OSTI)

Minimal obstructions to full homomorphisms to a graph B have been proved to be of size at most |B|+1. This turns out to require that disconnected obstructions be allowed. In this paper we prove that the size of minimal connected obstructions is at most ...

Pavol Hell, Aleš Pultr

2014-10-01T23:59:59.000Z

280

Friction in full view A. P. Merklea  

E-Print Network (OSTI)

Friction in full view A. P. Merklea and L. D. Marksb Materials Science and Engineering proposed friction mechanisms explaining the unique tribological properties of graphite. Wear of graphite chemical or struc- tural information from the interface during a friction experi- ment. Examples

Marks, Laurence D.

Note: This page contains sample records for the topic "full section production" 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

MODIS Land Products Subsets  

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

methods methods This section describes methods used to generate MODIS Land Subsets for Collection 4 and Collection 5 data products. Methods for Selected Sites (Collections 4 and 5) Methods for North America Tool (Collection 4) Methods for the Global Tool (Collection 5) Methods for Selected Sites (Collection 4 and 5) Source for Selected Site Data: Full MODIS scenes (1200-km x 1200-km) are initially subset to 11-km x 31-km (Collection 4) or 25-km x 25-km (Collection 5) by the MODAPS; these initial subsets contain the field site or flux tower. Reformatting and additional subsetting to 7-km x 7-km containing the field site or flux tower are done by the ORNL DAAC. Tools Used: The ORNL DAAC uses the MODIS Reprojection Tool (MRT) to reformat the MODIS data from HDF-EOS to binary format. A tool developed at ORNL is then used to convert the binary format to ASCII. The MRT is available from the Land Processes DAAC. Whereas the MRT can also be used to reproject data from its native projection to other projections, ORNL chose to forgo the resampling associated with reprojection to minimize data manipulation and distortion. The MOD12Q1 Land Cover Collection 3 data are in I-Sin projection, and the Collection 4 and Collection 5 data are in Sinusoidal projection.

282

The Colorado Section Welcomes You  

Science Journals Connector (OSTI)

The Colorado Section Welcomes You ... Among those at present affiliated with the section who have become nationally famous are John B. Ekeley, head of the Department of Chemistry of the University of Colorado, Boulder; W. D. Engle, president of Denver University and head of the Department of Chemistry, a member of the SOCIETY since 1898; Sidney J. Osborn, chief chemist of the Great Western Sugar Co., first chairman of the Division of Sugar Chemistry; M. F. Coolbaugh, president of Colorado State School of Mines; and R. G. Gustavson, noted for his contributions to the knowledge of the sex hormones. ...

1932-08-10T23:59:59.000Z

283

1 INTRODUCTION The full characterization of the vulnerability of criti-  

E-Print Network (OSTI)

the network are of- ten highly variable quantities both in space and time. Functional models are, then, often in Section 2; in Section 3, the physical characterization of interde- pendencies is introduced; in Section 4, the functional model for interdependent CIs is detailed; in Section 5, the proposed model is applied to three

Paris-Sud XI, Université de

284

Measurement of Heavy Quark cross-sections at CDF  

E-Print Network (OSTI)

The measurement of heavy quark cross-sections provides important tests of the QCD theory. This paper reviews recent measurements of single b-quark and correlated b-quark cross-sections at CDF. Two new measurements of the single b-quark production at CDF agree with the first result from CDF Run II. This clarifies the experimental situation and confirms the recent agreement of theoretical prediction with data. A new measurement of the correlated $b\\bar{b}$ cross-section with dimuon events at CDF is presented. It agrees with theory and it does not confirm the anomalously large $b\\bar{b}$ cross-section seen in Run I by CDF and D${\

A. Annovi

2007-09-28T23:59:59.000Z

285

Handbook of LHC Higgs Cross Sections: 2. Differential Distributions  

E-Print Network (OSTI)

This Report summarises the results of the second year's activities of the LHC Higgs Cross Section Working Group. The main goal of the working group was to present the state of the art of Higgs Physics at the LHC, integrating all new results that have appeared in the last few years. The first working group report Handbook of LHC Higgs Cross Sections: 1. Inclusive Observables (CERN-2011-002) focuses on predictions (central values and errors) for total Higgs production cross sections and Higgs branching ratios in the Standard Model and its minimal supersymmetric extension, covering also related issues such as Monte Carlo generators, parton distribution functions, and pseudo-observables. This second Report represents the next natural step towards realistic predictions upon providing results on cross sections with benchmark cuts, differential distributions, details of specific decay channels, and further recent developments.

Dittmaier, S; Passarino, G; Tanaka, R; Alekhin, S; Alwall, J; Bagnaschi, E A; Banfi, A; Blumlein, J; Bolognesi, S; Chanon, N; Cheng, T; Cieri, L; Cooper-Sarkar, A M; Cutajar, M; Dawson, S; Davies, G; De Filippis, N; Degrassi, G; Denner, A; D'Enterria, D; Diglio, S; Di Micco, B; Di Nardo, R; Ellis, R K; Farilla, A; Farrington, S; Felcini, M; Ferrera, G; Flechl, M; de Florian, D; Forte, S; Ganjour, S; Garzelli, M V; Gascon-Shotkin, S; Glazov, S; Goria, S; Grazzini, M; Guillet, J -Ph; Hackstein, C; Hamilton, K; Harlander, R; Hauru, M; Heinemeyer, S; Hoche, S; Huston, J; Jackson, C; Jimenez-Delgado, P; Jorgensen, M D; Kado, M; Kallweit, S; Kardos, A; Kauer, N; Kim, H; Kovac, M; Kramer, M; Krauss, F; Kuo, C -M; Lehti, S; Li, Q; Lorenzo, N; Maltoni, F; Mellado, B; Moch, S O; Muck, A; Muhlleitner, M; Nadolsky, P; Nason, P; Neu, C; Nikitenko, A; Oleari, C; Olsen, J; Palmer, S; Paganis, S; Papadopoulos, C G; Petersen, T C; Petriello, F; Petrucci, F; Piacquadio, G; Pilon, E; Potter, C T; Price, J; Puljak, I; Quayle, W; Radescu, V; Rebuzzi, D; Reina, L; Rojo, J; Rosco, D; Salam, G P; Sapronov, A; Schaarschmidt, J; Schonherr, M; Schumacher, M; Siegert, F; Slavich, P; Spira, M; Stewart, I W; Stirling, W J; Stockli, F; Sturm, C; Tackmann, F J; Thorne, R S; Tommasini, D; Torrielli, P; Tramontano, F; Trocsanyi, Z; Ubiali, M; Uccirati, S; Acosta, M Vazquez; Vickey, T; Vicini, A; Waalewijn, W J; Wackeroth, D; Warsinsky, M; Weber, M; Wiesemann, M; Weiglein, G; Yu, J; Zanderighi, G

2012-01-01T23:59:59.000Z

286

Handbook of LHC Higgs Cross Sections: 2. Differential Distributions  

E-Print Network (OSTI)

This Report summarises the results of the second year's activities of the LHC Higgs Cross Section Working Group. The main goal of the working group was to present the state of the art of Higgs Physics at the LHC, integrating all new results that have appeared in the last few years. The first working group report Handbook of LHC Higgs Cross Sections: 1. Inclusive Observables (CERN-2011-002) focuses on predictions (central values and errors) for total Higgs production cross sections and Higgs branching ratios in the Standard Model and its minimal supersymmetric extension, covering also related issues such as Monte Carlo generators, parton distribution functions, and pseudo-observables. This second Report represents the next natural step towards realistic predictions upon providing results on cross sections with benchmark cuts, differential distributions, details of specific decay channels, and further recent developments.

LHC Higgs Cross Section Working Group; S. Dittmaier; C. Mariotti; G. Passarino; R. Tanaka; S. Alekhin; J. Alwall; E. A. Bagnaschi; A. Banfi; J. Blumlein; S. Bolognesi; N. Chanon; T. Cheng; L. Cieri; A. M. Cooper-Sarkar; M. Cutajar; S. Dawson; G. Davies; N. De Filippis; G. Degrassi; A. Denner; D. D'Enterria; S. Diglio; B. Di Micco; R. Di Nardo; R. K. Ellis; A. Farilla; S. Farrington; M. Felcini; G. Ferrera; M. Flechl; D. de Florian; S. Forte; S. Ganjour; M. V. Garzelli; S. Gascon-Shotkin; S. Glazov; S. Goria; M. Grazzini; J. -Ph. Guillet; C. Hackstein; K. Hamilton; R. Harlander; M. Hauru; S. Heinemeyer; S. Hoche; J. Huston; C. Jackson; P. Jimenez-Delgado; M. D. Jorgensen; M. Kado; S. Kallweit; A. Kardos; N. Kauer; H. Kim; M. Kovac; M. Kramer; F. Krauss; C. -M. Kuo; S. Lehti; Q. Li; N. Lorenzo; F. Maltoni; B. Mellado; S. O. Moch; A. Muck; M. Muhlleitner; P. Nadolsky; P. Nason; C. Neu; A. Nikitenko; C. Oleari; J. Olsen; S. Palmer; S. Paganis; C. G. Papadopoulos; T . C. Petersen; F. Petriello; F. Petrucci; G. Piacquadio; E. Pilon; C. T. Potter; J. Price; I. Puljak; W. Quayle; V. Radescu; D. Rebuzzi; L. Reina; J. Rojo; D. Rosco; G. P. Salam; A. Sapronov; J. Schaarschmidt; M. Schonherr; M. Schumacher; F. Siegert; P. Slavich; M. Spira; I. W. Stewart; W. J. Stirling; F. Stockli; C. Sturm; F. J. Tackmann; R. S. Thorne; D. Tommasini; P. Torrielli; F. Tramontano; Z. Trocsanyi; M. Ubiali; S. Uccirati; M. Vazquez Acosta; T. Vickey; A. Vicini; W. J. Waalewijn; D. Wackeroth; M. Warsinsky; M. Weber; M. Wiesemann; G. Weiglein; J. Yu; G. Zanderighi

2012-01-15T23:59:59.000Z

287

Measurement of the forward W boson cross-section in pp collisions at \\( \\sqrt{s}=7 \\) TeV  

Science Journals Connector (OSTI)

A measurement of the inclusive W ? ?? production cross-section using data from pp collisions at a centre-of-mass energy of s

R. Aaij; B. Adeva; M. Adinolfi; A. Affolder; Z. Ajaltouni…

2014-12-01T23:59:59.000Z

288

Decorrelating the topology in full QCD  

E-Print Network (OSTI)

We investigate the performance of the hybrid Monte Carlo algorithm in updating non-trivial global topological structures. We find that the hybrid Monte Carlo algorithm has serious problems decorrelating the global topological charge. This represents a warning which must be seriously considered when simulating full QCD, regardless of the number and type of fermions, with this or any similar algorithm. Simulated tempering is examined as a means of accelerating the decorrelation.

G. Boyd; B. Allés; M. D'Elia; A. Di Giacomo; E. Vicari

1996-08-22T23:59:59.000Z

289

Technology development for gene discovery and full-length sequencing  

SciTech Connect

In previous years, with support from the U.S. Department of Energy, we developed methods for construction of normalized and subtracted cDNA libraries, and constructed hundreds of high-quality libraries for production of Expressed Sequence Tags (ESTs). Our clones were made widely available to the scientific community through the IMAGE Consortium, and millions of ESTs were produced from our libraries either by collaborators or by our own sequencing laboratory at the University of Iowa. During this grant period, we focused on (1) the development of a method for preferential cloning of tissue-specific and/or rare transcripts, (2) its utilization to expedite EST-based gene discovery for the NIH Mouse Brain Molecular Anatomy Project, (3) further development and optimization of a method for construction of full-length-enriched cDNA libraries, and (4) modification of a plasmid vector to maximize efficiency of full-length cDNA sequencing by the transposon-mediated approach. It is noteworthy that the technology developed for preferential cloning of rare mRNAs enabled identification of over 2,000 mouse transcripts differentially expressed in the hippocampus. In addition, the method that we optimized for construction of full-length-enriched cDNA libraries was successfully utilized for the production of approximately fifty libraries from the developing mouse nervous system, from which over 2,500 full-ORF-containing cDNAs have been identified and accurately sequenced in their entirety either by our group or by the NIH-Mammalian Gene Collection Program Sequencing Team.

Marcelo Bento Soares

2004-07-19T23:59:59.000Z

290

Interagency ADR Workplace Section Education Programs  

Energy.gov (U.S. Department of Energy (DOE))

The Interagency Alternative Dispute Resolution Working Group (IADRWG) Workplace Conflict Management Section (“Workplace Section”) provides guidance on “best practices” in ADR program development,...

291

Section 999 Program Library | Department of Energy  

Office of Environmental Management (EM)

Science & Innovation Oil & Gas Offshore Drilling Section 999 Program Library Section 999 Program Library Cost-Shared Program Publications October 2, 2013 UDAC Meeting -...

292

Integrated powerhead demonstration full flow cycle development  

Science Journals Connector (OSTI)

The Integrated Powerhead Demonstration (IPD) is a 1 112 000 N (250 000? lb f ) thrust (at sea level) LOX/LH2 demonstration of a full flow cycle in an integrated system configuration. Aerojet and Rocketdyne are on contract to the Air Force Research Laboratory to design develop and deliver the required components and to provide test support to accomplish the demonstration. Rocketdyne is on contract to provide a fuel and oxygen turbopump a gas-gas injector and system engineering and integration. Aerojet is on contract to provide a fuel and oxygen preburner a main combustion chamber and a nozzle. The IPD components are being designed with Military Spaceplane (MSP) performance and operability requirements in mind. These requirements include: lifetime ?200 missions mean time between overhauls ?100 cycles and a capability to throttle from 20% to 100% of full power. These requirements bring new challenges both in designing and testing the components. This paper will provide some insight into these issues. Lessons learned from operating and supporting the space shuttle main engine (SSME) have been reviewed and incorporated where applicable. The IPD program will demonstrate phase I goals of the Integrated High Payoff Rocket Propulsion Technology (IHPRPT) program while demonstrating key propulsion technologies that will be available for MSP concepts. The demonstration will take place on Test Stand 2A at the Air Force Research Laboratory at Edwards AFB. The component tests will begin in 1999 and the integrated system tests will be completed in 2002.

J. Mathew Jones; James T. Nichols; William F. Sack; William D. Boyce; William A. Hayes

1998-01-01T23:59:59.000Z

293

Full Counting Statistics of Stationary Particle Beams  

E-Print Network (OSTI)

We present a general scheme for treating particle beams as many particle systems. This includes the full counting statistics and the requirements of Bose/Fermi symmetry. In the stationary limit, i.e., for longer and longer beams, the total particle number diverges, and a description in Fock space is no longer possible. We therefore extend the formalism to include stationary beams. These beams exhibit a well-defined "local" counting statistics, by which we mean the full counting statistics of all clicks falling into any given finite interval. We treat in detail a model of a source, creating particles in a fixed state, which then evolve under the free time evolution, and we determine the resulting stationary beam in the far field. In comparison to the one-particle picture we obtain a correction due to Bose/Fermi statistics, which depends on the emission rate. We also consider plane waves as stationary many particle states, and determine the distribution of intervals between successive clicks in such a beam.

J. Kiukas; A. Ruschhaupt; R. F. Werner

2011-03-07T23:59:59.000Z

294

Projections of Full-Fuel-Cycle Energy and Emissions Metrics  

E-Print Network (OSTI)

from Conventional Oil Production and Oil Sands. ” Environ.6 Forecasts of Canadian oil production published in 2006 andPetroleum Fuels The oil production chain is similar to

Coughlin, Katie

2013-01-01T23:59:59.000Z

295

Symmetric Long Straight Section Lattices  

NLE Websites -- All DOE Office Websites (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,

296

Reports of Sections and Societies  

Science Journals Connector (OSTI)

...Flame Photometer Condensed Specifications. Metals An-alyzed and...by 41/2" low K factor insulation... Stryofoam used on exterior...Product Data Sheet giving specifications, typical drying perform-ance...ALSO AVAILABLE: * Thermal Conductivity Cells for Gas...

1961-02-17T23:59:59.000Z

297

SECTION J, APPENDIX A - SOW  

National Nuclear Security Administration (NNSA)

Replaced Mod 002; Modified Mod 016; Replaced Mod 002; Modified Mod 016; Replaced Mod 029; Modified Mod 0049) Honeywell FM&T, LLC Contract No. DE-NA0000622 SECTION J APPENDIX A STATEMENT OF WORK 09/19/12 TABLE OF CONTENTS CHAPTER I. OBJECTIVES, SCOPE, AND REQUIREMENTS ......................................................................... 1 1.0 OBJECTIVE .................................................................................................................................................. 1 2.0 BACKGROUND ............................................................................................................................................ 1 2.1 The NNSA Mission ...................................................................................................................................... 1

298

Alternative Fuels Data Center: Biofuels Production Incentive  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biofuels Production Biofuels Production Incentive to someone by E-mail Share Alternative Fuels Data Center: Biofuels Production Incentive on Facebook Tweet about Alternative Fuels Data Center: Biofuels Production Incentive on Twitter Bookmark Alternative Fuels Data Center: Biofuels Production Incentive on Google Bookmark Alternative Fuels Data Center: Biofuels Production Incentive on Delicious Rank Alternative Fuels Data Center: Biofuels Production Incentive on Digg Find More places to share Alternative Fuels Data Center: Biofuels Production Incentive on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Biofuels Production Incentive The Mississippi Department of Agriculture and Commerce (Department) provides incentive payments to qualified ethanol and biodiesel producers

299

Diffractive photon production at the LHC  

Science Journals Connector (OSTI)

In this paper we study photon production in single and double diffractive processes considering the resolved pomeron model. We estimate the rapidity and transverse momentum dependence of the cross section for the diffractive double photon and photon+jet production. A comparison with the inclusive production is presented. We predict large values for the total cross sections, which make the experimental analysis of these observables feasible at LHC energies.

