Sample records for fb faber fn

  1. Notation Index (there exists) Fn-4

    E-Print Network [OSTI]

    Bernstein, Daniel

    -subsets of A) CL-15, Fn-1 |A| (cardinality) CL-3, CL-14 X (standard deviation) Fn-25 S(n, k) (Stirling numbers is equivalent GT-27 probabilistic DT-30 RP-tree is equivalent GT-27 Towers of

  2. Journal Diffusion Factors a measure of diffusion? Tove Faber Frandsen

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    1 Journal Diffusion Factors ­ a measure of diffusion? Tove Faber Frandsen Royal School of Library In this paper we show that the measure of diffusion introduced by Ian Rowlands called the Journal Diffusion Factor (JDF) is highly negatively correlated with the number of citations, leading highly cited journals

  3. Generic Properties of Actions of F_n

    E-Print Network [OSTI]

    Hitchcock, James Mitchell

    2011-10-21T23:59:59.000Z

    GENERIC PROPERTIES OF ACTIONS OF FN A Dissertation by JAMES MITCHELL HITCHCOCK Submitted to the Office of Graduate Studies of Texas A&M University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY August 2010... Major Subject: Mathematics GENERIC PROPERTIES OF ACTIONS OF FN A Dissertation by JAMES MITCHELL HITCHCOCK Submitted to the Office of Graduate Studies of Texas A&M University in partial fulfillment of the requirements for the degree of DOCTOR...

  4. FB Line Basis for Interim Operation

    SciTech Connect (OSTI)

    Shedrow, B.

    1998-10-19T23:59:59.000Z

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

  5. Hkkjrh; izkS|ksfxdh laLFkku fnYyh INDIAN INSTITUTE OF TECHNOLOGY DELHI

    E-Print Network [OSTI]

    Kumar, M. Jagadesh

    /Tteatment:___________From___________To________ (?k) D;k jksxh dks Hkk-izkS-la-vLirky }kjk Hkstk x;k] ;fn ugh] rks lh/ks tkus dk dkj.k crk,a Whether

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

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

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

    2013-07-01T23:59:59.000Z

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

  7. RATIONAL HOMOLOGY OF AUT(Fn) Allen Hatcher* and Karen Vogtmann*

    E-Print Network [OSTI]

    Hatcher, Allen

    homology in dimensions less than seven of the group of automorphisms of a finitely generated free group of arbitrary rank. The only non-zero group in this range is H4(Aut(F4); Q), which is one-dimensional. §1. Introduction In [7] a space An was introduced on which the group Aut(Fn) of automorphisms of a free group

  8. Teaching an Old Scaffold New Tricks: Monobodies Constructed Using Alternative Surfaces of the FN3 Scaffold

    SciTech Connect (OSTI)

    Koide, Akiko; Wojcik, John; Gilbreth, Ryan N.; Hoey, Robert J.; Koide, Shohei (UC)

    2012-06-28T23:59:59.000Z

    The fibronectin type III domain (FN3) has become one of the most widely used non-antibody scaffolds for generating new binding proteins. Because of its structural homology to the immunoglobulin domain, combinatorial libraries of FN3 designed to date have primarily focused on introducing amino acid diversity into three loops that are equivalent to antibody complementarity-determining regions. Here, we report an FN3 library that utilizes alternative positions for presenting amino acid diversity. We diversified positions on a {beta}-sheet and surface loops that together form a concave surface. The new library produced binding proteins (termed 'monobodies') to multiple target proteins, generally with similar efficacy as the original, loop-focused library. The crystal structure of a monobody generated from the new library in complex with its target, the Abl SH2 domain, revealed that a concave surface of the monobody, as intended in our design, bound to a convex surface of the target with the interface area being among the largest of published structures of monobody-target complexes. This mode of interaction differs from a common binding mode for single-domain antibodies and antibody mimics in which recognition loops recognize clefts in targets. Together, this work illustrates the utilization of different surfaces of a single immunoglobulin-like scaffold to generate binding proteins with distinct characteristics.

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

    SciTech Connect (OSTI)

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

    2012-02-14T23:59:59.000Z

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

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

    E-Print Network [OSTI]

    Haller-Dintelmann, Robert

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

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

    E-Print Network [OSTI]

    Diekmann, Martin

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

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

    Open Energy Info (EERE)

    1-6fb9fb7fd076 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information...

  13. Discovery of blue companions to two southern Cepheids: WW Car and FN Vel

    E-Print Network [OSTI]

    Kovtyukh, V; Chekhonadskikh, F; Lemasle, B; Belik, S

    2015-01-01T23:59:59.000Z

    A large number of high-dispersion spectra of classical Cepheids were obtained in the region of the CaII H+K spectral lines. The analysis of these spectra allowed us to detect the presence of a strong Balmer line, H$\\epsilon$, for several Cepheids, interpreted as the signature of a blue companion: the presence of a sufficiently bright blue companion to the Cepheid results in a discernible strengthening of the CaII H + Hepsilon line relative to the CaII K line. We investigated 103 Cepheids, including those with known hot companions (B5-B6 main-sequence stars) in order to test the method. We could confirm the presence of a companion to WW Car and FN Vel (the existence of the former was only suspected before) and we found that these companions are blue hot stars. The method remains efficient when the orbital velocity changes in a binary system cannot be revealed and other methods of binarity detection are not efficient.