C. Brenner Mariotto and V. P. Goncalves

2013-10-22T23:59:59.000Z

300

LLNL-Generated Content for the California Academy of Sciences, Morrison Planetarium Full-Dome Show: Earthquake  

SciTech Connect

The California Academy of Sciences (CAS) Morrison Planetarium is producing a 'full-dome' planetarium show on earthquakes and asked LLNL to produce content for the show. Specifically the show features numerical ground motion simulations of the M 7.9 1906 San Francisco and a possible future M 7.05 Hayward fault scenario earthquake. The show also features concepts of plate tectonics and mantle convection using images from LLNL's G3D global seismic tomography. This document describes the data that was provided to the CAS in support of production of the 'Earthquake' show. The CAS is located in Golden Gate Park, San Francisco and hosts over 1.6 million visitors. The Morrison Planetarium, within the CAS, is the largest all digital planetarium in the world. It features a 75-foot diameter spherical section projection screen tilted at a 30-degree angle. Six projectors cover the entire field of view and give a three-dimensional immersive experience. CAS shows strive to use scientifically accurate digital data in their productions. The show, entitled simply 'Earthquake', will debut on 26 May 2012. They are working on graphics and animations based on the same data sets for display on LLNL powerwalls and flat-screens as well as for public release.

Rodgers, A J; Petersson, N A; Morency, C E; Simmons, N A; Sjogreen, B

2012-01-23T23:59:59.000Z

Note: This page contains sample records for the topic "full section production" 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

Diboson Cross Sections at sqrt(s) = 1.96 TeV  

E-Print Network (OSTI)

A brief survey of the results on diboson production at the Tevatron is presented. Measured cross sections for $W\\gamma$, $Z\\gamma$, $WW$, and limits on WZ/ZZ are summarized.

A. W. Askew

2005-05-12T23:59:59.000Z

302

A Conjecture on 180° Production of High Energy Hydrogen Isotopes from Nuclei  

Science Journals Connector (OSTI)

......of 1 1igh energy hydrogen isotopes in the reac...func- tion. The production cross sections of the hydrogen isotopes are well...Assuming the production cross section of...the above mentioned method, we find it tend......

Fumiyo Uchiyama

1978-03-01T23:59:59.000Z

303

Two photon radiation in W and Z boson production at the Fermilab Tevatron collider  

Science Journals Connector (OSTI)

We present a calculation of two photon radiation in W and Z boson production in hadronic collisions, based on the complete matrix elements for the processes qq??l±??? and qq¯?l+l-??, including finite charged lepton masses. In order to achieve stable numerical results over the full phase space, multiconfiguration Monte Carlo techniques are used to map the peaks in the differential cross section. Numerical results are presented for the Fermilab Tevatron.

U. Baur and T. Stelzer

2000-03-07T23:59:59.000Z

304

SECTION THIRTY SEVEN Consultants Section Thirty Seven Consultants, Inc.  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

THIRTY SEVEN THIRTY SEVEN Consultants Section Thirty Seven Consultants, Inc. A California Corporation 1 DEPARTMENT OF ENERGY [OE Docket No. RRTT-IR-001] Rapid Response Team for Transmission AGENCY: Office of Electricity Delivery and Energy Reliability, Department of Energy, DoE. ACTION: Request for information. (1) The development timelines for generation and attendant transmission are often not coordinated or run concurrently. Because of the lengthy time to obtain regulatory reviews, permits and approvals (collectively ''Regulatory Permits''), major new transmission lines can take significantly longer to develop than some types of generation to which the transmission would connect. This Request for Information will refer to the difference in development times between generation and transmission as

305

Reports of Sections and Societies  

Science Journals Connector (OSTI)

...Explosion-proof, doesn't use electricity. But versatile: Flexible...laboratory, pilot plant, production. But temperature-tolerant...degradation of dedicated sites. Summarizing a four-year...need to correlate school sites with total curriculum...An Approach to School Site De-velopment," developed...

1967-02-17T23:59:59.000Z

306

Section 2. Our Scientific Journeys  

Science Journals Connector (OSTI)

...gas production by fracking and a subject of...would have a major impact on my career in...near-surface environment (its exogenic...Precambrian aquatic environment. This led us to...and the Global Environment: Assessing Human...the environmental impacts of humankind...

Fred T. Mackenzie; Andreas J. Andersson

307

Estimation of simultaneous systems of spatially interrelated cross sectional equations  

Science Journals Connector (OSTI)

In this paper we consider a simultaneous system of spatially interrelated cross sectional equations. Our specification incorporates spatial lags in the endogenous and exogenous variables. In modelling the disturbance process we allow for both spatial correlation as well as correlation across equations. The data set is taken to be a single cross section of observations. The model may be viewed as an extension of the widely used single equation Cliff-Ord model. We suggest computationally simple limited and full information instrumental variable estimators for the parameters of the system and give formal large sample results.

Harry H. Kelejian; Ingmar R. Prucha

2004-01-01T23:59:59.000Z

308

Evaluation tests for photovoltaic concentrator receiver sections and modules  

SciTech Connect

Sandia has developed a third-generation set of specifications for performance and reliability testing of photovoltaic concentrator modules. Several new requirements have been defined. The primary purpose of the tests is to screen new concentrator designs and new production runs for susceptibility to known failure mechanisms. Ultraviolet radiation testing of materials precedes receiver section and module performance and environmental tests. The specifications include the purpose, procedure, and requirements for each test. Recommendations for future improvements are presented.

Woodworth, J.R.; Whipple, M.L.

1992-06-01T23:59:59.000Z

309

Clean Air Act, Section 309  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

CLEAN AIR ACT § 309* CLEAN AIR ACT § 309* §7609. Policy review (a) The Administrator shall review and comment in writing on the environmental impact of any matter relating to duties and responsibilities granted pursuant to this chapter or other provisions of the authority of Administrator, contained in any (1) legislation proposed by any Federal department or agency, (2) newly authorized Federal projects for construction and any major Federal agency action (other than a project for construction) to which section 4332(2)(C) of this title applies, and (3) proposed regulations published by any department or agency of the Federal Government. Such written comment shall be made public at the conclusion of any such review. (b) In the event the Administrator determines that any such legislation, action, or regulation

310

Electron-impact ionization cross section of rubidium  

Science Journals Connector (OSTI)

A theoretical model for electron-impact ionization cross section has been applied to Rb and the theoretical cross section (from the threshold to 1 keV in incident energy) is in good agreement with the recent experimental data obtained using Rb atoms trapped in a magneto-optical trap. The theoretical model, called the binary-encounter–dipole (BED) model, combines a modified Mott cross section with the high-energy behavior of Born cross sections. To obtain the continuum dipole oscillator strength df/dE of the 5s electron required in the BED model, we used Dirac-Fock continuum wave functions with a core polarization potential that reproduced the known position of the Cooper minimum in the photoionization cross section. For inner-shell ionization, we used a simpler version of df/dE, which retained the hydrogenic shape. The contributions of the 4p?4d, 5s, and 5p autoionizing excitations were estimated using the plane-wave Born approximation. As a by-product, we also present the dipole oscillator strengths for the 5s?np1/2 and 5s?np3/2 transitions for high principal quantum numbers n near the ionization threshold obtained from the Dirac-Fock wave functions with the same core polarization potential as that used for the continuum wave functions.

Yong-Ki Kim; Jacek Migda?ek; Wojciech Siegel; Jacek Biero?

1998-01-01T23:59:59.000Z

311

Section 12 | OpenEI Community  

Open Energy Info (EERE)

Contributor 4 September, 2012 - 21:36 Idaho Meeting 2 endangered species Fauna Fish and Wildlife Flora FWS Section 12 Section 7 The second Idaho GRR meeting was held today...

312

Section B: Supplies, Services and Costs  

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

SECTION B SUPPLIES AND SERVICES AND PRICECOSTS Request for Proposal DE-RP36-07GO97036 PART I SECTION B SUPPLIES AND SERVICES AND PRICECOSTS TABLE OF CONTENTS B.1 Service Being...

313

Section 7 | OpenEI Community  

Open Energy Info (EERE)

Contributor 4 September, 2012 - 22:36 Idaho Meeting 2 endangered species Fauna Fish and Wildlife Flora FWS Section 12 Section 7 The second Idaho GRR meeting was held today...

314

Computers & Graphics 28 (2004) 907918 Technical section  

E-Print Network (OSTI)

. For the straight homogeneous generalized cylinder (SHGC) [6,7], their cross-sections have the same shape but may) a constant axis direction (SHGC), (ii) a constant size of cross-section (PRCGC), or (iii) a fixed shape

Ahuja, Narendra

315

SECTION FOUR Site Design Guidelines Bicycle Systems  

E-Print Network (OSTI)

SECTION FOUR Site Design Guidelines Bicycle Systems 26 4, the following should be considered when designa ng bicycle routes on roadways: Vehicular speed limits; SECTION FOUR Site Design Guidelines Bicycle Systems 27 4.2 BIKE LANES Bike lanes

Duchowski, Andrew T.

316

Intro to Least Squares Problems (LSQ) Full rank, m = n Full rank, m>n  

E-Print Network (OSTI)

Oct 19, 2014 ... doesn't have an exact solution – maybe A isn't full rank, or m > n, or for whatever reason b isn't in the column-space of A, i.e. b /? col(A).

2014-10-19T23:59:59.000Z

317

Associated production of Higgs bosons and Z particles  

Science Journals Connector (OSTI)

We estimate the cross section for Higgs-boson production via bremsstrahlung from intermediate vector bosons produced in pp and p¯p collisions.

S. L. Glashow; D. V. Nanopoulos; A. Yildiz

1978-09-01T23:59:59.000Z

318

Absorption cross section in Lifshitz black hole  

E-Print Network (OSTI)

We derive the absorption cross section of a minimally coupled scalar in the Lifshitz black hole obtained from the new massive gravity. The absorption cross section reduces to the horizon area in the low energy and massless limit of s-wave mode propagation, indicating that the Lifshitz black hole also satisfies the universality of low energy absorption cross section for black holes.

Taeyoon Moon; Yun Soo Myung

2012-05-10T23:59:59.000Z

319

Connecting section and associated systems concept for the spray calciner/in-can melter process  

SciTech Connect

For a number of years, researchers at the Pacific Northwest Laboratory have been developing processes and equipment for converting high-level liquid wastes to solid forms. One of these processes is the Spray Calciner/In-Can Melter system. To immobilize high-level liquid wastes, this system must be operated remotely, and the calcine must be reliably conveyed from the calciner to the melting furnace. A concept for such a remote conveyance system was developed at the Pacific Northwest Laboratory, and equipment was tested under full-scale, nonradioactive conditions. This concept and the design of demonstration equipment are described, and the results of equipment operation during experimental runs of 7 d are presented. The design includes a connecting section and its associated systems - a canister sypport and alignment concept and a weight-monitoring system for the melting furnace. Overall, the runs demonstrated that the concept design is an acceptable method of connecting the two pieces of process equipment together. Although the connecting section has not been optimized in all areas of concern, it provides a first-generation design of a production-oriented system.

Petkus, L.L.; Gorton, P.S.; Blair, H.T.

1981-06-01T23:59:59.000Z

320

From ZZ to ZH : How Low Can These Cross Sections Go or Everybody, Let's Cross Section Limbo!  

SciTech Connect

We report on two searches performed at the D0 detector at the Fermi National Laboratory. The first is a search for Z di-boson production with a theoretical cross section of 1.4 pb. The search was performed on 2.6 fb{sup -1} of data and contributed to the first observation of ZZ production at a hadron collider. The second is a search for a low mass Standard Model Higgs in 4.2 fb{sup -1} of data. The Higgs boson is produced in association with a Z boson where the Higgs decays hadronically and the Z decays to two leptons. The ZZ search was performed in both the di-electron and di-muon channels. For the ZH search, we will focus on the muonic decays where we expanded the traditional coverage by considering events in which one of the two muons fails the selection requirement, and is instead reconstructed as an isolated track. We consider Higgs masses between 100 and 150 GeV, with theoretical cross sections ranging from 0.17 to 0.042 pb, and set upper limits on the ZH production cross-section at 95% confidence level.

Strauss, Emanuel Alexandre; /SUNY, Stony Brook

2009-08-01T23:59:59.000Z

Note: This page contains sample records for the topic "full section production" 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

Measurement on the thermal neutron capture cross section of w-180  

E-Print Network (OSTI)

We have measured the thermal neutron capture cross section for w-180 nucleus. There is only one previous data on this cross section with a value of 30 $^{+300%}_{-100%}$ barn. To consider w-181 as a low energy neutrino source, the thermal neutron capture cross section should be measured more precisely to estimate the production rate of w-181 inside a nuclear reactor. We measured the cross section of w-180 with a natural tungsten foil and obtained a new value of 21.9 $\\pm$ 2.5 barn

W. G. Kang; Y. D. Kim; J. I. Lee; I. S. Hahn; A. R. Kim; H. J. Kim

2007-04-24T23:59:59.000Z

322

On Primitivity and the Unital Full Free Product of Finite Dimensional C*-algebras  

E-Print Network (OSTI)

= kp1 and k2 = kp2 Assume B is {isomorphic to Ll j=1Mnj . To prove the result it is enough to show there are positive integers (m(1); : : :m(l)) such that n1m(1) + + nlm(l) = k: Let (B1; B) = [m1(1); : : : ;m1(l)]; (B2; u Bu) = [m2...(1); : : : ;m2(l)]: Since (MN ; B1) (B1; B) = (MN ; B2) (B2; u Bu) we deduce thatm1m1(j) = m2m2(j) for all 1 j l. Multiplying by k and using N = m1k1 = m2k2 we conclude N p1 m1(j) = km1m1(j) = km2m2(j) = N p2 m2(j); so p2m1(j) = p1m2(j). Since gcd...

Torres Ayala, Francisco

2012-07-16T23:59:59.000Z

323

COMBINE7.1 - A Portable ENDF/B-VII.0 Based Neutron Spectrum and Cross-Section Generation Program  

SciTech Connect

COMBINE7.1 is a FORTRAN 90 computer code that generates multigroup neutron constants for use in the deterministic diffusion and transport theory neutronics analysis. The cross-section database used by COMBINE7.1 is derived from the Evaluated Nuclear Data Files (ENDF/B-VII.0). The neutron energy range covered is from 20 MeV to 1.0E-5 eV. The Los Alamos National Laboratory NJOY code is used as the processing code to generate a 167 fine-group cross-section library in MATXS format for Bondarenko self-shielding treatment. Resolved resonance parameters are extracted from ENDF/B-VII.0 File 2 for a separate library to be used in an alternate Nordheim self-shielding treatment in the resolved resonance energy range. The equations solved for energy dependent neutron spectrum in the 167 fine-group structure are the B3 or B1 zero-dimensional approximations to the transport equation. The fine group cross sections needed for the spectrum calculation are first prepared by Bondarenko self-shielding interpolation in terms of background cross section and temperature. The geometric lump effect, when present, is accounted for by augmenting the background cross section. Nordheim self-shielded fine group cross sections for a material having resolved resonance parameters overwrite correspondingly the existing self-shielded fine group cross sections when this option is used. COMBINE7.1 coalesces fine group cross sections into broad group macroscopic and microscopic constants. The coalescing is performed by utilizing fine-group fluxes and/or currents obtained by spectrum calculation as the weighting functions. The multigroup constants may be output in any of several standard formats including INL format, ANISN 14** free format, CCCC ISOTXS format, and AMPX working library format. ANISN-PC, a one-dimensional (1-D) discrete-ordinate transport code, is incorporated into COMBINE7.1. As an option, the 167 fine-group constants generated by zero-dimensional COMBINE portion in the program can be used to calculate regionwise spectra in the 1-D ANISN portion, all internally to reflect the 1-D transport correction. The regionwise spectra are then used to generate mutigroup regionwise neutron constants. The 1-D neutron transport can be performed up to three stages, e.g., from a TRISO fuel to PEBBLE to 1-D full core wedge. In addition, COMBINE7.1 has now the capability of adjoint flux calculation through the 1-D ANISN transport. Photon transport capability is also added. For this, a photon production and photo-atomic cross section library, MATNG.LIB, was generated in MATXS format through NJOY code. The photon production cross section matrix is of 167 neutron - 18 photon groups. Photo-atomic cross sections, including heating, are in 18 energy groups.

Woo Y. Yoon; David W. Nigg

2011-09-01T23:59:59.000Z

324

CORRELATED EVOLUTION OF FRUIT SIZE AND SEXUAL EXPRESSION IN ANDROMONOECIOUS SOLANUM SECTIONS  

E-Print Network (OSTI)

CORRELATED EVOLUTION OF FRUIT SIZE AND SEXUAL EXPRESSION IN ANDROMONOECIOUS SOLANUM SECTIONS production is a mechanism to regulate allocation to female function (i.e., fruit production), then large-fruited species should be more strongly andromonoecious than smaller-fruited taxa because more resources

Miller, Jill S.