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

    E-Print Network [OSTI]

    Seidl, Helmut

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

  15. Constraints to Stop HigherOrder Deforestation FB IV Informatik

    E-Print Network [OSTI]

    Seidl, Helmut

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

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

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

    LeCompte, Thomas J.; Martin, Stephen P.

    2012-02-01T23:59:59.000Z

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

  17. FB EcoSolutions LLC | Open Energy Information

    Open Energy Info (EERE)

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

  18. v9fb: a remote framebuffer infrastructure of linux

    SciTech Connect (OSTI)

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

    2008-01-01T23:59:59.000Z

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

  19. FB-line neutron multiplicity counter operation manual

    SciTech Connect (OSTI)

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

    1997-12-31T23:59:59.000Z

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

  20. Complete genome sequence of Arthrobacter sp. strain FB24

    SciTech Connect (OSTI)

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

    2013-09-30T23:59:59.000Z

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

  1. *DEEP team: S.Faber,G.Illingworth,D.C.Koo,R.Guhathakurta,K.Denda,K.Gebhardt,A.C.Phillips,L.Simard,C.Willmer,M.Im(UCSC) and partners in UC Berkeley, U.Chicago, JHU, and Caltech evolution for E/S0s at z < 1, contrary to the theoretical models and some obser

    E-Print Network [OSTI]

    . For more information on DEEP, check our web site at http://www.ucolick.org/~deep/home.html 4. Conclusion*DEEP team: S.Faber,G.Illingworth,D.C.Koo,R.Guhathakurta,K.Denda,K.Gebhardt,A for a reduced set of DEEP data in the Groth strip. models based on CDM dominated universe predict that 50

  2. Top Quark Production Asymmetries AFBt and AFBl

    SciTech Connect (OSTI)

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

    2012-02-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

    Hodge, C.A.

    2001-06-20T23:59:59.000Z

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

  4. Review of Results from the FN-II Dense Plasma Focus Machine J.J.E. Herrera, F. Castillo, I. Gamboa, J. Rangel

    E-Print Network [OSTI]

    Boyer, Edmond

    Review of Results from the FN-II Dense Plasma Focus Machine J.J.E. Herrera, F. Castillo, I. Gamboa-II is a small dense plasma focus (4.8 kJ at 36 kV), operated at the Universidad Nacional Autónoma de México of the device for X rays within the 20-200 keV range. PACS: 52.58.Lq #12;1. Introduction The dense plasma focus

  5. Annual Report FY2013-- A Kinematically Complete, Interdisciplinary, and Co-Institutional Measurement of the 19F(?,n) Cross-section for Nuclear Safeguards Science

    SciTech Connect (OSTI)

    Peters, William A [ORNL; Smith, Michael Scott [ORNL; Clement, Ryan [INL; Tan, Wanpeng [University of Notre Dame; Stech, Ed [University of Notre Dame; Cizewski, J A [Rutgers University; Febbraro, Michael [University of Michigan; Madurga Flores, Miguel [ORNL

    2013-10-01T23:59:59.000Z

    The goal of this proposal is to enable neutron detection for precision Non-Destructive Assays (NDAs) of actinide-fluoride samples. Neutrons are continuously generated from a UFx matrix in a container or sample as a result of the interaction of alpha particles from uranium-decay ? particles with fluorine nuclei in the matrix. Neutrons from 19F(?,n)22Na were once considered a poorly characterized background for assays of UFx samples via 238U spontaneous fission neutron detection [SMI2010B]. However, the yield of decay-?-driven neutrons is critical for 234,235U LEU and HEU assays, as it can used to determine both the total amount of uranium and the enrichment [BER2010]. This approach can be extremely valuable in a variety of safeguard applications, such as cylinder monitoring in underground uranium storage facilities, nuclear criticality safety studies, nuclear materials accounting, and other nonproliferation applications. The success of neutron-based assays critically depends on an accurate knowledge of the cross section of the (?,n) reaction that generates the neutrons. The 40% uncertainty in the 19F(?,n)22Na cross section currently limits the precision of such assays, and has been identified as a key factor in preventing accurate enrichment determinations [CRO2003]. The need for higher quality cross section data for (?,n) reactions has been a recurring conclusion in reviews of the nuclear data needs to support safeguards. The overarching goal of this project is to enable neutron detection to be used for precision Non- Destructive Assays (NDAs) of actinide-fluoride samples. This will significantly advance safeguards verification at existing declared facilities, nuclear materials accounting, process control, nuclear criticality safety monitoring, and a variety of other nonproliferation applications. To reach this goal, Idaho National Laboratory (INL), in partnership with Oak Ridge National Laboratory (ORNL), Rutgers University (RU), and the University of Notre Dame (UND), will focus on three specific items: (1) making a precision (better than 10 %) determination of the absolute cross section of the 19F(?,n)22Na reaction as a function of energy; (2) determining the spectrum of neutrons and ?-rays emitted from 19F(?,n)22Na over an energy range pertinent to NDA; and (3) performing simulations with this new cross section to extract the neutron yield (neutrons/gram/second) and resulting neutron- and gamma ray-spectra when ? particles interact with fluorine nuclei in actinide samples, to aid in the design and reduce uncertainty of future NDA measurements and simulations.

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

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

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

    2011-09-01T23:59:59.000Z

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

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

    E-Print Network [OSTI]

    Uriarte, Maria

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

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

    Open Energy Info (EERE)

    e40-b090-b31b94f1fb1f No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic...

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

    Open Energy Info (EERE)

    91fb0096e62 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2....

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

    Open Energy Info (EERE)

    5-42c9-bb84-4e9616fb6e55 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic...

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

    Open Energy Info (EERE)

    5-34941e21fb14 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information...

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

    E-Print Network [OSTI]

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

    2010-11-05T23:59:59.000Z

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

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

    Open Energy Info (EERE)

    1-d726fb8fea9e No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information...

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

    Open Energy Info (EERE)

    f-b60505435ca2 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information...

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

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

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

    2011-02-01T23:59:59.000Z

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

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

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

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

    2011-02-01T23:59:59.000Z

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    E-Print Network [OSTI]

    Taylor, Frank E.

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

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

    E-Print Network [OSTI]

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

    2011-07-25T23:59:59.000Z

    We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in ppbar collisions at the Fermilab Tevatron at sqrt{s}=1.96 TeV, focusing on the decay H\\rightarrow\\gamma\\gamma. We compute upper limits on the Higgs boson production cross section times the decay branching fraction in the range 100Higgs boson. With datasets corresponding to 7.0 fb-1 (CDF) and 8.2 fb-1 (D0), the 95% C.L. upper limits on Higgs boson production is a factor of 10.5 times the SM cross section for a Higgs boson mass of 115 GeV/c^2.

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

    SciTech Connect (OSTI)

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

    2013-07-01T23:59:59.000Z

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

  2. 222-S Laboratory analytical report for tank 241-C-106, grab samples 6C-96-1 through 6C-96-16 {ampersand} 6C-96-17-FB

    SciTech Connect (OSTI)

    Esch, R.A.

    1996-08-06T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

    Zhou, Ning; /Columbia U.

    2010-03-01T23:59:59.000Z

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

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

    E-Print Network [OSTI]

    Tevatron Electroweak Working Group

    2014-07-12T23:59:59.000Z

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

  5. Combined CDF and D0 Upper Limits on Standard Model Higgs Boson Production with up to 8.2 fb-1 of Data

    E-Print Network [OSTI]

    The CDF; D0 Collaborations; the TEVNPHWG Working Group

    2011-08-16T23:59:59.000Z

    We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in p-pbar collisions at the Fermilab Tevatron at sqrt(s)=1.96 TeV. The results presented here include those channels which are most sensitive to Higgs bosons with mass between 130 and 200 GeV/c^2, namely searches targeted at Higgs boson decays to W+W-, although acceptance for decays into tau+tau- and gamma gamma is included. Compared to the previous Tevatron Higgs search combination, more data have been added and the analyses have been improved to gain sensitivity. We use the MSTW08 parton distribution functions and the latest gg to H theoretical cross section predictions when testing for the presence of a SM Higgs boson. With up to 7.1 fb-1 of data analyzed at CDF, and up to 8.2 fb-1 at D0, the 95% C.L. upper limits on Higgs boson production is a factor of 0.54 times the SM cross section for a Higgs boson mass of 165 GeV/c^2. We exclude at the 95% C.L. the region 158

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

    SciTech Connect (OSTI)

    Not Available

    2011-07-01T23:59:59.000Z

    We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV, focusing on the decay H {yields} {gamma}{gamma}. We compute upper limits on the Higgs boson production cross section times the decay branching fraction in the range 100 < m{sub H} < 150 GeV/c{sup 2}, and we interpret the results in the context of the standard model. We use the MSTW08 parton distribution functions and the latest theoretical cross section predictions when testing for the presence of a SM Higgs boson. With datasets corresponding to 7.0 fb{sup -1} (CDF) and 8.2 fb{sup -1} (D0), the 95% C.L. upper limits on Higgs boson production is a factor of 10.5 times the SM cross section for a Higgs boson mass of 115 GeV/c{sup 2}.

  7. fn ? C(M,P),M compact. Show that fn converges, uniformly ...

    E-Print Network [OSTI]

    2009-01-09T23:59:59.000Z

    Let M be compact , f,g? : M ? R continuous, ? ? A (A is some index set). Supposing for every ... Prove that the sum of the two u.s.c functions M ? R is also u.s.c..