325

EIA - Annual Energy Outlook 2008 - Overview Section  

Gasoline and Diesel Fuel Update (EIA)

Overview Overview Annual Energy Outlook 2008 with Projections to 2030 Energy Trends to 2030 In preparing projections for the Annual Energy Outlook 2008 (AEO2008), the Energy Information Administration (EIA) evaluated a wide range of trends and issues that could have major implications for U.S. energy markets between today and 2030. This overview focuses on one case, the reference case, which is presented and compared with the Annual Energy Outlook 2007 (AEO2007) reference case (see Table 1). Readers are encouraged to review the full range of alternative cases included in other sections of AEO2008. As in previous editions of the Annual Energy Outlook (AEO), the reference case assumes that current policies affecting the energy sector remain unchanged throughout the projection period. The reference case provides a clear basis against which alternative cases and policies can be compared. Although current laws and regulations may change over the next 25 years, and new ones may be created, it is not possible to predict what they will be or how they will be implemented [1].

326

In situ oil shale retort with a generally T-shaped vertical cross section  

DOE Patents (OSTI)

An in situ oil shale retort is formed in a subterranean formation containing oil shale. The retort contains a fragmented permeable mass of formation particles containing oil shale and has a production level drift in communication with a lower portion of the fragmented mass for withdrawing liquid and gaseous products of retorting during retorting of oil shale in the fragmented mass. The principal portion of the fragmented mass is spaced vertically above a lower production level portion having a generally T-shaped vertical cross section. The lower portion of the fragmented mass has a horizontal cross sectional area smaller than the horizontal cross sectional area of the upper principal portion of the fragmented mass above the production level.

Ricketts, Thomas E. (Grand Junction, CO)

1981-01-01T23:59:59.000Z

327

Section 38 - HVAC (Heating, Ventilation, Air Conditioning)  

Science Journals Connector (OSTI)

The term HVAC is an acronym for Heating, Ventilation (and) Air Conditioning, the industry term for any of various efforts to control conditions in a building or other enclosed area to improve comfort and efficiency. A closely related section is Refrigeration, which follows this one. Some contemporary HVAC techniques have ancient roots. Early forms of central heating and solar home heating were in use in Rome in the first century A.D. The earliest use of glass in windows (as opposed to a covering of wood, cloth, or hide, or simply an opening) is also attributed to the Romans at this same time. The first known use of solar-oriented building design in North America dates back to about the year 1050; i.e., the cliff dwellings built by the Anasazi (Ancient Pueblo) people of the Colorado Plateau area. Geothermal district heating was employed as early as the 1300s, in the Auvergne region of southern France. The foundation for modern central heating was established in the 1700s, first in England and then in France. The 1800s saw significant advances in the use of water heaters, especially the first automatic storage water heater (Edwin Ruud, 1889) and the first commercial solar water heater (Clarence Kemp, 1891). In comparison with heating, cooling technology was late in developing. The first successful method of producing ice occurred in 1851, and it was not until 1902 that Willis Haviland Carrier designed the first industrial air-conditioning system. His Carrier Air Conditioning Corporation would go on to develop air-conditioning systems for stores and theaters (1924) and for residential buildings (1928). Carrier remains the global leader in air conditioner production. The first air-conditioned automobile was produced by Packard in 1939. Recent entries in this section emphasize the use of alternative energy sources in heating and cooling, such as solar, photovoltaic, geothermal, and fuel cells. These advances include the ground-source heat pump, the Trombe wall, the heat pipe, and the PV/thermal hybrid system.

Cutler J. Cleveland; Christopher Morris

2014-01-01T23:59:59.000Z

328

Measurement Of Differential Cross Sections Of p(e,e'{pi}{sup +})n For High-Lying Resonances At Q{sup 2} < 5 GeV{sup 2}  

SciTech Connect

The exclusive electro-production process ep -> e'n{pi}{sup +} was measured in the range of the invariant mass for n{pi}{sup +} system 1.6 GeV <= W <= 2.0 GeV, and the photon virtuality 1.8 GeV{sup 2} <= Q{sup 2} <= 4.0 GeV{sup 2} using CLAS. For the first time, these kinematics are probed in exclusive {pi}{sup +} production from the protons with nearly full coverage in the azimuthal and polar angles of the n{pi}{sup +} center-of-mass system. In this experiment, approximately 39,000 differential cross-section data points were measured. In this proceeding, preliminary results of our latest analysis work are presented on differential cross sections and structure functions as well as Legendre Moments.

Park, Kijun

2014-01-01T23:59:59.000Z

329

Upsilon Productions at STAR  

E-Print Network (OSTI)

The $\\Upsilon(1S+2S+3S)\\to e^{+}e^{-}$ cross section is measured at mid-rapidity ($y$) in $p+p$ collisions and in d$+Au$ collisions at center-of-mass energy $\\sqrt{s}$ = 200 GeV with the STAR detector at RHIC. In $p+p$, the measured cross section is found to be consistent with the world data trend as a function of $\\sqrt{s}$, in agreement with the Color Evaportaion Model (CEM), and underestimated by the Color Singlet Model (CSM) up to the Next-to-Leading-Order Quantum Chromodynamics (NLO QCD) calculations. In d+$Au$, the measured cross section is in agreement with the CEM prediction with anti-shadowing effects, and the nuclear modification factor indicates that $\\Upsilon(1S+2S+3S)$ production follows binary scaling within the current uncertainties. These measurements provide a benchmark for the future measurements of $\\Upsilon$ production in $Au+Au$ collisions.

A. M. Hamed

2010-05-22T23:59:59.000Z

330

Alternative Fuels Data Center: Ethanol Production Incentive  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Ethanol Production Ethanol Production Incentive to someone by E-mail Share Alternative Fuels Data Center: Ethanol Production Incentive on Facebook Tweet about Alternative Fuels Data Center: Ethanol Production Incentive on Twitter Bookmark Alternative Fuels Data Center: Ethanol Production Incentive on Google Bookmark Alternative Fuels Data Center: Ethanol Production Incentive on Delicious Rank Alternative Fuels Data Center: Ethanol Production Incentive on Digg Find More places to share Alternative Fuels Data Center: Ethanol Production Incentive on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Ethanol Production Incentive The Ethanol Production Incentive provides qualified ethanol producers with quarterly payments based on production volume during times when ethanol

331

Backscattering cross section of a roughened sphere  

Science Journals Connector (OSTI)

The backscattering cross section of a perfectly conducting, roughened sphere is presented. It is derived from the calculation of the electric-field cross correlation at two temporal...

Schertler, Donald J; George, Nicholas

1994-01-01T23:59:59.000Z

332

Section 10 (cont.): More Risk Management Concepts  

E-Print Network (OSTI)

Dec 4, 2014 ... Section 10 (cont.) .... next ten years is Poisson distributed with mean 4. Each ... due to hurricanes hitting the house in the next ten years. Lesson ...

2014-12-04T23:59:59.000Z

333

Vibration assisted filling of thin section castings.  

E-Print Network (OSTI)

??Understanding of the mechanism of the vibration needed to fill thin section or one with sharp edges in profile shapes and clarifying the dominant control… (more)

Abdul Karem, Waleed

2009-01-01T23:59:59.000Z

334

ACHP - Section 106 Regulations Flowchart Explanatory Material...  

Open Energy Info (EERE)

Explanatory Material Jump to: navigation, search OpenEI Reference LibraryAdd to library Web Site: ACHP - Section 106 Regulations Flowchart Explanatory Material Abstract This...

335

RMOTC - Production  

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

Production Production RMOTC Pumpjack in action During the process of the sale of NPR-3, RMOTC will focus on maximizing the value of the NPR-3 site and will continue with its Production Optimization Projects. NPR-3 includes 9,481 acres with more than 400 oil-producing wells. Current oil production is at approximately 240 barrels of oil per day. In July 2013, RMOTC began working on a number of Production Optimization Projects within the NPR-3 field, with the goal to optimize and improve flow and efficiency. Production Optimization Projects include repairing and replacing existing infrastructure with new infrastructure in order to optimize current wells and bring additional wells online. These Production Optimization Projects will continue throughout 2013 and are focused on improving current production and creating revenue for the America tax payer.

336

PRODUCTS & MATERIALS  

Science Journals Connector (OSTI)

...1995-96 Spectrum Chemical and Safety Prod-ucts Catalog features products for molecular and life science laboratories and cleanroom environments. Spectrum Chemical Manu-facturing. Circle 150. SCIENCE * VOL. 268 * 23 JUNE 1995

1995-06-23T23:59:59.000Z

337

Midstream Infrastructure Improvements Key to Realizing Full Potential...  

Office of Environmental Management (EM)

Midstream Infrastructure Improvements Key to Realizing Full Potential of Domestic Natural Gas Midstream Infrastructure Improvements Key to Realizing Full Potential of Domestic...

338

POLICY FLASH 2014-10 UPDATE TO CONGRESSIONAL NOTIFICATION_ FULL...  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

0 UPDATE TO CONGRESSIONAL NOTIFICATION FULL IMPLEMENTATION OF ANA SYSTEM POLICY FLASH 2014-10 UPDATE TO CONGRESSIONAL NOTIFICATION FULL IMPLEMENTATION OF ANA SYSTEM An updated...

339

Full Fuel-Cycle Comparison of Forklift Propulsion Systems | Department...  

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

Full Fuel-Cycle Comparison of Forklift Propulsion Systems Full Fuel-Cycle Comparison of Forklift Propulsion Systems This report examines forklift propulsion systems and addresses...

340

GRR/Section 11-FD-a - NHPA Section 106 - Resource Survey | Open Energy  

Open Energy Info (EERE)

11-FD-a - NHPA Section 106 - Resource Survey 11-FD-a - NHPA Section 106 - Resource Survey < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 11-FD-a - NHPA Section 106 - Resource Survey 11-FD-a NHPA Section 106 Consultation.pdf Click to View Fullscreen Contact Agencies Advisory Council on Historic Preservation National Park Service Bureau of Indian Affairs Regulations & Policies National Historic Preservation Act 36 CFR Part 800 Triggers None specified Click "Edit With Form" above to add content 11-FD-a NHPA Section 106 Consultation.pdf 11-FD-a NHPA Section 106 Consultation.pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Flowchart Narrative Section 106 applies when two thresholds are met:

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


341

GRR/Section 17-FD-a - Wild & Scenic Rivers Section 7(a) | Open Energy  

Open Energy Info (EERE)

GRR/Section 17-FD-a - Wild & Scenic Rivers Section 7(a) GRR/Section 17-FD-a - Wild & Scenic Rivers Section 7(a) < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 17-FD-a - Wild & Scenic Rivers Section 7(a) 17FDAWildScenicRiversSection7AProcess.pdf Click to View Fullscreen Contact Agencies National Park Service Bureau of Land Management United States Forest Service United States Forest Service Federal Energy Regulatory Commission Regulations & Policies Wild and Scenic Rivers Act 36 CFR 297 Wild and Scenic Rivers Triggers None specified Click "Edit With Form" above to add content 17FDAWildScenicRiversSection7AProcess.pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range.

342

GRR/Section 14-NV-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

GRR/Section 14-NV-d - Section 401 Water Quality Certification GRR/Section 14-NV-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-NV-d - Section 401 Water Quality Certification 14NVDSection401WaterQualityCertification.pdf Click to View Fullscreen Contact Agencies Nevada Division of Environmental Protection Regulations & Policies Section 401 of the Clean Water Act (33 U.S.C. 1341) Triggers None specified Click "Edit With Form" above to add content 14NVDSection401WaterQualityCertification.pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Flowchart Narrative Section 401 of the Clean Water Act (33 U.S.C. 1341) requires activities in

343

GRR/Section 14-WA-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

GRR/Section 14-WA-d - Section 401 Water Quality Certification GRR/Section 14-WA-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-WA-d - Section 401 Water Quality Certification 14-WA-d - 401 Water Quality Certification.pdf Click to View Fullscreen Contact Agencies U S Army Corps of Engineers Washington State Department of Ecology Regulations & Policies Revised Statute of Washington Chapter 90.48 Washington Administrative Code Chapter 173-201A Washington Administrative Code 173-225-030 Triggers None specified Developers requiring a Section 404 Dredge and Fill Permit from the U S Army Corps of Engineers (Corps) are required to obtain a Section 401 Water Quality Certification from the state of Washington. The Washington State

344

GRR/Section 14-CA-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

GRR/Section 14-CA-d - Section 401 Water Quality Certification GRR/Section 14-CA-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-CA-d - Section 401 Water Quality Certification 14CADSection401WaterQualityCertification (1).pdf Click to View Fullscreen Contact Agencies California State Water Resources Control Board Regulations & Policies Section 401 Clean Water Act (33 U.S.C. 1251 et seq.) Porter-Cologne Water Quality Control Act Code of Regulations Title 23, Section 3855 et. seq. Triggers None specified Click "Edit With Form" above to add content 14CADSection401WaterQualityCertification (1).pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range.

345

GRR/Section 14-UT-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

GRR/Section 14-UT-d - Section 401 Water Quality Certification GRR/Section 14-UT-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-UT-d - Section 401 Water Quality Certification 14-UT-d - Section 401 Water Quality Certification.pdf Click to View Fullscreen Triggers None specified Section 401 of the Clean Water Act (CWA) requires a Water Quality Certification for any federal license or permit that is issued to construct or operate a facility, which may result in any fill or discharge into the navigable waters of the United States. The Utah Division of Water Quality oversees the 401 Water Quality Certification process in the state of Utah. The director of the Utah Division of Water Quality ("director") handles

346

Alternative Fuels Data Center: Propane Production and Distribution  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Production and Production and Distribution to someone by E-mail Share Alternative Fuels Data Center: Propane Production and Distribution on Facebook Tweet about Alternative Fuels Data Center: Propane Production and Distribution on Twitter Bookmark Alternative Fuels Data Center: Propane Production and Distribution on Google Bookmark Alternative Fuels Data Center: Propane Production and Distribution on Delicious Rank Alternative Fuels Data Center: Propane Production and Distribution on Digg Find More places to share Alternative Fuels Data Center: Propane Production and Distribution on AddThis.com... More in this section... Propane Basics Production & Distribution Related Links Benefits & Considerations Stations Vehicles Laws & Incentives Propane Production and Distribution

347

Alternative Fuels Data Center: Natural Gas Production and Distribution  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Production Production and Distribution to someone by E-mail Share Alternative Fuels Data Center: Natural Gas Production and Distribution on Facebook Tweet about Alternative Fuels Data Center: Natural Gas Production and Distribution on Twitter Bookmark Alternative Fuels Data Center: Natural Gas Production and Distribution on Google Bookmark Alternative Fuels Data Center: Natural Gas Production and Distribution on Delicious Rank Alternative Fuels Data Center: Natural Gas Production and Distribution on Digg Find More places to share Alternative Fuels Data Center: Natural Gas Production and Distribution on AddThis.com... More in this section... Natural Gas Basics Production & Distribution Related Links Benefits & Considerations Stations Vehicles Laws & Incentives Natural Gas Production and Distribution

348

Download Full-text PDF - American Society of Limnology and ...  

Science Journals Connector (OSTI)

vestigated whether benthic photosynthesis could contribute to primary production ... occurrence and light dependence of benthic photosynthesis in the lake was ...

2002-06-25T23:59:59.000Z

349

Projections of Full-Fuel-Cycle Energy and Emissions Metrics  

E-Print Network (OSTI)

energy and emissions intensity of unconventional production are at best a lower bound, and current projections of future

Coughlin, Katie

2013-01-01T23:59:59.000Z

350

Cosine Products, Fourier Transforms, and Random Sums Kent E. Morrison  

E-Print Network (OSTI)

, dating from 1593 and due to Fran¸cois Vi`ete (1540-1603), whose Latinized name is Vieta. (Was any notice the characteristic function of the interval [-1, 1] (modulo a scalar factor). In section 2 we prove the infinite product expansion for sin x/x and derive Vi`ete's formula. In section 3 we transform the product expansion

Morrison, Kent E.

351

Section 4 -Financial Information A. General Information  

E-Print Network (OSTI)

Section 4 - Financial Information A. General Information 1. All University Housing and Dining fees. The security deposit, less any charges for damages, will be returned approximately ten weeks after the end according to Section 5 ­ Termination of Occupancy, will result in the forfeiture of the security deposit

Pantaleone, Jim

352

THE PHILADELPHIA SESSIONS OF SECTIONS AND SOCIETIES  

Science Journals Connector (OSTI)

...of the coal-tar products, the production of a lard-like fat from cottonseed...possibilities of the reduction of wheat production to a self-sufficiency basis, the agricultural surplus, increasing production per worker in agriculture and more...

1927-01-28T23:59:59.000Z

353

Section 999: Annual Plans | Department of Energy  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Section 999: Annual Plans Section 999: Annual Plans Section 999: Annual Plans October 2, 2013 URTAC Meeting - October 2013 Federal Register Notice for October 10, 2013 URTAC Meeting The 24th Meeting of the Unconventional Resources Technology Advisory Committee (URTAC), previously scheduled for October 10, 2013, is postponed until further notice due to a lapse in Federal funding. October 2, 2013 UDAC Meeting - October 2013 Federal Register Notice for October 8, 2013 UDAC Meeting The 24th Meeting of the Ultra-Deepwater Advisory Committee (UDAC), previously scheduled for October 8, 2013, is postponed until further notice due to a lapse in Federal funding. September 10, 2013 Draft 2014 Annual Plan Section 999: Draft 2014 Annual Plan July 8, 2013 2013 Annual Plan Section 999: 2013 Annual Plan

354

Collision Cross Sections for D — D Neutrons  

Science Journals Connector (OSTI)

The nuclear collision cross sections of 22 elements for the neutrons from a deuteron-deuteron source have been measured. The geometrical arrangement of the experiment was such that only small corrections to the measured transmission were necessary. The neutron energy was 2.88±0.04 Mev. The cross sections are found to vary irregularly with the atomic weight. The proton cross section determined for both paraffin and water scatterers is found to be 2.36×10-24 cm2, which is smaller than the value predicted by theory. In addition, the cross sections of a number of elements for neutrons of 2.46 Mev energy have been measured. For some elements the cross section is found to increase with an increase in neutron energy, for others it decreases.