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

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

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

    2015-04-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

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

    2010-11-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

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

    2010-12-01T23:59:59.000Z

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

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

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

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

    2012-06-01T23:59:59.000Z

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

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

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

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

    2013-06-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

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

    2012-01-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

    Cooke, Mark Stephen; /Columbia U.

    2010-09-01T23:59:59.000Z

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

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

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

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

    2011-10-27T23:59:59.000Z

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

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

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

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

    2012-09-01T23:59:59.000Z

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

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

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

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

    2012-09-01T23:59:59.000Z

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

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

    E-Print Network [OSTI]

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

    2013-06-12T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

    Kim, Tae Jeong; /Korea U.

    2007-06-01T23:59:59.000Z

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

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

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

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

    2012-02-01T23:59:59.000Z

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

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

    E-Print Network [OSTI]

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

    2011-09-20T23:59:59.000Z

    We combine results from CDF and D0 on direct searches for the standard model (SM) Higgs boson (H) in ppbar collisions at the Fermilab Tevatron at sqrt{s}=1.96 TeV. Compared to the previous Tevatron Higgs boson search combination more data have been added, additional channels have been incorporated, and some previously used channels have been reanalyzed to gain sensitivity. We use the MSTW08 parton distribution functions and the latest theoretical cross sections when comparing our limits to the SM predictions. With up to 8.2 fb-1 of data analyzed at CDF and up to 8.6 fb-1 at D0, the 95% C.L. our upper limits on Higgs boson production are factors of 1.17, 1.71, and 0.48 times the values of the SM cross section for Higgs bosons of mass m_H=115 GeV/c^2, 140 GeV/c^2, and 165 GeV/c^2, respectively. The corresponding median upper limits expected in the absence of Higgs boson production are 1.16, 1.16, and 0.57. There is a small (approx. 1 sigma) excess of data events with respect to the background estimation in searches for the Higgs boson in the mass range 125

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

    SciTech Connect (OSTI)

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

    2011-07-01T23:59:59.000Z

    We combine results from CDF and D0 on direct searches for the standard model (SM) Higgs boson (H) in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV. Compared to the previous Tevatron Higgs boson search combination more data have been added, additional channels have been incorporated, and some previously used channels have been reanalyzed to gain sensitivity. We use the MSTW08 parton distribution functions and the latest theoretical cross sections when comparing our limits to the SM predictions. With up to 8.2 fb{sup -1} of data analyzed at CDF and up to 8.6 fb{sup -1} at D0, the 95% C.L. our upper limits on Higgs boson production are factors of 1.17, 1.71, and 0.48 times the values of the SM cross section for Higgs bosons of mass m{sub H} = 115 GeV/c{sup 2}, 140 GeV/c{sup 2}, and 165 GeV/c{sup 2}, respectively. The corresponding median upper limits expected in the absence of Higgs boson production are 1.16, 1.16, and 0.57. There is a small ({approx} 1{sigma}) excess of data events with respect to the background estimation in searches for the Higgs boson in the mass range 125 < m{sub H} < 155 GeV/c{sup 2}. We exclude, at the 95% C.L., a new and larger region at high mass between 156 < m{sub H} < 177 GeV/c{sup 2}, with an expected exclusion region of 148 < m{sub H} < 180 GeV/c{sup 2}.

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

    E-Print Network [OSTI]

    Taylor, Frank E.

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

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

    E-Print Network [OSTI]

    Xie, Si

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

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

    E-Print Network [OSTI]

    Lovley, Derek

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

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

    E-Print Network [OSTI]

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

    2013-09-17T23:59:59.000Z

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

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

    E-Print Network [OSTI]

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

    2013-09-17T23:59:59.000Z

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

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

    E-Print Network [OSTI]

    Taylor, Frank E.

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

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

    E-Print Network [OSTI]

    Alan Barr; James Scoville

    2015-01-27T23:59:59.000Z

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

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

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

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

    2013-07-01T23:59:59.000Z

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

  11. y12 disc 1954 FB

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

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

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

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

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

    2012-08-01T23:59:59.000Z

    We present a search for the standard model Higgs boson produced in association with a W± boson. This search uses data corresponding to an integrated luminosity of 7.5 fb?¹ collected by the CDF detector at the Tevatron. We select WH?l?bb¯ candidate events with two jets, large missing transverse energy, and exactly one charged lepton. We further require that at least one jet be identified to originate from a bottom quark. Discrimination between the signal and the large background is achieved through the use of a Bayesian artificial neural network. The number of tagged events and their distributions are consistent withmore »the standard model expectations. We observe no evidence for a Higgs boson signal and set 95% C.L. upper limits on the WH production cross section times the branching ratio to decay to bb¯ pairs, ?(pp¯?W±H)×B(H?bb¯), relative to the rate predicted by the standard model. For the Higgs boson mass range of 100 to 150 GeV/c² we set observed (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For 115 GeV/c² the upper limit is 3.64 (2.78). The combination of the present search with an independent analysis that selects events with three jets yields more stringent limits ranging from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For 115 and 125 GeV/c² the upper limits are 2.65 (2.60) and 4.36 (3.69), respectively.« less

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

    SciTech Connect (OSTI)

    Aaltonen, T.; Álvarez González, B.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J. A.; Arisawa, T.; Artikov, A.; Asaadi, J.; Ashmanskas, W.; Auerbach, B.; Aurisano, A.; Azfar, F.; Badgett, W.; Bae, T.; Barbaro-Galtieri, A.; Barnes, V. E.; Barnett, B. A.; Barria, P.; Bartos, P.; Bauce, M.; Bedeschi, F.; Behari, S.; Bellettini, G.; Bellinger, J.; Benjamin, D.; Beretvas, A.; Bhatti, A.; Bisello, D.; Bizjak, I.; Bland, K. R.; Blumenfeld, B.; Bocci, A.; Bodek, A.; Bortoletto, D.; Boudreau, J.; Boveia, A.; Brigliadori, L.; Bromberg, C.; Brucken, E.; Budagov, J.; Budd, H. S.; Burkett, K.; Busetto, G.; Bussey, P.; Buzatu, A.; Calamba, A.; Calancha, C.; Camarda, S.; Campanelli, M.; Campbell, M.; Canelli, F.; Carls, B.; Carlsmith, D.; Carosi, R.; Carrillo, S.; Carron, S.; Casal, B.; Casarsa, M.; Castro, A.; Catastini, P.; Cauz, D.; Cavaliere, V.; Cavalli-Sforza, M.; Cerri, A.; Cerrito, L.; Chen, Y. C.; Chertok, M.; Chiarelli, G.; Chlachidze, G.; Chlebana, F.; Cho, K.; Chokheli, D.; Chung, W. H.; Chung, Y. S.; Ciocci, M. A.; Clark, A.; Clarke, C.; Compostella, G.; Convery, M. E.; Conway, J.; Corbo, M.; Cordelli, M.; Cox, C. A.; Cox, D. J.; Crescioli, F.; Cuevas, J.; Culbertson, R.; Dagenhart, D.; d’Ascenzo, N.; Datta, M.; de Barbaro, P.; Dell’Orso, M.; Demortier, L.; Deninno, M.; Devoto, F.; d’Errico, M.; Di Canto, A.; Di Ruzza, B.; Dittmann, J. R.; D’Onofrio, M.; Donati, S.; Dong, P.; Dorigo, M.; Dorigo, T.; Ebina, K.; Elagin, A.; Eppig, A.; Erbacher, R.; Errede, S.; Ershaidat, N.; Eusebi, R.; Farrington, S.; Feindt, M.; Fernandez, J. P.; Field, R.; Flanagan, G.; Forrest, R.; Frank, M. J.; Franklin, M.; Freeman, J. C.; Funakoshi, Y.; Furic, I.; Gallinaro, M.; Garcia, J. E.; Garfinkel, A. F.; Garosi, P.; Gerberich, H.; Gerchtein, E.; Giagu, S.; Giakoumopoulou, V.; Giannetti, P.; Gibson, K.; Ginsburg, C. M.; Giokaris, N.; Giromini, P.; Giurgiu, G.; Glagolev, V.; Glenzinski, D.; Gold, M.; Goldin, D.; Goldschmidt, N.; Golossanov, A.; Gomez, G.; Gomez-Ceballos, G.; Goncharov, M.; González, O.; Gorelov, I.; Goshaw, A. T.; Goulianos, K.; Grinstein, S.; Grosso-Pilcher, C.; Group, R. C.; Guimaraes da Costa, J.; Hahn, S. R.; Halkiadakis, E.; Hamaguchi, A.; Han, J. Y.; Happacher, F.; Hara, K.; Hare, D.; Hare, M.; Harr, R. F.; Hatakeyama, K.; Hays, C.; Heck, M.; Heinrich, J.; Herndon, M.; Hewamanage, S.; Hocker, A.; Hopkins, W.; Horn, D.; Hou, S.; Hughes, R. E.; Hurwitz, M.; Husemann, U.; Hussain, N.; Hussein, M.; Huston, J.; Introzzi, G.; Iori, M.; Ivanov, A.; James, E.; Jang, D.; Jayatilaka, B.; Jeon, E. J.; Jindariani, S.; Jones, M.; Joo, K. K.; Jun, S. Y.; Junk, T. R.; Kamon, T.; Karchin, P. E.; Kasmi, A.; Kato, Y.; Ketchum, W.; Keung, J.; Khotilovich, V.; Kilminster, B.; Kim, D. H.; Kim, H. S.; Kim, J. E.; Kim, M. J.; Kim, S. B.; Kim, S. H.; Kim, Y. K.; Kim, Y. J.; Kimura, N.; Kirby, M.; Klimenko, S.; Knoepfel, K.; Kondo, K.; Kong, D. J.; Konigsberg, J.; Kotwal, A. V.; Kreps, M.; Kroll, J.; Krop, D.; Kruse, M.; Krutelyov, V.; Kuhr, T.; Kurata, M.; Kwang, S.; Laasanen, A. T.; Lami, S.; Lammel, S.; Lancaster, M.; Lander, R. L.; Lannon, K.; Lath, A.; Latino, G.; LeCompte, T.; Lee, E.; Lee, H. S.; Lee, J. S.; Lee, S. W.; Leo, S.; Leone, S.; Lewis, J. D.; Limosani, A.; Lin, C.-J.; Lindgren, M.; Lipeles, E.; Lister, A.; Litvintsev, D. O.; Liu, C.; Liu, H.; Liu, Q.; Liu, T.; Lockwitz, S.; Loginov, A.; Lucchesi, D.; Lueck, J.; Lujan, P.; Lukens, P.; Lungu, G.; Lys, J.; Lysak, R.; Madrak, R.; Maeshima, K.; Maestro, P.; Malik, S.; Manca, G.; Manousakis-Katsikakis, A.; Margaroli, F.; Marino, C.; Martínez, M.; Mastrandrea, P.; Matera, K.; Mattson, M. E.; Mazzacane, A.; Mazzanti, P.; McFarland, K. S.; McIntyre, P.; McNulty, R.; Mehta, A.; Mehtala, P.; Mesropian, C.; Miao, T.; Mietlicki, D.; Mitra, A.; Miyake, H.; Moed, S.; Moggi, N.; Mondragon, M. N.; Moon, C. S.; Moore, R.; Morello, M. J.; Morlock, J.; Movilla Fernandez, P.; Mukherjee, A.; Muller, Th.; Murat, P.; Mussini, M.; Nachtman, J.; Nagai, Y.; Naganoma, J.; Nakano, I.; Napier, A.; Nett, J.; Neu, C.; Neubauer, M. S.; Nielsen, J.; Nodulman, L.; Noh, S. Y.; Norniella, O.; Oakes, L.; Oh, S. H.; Oh, Y. D.; Oksuzian, I.; Okusawa, T.; Orava, R.; Ortolan, L.; Pagan Griso, S.; Pagliarone, C.; Palencia, E.; Papadimitriou, V.; Paramonov, A. A.; Patrick, J.; Pauletta, G.; Paulini, M.; Paus, C.; Pellett, D. E.; Penzo, A.; Phillips, T. J.; Piacentino, G.; Pianori, E.; Pilot, J.; Pitts, K.; Plager, C.; Pondrom, L.; Poprocki, S.; Potamianos, K.; Prokoshin, F.; Pranko, A.; Ptohos, F.; Punzi, G.; Rahaman, A.; Ramakrishnan, V.; Ranjan, N.; Redondo, I.; Renton, P.; Rescigno, M.; Riddick, T.; Rimondi, F.; Ristori, L.; Robson, A.; Rodrigo, T.; Rodriguez, T.; Rogers, E.; Rolli, S.; Roser, R.; Ruffini, F.; Ruiz, A.; Russ, J.; Rusu, V.; Safonov, A.; Sakumoto, W. K.