W. H. Zinn; S. Seely; V. W. Cohen

1939-08-01T23:59:59.000Z

355

Measurement of multi-jet cross sections at ATLAS  

E-Print Network (OSTI)

Inclusive multi-jet production is studied using the ATLAS detector for proton-proton collisions with a center-of-mass energy of 7 TeV. The data sample corresponds to an integrated luminosity of 2.43 pb^-1, using the first proton-proton data collected by the ATLAS detector in 2010. Results on multi-jet cross sections are presented and compared to both leading-order plus parton-shower Monte Carlo predictions and next-to-leading-order QCD calculations.

Matthew Tamsett on behalf of the ATLAS collaboration

2011-09-30T23:59:59.000Z

356

Alternative Fuels Data Center: Ethanol Production Incentive  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Production Production Incentive to someone by E-mail Share Alternative Fuels Data Center: Ethanol Production Incentive on Facebook Tweet about Alternative Fuels Data Center: Ethanol Production Incentive on Twitter Bookmark Alternative Fuels Data Center: Ethanol Production Incentive on Google Bookmark Alternative Fuels Data Center: Ethanol Production Incentive on Delicious Rank Alternative Fuels Data Center: Ethanol Production Incentive on Digg Find More places to share Alternative Fuels Data Center: Ethanol Production Incentive on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Ethanol Production Incentive Montana-based ethanol producers are eligible for a tax incentive of $0.20 per gallon of ethanol produced solely from Montana agricultural products or

357

Alternative Fuels Data Center: Biodiesel Production Incentive  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biodiesel Production Biodiesel Production Incentive to someone by E-mail Share Alternative Fuels Data Center: Biodiesel Production Incentive on Facebook Tweet about Alternative Fuels Data Center: Biodiesel Production Incentive on Twitter Bookmark Alternative Fuels Data Center: Biodiesel Production Incentive on Google Bookmark Alternative Fuels Data Center: Biodiesel Production Incentive on Delicious Rank Alternative Fuels Data Center: Biodiesel Production Incentive on Digg Find More places to share Alternative Fuels Data Center: Biodiesel Production Incentive on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Biodiesel Production Incentive A qualified Kansas biodiesel producer is eligible for a production incentive of $0.30 per gallon of biodiesel sold. The incentive is payable

358

Alternative Fuels Data Center: Ethanol Production  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Production to Production to someone by E-mail Share Alternative Fuels Data Center: Ethanol Production on Facebook Tweet about Alternative Fuels Data Center: Ethanol Production on Twitter Bookmark Alternative Fuels Data Center: Ethanol Production on Google Bookmark Alternative Fuels Data Center: Ethanol Production on Delicious Rank Alternative Fuels Data Center: Ethanol Production on Digg Find More places to share Alternative Fuels Data Center: Ethanol Production on AddThis.com... More in this section... Ethanol Basics Blends Specifications Production & Distribution Feedstocks Related Links Benefits & Considerations Stations Vehicles Laws & Incentives Ethanol Production and Distribution Ethanol is a domestically produced alternative fuel that's most commonly made from corn. It can also be made from cellulosic feedstocks, such as

359

Alternative Fuels Data Center: Biofuels Production Grants  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biofuels Production Biofuels Production Grants to someone by E-mail Share Alternative Fuels Data Center: Biofuels Production Grants on Facebook Tweet about Alternative Fuels Data Center: Biofuels Production Grants on Twitter Bookmark Alternative Fuels Data Center: Biofuels Production Grants on Google Bookmark Alternative Fuels Data Center: Biofuels Production Grants on Delicious Rank Alternative Fuels Data Center: Biofuels Production Grants on Digg Find More places to share Alternative Fuels Data Center: Biofuels Production Grants on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Biofuels Production Grants The Biofuels Production Incentive Grant Program provides grants to producers of advanced biofuels, specifically fuels derived from any

360

Alternative Fuels Data Center: Ethanol Production Incentive  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Ethanol Production Ethanol Production Incentive to someone by E-mail Share Alternative Fuels Data Center: Ethanol Production Incentive on Facebook Tweet about Alternative Fuels Data Center: Ethanol Production Incentive on Twitter Bookmark Alternative Fuels Data Center: Ethanol Production Incentive on Google Bookmark Alternative Fuels Data Center: Ethanol Production Incentive on Delicious Rank Alternative Fuels Data Center: Ethanol Production Incentive on Digg Find More places to share Alternative Fuels Data Center: Ethanol Production Incentive on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Ethanol Production Incentive Ethanol producers may qualify for an income tax credit equal to 30% of production facility nameplate capacity between 500,000 and 15 million

Note: This page contains sample records for the topic "full section production" 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

Alternative Fuels Data Center: Biofuels Production Incentive  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biofuels Production Biofuels Production Incentive to someone by E-mail Share Alternative Fuels Data Center: Biofuels Production Incentive on Facebook Tweet about Alternative Fuels Data Center: Biofuels Production Incentive on Twitter Bookmark Alternative Fuels Data Center: Biofuels Production Incentive on Google Bookmark Alternative Fuels Data Center: Biofuels Production Incentive on Delicious Rank Alternative Fuels Data Center: Biofuels Production Incentive on Digg Find More places to share Alternative Fuels Data Center: Biofuels Production Incentive on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Biofuels Production Incentive Qualified ethanol and biodiesel producers are eligible for production incentives on a per gallon basis. To be eligible for the incentive, the

362

Alternative Fuels Data Center: Ethanol Production Incentive  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Ethanol Production Ethanol Production Incentive to someone by E-mail Share Alternative Fuels Data Center: Ethanol Production Incentive on Facebook Tweet about Alternative Fuels Data Center: Ethanol Production Incentive on Twitter Bookmark Alternative Fuels Data Center: Ethanol Production Incentive on Google Bookmark Alternative Fuels Data Center: Ethanol Production Incentive on Delicious Rank Alternative Fuels Data Center: Ethanol Production Incentive on Digg Find More places to share Alternative Fuels Data Center: Ethanol Production Incentive on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Ethanol Production Incentive Qualified ethanol producers are eligible for a production incentive payable from the Kansas Qualified Agricultural Ethyl Alcohol Producer Fund. An

363

Catalyst-Assisted Production of Olefins from Natural Gas Liquids...  

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

Catalyst-Assisted Production of Olefins from Natural Gas Liquids: Prototype Development and Full-Scale Testing, April 2013 Catalyst-Assisted Production of Olefins from Natural Gas...

364

PHYSICS EDUCATION RESEARCH SECTION The Physics Education Research Section PERS publishes articles describing important results from  

E-Print Network (OSTI)

PHYSICS EDUCATION RESEARCH SECTION The Physics Education Research Section PERS publishes articles because students of- ten confuse electric and magnetic fields.9,10 It has been shown that when a particle

Heckler, Andrew F.

365

GRR/Section 14-HI-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

HI-d - Section 401 Water Quality Certification HI-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-HI-d - Section 401 Water Quality Certification 14HID - Section401WaterQualityCertification (1).pdf Click to View Fullscreen Contact Agencies Hawaii Department of Health Clean Water Branch United States Environmental Protection Agency Regulations & Policies Clean Water Act (33 U.S.C. 1251) Section 401 Hawaii Administrative Rules Title 11, Chapter 54 Triggers None specified Click "Edit With Form" above to add content 14HID - Section401WaterQualityCertification (1).pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range.

366

High-Energy Cross Sections. II. Nucleon-Nucleon Cross Section at Cosmic-Ray Energies  

Science Journals Connector (OSTI)

Cosmic-ray measurements are capable of yielding reliable results for the cross section of a nucleus for proton or neutron collisions involving a not too small energy transfer. This cross section should therefore be less than, or at most equal to, the true nonelastic cross section (reaction cross section). Results of recent cosmic-ray work are assembled and compared with the reaction cross sections measured at 1.4 Bev with the Brookhaven Cosmotron; it is found that the cosmic-ray cross sections are significantly larger, even for Pb. Assuming a nonuniform distribution of the density of nuclear matter, one can explain this surprising effect as the result of an increase in the elementary nucleon-nucleon cross section with energy. It is shown that the elementary cross section (the average of ?pp and ?np) must be (120-20+30)×10-27 cm2 in the neighborhood of 30 Bev.

Robert W. Williams

1955-06-01T23:59:59.000Z

367

Bacterial community structures are unique and resilient in full-scale bioenergy systems  

E-Print Network (OSTI)

Bacterial community structures are unique and resilient in full-scale bioenergy systems Jeffrey J digestion is the most successful bioenergy technology worldwide with, at its core, undefined microbialFrac | community function | digester | sludge The production of bioenergy from wastes is an essential com- ponent

Hammerton, James

368

Full Name: Vicki Gray, PT, PhD Title(s): UMANRRT PostDoctoral Fellow  

E-Print Network (OSTI)

Full Name: Vicki Gray, PT, PhD Title(s): UMANRRT PostDoctoral Fellow Email: vgray and Rehabilitation Sciences in the field of Physical Therapy. Her Ph.D. thesis focused on the motor control of fast continued to work in Dr Jayne Garland's Neural Control of Force Production and Movement Lab

Weber, David J.

369

Sample Contract Language for Construction Using Energy-Efficient Products  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

CONSTRUCTION USING ENERGY-EFFICIENT CONSTRUCTION USING ENERGY-EFFICIENT PRODUCTS Section C - Performance Work Statement/Descriptions, Specifications The Contractor shall comply with Sections 524 and Sections 525 of the Energy Independence and Security Act of 2007; Section 104 of the Energy Policy Act of 2005; Executive Order 13514, "Federal Leadership in Environmental, Energy, and Economic Performance," dated October 5, 2009; Executive Order 13423, "Strengthening Federal Environmental, Energy, and Transportation Management," dated

370

Angular and energy dependence of cross sections for ejection of electrons from water vapor. III. 20–150-keV neutral-hydrogen impact  

Science Journals Connector (OSTI)

Absolute values of cross sections for electron production in collisions of neutral hydrogen atoms of 20–150 keV energy with water vapor molecules have been measured as a function of the ejection energy and angle. The range of angles was 10° to 160° and the electron energy range was 1–300 eV. The doubly differential cross sections were integrated over angle and/or energy to obtain singly differential cross sections, total electron production cross sections, and average energies of ejection. The angular distribution of the electron loss peak was found to have some features in common with the cross section for elastic scattering of electrons.

M. A. Bolorizadeh and M. E. Rudd

1986-02-01T23:59:59.000Z

371

Public Comment re Section 934 of the Energy Independence and Security Act  

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

Section 934 of the Energy Independence and Section 934 of the Energy Independence and Security Act of 2007 Public Comment re Section 934 of the Energy Independence and Security Act of 2007 Public Comment by the Uranium Producers of America (UPA) re Section 934 of the Energy Independence and Security Act of 2007 (EISA). The UPA urges DOE to clarify the definition of nuclear supplier to not include uranium production or conversion services as a covered person under EISA. In the alternative, uranium producers and converters should be excluded under the regulations from any cost allocation formula because neither of these entities would contribute to the proximate causation of a covered nuclear incident. Public Comment re Section 934 of the Energy Independence and Security Act of 2007 More Documents & Publications

372

V+jets production at the CMS  

E-Print Network (OSTI)

Measurements of Vector Boson production in association with jets are presented, using p-p collision data at sqrt{s} = 7 TeV. The measurements presented include Z + jets azimuthal correlations, event shapes, vector boson + jets differential cross section measurements, hard double-parton scattering using W + jets events and electroweak Z + forward - backward jet production.

B. Bilin; for the CMS Collaboration

2014-10-22T23:59:59.000Z

373

Summary: Section 4.1, Part 1 Summary: Section 4.1, Part 1  

E-Print Network (OSTI)

all ten vector space axioms hold, we can conclude that S is a vector space. Summary: Section 4.1, PartSummary: Section 4.1, Part 1 Summary: Section 4.1, Part 1 #12;A vector space is a nonempty set V of objects, called vectors, on which are defined addition and scalar multiplication, subject to the ten

Myers, Amy

374

Total cross-section for photon-axion conversions in external electromagnetic field  

E-Print Network (OSTI)

We reconsider the conversion of the photon into axion in the external electromagnetic fields, namely in the static fields and in a periodic field of the wave guide. The total cross-sections for the conversion are evaluated in detail. The result shows that with strong strength of external electromagnetic fields, the cross-sections are large enough to measure the axion production. In the wave guide there exists the resonant conversion at the low energies, in which the value of cross-sections is much enhanced

D. V. Soa; H. N. Long; T. D. Tham

2014-02-20T23:59:59.000Z

375

Neutron Total Cross Sections at 20 Mev  

Science Journals Connector (OSTI)

With the T(d, n)He4 reaction as a monoenergetic source of neutrons of about 20 Mev, the total cross sections of 13 elements have been measured by a transmission experiment. These cross sections vary approximately as A23 as is to be expected from the continuum theory of nuclear reactions. The cross section for hydrogen at 19.93 Mev is 0.504±0.01 barn. This result, together with other results at lower energies, seems to require a Yukawa potential in both the singlet and triplet n-p states and a singlet effective range that is lower than that obtained from p-p scattering data.

Robert B. Day and Richard L. Henkel

1953-10-15T23:59:59.000Z

376

Squark and gluino production with jets  

SciTech Connect

We present cross section predictions for squark and gluino production at the LHC, in association with up to two additional hard jets. These cross sections can be very large in comparison to the inclusive Born rates. Because hadron collider experiments utilize hard jets in the reconstruction of cascade decays or as a way to separate squark and gluino production, the understanding of these processes is crucial. We show to what degree hard jet radiation can be described by shower algorithms and point out how tuning these showers, for example to top quark pair production, could help reduce theoretical uncertainties for new physics searches at the LHC.

Plehn, T.; /Munich, Max Planck Inst.; Rainwater, D.; /Rochester U.; Skands, P.; /Fermilab

2005-10-01T23:59:59.000Z

377

Alternative Fuels Data Center: Ethanol Production Equipment Tax Exemption  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Ethanol Production Ethanol Production Equipment Tax Exemption to someone by E-mail Share Alternative Fuels Data Center: Ethanol Production Equipment Tax Exemption on Facebook Tweet about Alternative Fuels Data Center: Ethanol Production Equipment Tax Exemption on Twitter Bookmark Alternative Fuels Data Center: Ethanol Production Equipment Tax Exemption on Google Bookmark Alternative Fuels Data Center: Ethanol Production Equipment Tax Exemption on Delicious Rank Alternative Fuels Data Center: Ethanol Production Equipment Tax Exemption on Digg Find More places to share Alternative Fuels Data Center: Ethanol Production Equipment Tax Exemption on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Ethanol Production Equipment Tax Exemption

378

Alternative Fuels Data Center: Hydrogen Production and Distribution  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Production Production and Distribution to someone by E-mail Share Alternative Fuels Data Center: Hydrogen Production and Distribution on Facebook Tweet about Alternative Fuels Data Center: Hydrogen Production and Distribution on Twitter Bookmark Alternative Fuels Data Center: Hydrogen Production and Distribution on Google Bookmark Alternative Fuels Data Center: Hydrogen Production and Distribution on Delicious Rank Alternative Fuels Data Center: Hydrogen Production and Distribution on Digg Find More places to share Alternative Fuels Data Center: Hydrogen Production and Distribution on AddThis.com... More in this section... Hydrogen Basics Production & Distribution Research & Development Related Links Benefits & Considerations Stations Vehicles Laws & Incentives

379

Alternative Fuels Data Center: Biodiesel Production and Distribution  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biodiesel Production Biodiesel Production and Distribution to someone by E-mail Share Alternative Fuels Data Center: Biodiesel Production and Distribution on Facebook Tweet about Alternative Fuels Data Center: Biodiesel Production and Distribution on Twitter Bookmark Alternative Fuels Data Center: Biodiesel Production and Distribution on Google Bookmark Alternative Fuels Data Center: Biodiesel Production and Distribution on Delicious Rank Alternative Fuels Data Center: Biodiesel Production and Distribution on Digg Find More places to share Alternative Fuels Data Center: Biodiesel Production and Distribution on AddThis.com... More in this section... Biodiesel Basics Blends Production & Distribution Specifications Related Links Benefits & Considerations Stations Vehicles Laws & Incentives

380

Alternative Fuels Data Center: Biofuels Production Facility Grants  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biofuels Production Biofuels Production Facility Grants to someone by E-mail Share Alternative Fuels Data Center: Biofuels Production Facility Grants on Facebook Tweet about Alternative Fuels Data Center: Biofuels Production Facility Grants on Twitter Bookmark Alternative Fuels Data Center: Biofuels Production Facility Grants on Google Bookmark Alternative Fuels Data Center: Biofuels Production Facility Grants on Delicious Rank Alternative Fuels Data Center: Biofuels Production Facility Grants on Digg Find More places to share Alternative Fuels Data Center: Biofuels Production Facility Grants on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Biofuels Production Facility Grants The Renewable Fuels Development Program provides grants for the