    2012-08-01T23:59:59.000Z

    We present a search for the standard model Higgs boson produced in association with a W± boson. This search uses data corresponding to an integrated luminosity of 7.5 fb?¹ collected by the CDF detector at the Tevatron. We select WH?l?bb¯ candidate events with two jets, large missing transverse energy, and exactly one charged lepton. We further require that at least one jet be identified to originate from a bottom quark. Discrimination between the signal and the large background is achieved through the use of a Bayesian artificial neural network. The number of tagged events and their distributions are consistent with the standard model expectations. We observe no evidence for a Higgs boson signal and set 95% C.L. upper limits on the WH production cross section times the branching ratio to decay to bb¯ pairs, ?(pp¯?W±H)×B(H?bb¯), relative to the rate predicted by the standard model. For the Higgs boson mass range of 100 to 150 GeV/c² we set observed (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For 115 GeV/c² the upper limit is 3.64 (2.78). The combination of the present search with an independent analysis that selects events with three jets yields more stringent limits ranging from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For 115 and 125 GeV/c² the upper limits are 2.65 (2.60) and 4.36 (3.69), respectively.

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

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

    Aaltonen, T.; Álvarez González, B.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J. A.; Arisawa, T.; Artikov, A.; Asaadi, J.; Ashmanskas, W.; Auerbach, B.; Aurisano, A.; Azfar, F.; Badgett, W.; Bae, T.; Barbaro-Galtieri, A.; Barnes, V. E.; Barnett, B. A.; Barria, P.; Bartos, P.; Bauce, M.; Bedeschi, F.; Behari, S.; Bellettini, G.; Bellinger, J.; Benjamin, D.; Beretvas, A.; Bhatti, A.; Bisello, D.; Bizjak, I.; Bland, K. R.; Blumenfeld, B.; Bocci, A.; Bodek, A.; Bortoletto, D.; Boudreau, J.; Boveia, A.; Brigliadori, L.; Bromberg, C.; Brucken, E.; Budagov, J.; Budd, H. S.; Burkett, K.; Busetto, G.; Bussey, P.; Buzatu, A.; Calamba, A.; Calancha, C.; Camarda, S.; Campanelli, M.; Campbell, M.; Canelli, F.; Carls, B.; Carlsmith, D.; Carosi, R.; Carrillo, S.; Carron, S.; Casal, B.; Casarsa, M.; Castro, A.; Catastini, P.; Cauz, D.; Cavaliere, V.; Cavalli-Sforza, M.; Cerri, A.; Cerrito, L.; Chen, Y. C.; Chertok, M.; Chiarelli, G.; Chlachidze, G.; Chlebana, F.; Cho, K.; Chokheli, D.; Chung, W. H.; Chung, Y. S.; Ciocci, M. A.; Clark, A.; Clarke, C.; Compostella, G.; Convery, M. E.; Conway, J.; Corbo, M.; Cordelli, M.; Cox, C. A.; Cox, D. J.; Crescioli, F.; Cuevas, J.; Culbertson, R.; Dagenhart, D.; d’Ascenzo, N.; Datta, M.; de Barbaro, P.; Dell’Orso, M.; Demortier, L.; Deninno, M.; Devoto, F.; d’Errico, M.; Di Canto, A.; Di