Note: This page contains sample records for the topic "full section production" 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

Alternative Fuels Data Center: Biodiesel Production Investment Tax Credit  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biodiesel Production Biodiesel Production Investment Tax Credit to someone by E-mail Share Alternative Fuels Data Center: Biodiesel Production Investment Tax Credit on Facebook Tweet about Alternative Fuels Data Center: Biodiesel Production Investment Tax Credit on Twitter Bookmark Alternative Fuels Data Center: Biodiesel Production Investment Tax Credit on Google Bookmark Alternative Fuels Data Center: Biodiesel Production Investment Tax Credit on Delicious Rank Alternative Fuels Data Center: Biodiesel Production Investment Tax Credit on Digg Find More places to share Alternative Fuels Data Center: Biodiesel Production Investment Tax Credit on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Biodiesel Production Investment Tax Credit

382

Alternative Fuels Data Center: Hydrogen Production and Retail Requirements  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Hydrogen Production Hydrogen Production and Retail Requirements to someone by E-mail Share Alternative Fuels Data Center: Hydrogen Production and Retail Requirements on Facebook Tweet about Alternative Fuels Data Center: Hydrogen Production and Retail Requirements on Twitter Bookmark Alternative Fuels Data Center: Hydrogen Production and Retail Requirements on Google Bookmark Alternative Fuels Data Center: Hydrogen Production and Retail Requirements on Delicious Rank Alternative Fuels Data Center: Hydrogen Production and Retail Requirements on Digg Find More places to share Alternative Fuels Data Center: Hydrogen Production and Retail Requirements on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Hydrogen Production and Retail Requirements

383

Alternative Fuels Data Center: Biofuels Production Property Tax Exemption  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biofuels Production Biofuels Production Property Tax Exemption to someone by E-mail Share Alternative Fuels Data Center: Biofuels Production Property Tax Exemption on Facebook Tweet about Alternative Fuels Data Center: Biofuels Production Property Tax Exemption on Twitter Bookmark Alternative Fuels Data Center: Biofuels Production Property Tax Exemption on Google Bookmark Alternative Fuels Data Center: Biofuels Production Property Tax Exemption on Delicious Rank Alternative Fuels Data Center: Biofuels Production Property Tax Exemption on Digg Find More places to share Alternative Fuels Data Center: Biofuels Production Property Tax Exemption on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Biofuels Production Property Tax Exemption

384

Alternative Fuels Data Center: Ethanol Production Investment Tax Credits  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Ethanol Production Ethanol Production Investment Tax Credits to someone by E-mail Share Alternative Fuels Data Center: Ethanol Production Investment Tax Credits on Facebook Tweet about Alternative Fuels Data Center: Ethanol Production Investment Tax Credits on Twitter Bookmark Alternative Fuels Data Center: Ethanol Production Investment Tax Credits on Google Bookmark Alternative Fuels Data Center: Ethanol Production Investment Tax Credits on Delicious Rank Alternative Fuels Data Center: Ethanol Production Investment Tax Credits on Digg Find More places to share Alternative Fuels Data Center: Ethanol Production Investment Tax Credits on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Ethanol Production Investment Tax Credits

385

SECTION 205 FCA 48, AS AMENDED MODEL PROJECT PARTNERSHIP AGREEMENT  

E-Print Network (OSTI)

features for Section 205 non- structural flood risk management, Section 206 aquatic ecosystem restoration. Section 205 Structural Flood Risk Management and Section 206 Aquatic Ecosystem Restoration ­ Use only structural flood risk management and to Section 206 aquatic ecosystem restoration. Section 205 Structural

US Army Corps of Engineers

386

SECTION 205 FCA 48, AS AMENDED MODEL PROJECT PARTNERSHIP AGREEMENT  

E-Print Network (OSTI)

allocable to Section 205 structural flood risk management and to Section 206 aquatic ecosystem restoration. Section 205 Structural Flood Risk Management, Section 206 Aquatic Ecosystem Restoration, and Recreation to Section 205 structural flood risk management, to Section 206 aquatic ecosystem restoration

US Army Corps of Engineers

387

Projections of Full-Fuel-Cycle Energy and Emissions Metrics  

E-Print Network (OSTI)

well Drilling and Hydraulic Fracturing. ” Proceedings of thedrilling or by hydraulic fracturing (Holditch 2006; Van Dykegas production by hydraulic fracturing (also known as “

Coughlin, Katie

2013-01-01T23:59:59.000Z

388

Projections of Full-Fuel-Cycle Energy and Emissions Metrics  

E-Print Network (OSTI)

function of the FFC energy intensity parameters. The FFCand c as the energy intensity of fuel production, defined asrepresenting the energy intensity and material losses at

Coughlin, Katie

2013-01-01T23:59:59.000Z

389

Part VI: Section I: Contract Clause  

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

with the same force and effect as if they were given in full text. Upon request, the Contracting Officer will make their full text available. Also, the full text of a clause may be...

390

EOC Title: Logistics Section Chief General Description The Logistics Section Chief is responsible for providing facilities, services, and  

E-Print Network (OSTI)

LOGISTICS EOC Title: Logistics Section Chief General Description The Logistics Section Chief EOC operating requirements. Key Role & Responsibilities � Ensure the logistics function is carried out Staff for Complex Incidents Training for Section Chiefs � Logistics Section Chief Training #12;

Walker, Matthew P.

391

St. Augustinegrass Warm-season turfgrass. Prefers full sun, but  

E-Print Network (OSTI)

St. Augustinegrass Warm-season turfgrass. Prefers full sun, but has a high tolerance for shade-season grass. It does best in full sun and high temperatures. Goes dormant and turns brown in winter. Very

Ishida, Yuko

392

GRR/Section 14-OR-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

GRR/Section 14-OR-d - Section 401 Water Quality Certification GRR/Section 14-OR-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-OR-d - Section 401 Water Quality Certification 14ORDSection410WaterQualityCertification.pdf Click to View Fullscreen Contact Agencies Oregon Department of Environmental Quality U S Army Corps of Engineers Regulations & Policies OAR 340-048: Certification of Compliance with Water Quality Requirements Triggers None specified Click "Edit With Form" above to add content 14ORDSection410WaterQualityCertification.pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range.

393

GRR/Section 14-ID-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

GRR/Section 14-ID-d - Section 401 Water Quality Certification GRR/Section 14-ID-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-ID-d - Section 401 Water Quality Certification 14IDDSection401WaterQualityCertificationProcess.pdf Click to View Fullscreen Contact Agencies Idaho Department of Environmental Quality United States Environmental Protection Agency U S Army Corps of Engineers Regulations & Policies Idaho Environmental Protection and Health Act Idaho Administrative Procedure Act Triggers None specified Click "Edit With Form" above to add content 14IDDSection401WaterQualityCertificationProcess.pdf 14IDDSection401WaterQualityCertificationProcess.pdf Error creating thumbnail: Page number not in range.

394

GRR/Section 14-AK-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

GRR/Section 14-AK-d - Section 401 Water Quality Certification GRR/Section 14-AK-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-AK-d - Section 401 Water Quality Certification 14AKDSection401WaterQualityCertification.pdf Click to View Fullscreen Contact Agencies Alaska Department of Environmental Conservation United States Environmental Protection Agency U S Army Corps of Engineers Regulations & Policies Alaska Water Quality Standards Alaska Statutes Alaska Administrative Code Triggers None specified Click "Edit With Form" above to add content 14AKDSection401WaterQualityCertification.pdf 14AKDSection401WaterQualityCertification.pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range.

395

GRR/Section 14-MT-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

GRR/Section 14-MT-d - Section 401 Water Quality Certification GRR/Section 14-MT-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-MT-d - Section 401 Water Quality Certification 14MTD401WaterQualityCertification (2).pdf Click to View Fullscreen Contact Agencies Montana Department of Environmental Quality Regulations & Policies Federal Clean Water Act (33 USC § 1251 et seq.) Montana Codes Annotated 75-5-401 Aministrative Rules of Montana Chapter 30 Administrative Rules of Montana 17.30.101 through 109 Triggers None specified Click "Edit With Form" above to add content 14MTD401WaterQualityCertification (2).pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range.

396

GRR/Section 12-FD-f - ESA Section 7 Formal Consultation | Open Energy  

Open Energy Info (EERE)

f - ESA Section 7 Formal Consultation f - ESA Section 7 Formal Consultation < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 12-FD-f - ESA Section 7 Formal Consultation 12FDF - ESA Section 7 Formal Consultation.pdf Click to View Fullscreen Contact Agencies Fish and Wildlife Service Bureau of Land Management United States Forest Service Bureau of Reclamation Regulations & Policies Endangered Species Act ESA Sec. 3 ESA Sec. 7 ESA Sec. 9 ESA Sec. 10 50 CFR 17.11-17.12 50 CFR 226 50 CFR 402.02 50 CFR 402.14 Triggers None specified Click "Edit With Form" above to add content 12FDF - ESA Section 7 Formal Consultation.pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range.

397

West Virginia University 1 In this section  

E-Print Network (OSTI)

West Virginia University 1 Minors In this section: � General Statement � Rationale � Requirements to assure that completion of a minor is appropriately recognized and posted to the student's transcript: 1

Mohaghegh, Shahab

398

West Virginia University 1 In this section  

E-Print Network (OSTI)

West Virginia University 1 FERPA In this section: � Notice to Students Regarding FERPA not contractually affiliated with the University. Use and disclosure of this information shall be limited to (1

Mohaghegh, Shahab

399

SECTION J, APPENDIX L - DIVERSITY PLAN GUIDANCE  

National Nuclear Security Administration (NNSA)

L, Page 1 SECTION J APPENDIX L Note: The Diversity Plan shall be submitted to the Contracting Officer in accordance with DEAR 970.5226-1 DIVERSITY PLAN GUIDANCE 12110 In...

400

Part IV: Section G: Contract Administration  

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

G - Page ii PART I SECTION G CONTRACT ADMINISTRATION DATA TABLE OF CONTENTS G.1 Contracting Officer's Representative(s) 1 G.2 Contract Administration 1 G.3 Modification...

Note: This page contains sample records for the topic "full section production" 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

MODELING AND FISSION CROSS SECTIONS FOR AMERICIUM.  

SciTech Connect

This is the final report of the work performed under the LANL contract on the modeling and fission cross section for americium isotopes (May 2004-June 2005). The purpose of the contract was to provide fission cross sections for americium isotopes with the nuclear reaction model code EMPIRE 2.19. The following work was performed: (1) Fission calculations capability suitable for americium was implemented to the EMPIRE-2.19 code. (2) Calculations of neutron-induced fission cross sections for {sup 239}Am to {sup 244g}Am were performed with EMPIRE-2.19 for energies up to 20 MeV. For the neutron-induced reaction of {sup 240}Am, fission cross sections were predicted and uncertainties were assessed. (3) Set of fission barrier heights for each americium isotopes was chosen so that the new calculations fit the experimental data and follow the systematics found in the literature.

ROCHMAN, D.; HERMAN, M.; OBLOZINSKY, P.

2005-05-01T23:59:59.000Z

402

GRR/Sections | Open Energy Information  

Open Energy Info (EERE)

GRR/Sections GRR/Sections < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Roadmap Coverage The roadmapping initiative covers the states show in green on the map below, including California, Nevada, Hawai'i, Alaska, Idaho, Utah, Oregon, and Montana. The roadmap is being developed at the federal and state levels, allowing for future expansion to the local (county) level. Development of the roadmap for two additional states (Colorado and Texas) is underway for Fiscal Year 2013. Click on a state to view Regulatory Roadmap information specific to that state. List of Roadmap Sections Overview Flowchart The flowcharts listed below were developed as part of the Geothermal Regulatory Roadmap project. The flowcharts cover the major requirements for

403

Full-rank Tilings of F 2 Do Not Exist  

E-Print Network (OSTI)

Full-rank Tilings of F 8 2 Do Not Exist #3; Ari Trachtenberg y Alexander Vardy z February 3, 2003 Abstract We show that there are no full-rank tilings of F 8 2 , using a carefully designed exhaustive search. This solves an open problem posed in [5] and implies that a full-rank perfect binary code

Goldberg, Bennett

404

Ultra Low Power Full Adder Topologies Farshad Moradi1  

E-Print Network (OSTI)

on the sense energy recovery full adder (SERF) design and the GDI (Gate diffusion input) technique designs. In this paper, 65nm standard models are used for simulations. Keywords: GDI, SERF, Full adder topologies for full adder based on GDI technique are presented. Moreover, several circuit topologies based

Mahmoodi, Hamid

405

PRODUCTS & MATERIALS  

Science Journals Connector (OSTI)

...Phar-macia Biotech. Circle 141. Cell Culture Production The CellCube offers the fastest, most com-pact system available for high-volume...culture production, according to the manu-facturer. The CellCube not only saves up to four times the space of roller bottles...

1995-08-04T23:59:59.000Z

406

Beauty production in pp collisions at $\\sqrt{s}$ = 2.76 TeV measured via semi-electronic decays  

E-Print Network (OSTI)

The ALICE collaboration at the LHC reports measurement of the inclusive production cross section of electrons from semi-leptonic decays of beauty hadrons with rapidity $|y|Electrons not originating from semi-electronic decay of beauty hadrons are suppressed using the impact parameter of the corresponding tracks. The production cross section of beauty decay electrons is compared to the result obtained with an alternative method which uses the distribution of the azimuthal angle between heavy-flavour decay electrons and charged hadrons. Perturbative QCD calculations agree with the measured cross section within the experimental and theoretical uncertainties. The integrated visible cross section, $\\sigma_{\\mathrm{b} \\rightarrow \\mathrm{e}} = 3.47\\pm0.40(\\mathrm{stat})^{+1.12}_{-1.33}(\\mathrm{sys})\\pm0.07(\\mathrm{norm}) \\mu$b, was extrapolated to full phase space using Fixed Order plus Next-to-Leading Log (FONLL) predictions to obtain the total b$\\bar{\\mathrm{b}}$ production cross section, $\\sigma_{\\mathrm{b\\bar{b}}} = 130\\pm15.1(\\mathrm{stat})^{+42.1}_{-49.8}(\\mathrm{sys})^{+3.4}_{-3.1}(\\mathrm{extr})\\pm2.5(\\mathrm{norm})\\pm4.4(\\mathrm{BR}) \\mu$b.

The ALICE Collaboration

2014-05-16T23:59:59.000Z

407

Absorption cross section of RN black hole  

E-Print Network (OSTI)

The behavior of a charged scalar field in the RN black hole space time is studied using WKB approximation. In the present work it is assumed that matter waves can get reflected from the event horizon. Using this effect, the Hawking temperature and the absorption cross section for RN black hole placed in a charged scalar field are calculated. The absorption cross section $\\sigma _{abs}$ is found to be inversely proportional to square of the Hawking temperature of the black hole.

Sini R.; V. C. Kuriakose

2007-08-23T23:59:59.000Z

408

Alternative Fuels Data Center: Ethanol Production Credit  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Ethanol Production Ethanol Production Credit to someone by E-mail Share Alternative Fuels Data Center: Ethanol Production Credit on Facebook Tweet about Alternative Fuels Data Center: Ethanol Production Credit on Twitter Bookmark Alternative Fuels Data Center: Ethanol Production Credit on Google Bookmark Alternative Fuels Data Center: Ethanol Production Credit on Delicious Rank Alternative Fuels Data Center: Ethanol Production Credit on Digg Find More places to share Alternative Fuels Data Center: Ethanol Production Credit on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Ethanol Production Credit County governments are eligible to receive waste reduction credits for using yard clippings, clean wood waste, or paper waste as feedstock for the

409

Alternative Fuels Data Center: Biofuels Production Promotion  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biofuels Production Biofuels Production Promotion to someone by E-mail Share Alternative Fuels Data Center: Biofuels Production Promotion on Facebook Tweet about Alternative Fuels Data Center: Biofuels Production Promotion on Twitter Bookmark Alternative Fuels Data Center: Biofuels Production Promotion on Google Bookmark Alternative Fuels Data Center: Biofuels Production Promotion on Delicious Rank Alternative Fuels Data Center: Biofuels Production Promotion on Digg Find More places to share Alternative Fuels Data Center: Biofuels Production Promotion on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Biofuels Production Promotion The state legislature supports the Federal "25 x 25" initiative, under which 25% of the total energy consumed in the United States by 2025 would

410

Alternative Fuels Data Center: Biodiesel Production Tax  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biodiesel Production Biodiesel Production Tax to someone by E-mail Share Alternative Fuels Data Center: Biodiesel Production Tax on Facebook Tweet about Alternative Fuels Data Center: Biodiesel Production Tax on Twitter Bookmark Alternative Fuels Data Center: Biodiesel Production Tax on Google Bookmark Alternative Fuels Data Center: Biodiesel Production Tax on Delicious Rank Alternative Fuels Data Center: Biodiesel Production Tax on Digg Find More places to share Alternative Fuels Data Center: Biodiesel Production Tax on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Biodiesel Production Tax A private biodiesel producer that produces less than 5,000 gallons of biodiesel annually is subject to the annual state motor fuel tax. The

411

Alternative Fuels Data Center: Ethanol Production Incentive  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Ethanol Production Ethanol Production Incentive to someone by E-mail Share Alternative Fuels Data Center: Ethanol Production Incentive on Facebook Tweet about Alternative Fuels Data Center: Ethanol Production Incentive on Twitter Bookmark Alternative Fuels Data Center: Ethanol Production Incentive on Google Bookmark Alternative Fuels Data Center: Ethanol Production Incentive on Delicious Rank Alternative Fuels Data Center: Ethanol Production Incentive on Digg Find More places to share Alternative Fuels Data Center: Ethanol Production Incentive on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Ethanol Production Incentive The Missouri Department of Agriculture manages the Missouri Ethanol Producer Incentive Fund (Fund), which provides monthly grants to qualified

412

?^+ and ?(1520) production in pp reactions at high energies  

E-Print Network (OSTI)

We estimate the cross sections for the inclusive production of $\\Theta^+$ and $\\Lambda(1520)$ in $pp$ collisions at high energy using the $K$ exchange diagrams. We find that inclusive $\\Theta^+$ production should be at the level of 1 $\\mu$b at energies~ $\\sqrt{s}~\\gtrsim~10~{\\rm GeV}$. The ratio of $\\Theta^+(1540)$ to $\\Lambda(1520)$ production cross-sections is $\\sim 1%$.