Ruzza, B.; Dittmann, J. R.; D’Onofrio, M.; Donati, S.; Dong, P.; Dorigo, M.; Dorigo, T.; Ebina, K.; Elagin, A.; Eppig, A.; Erbacher, R.; Errede, S.; Ershaidat, N.; Eusebi, R.; Farrington, S.; Feindt, M.; Fernandez, J. P.; Field, R.; Flanagan, G.; Forrest, R.; Frank, M. J.; Franklin, M.; Freeman, J. C.; Funakoshi, Y.; Furic, I.; Gallinaro, M.; Garcia, J. E.; Garfinkel, A. F.; Garosi, P.; Gerberich, H.; Gerchtein, E.; Giagu, S.; Giakoumopoulou, V.; Giannetti, P.; Gibson, K.; Ginsburg, C. M.; Giokaris, N.; Giromini, P.; Giurgiu, G.; Glagolev, V.; Glenzinski, D.; Gold, M.; Goldin, D.; Goldschmidt, N.; Golossanov, A.; Gomez, G.; Gomez-Ceballos, G.; Goncharov, M.; González, O.; Gorelov, I.; Goshaw, A. T.; Goulianos, K.; Grinstein, S.; Grosso-Pilcher, C.; Group, R. C.; Guimaraes da Costa, J.; Hahn, S. R.; Halkiadakis, E.; Hamaguchi, A.; Han, J. Y.; Happacher, F.; Hara, K.; Hare, D.; Hare, M.; Harr, R. F.; Hatakeyama, K.; Hays, C.; Heck, M.; Heinrich, J.; Herndon, M.; Hewamanage, S.; Hocker, A.; Hopkins, W.; Horn, D.; Hou, S.; Hughes, R. E.; Hurwitz, M.; Husemann, U.; Hussain, N.; Hussein, M.; Huston, J.; Introzzi, G.; Iori, M.; Ivanov, A.; James, E.; Jang, D.; Jayatilaka, B.; Jeon, E. J.; Jindariani, S.; Jones, M.; Joo, K. K.; Jun, S. Y.; Junk, T. R.; Kamon, T.; Karchin, P. E.; Kasmi, A.; Kato, Y.; Ketchum, W.; Keung, J.; Khotilovich, V.; Kilminster, B.; Kim, D. H.; Kim, H. S.; Kim, J. E.; Kim, M. J.; Kim, S. B.; Kim, S. H.; Kim, Y. K.; Kim, Y. J.; Kimura, N.; Kirby, M.; Klimenko, S.; Knoepfel, K.; Kondo, K.; Kong, D. J.; Konigsberg, J.; Kotwal, A. V.; Kreps, M.; Kroll, J.; Krop, D.; Kruse, M.; Krutelyov, V.; Kuhr, T.; Kurata, M.; Kwang, S.; Laasanen, A. T.; Lami, S.; Lammel, S.; Lancaster, M.; Lander, R. L.; Lannon, K.; Lath, A.; Latino, G.; LeCompte, T.; Lee, E.; Lee, H. S.; Lee, J. S.; Lee, S. W.; Leo, S.; Leone, S.; Lewis, J. D.; Limosani, A.; Lin, C.-J.; Lindgren, M.; Lipeles, E.; Lister, A.; Litvintsev, D. O.; Liu, C.; Liu, H.; Liu, Q.; Liu, T.; Lockwitz, S.; Loginov, A.; Lucchesi, D.; Lueck, J.; Lujan, P.; Lukens, P.; Lungu, G.; Lys, J.; Lysak, R.; Madrak, R.; Maeshima, K.; Maestro, P.; Malik, S.; Manca, G.; Manousakis-Katsikakis, A.; Margaroli, F.; Marino, C.; Martínez, M.; Mastrandrea, P.; Matera, K.; Mattson, M. E.; Mazzacane, A.; Mazzanti, P.; McFarland, K. S.; McIntyre, P.; McNulty, R.; Mehta, A.; Mehtala, P.; Mesropian, C.; Miao, T.; Mietlicki, D.; Mitra, A.; Miyake, H.; Moed, S.; Moggi, N.; Mondragon, M. N.; Moon, C. S.; Moore, R.; Morello, M. J.; Morlock, J.; Movilla Fernandez, P.; Mukherjee, A.; Muller, Th.; Murat, P.; Mussini, M.; Nachtman, J.; Nagai, Y.; Naganoma, J.; Nakano, I.; Napier, A.; Nett, J.; Neu, C.; Neubauer, M. S.; Nielsen, J.; Nodulman, L.; Noh, S. Y.; Norniella, O.; Oakes, L.; Oh, S. H.; Oh, Y. D.; Oksuzian, I.; Okusawa, T.; Orava, R.; Ortolan, L.; Pagan Griso, S.; Pagliarone, C.; Palencia, E.; Papadimitriou, V.; Paramonov, A. A.; Patrick, J.; Pauletta, G.; Paulini, M.; Paus, C.; Pellett, D. E.; Penzo, A.; Phillips, T. J.; Piacentino, G.; Pianori, E.; Pilot, J.; Pitts, K.; Plager, C.; Pondrom, L.; Poprocki, S.; Potamianos, K.; Prokoshin, F.; Pranko, A.; Ptohos, F.; Punzi, G.; Rahaman, A.; Ramakrishnan, V.; Ranjan, N.; Redondo, I.; Renton, P.; Rescigno, M.; Riddick, T.; Rimondi, F.; Ristori, L.; Robson, A.; Rodrigo, T.; Rodriguez, T.; Rogers, E.; Rolli, S.; Roser, R.; Ruffini, F.; Ruiz, A.; Russ, J.; Rusu, V.; Safonov, A.; Sakumoto, W. K.