I. M. Narodetskii; M. A. Trusov

2006-01-25T23:59:59.000Z

413

Monthly/Annual Energy Review - renewable section  

Reports and Publications (EIA)

Monthly and latest annual statistics on renewable energy production and consumption and overviews of fuel ethanol and biodiesel.

2015-01-01T23:59:59.000Z

414

Widget:PrintFullVersionButton | Open Energy Information  

Open Energy Info (EERE)

PrintFullVersionButton PrintFullVersionButton Jump to: navigation, search This widget creates a button, which create a button matching the PrintPDF button style, which will direct the user to the assembled page. This template assumes the existence of the PrintPDFButton widget and template. Parameters page - The wiki address of the assembled page, or full version to be printed. cover - The name of a wiki page to use as a cover page (optional) Dependencies Template:PrintFullVersionButton Template:PrintPDFButton Widget:PrintPDFButton Usage This Widget assumes the existence of HTML elements created by the PrintFullVersionButton template, and is called via that template. {{PrintFullVersionButton}} Example {{PrintFullVersionButton}} (displays in the upper right corner of the page) Retrieved from

415

Feasibility Study --Project Full Breeze By the Wind Energy Projects in Action (WEPA) Full Breeze Project team  

E-Print Network (OSTI)

Feasibility Study -- Project Full Breeze By the Wind Energy Projects in Action (WEPA) Full Breeze Department of Facilities approached the wind energy sub-community in the spring of 2009 to assist in a study

416

File:Section106examplereport.pdf | Open Energy Information  

Open Energy Info (EERE)

Section106examplereport.pdf Section106examplereport.pdf Jump to: navigation, search File File history File usage File:Section106examplereport.pdf Size of this preview: 463 × 599 pixels. Other resolution: 464 × 600 pixels. Go to page 1 2 3 4 5 6 7 8 Go! next page → next page → Full resolution ‎(1,272 × 1,645 pixels, file size: 2.23 MB, MIME type: application/pdf, 8 pages) File history Click on a date/time to view the file as it appeared at that time. Date/Time Thumbnail Dimensions User Comment current 10:35, 20 November 2012 Thumbnail for version as of 10:35, 20 November 2012 1,272 × 1,645, 8 pages (2.23 MB) Dklein2012 (Talk | contribs) You cannot overwrite this file. Edit this file using an external application (See the setup instructions for more information) File usage There are no pages that link to this file.

417

GRR/Section 14-CO-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

4-CO-d - Section 401 Water Quality Certification 4-CO-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-CO-d - Section 401 Water Quality Certification 14CODSection401WaterQualityCertification.pdf Click to View Fullscreen Contact Agencies Colorado Department of Public Health and Environment Regulations & Policies 5 CCR 1002-82 Colorado Water Quality Control Act Triggers None specified Click "Edit With Form" above to add content 14CODSection401WaterQualityCertification.pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Flowchart Narrative Section 401 of the Clean Water Act (CWA) requires a Water Quality

418

GRR/Section 14-TX-d - Section 401 Water Quality Certification | Open Energy  

Open Energy Info (EERE)

4-TX-d - Section 401 Water Quality Certification 4-TX-d - Section 401 Water Quality Certification < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 14-TX-d - Section 401 Water Quality Certification 14TXDSection401WaterQualityCertification (2).pdf Click to View Fullscreen Contact Agencies Railroad Commission of Texas Regulations & Policies 16 TAC 3.93 - RRC Water Quality Certification 16 TAC 3.30 - MOU between the RRC and the TCEQ Triggers None specified Click "Edit With Form" above to add content 14TXDSection401WaterQualityCertification (2).pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Flowchart Narrative Section 401 of the Clean Water Act (CWA) requires a Water Quality

419

Uploading STI Products vs. Site Hosting of STI Products | Scientific and  

Office of Scientific and Technical Information (OSTI)

Uploading STI Products vs. Site Hosting of STI Products Uploading STI Products vs. Site Hosting of STI Products Print page Print page Email page Email page For unclassified unlimited and controlled unclassified (except for UCNI) there are currently two options (described below) for sites to provide the actual electronic STI products resulting from DOE-funded activities to OSTI. An important note, regardless of method used to provide the STI product to OSTI, the product cannot be encrypted or password protected. Site Uploads the STI Product Sites can upload their unclassified unlimited and controlled unclassified (except UCNI) STI products to OSTI via the following STI product submission/transmission methods: AN 241.1 Web Version Batch Upload AN 241.3 Web Version Refer to the formats section of this website for additional details related

420

New Products  

Science Journals Connector (OSTI)

...security of unmatched sample traceability. Manufactured from high-quality polypropylene in a fully automated class-7 cleanroom environment ensures the laser-etched alphanumeric tubes exhibit absolute product consistency, near-zero contaminants...

2013-01-11T23:59:59.000Z

Note: This page contains sample records for the topic "full section production" 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

New Products  

Science Journals Connector (OSTI)

...bind cells and biomolecules through passive hydrophobic interactions. Molded from ultrapure polystyrene in a class 100,000 cleanroom production environment, the untreated culture plates are supplied with lids in individual sterile packs. The plates include...

2013-06-28T23:59:59.000Z

422

Production Materials  

Science Journals Connector (OSTI)

It is obvious that we must bring a number of things into our controlled environment besides clean conditioned air, equipment, and ultrapure water. If we are to do any production work, or research involving the pr...

M. Kozicki; S. Hoenig; P. Robinson

1991-01-01T23:59:59.000Z

423

New Products  

Science Journals Connector (OSTI)

...Finally, as a personal pipetting system, Liquidator 96 fits any benchtop or laminar-flow cabinet making it suitable for cleanroom conditions. Mettler Toledo For info: 800-472-4646 www.mt.com/liquidator Electronically submit your new product...

2014-01-03T23:59:59.000Z

424

Forest Products  

Energy.gov (U.S. Department of Energy (DOE))

Purchased energy remains the third largest manufacturing cost for the forest products industry–despite its extensive use of highly efficient co-generation technology. The industry has worked with...

425

NEW PRODUCTS:  

Science Journals Connector (OSTI)

......also be used with other heating elements and probes...content of diesel and heating oils. A highly specific titration...requirements for fuel oil products are consistently...de- scriptions, and prices are included for columns......

New Products

1979-12-01T23:59:59.000Z

426

New Products  

Science Journals Connector (OSTI)

...the area scanned. When the earth's thermal gradient appears, the vibrating mirror...Write for a Product Data Sheet giving specifications, typical drying perform-ance, and...pebble-bed heaters and electrical insulation at elevated temperatures. (Minneapolis-Honeywell...

Joshua Stern

1961-11-10T23:59:59.000Z

427

Hydrogen Production  

Fuel Cell Technologies Publication and Product Library (EERE)

This 2-page fact sheet provides a brief introduction to hydrogen production technologies. Intended for a non-technical audience, it explains how different resources and processes can be used to produ

428

Observation of $t$-channel electroweak top quark production  

SciTech Connect

The top quark is the heaviest known fundamental particle, with a mass of 172.0{sub -1.3}{sup +0.9}GeV. This is nearly twice the mass of the second heaviest known particle, the Z boson, and roughly the mass of a gold atom. Because of its unusually large mass, studying the top quark may provide insight into the Higgs mechanism and other beyond the standard model physics. Only two accelerators in the world are powerful enough to produce top quarks. The Tevatron, which first accelerated protons in 1983, has produced almost 400,000 top quarks, roughly half at each of its two detectors: DO and CDF. The LHC is a much newer accelerator which currently has accumulated about 0.5% as much data as the Tevatron. However, when running at full luminosity, the LHC is capable of producing a top quark about once every second and will quickly surpass the Tevatron as the leading producer of top quarks. This analysis uses data from the D0 detector at the Tevatron, which are described in chapter 3. Top quarks are produced most often in pairs of top and anti-top quarks through an interaction of the strong force. This production mode was first observed in 1995 at the Tevatron. However, top quarks can also be produced though an electroweak interaction, which produces just one top quark. This production mode was first observed at the Tevatron in 2008. Single top quark production can occur in different channels. In this analysis, a measurement of the cross section of the t-channel production mode is performed. This measurement uses 5.4 fb{sup -1} of data and uses the technique of boosted decision trees in order to separate signal from background events. The t-channel cross section is measured to be: {sigma}(p{bar p} {yields} tqb + X) = 3.03{sub -0.66}{sup +0.78}pb (0.0.1). Additional cross section measurements were also performed for the s-channel as well as the s + t-channel. The measurement of each one of these three cross sections was repeated three times using different techniques, and all three methods were combined into a 'super-method' which achieves the best performance. The details of these additional measurements are shown in appendix A.

Triplett, Nathan; /Iowa State U.

2011-04-01T23:59:59.000Z

429

Alternative Fuels Data Center: Ethanol and Biobutanol Production Incentive  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Ethanol and Biobutanol Ethanol and Biobutanol Production Incentive to someone by E-mail Share Alternative Fuels Data Center: Ethanol and Biobutanol Production Incentive on Facebook Tweet about Alternative Fuels Data Center: Ethanol and Biobutanol Production Incentive on Twitter Bookmark Alternative Fuels Data Center: Ethanol and Biobutanol Production Incentive on Google Bookmark Alternative Fuels Data Center: Ethanol and Biobutanol Production Incentive on Delicious Rank Alternative Fuels Data Center: Ethanol and Biobutanol Production Incentive on Digg Find More places to share Alternative Fuels Data Center: Ethanol and Biobutanol Production Incentive on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Ethanol and Biobutanol Production Incentive

430

Alternative Fuels Data Center: Biofuels Production and Distribution  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biofuels Production Biofuels Production and Distribution Contracts to someone by E-mail Share Alternative Fuels Data Center: Biofuels Production and Distribution Contracts on Facebook Tweet about Alternative Fuels Data Center: Biofuels Production and Distribution Contracts on Twitter Bookmark Alternative Fuels Data Center: Biofuels Production and Distribution Contracts on Google Bookmark Alternative Fuels Data Center: Biofuels Production and Distribution Contracts on Delicious Rank Alternative Fuels Data Center: Biofuels Production and Distribution Contracts on Digg Find More places to share Alternative Fuels Data Center: Biofuels Production and Distribution Contracts on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type

431

Alternative Fuels Data Center: Biodiesel Production and Blending Equipment  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Biodiesel Production Biodiesel Production and Blending Equipment Tax Credit to someone by E-mail Share Alternative Fuels Data Center: Biodiesel Production and Blending Equipment Tax Credit on Facebook Tweet about Alternative Fuels Data Center: Biodiesel Production and Blending Equipment Tax Credit on Twitter Bookmark Alternative Fuels Data Center: Biodiesel Production and Blending Equipment Tax Credit on Google Bookmark Alternative Fuels Data Center: Biodiesel Production and Blending Equipment Tax Credit on Delicious Rank Alternative Fuels Data Center: Biodiesel Production and Blending Equipment Tax Credit on Digg Find More places to share Alternative Fuels Data Center: Biodiesel Production and Blending Equipment Tax Credit on AddThis.com... More in this section... Federal State

432

Alternative Fuels Data Center: Alternative Fuel Production Subsidy  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Fuel Fuel Production Subsidy Prohibition to someone by E-mail Share Alternative Fuels Data Center: Alternative Fuel Production Subsidy Prohibition on Facebook Tweet about Alternative Fuels Data Center: Alternative Fuel Production Subsidy Prohibition on Twitter Bookmark Alternative Fuels Data Center: Alternative Fuel Production Subsidy Prohibition on Google Bookmark Alternative Fuels Data Center: Alternative Fuel Production Subsidy Prohibition on Delicious Rank Alternative Fuels Data Center: Alternative Fuel Production Subsidy Prohibition on Digg Find More places to share Alternative Fuels Data Center: Alternative Fuel Production Subsidy Prohibition on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Alternative Fuel Production Subsidy Prohibition

433

Alternative Fuels Data Center: Sustainable Biofuels Production Practices  

Alternative Fuels and Advanced Vehicles Data Center (EERE)

Sustainable Biofuels Sustainable Biofuels Production Practices to someone by E-mail Share Alternative Fuels Data Center: Sustainable Biofuels Production Practices on Facebook Tweet about Alternative Fuels Data Center: Sustainable Biofuels Production Practices on Twitter Bookmark Alternative Fuels Data Center: Sustainable Biofuels Production Practices on Google Bookmark Alternative Fuels Data Center: Sustainable Biofuels Production Practices on Delicious Rank Alternative Fuels Data Center: Sustainable Biofuels Production Practices on Digg Find More places to share Alternative Fuels Data Center: Sustainable Biofuels Production Practices on AddThis.com... More in this section... Federal State Advanced Search All Laws & Incentives Sorted by Type Sustainable Biofuels Production Practices

434

Category:Regulatory Roadmap Federal Sections | Open Energy Information  

Open Energy Info (EERE)

Category Category Edit History Facebook icon Twitter icon » Category:Regulatory Roadmap Federal Sections Jump to: navigation, search GRR-logo.png Looking for the Geothermal Regulatory Roadmap? Click here for a user-friendly list of Geothermal Regulatory Roadmap pages. This is the Regulatory Roadmap Federal Sections category. Add.png Add an Section Pages in category "Regulatory Roadmap Federal Sections" The following 48 pages are in this category, out of 48 total. G GRR/Section 1-FD-a - Land Use Planning Process GRR/Section 1-FD-b - Land Use Plan Amendment Process GRR/Section 11-FD-a - NHPA Section 106 - Resource Survey GRR/Section 11-FD-b - Tribal Consultation GRR/Section 11-FD-c - NHPA Section 106 - Effects Assessment GRR/Section 11-FD-d - NHPA Section 106 - Consultation

435

Property:GRR/SectionNumber | Open Energy Information  

Open Energy Info (EERE)

SectionNumber SectionNumber Jump to: navigation, search Property Name GRR/SectionNumber Property Type Number Description The section number of a section in the Geothermal Regulatory Roadmap. The value of this property is derived automatically by the section template and is used in sorting sections on the GRR Home page. Subproperties This property has the following 2 subproperties: G GRR/Section 6-HI-d - Oversize and/or Overweight Vehicles and Loads Permit GRR/Section 7 - Power Plant Siting/Construction Overview Pages using the property "GRR/SectionNumber" Showing 25 pages using this property. (previous 25) (next 25) G GRR/Section 1 - Land Use Overview + 1 + GRR/Section 1-AK-a - Land Use Considerations + 1 + GRR/Section 1-CA-a - State Land Use Planning + 1 +

436

Category:Regulatory Roadmap Overview Sections | Open Energy Information  

Open Energy Info (EERE)

Sections Sections Jump to: navigation, search GRR-logo.png Looking for the Geothermal Regulatory Roadmap? Click here for a user-friendly list of Geothermal Regulatory Roadmap pages. This is the Regulatory Roadmap Overview Sections category. Add.png Add an Section Pages in category "Regulatory Roadmap Overview Sections" The following 22 pages are in this category, out of 22 total. G GRR/Section 1 - Land Use Overview GRR/Section 10 - On-Site Evaluation Process GRR/Section 11 - Cultural Resource Assessment GRR/Section 12 - Flora & Fauna Resource Assessment Process GRR/Section 13 - Land Use Assessment Process GRR/Section 14 - Water Resource Assessment GRR/Section 15 - Air Quality Assessment Process GRR/Section 16 - Geological Resources Assessment Process G cont.

437

Category:Regulatory Roadmap State Sections | Open Energy Information  

Open Energy Info (EERE)

Regulatory Roadmap State Sections Regulatory Roadmap State Sections Jump to: navigation, search GRR-logo.png Looking for the Geothermal Regulatory Roadmap? Click here for a user-friendly list of Geothermal Regulatory Roadmap pages. This is the Regulatory Roadmap State Sections category. Add.png Add an Section Pages in category "Regulatory Roadmap State Sections" The following 200 pages are in this category, out of 339 total. (previous 200) (next 200) G GRR/Section 1-AK-a - Land Use Considerations GRR/Section 1-CA-a - State Land Use Planning GRR/Section 1-HI-a - Land Use Considerations GRR/Section 1-ID-a - Land Use Considerations GRR/Section 1-MT-a - Land Use Considerations GRR/Section 1-NV-a - State Land Use Planning GRR/Section 1-OR-a - Land Use Considerations GRR/Section 11-AK-a - State Cultural Considerations

438

Sectional Model Flume Facilities | Open Energy Information  

Open Energy Info (EERE)

Sectional Model Flume Facilities Sectional Model Flume Facilities Jump to: navigation, search Basic Specifications Facility Name Sectional Model Flume Facilities Overseeing Organization United States Army Corp of Engineers (ERDC) Hydrodynamic Testing Facility Type Flume Length(m) 21.3 Beam(m) 1.4 Depth(m) 2.4 Water Type Freshwater Cost(per day) Contact POC Towing Capabilities Towing Capabilities None Wavemaking Capabilities Wavemaking Capabilities Yes Maximum Wave Height(m) 0.0 Wave Period Range(s) 0.0 Current Velocity Range(m/s) 0.0 Programmable Wavemaking No Simulated Beach No Channel/Tunnel/Flume Channel/Tunnel/Flume Yes Recirculating No Wind Capabilities Wind Capabilities None Control and Data Acquisition Description Automated data acquisition and control system Cameras None Available Sensors Flow, Pressure Range(psi), Turbulence, Velocity, Wave Probe

439

Utah Antiquities Section | Open Energy Information  

Open Energy Info (EERE)

Antiquities Section Antiquities Section Jump to: navigation, search Name Utah Antiquities Section Address 300 S. Rio Grande Street Place Salt Lake City, Utah Zip 84101 Coordinates 40.7623958°, -111.9047846° 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":40.7623958,"lon":-111.9047846,"alt":0,"address":"","icon":"","group":"","inlineLabel":"","visitedicon":""}]}

440

Temperature Dependent Neutron Scattering Sections for Polyethylene  

E-Print Network (OSTI)

This note presents neutron scattering cross sections for polyethylene at 296 K, 77 K and 4 K derived from a new scattering kernel for neutron scattering off of hydrogen in polyethylene. The kernel was developed in ENDF-6 format as a set of S(alpha,beta) tables using the LEAPR module of the NJOY94 code package. The polyethylene density of states (from 0 to sub eV) adopted to derive the new kernel is presented. We compare our calculated room temperature total scattering cross sections and double differential cross sections at 232 meV at various angles with the available experimental data (at room temperature), and then extrapolate the calculations to lower temperatures (77K and 4K). The new temperature dependent scattering kernel gives a good quantitative fit to the available room temperature data and has a temperature dependence that is qualitatively consistent with thermodynamics.

Roger E. Hill; C. -Y. Liu

2003-09-05T23:59:59.000Z

Note: This page contains sample records for the topic "full section production" 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

One-piece, composite crucible with integral withdrawal/discharge section  

DOE Patents (OSTI)

A one-piece, composite open-bottom casting mold with integral withdrawal section is fabricated by thermal spraying of materials compatible with and used for the continuous casting of shaped products of reactive metals and alloys such as, for example, titanium and its alloys or for the gas atomization thereof.

Besser, Matthew (Iowa State Univ., Ames, IA); Terpstra, Robert L. (Iowa State Univ., Ames, IA); Sordelet, Daniel J. (Iowa State Univ., Ames, IA); Anderson, Iver E. (Iowa State Univ., Ames, IA); Hartman, Alan D.; Argetsinger, Edward R.; Hansen, Jeffrey S.; Paige, Jack I.; Turner, Paul C.

2002-07-30T23:59:59.000Z

442

Charm quark and D^* cross sections in deeply inelastic scattering at DESY HERA  

E-Print Network (OSTI)

A next-to-leading order Monte Carlo program for the calculation of heavy quark cross sections in deeply inelastic scattering is described. Concentrating on charm quark and D^*(2010) production at HERA, several distributions are presented and their variation with respect to charm quark mass, parton distribution set, and renormalization-factorization scale is studied.

B. W. Harris; J. Smith

1997-06-11T23:59:59.000Z

443

MTRG/Ascension Management Plan 2002 SECTION 5: THREATS AND RECOMMENDED MANAGEMENT  

E-Print Network (OSTI)

MTRG/Ascension Management Plan 2002 14 SECTION 5: THREATS AND RECOMMENDED MANAGEMENT and control of pet cats 8) Continuation of ban on harvest of turtle products We give an account of all threats.1 General Habitat Degradation 5.1.1. Mining of Beach Sand 5.1.2. Light Pollution 5.1.3 Threat of Fuel Spill

Exeter, University of

444

SECTION 205 FCA 48, AS AMENDED MODEL PROJECT PARTNERSHIP AGREEMENT  

E-Print Network (OSTI)

for Section 205 non- structural flood risk management, Section 206 aquatic ecosystem restoration 205 Structural Flood Risk Management and Section 206 Aquatic Ecosystem Restoration ­ Use only structural flood risk management and to Section 206 aquatic ecosystem restoration. Section 205 Structural

US Army Corps of Engineers

445

Appendix - Neutron Scattering Lengths and Cross Sections  

Science Journals Connector (OSTI)

Abstract In this appendix, we present an updated table of neutron scattering lengths and cross sections for most of the known nuclides, based on preexisting works. We include the coherent and incoherent scattering lengths, as well as the spin-dependent scattering lengths b+ and b?, in cases where this information is available. Also presented are the scattering coherent, incoherent, total, and absorption cross sections. We present an overview of the fundamental theory of the magnitudes to which the table is referred, and also a summary of the main experimental techniques used in determining these magnitudes.

Javier Dawidowski; José Rolando Granada; Javier Roberto Santisteban; Florencia Cantargi; Luis Alberto Rodríguez Palomino

2013-01-01T23:59:59.000Z

446

Precise neutron inelastic cross section measurements  

SciTech Connect

The design of a new generation of nuclear reactors requires the development of a very precise neutron cross section database. Ongoing experiments performed at dedicated facilities aim to the measurement of such cross sections with an unprecedented uncertainty of the order of 5% or even smaller. We give an overview of such a facility: the Gamma Array for Inelastic Neutron Scattering (GAINS) installed at the GELINA neutron source of IRMM, Belgium. Some of the most challenging difficulties of the experimental approach are emphasized and recent results are shown.

Negret, Alexandru [Horia Hulubei National Institute for Physics and Nuclear Engineering, Reactorului 30, 077125 Bucharest-Magurele (Romania)

2012-11-20T23:59:59.000Z

447

Total Cross Sections for Neutron Scattering  

E-Print Network (OSTI)

Measurements of neutron total cross-sections are both extensive and extremely accurate. Although they place a strong constraint on theoretically constructed models, there are relatively few comparisons of predictions with experiment. The total cross-sections for neutron scattering from $^{16}$O and $^{40}$Ca are calculated as a function of energy from $50-700$~MeV laboratory energy with a microscopic first order optical potential derived within the framework of the Watson expansion. Although these results are already in qualitative agreement with the data, the inclusion of medium corrections to the propagator is essential to correctly predict the energy dependence given by the experiment.

C. R. Chinn; Ch. Elster; R. M. Thaler; S. P. Weppner

1994-10-19T23:59:59.000Z

448

FULL FUEL CYCLE ASSESSMENT WELL TO TANK ENERGY INPUTS,  

E-Print Network (OSTI)

FULL FUEL CYCLE ASSESSMENT WELL TO TANK ENERGY INPUTS, EMISSIONS, AND WATER IMPACTS Prepared For be divided into two parts: · Well-to-Tank (WTT) Feedstock extraction, transport, storage, processing, distribution, transport, and storage · Tank-to-Wheels (TTW) Refueling, consumption and evaporation The full

449

Towards Topic Driven Access to Full Text Documents  

E-Print Network (OSTI)

Towards Topic Driven Access to Full Text Documents Caterina Caracciolo, Willem van Hage access to full text documents. The methodology we propose is a combination of topic segmentation and coherent documents that can be used in two ways: as a basis for automatically generating hypertext links

de Rijke, Maarten

450

New orthogonal space-time block codes with full diversity  

E-Print Network (OSTI)

It has been shown from the Hurwitz-Radon theorem that square complex orthogonal space-time code designs cannot achieve full diversity and full rate simul-taneously, except in the two transmit antenna case. However, this result does not consider non...

Dalton, Lori Anne

2012-06-07T23:59:59.000Z

451

Kaon photo-production on the nucleon and deuteron  

E-Print Network (OSTI)

Isobaric models for the photo-production of K$^+$ are discussed and their predictions are shown in the K$^0$ photo-production. The models are further used in spectator model calculations of the K$^0$ photo-production on deuteron. Considerable dependence of the inclusive cross section on the elementary amplitude was found.

P. Bydzovsky; M. Sotona; O. Hashimoto; T. Takahashi

2004-12-09T23:59:59.000Z

452

Annual Energy Review - financial indicators section  

Reports and Publications (EIA)

Annual statistics on consumer energy prices and expenditures, fossil fuel production prices and value, and value of fossil fuel imports and exports back to 1949.

2012-01-01T23:59:59.000Z

453

Fusion of Li and C and a search for entrance channel limitations to fusion cross sections  

Science Journals Connector (OSTI)

Excitation functions have been measured for reaction products from the Li6 and Li7 induced reactions Li6+C12, Li6+C13, Li7+C12, and Li7+C13. These data cover the energy range from Elab=9 to 36 MeV. It was found that the maximum fusion cross sections for these reactions are 780 and 770 mb for the Li6+C12 and Li6+C13, respectively, and 960 and 930 mb for the Li7+C12 and Li7+C13, respectively. The relative uncertainties for these maximum fusion cross sections are about 5%. Comparisons between optical model calculations of the total reaction cross sections and the measured fusion cross sections indicate that total fusion cross sections are substantially smaller than the total reaction cross sections for all four reactions at all energies. For each of the four entrance channels, energy and angular distributions have been measured at four energies for individual mass groups between A=9 and 19 u. Most of these products appear to be evaporation residues. The critical angular momenta deduced from the experimental fusion cross sections are discussed in terms of entrance channel and compound nucleus limitation models for compound nucleus formation. The individual mass groups are discussed in terms of systematics for evaporation residues.NUCLEAR REACTIONS Li6+C12, ELi6=10 to 36 MeV; Li6+C13, ELi6=9.23 to 35.08 MeV; Li7+C12, ELi7=10 to 38 MeV; Li7+C13, ELi7=10 to 34 MeV, measured d2?d? dE for reaction products from A=9 to 19. Extracted ?fus.

L. C. Dennis; K. M. Abdo; A. D. Frawley; K. W. Kemper

1982-09-01T23:59:59.000Z

454

GRR/Section 5-TX-a - Drilling and Well Development | Open Energy  

Open Energy Info (EERE)

GRR/Section 5-TX-a - Drilling and Well Development GRR/Section 5-TX-a - Drilling and Well Development < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 5-TX-a - Drilling and Well Development 05TXADrillingAndWellDevelopment.pdf Click to View Fullscreen Contact Agencies Railroad Commission of Texas Texas Water Development Board Regulations & Policies 16 TAC 3.5: Application To Drill, Deepen, Reenter, or Plug Back 16 TAC 3.78: Fees and Financial Security Requirements 16 TAC 3.37: Statewide Spacing Rule 16 TAC 3.38: Well Densities 16 TAC 3.39: Proration and Drilling Units: Contiguity of Acreage and Exception 16 TAC 3.33: Geothermal Resource Production Test Forms Required Triggers None specified Click "Edit With Form" above to add content

455

GRR/Section 5-WA-a - Drilling and Well Development | Open Energy  

Open Energy Info (EERE)

GRR/Section 5-WA-a - Drilling and Well Development GRR/Section 5-WA-a - Drilling and Well Development < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 5-WA-a - Drilling and Well Development 5-WA-a.pdf Click to View Fullscreen Contact Agencies Washington State Department of Natural Resources Regulations & Policies Geothermal Act 78.60 RCW Geothermal Rules 332-17 WAC Triggers None specified In Washington geothermal drilling and well development are regulated by the Washington State Department of Natural Resources (WSDNR). Geothermal production wells and core holes deeper than 750ft require the developer go through the whole WSDNR permitting process (which requires a public hearing) and require that the developer complete the State Environmental

456

Differential Photoproduction Cross Sections of the Sigma0(1385), Lambda(1405), and Lambda(1520)  

SciTech Connect

We report the exclusive photoproduction cross sections for the Sigma(1385), Lambda(1405), and Lambda(1520) in the reactions gamma + p -> K+ + Y* using the CLAS detector for energies from near the respective production thresholds up to a center-of-mass energy W of 2.85 GeV. The differential cross sections are integrated to give the total exclusive cross sections for each hyperon. Comparisons are made to current theoretical models based on the effective Lagrangian approach and fitted to previous data. The accuracy of these models is seen to vary widely. The cross sections for the Lambda(1405) region are strikingly different for the Sigma+pi-, Sigma0 pi0, and Sigma- pi+ decay channels, indicating the effect of isospin interference, especially at W values close to the threshold.

Moriya, Kei [Indiana U.; Schumacher, Reinhard A. [Carnegie Mellon U.

2013-10-01T23:59:59.000Z

457

GRR/Section 7-MT-a - Energy Facility Siting | Open Energy Information  

Open Energy Info (EERE)

GRR/Section 7-MT-a - Energy Facility Siting GRR/Section 7-MT-a - Energy Facility Siting < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 7-MT-a - Energy Facility Siting 07MTAEnergyFacilitySiting (6).pdf Click to View Fullscreen Contact Agencies Montana Department of Environmental Quality Regulations & Policies Montana Major Facility Siting Act ARM Title 17 Triggers None specified Click "Edit With Form" above to add content 07MTAEnergyFacilitySiting (6).pdf 07MTAEnergyFacilitySiting (6).pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Flowchart Narrative The Montana Major Facility Siting Act governs the siting of energy facilities in Montana. 7-MT-a.1 to 7-MT-a.2 - Does the Power Plant Have a Production Capacity of

458

A review of "Full of Soup and Gold: The Life of Henry Jermyn" by Anthony Adolph  

E-Print Network (OSTI)

of considering the significance of the sites of production and the modes of transmission as part of understanding the poetics of the text and the dynamics of the period. Anthony Adolph. Full of Soup and Gold: The Life of Henry Jermyn. London: Anthony Adolph... the vilified view of Jermyn with a substantial body of new facts and infer- ences which enable him to convincingly reconfigure (indeed, radically reconfigure) his subject?s character and achievements. Adolph presents Jermyn as a capable, energetic...

Maureen E. Mulvihill

2007-01-01T23:59:59.000Z

459

Full-length high-temperature severe fuel damage test No. 2. Final safety analysis  

SciTech Connect

Hazardous conditions associated with performing the Full-Length High- Temperature (FLHT). Severe Fuel Damage Test No. 2 experiment have been analyzed. Major hazards that could cause harm or damage are (1) radioactive fission products, (2) radiation fields, (3) reactivity changes, (4) hydrogen generation, (5) materials at high temperature, (6) steam explosion, and (7) steam pressure pulse. As a result of this analysis, it is concluded that with proper precautions the FLHT- 2 test can be safely conducted.

Hesson, G.M.; Lombardo, N.J.; Pilger, J.P.; Rausch, W.N.; King, L.L.; Hurley, D.E.; Parchen, L.J.; Panisko, F.E.

1993-09-01T23:59:59.000Z

460

UDAC Activities and Products | Department of Energy  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

UDAC Activities and Products UDAC Activities and Products UDAC Activities and Products December 18, 2009 2010 Annual Plan Section 999: 2010 Annual Plan October 22, 2009 UDAC Meeting - October 22, 2009 Meeting minutes from the October 22, 2009 Meeting October 22, 2009 Recommendations: Draft 2010 Section 999 Annual Plan UDAC - Recommendations on Draft 2010 Section 999 Annual Plan October 14, 2009 UDAC Meeting - October 14, 2009 Meeting minutes from the October 14, 2009 meeting September 16, 2009 UDAC Meeting - September 2009 Meeting minutes, agenda, Federal Register notice and presentations from the September 16-17, 2009 meeting July 15, 2009 UDAC Meeting - July 2009 Meeting minutes, Federal Register notice, agenda and presentations from the July 15, 2009 meeting December 19, 2008 UDAC Meeting - December 2008

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461

Secondary Charmonium Production at LHC Energy  

E-Print Network (OSTI)

We consider the production of charmonium by $D\\bar D$ annihilation during the mixed and hadronic phase of Pb-Pb collision at LHC energy. The calculations for secondary $J/\\psi$ and $\\psi^,$ production are performed within a kinetic model taking into account the space-time evolution of a longitudinally and transversely expanding medium. It is shown that the yield of secondary $J/\\psi$ mesons depends strongly on the $J/\\psi$ dissociation cross section with co-moving hadrons. Within the most likely scenario for the dissociation cross section it will be negligible. The secondary production of $\\psi^,$ mesons, however, due to their large cross section above the threshold, can substantially exceed the primary yield.

P. Braun-Munzinger; K. Redlich

1999-08-06T23:59:59.000Z

462

Section I. Summary of Project Activities Section I-A. 2008-2009 Project Summary  

E-Print Network (OSTI)

Section I. Summary of Project Activities Section I-A. 2008-2009 Project Summary University year, we accomplished the following: · Established a dual career opportunity procedure vetted to address, communicate procedures for the new daycare facility, and to explore the potential

Farritor, Shane

463

SECTION 2 -HOSPITAL SALARY (salary paid to the employee by the hospital) SECTION 1 -PERSONAL DETAILS  

E-Print Network (OSTI)

SECTION 2 - HOSPITAL SALARY (salary paid to the employee by the hospital) SECTION 1 - PERSONAL to Advertise via eRecruitment in conjunction with this document. Position Title Appointment Term Hospital - HOSPITAL SUPERANNUATION A base hospital salary amount (including a supplementary clinical loading) plus

Tobar, Michael

464

SECTION 2 -HOSPITAL SALARY (salary paid to the employee by the hospital) SECTION 1 -PERSONAL DETAILS  

E-Print Network (OSTI)

SECTION 2 - HOSPITAL SALARY (salary paid to the employee by the hospital) SECTION 1 - PERSONAL with this document. Funding % Base Salary UWA % HOSPITAL % $ Private Practice Allowance $ Head of Department % Salary Level UWA % HOSPITAL % Base Salary $ Clinical Loading $ Head of School Allowance $ Other

Tobar, Michael

465

Invasion Ecology of Aquatic Animals FAS 4932 (section 8143) and FAS 6932 (Section 6725)  

E-Print Network (OSTI)

Invasion Ecology of Aquatic Animals FAS 4932 (section 8143) and FAS 6932 (Section 6725) Fall 2006 will provide a comprehensive overview of the field of invasion ecology and will emphasize aspects related will be presented the ecological concepts and debates underlying this developing field; the biology and life history

Watson, Craig A.

466

E-Print Network 3.0 - advanced biofuels production Sample Search...  

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

biomass supply, . . . how much land? Future Biofuel Production... Program Section 9005: Bioenergy Program for Advanced Biofuels ... Source: Gray, Matthew - Department of...

467

E-Print Network 3.0 - advanced biofuel production Sample Search...  

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

biomass supply, . . . how much land? Future Biofuel Production... Program Section 9005: Bioenergy Program for Advanced Biofuels ... Source: Gray, Matthew - Department of...

468

HISTORY OF PSYCHOLOGY Psychology 405, Section 001  

E-Print Network (OSTI)

1 HISTORY OF PSYCHOLOGY Psychology 405, Section 001 Department of Psychology Michigan State University Fall, 2012 Class meeting times: Tuesday, Thursday, 12:40-2:00 p.m. Place: 120 Psychology Building Instructor: L.J. Harris Office: 217 Psychology Building Office Hours: Mondays, 3:00 - 5 p.m.; other times

Liu, Taosheng

469

SECTION 1 -CERTIFICATION BY AUTHORISED DEPARTMENTAL OFFICER  

E-Print Network (OSTI)

SECTION 1 - CERTIFICATION BY AUTHORISED DEPARTMENTAL OFFICER Earnings Code Description Rate No Ext. Employee ID Surname Given Names Title Date of Birth (dd/mm/yy) Sex (tick one) male female Home Phone No. Postal Address (for group certificates, etc) Postcode Is an Employment Declaration Form

Tobar, Michael

470

electronic reprint Acta Crystallographica Section D  

E-Print Network (OSTI)

electronic reprint Acta Crystallographica Section D Biological Crystallography ISSN 0907 is retained. Republication of this article or its storage in electronic databases or the like is not permitted of hidden Markov models electronic reprint #12;research papers 1898 Gough SUPERFAMILY database Acta Cryst

Gough, Julian

471

Navy's Section 2922a Legislation Success Stories  

Energy.gov (U.S. Department of Energy (DOE))

Presentation—given at the Fall 2011 Federal Utility Partnership Working Group (FUPWG) meeting—features U.S. Department of Navy success stories in relation to Section 2922a legislation, which involves contracts for energy or fuel for military installations.

472

Student's Department: Course/Section Number  

E-Print Network (OSTI)

Student's Department: Course/Section Number: Course Title: Instructor: Explanation of why coursework has not yet been completed: Description of coursework remaining to be completed: Graduate Student is Requested: Arts & Sciences Students: Shriver Hall 28 (Graduate Affairs and Admissions Office) Engineering

Weaver, Harold A. "Hal"

473

Finance 400 Section 001 (10591) Investment Analysis  

E-Print Network (OSTI)

1 Finance 400 Section 001 (10591) Investment Analysis Fall 2013 Instructor Mark Pyles Class 9 covers basic investment theory with emphasis given to the analysis of securities, portfolio management will entail the student has a working knowledge in: types of financial investments financial market

Young, Paul Thomas

474

Employee Handbook & Policy Manual Section Heading  

E-Print Network (OSTI)

Employee Handbook & Policy Manual Section Heading: 2.00 ­ Administrative & Personnel Policies in this document: · Person With Disabilities: a person having a physical or mental impairment which substantially. A "common wheelchair" does not exceed 30 inches in width and 48 inches in length measured two inches from

475

Energy and Society Week 4 Section Solution  

E-Print Network (OSTI)

. What is the main flaw of GDP per capita as the development metric? ANS: Open end question. Main flaw1 9/17/2014 Energy and Society Week 4 Section Solution TOPIC 1: Energy & Development: [iClicker]-1. Influence = B. Energy consumption = (/$) C. Carbon = 2 (/) ANS: [C] Note carbon

Kammen, Daniel M.

476

Energy and Society Section Handout Week 9  

E-Print Network (OSTI)

Power loss Loss of electrical power to heat in a resistor = 2 Key components of a power grid1 Energy and Society Section Handout ­ Week 9 Topics 1. Grid 2. Q&A on midterm 1. Grid Key Concepts 10 = 12 Total current = 10 = 100 b) The power is delivered to the distribution grid by a 240. k

Kammen, Daniel M.

477

and Cross-Sections at the LHC  

Science Journals Connector (OSTI)

Abstract Measurements of the Z ? ? ? and W ? ? ? ? cross-sections at the LHC with data taken at s = 7 TeV are reported for the ATLAS, CMS, and \\{LHCb\\} experiments. All results are found to agree with the Standard Model.

Philip Ilten

2014-01-01T23:59:59.000Z

478

Microsoft Word - Section 311 AL FAL Feb 17 2010 | Department...  

Office of Environmental Management (EM)

Section 311 AL FAL Feb 17 2010 Microsoft Word - Section 311 AL FAL Feb 17 2010 Microsoft Word - Section 311 AL FAL Feb 17 2010 More Documents & Publications Microsoft Word -...

479

GRR/Section 12-FD-d - ESA Section 10 Take Permit | Open Energy Information  

Open Energy Info (EERE)

Page Page Edit with form History Facebook icon Twitter icon » GRR/Section 12-FD-d - ESA Section 10 Take Permit < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 12-FD-d - ESA Section 10 Take Permit 12FDDESASection10TakePermit.pdf Click to View Fullscreen Contact Agencies Fish and Wildlife Service National Marine Fisheries Service Regulations & Policies Endangered Species Act National Environmental Policy Act Triggers None specified Click "Edit With Form" above to add content 12FDDESASection10TakePermit.pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Flowchart Narrative

480

GRR/Section 11-FD-c - NHPA Section 106 - Effects Assessment | Open Energy  

Open Energy Info (EERE)

FD-c - NHPA Section 106 - Effects Assessment FD-c - NHPA Section 106 - Effects Assessment < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 11-FD-c - NHPA Section 106 - Effects Assessment 11FDCNHPASection106EffectsAssessment.pdf Click to View Fullscreen Contact Agencies Advisory Council on Historic Preservation Regulations & Policies National Historic Preservation Act 36 CFR 800 - Protection of Historic Properties Triggers None specified Click "Edit With Form" above to add content 11FDCNHPASection106EffectsAssessment.pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Flowchart Narrative The Federal agency must proceed to the assessment of adverse effects when

Note: This page contains sample records for the topic "full section production" 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.


481

GRR/Section 11-FD-d - NHPA Section 106 - Consultation | Open Energy  

Open Energy Info (EERE)

form form View source History View New Pages Recent Changes All Special Pages Semantic Search/Querying Get Involved Help Apps Datasets Community Login | Sign Up Search Page Edit with form History Facebook icon Twitter icon » GRR/Section 11-FD-d - NHPA Section 106 - Consultation < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 11-FD-d - NHPA Section 106 - Consultation 11FDDNHPASection106Consultation.pdf Click to View Fullscreen Contact Agencies Advisory Council on Historic Preservation Regulations & Policies National Historic Preservation Act 36 CFR 800 - Protection of Historic Properties Triggers None specified Click "Edit With Form" above to add content 11FDDNHPASection106Consultation.pdf

482

GRR/Section 12-FD-e -ESA Section 7 Informal Consultation | Open Energy  

Open Energy Info (EERE)

e -ESA Section 7 Informal Consultation e -ESA Section 7 Informal Consultation < GRR Jump to: navigation, search GRR-logo.png GEOTHERMAL REGULATORY ROADMAP Roadmap Home Roadmap Help List of Sections Section 12-FD-e -ESA Section 7 Informal Consultation 12FDE - ESASection7InformalConsultation.pdf Click to View Fullscreen Contact Agencies Fish and Wildlife Service Bureau of Land Management United States Forest Service Bureau of Reclamation Regulations & Policies Endangered Species Act 50 CFR 17.11-17.12 50 CFR 402.02 50 CFR 402.13 50 CFR 402.14 Triggers None specified Click "Edit With Form" above to add content 12FDE - ESASection7InformalConsultation.pdf Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range. Error creating thumbnail: Page number not in range.

483

Eastern Section?SSA 2012 Meeting Report  

Science Journals Connector (OSTI)

...Characterization Program for Coal Combustion Products...over 100 million tons of coal combustion products...Troublingly, CCP and mining waste facilities have...earthquake reminds us that Appalachia is susceptible to potential...dynamic properties of coal fly ash. The goal of...

484

SECTION E-GEOLOGY AND GEOGRAPHY  

Science Journals Connector (OSTI)

...pumped. The daily production was recently about...interesting facts. Production is from four sands...of these was the site of Springfield...Summer Series of Kansas. The Abo sandstone...and probably into Kansas. It is the surface...Terrestrial Magnetism and Electricity, Chaiirman, L...

Rollin T. Chamberlin

1920-05-14T23:59:59.000Z

485

THE PHILADELPHIA SESSIONS OF SECTIONS AND SOCIETIES  

Science Journals Connector (OSTI)

...products, the production of a lard-like fat from cottonseed oil, and the new lacqueroid...certain spraying oils, at the College...the University of Illinois. The study of...sciences through cumulative research in a given field and education should...

1927-01-28T23:59:59.000Z

486

Policy Flash 2014-10 Update to Congressional Notifications - Full  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

0 Update to Congressional Notifications - Full 0 Update to Congressional Notifications - Full Implementation of Advanced Notification of Awards (ANA) System Policy Flash 2014-10 Update to Congressional Notifications - Full Implementation of Advanced Notification of Awards (ANA) System The ANA system can be accessed directly at: https://iportalwc.doe.gov/pls/apex/f?p=ANA This flash and its attachments may be viewed at http://management.energy.gov/policy_guidance/policy_flashes.htm. Questions concerning this policy flash should be directed to Elle Clayton at 202-287-1444 or ellen.clayton@hq.doe.gov. New Policy_Flash_2013- ANA1172013 ec.pdf ANA User's Guide.pdf More Documents & Publications POLICY FLASH 2014-10 UPDATE TO CONGRESSIONAL NOTIFICATION_ FULL IMPLEMENTATION OF ANA SYSTEM Policy Flash 2013-36 Update to Congressional Notifications - Acquisition

487

2012 Reliability & Markets Peer Review - Full Presentations | Department of  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Reliability & Markets Peer Review - Full Presentations Reliability & Markets Peer Review - Full Presentations 2012 Reliability & Markets Peer Review - Full Presentations The Transmission Reliability R&D Reliability & Markets Peer Review included 11 presentations over 2 days on August 7 - 8, 2012 at Cornell University in Ithaca, NY. The full presentations are available below. Presentation summaries are also available. 2012 R&M Peer Review - Transmission Investment Assessment Under Uncertainty - Ben Hobbs 2012 R&M Peer Review - Renewable Integration Through Risk-Limiting Dispatch - Pravin Varaiya 2012 R&M Peer Review - Development and Testing of New Tools - Ray Zimmerman 2012 R&M Peer Review - Commercialization of the SuperOPF Framework - Hsiao-Dong Chiang 2012 R&M Peer Review - Essence of Structure Preserving Network Reductions -

488

Business, Government and Tech Leaders Give the Full Perspective |  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Business, Government and Tech Leaders Give the Full Perspective Business, Government and Tech Leaders Give the Full Perspective Business, Government and Tech Leaders Give the Full Perspective February 24, 2012 - 4:45pm Addthis Secretary of Energy Steven Chu speaking at the 2011 ARPA-E Energy Innovation Summit. | Energy Department file photo. Secretary of Energy Steven Chu speaking at the 2011 ARPA-E Energy Innovation Summit. | Energy Department file photo. Ben Dotson Ben Dotson Project Coordinator for Digital Reform, Office of Public Affairs Check out the full conference program for more on the 2012 ARPA-E Energy Innovation Summit. When the third annual ARPA-E Energy Innovation Summit convenes in Washington, DC, next week, key innovators from across the country and around the world will meet to share ideas for solving our greatest energy

489

Category:FullServiceRestaurant | Open Energy Information  

Open Energy Info (EERE)

FullServiceRestaurant FullServiceRestaurant Jump to: navigation, search Go Back to PV Economics By Building Type Pages in category "FullServiceRestaurant" This category contains only the following page. O Openei test page Media in category "FullServiceRestaurant" The following 77 files are in this category, out of 77 total. SVFullServiceRestaurant Albuquerque NM Public Service Co of NM.png SVFullServiceRestauran... 66 KB SVFullServiceRestaurant Atlantic City NJ Public Service Elec & Gas Co.png SVFullServiceRestauran... 63 KB SVFullServiceRestaurant Baltimore MD Baltimore Gas & Electric Co.png SVFullServiceRestauran... 69 KB SVFullServiceRestaurant Bismarck ND Montana-Dakota Utilities Co (North Dakota).png SVFullServiceRestauran... 72 KB SVFullServiceRestaurant Boulder CO Public Service Co of Colorado.png

490

Full-length Ebola glycoprotein accumulates in the endoplasmic reticulum  

Science Journals Connector (OSTI)

The Filoviridae family comprises of Ebola and Marburg viruses, which are known to ... pathogens. The envelope glycoprotein (GP) of Ebola virus, which mediates entry into target cells ... with full-length and muci...

Suchita Bhattacharyya; Thomas J Hope

2011-01-01T23:59:59.000Z

491

FULL FUEL CYCLE ASSESSMENT TANK TO WHEELS EMISSIONS  

E-Print Network (OSTI)

FULL FUEL CYCLE ASSESSMENT TANK TO WHEELS EMISSIONS AND ENERGY CONSUMPTION Prepared For: California to Tank, Criteria Pollutants, Multi-media impacts, EMFAC #12;#12;vii Table of Contents Acknowledgements

492

Putting together the full solar tandem cell | Center for Bio...  

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

Center Video Library Bisfuel Picture Gallery Putting together the full solar tandem cell 24 Oct 2012 Ben Sherman is a graduate student working in the Gust-Moore-Moore...

493

Full-Field Stress Measurement From Strain and Load Data  

Science Journals Connector (OSTI)

In experimental mechanics, the possibility of tracking on component surfaces the full-field stress and strain states during deformation, always stimulated the research and the study of new measurement techniqu...

Giovanni B. Broggiato; Luca Cortese

2007-01-01T23:59:59.000Z

494

Full Useful Life (120,000 miles) Exhaust Emission Performance...  

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

Full Useful Life (120,000 miles) Exhaust Emission Performance of a NOx Adsorber and Diesel Particle Filter Equipped Passenger Car and Medium-Duty Engine in Conjunction with...

495

Full-Color Emission and Temperature Dependence of the Luminescence...  

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

Luminescence in Poly-P -Phenylene Ethynylene-ZnS:Mn2+ Composite Particles. Full-Color Emission and Temperature Dependence of the Luminescence in Poly-P -Phenylene...

496

Full-Arm Haptics in an Accessibility Task Matthew Frey  

E-Print Network (OSTI)

Full-Arm Haptics in an Accessibility Task Matthew Frey Department of Mechanical Engineering University of Utah David E. Johnson John Hollerbach School of Computing University of Utah ABSTRACT

Hollerbach, John M.

497

Full Steam Ahead for PV in US Homes?  

E-Print Network (OSTI)

solar investment tax credits (ITCs) for an unprecedentedITC on the full cost (or “tax credit basis”) of the system.of the rebate, the tax credit basis to which the federal ITC

Bolinger, Mark A

2009-01-01T23:59:59.000Z

498

Pre- and Post-Full-Application General Information  

Office of Energy Efficiency and Renewable Energy (EERE)

Only those applicants that submit an LOI through the DOE PAMS system by the due date at 5 p.m. Eastern time (ET) are eligible to submit a full application.

499

The spin content of the proton in full QCD  

E-Print Network (OSTI)

We present preliminary results on the proton spin structure function in full QCD. The measurement has been done using 4 flavours of staggered fermions and an improved definition of the lattice topological charge density.

B. Alles; G. Boyd; M. D'Elia; A. Di Giacomo

1997-09-21T23:59:59.000Z

500

The stellar (n,gamma) cross section of 62Ni  

E-Print Network (OSTI)

The 62Ni(n,gamma)63Ni(t_1/2=100+-2 yrs) reaction plays an important role in the control of the flow path of the slow neutron-capture (s-) nucleosynthesis process. We have measured for the first time the total cross section of this reaction for a quasi-Maxwellian (kT = 25 keV) neutron flux. The measurement was performed by fast-neutron activation, combined with accelerator mass spectrometry to detect directly the 63Ni product nuclei. The experimental value of 28.4+-2.8 mb, fairly consistent with a recent theoretical estimate, affects the calculated net yield of 62Ni itself and the whole distribution of nuclei with 62