    2012-08-01T23:59:59.000Z

    We present a search for the standard model Higgs boson produced in association with a W± boson. This search uses data corresponding to an integrated luminosity of 7.5 fb?¹ collected by the CDF detector at the Tevatron. We select WH?l?bb¯ candidate events with two jets, large missing transverse energy, and exactly one charged lepton. We further require that at least one jet be identified to originate from a bottom quark. Discrimination between the signal and the large background is achieved through the use of a Bayesian artificial neural network. The number of tagged events and their distributions are consistent with the standard model expectations. We observe no evidence for a Higgs boson signal and set 95% C.L. upper limits on the WH production cross section times the branching ratio to decay to bb¯ pairs, ?(pp¯?W±H)×B(H?bb¯), relative to the rate predicted by the standard model. For the Higgs boson mass range of 100 to 150 GeV/c² we set observed (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For 115 GeV/c² the upper limit is 3.64 (2.78). The combination of the present search with an independent analysis that selects events with three jets yields more stringent limits ranging from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For 115 and 125 GeV/c² the upper limits are 2.65 (2.60) and 4.36 (3.69), respectively.

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

    SciTech Connect (OSTI)

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

    2010-06-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

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

    2010-04-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

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

    2010-07-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

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

    2012-03-29T23:59:59.000Z

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

  19. The TIME-WAIT state in TCP and Its Effect on Busy Servers Theodore Faber

    E-Print Network [OSTI]

    Faber, Ted

    and other sharing methods will not alleviate it. We have observed HTTP throughput reductions of as much such as HTTP and FTP incur a per-connection memory load from TCP that can adversely affect their connection as 50% under SunOS 4.1.3 due to this loading. This paper advocates off-loading the memory requirements

  20. The TIME-WAIT state in TCP and Its Effect on Busy Servers Theodore Faber

    E-Print Network [OSTI]

    Faber, Ted

    and other sharing methods will not alleviate it. We have observed HTTP throughput reductions of as much such as HTTP and FTP incur a per­connection memory load from TCP that can adversely affect their connection as 50% under SunOS 4.1.3 due to this loading. This paper advocates off­loading the memory requirements

  1. Replicated Placements in the Polyhedron Model Peter Faber, Martin Griebl, and Christian Lengauer

    E-Print Network [OSTI]

    Passau, Universität

    communication time. We aim at minimizing the communication time by using replicated storage. 1 Introduction be recognized by traditional code mo- tion techniques. However, this comes possibly at the price of increased, this improvement may come at the price of in- creased communication time. This is because intermediate results have

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

    SciTech Connect (OSTI)

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

    2010-08-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

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

    2010-08-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

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

    2010-08-01T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

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

    2011-10-27T23:59:59.000Z

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

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

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

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

    2012-09-01T23:59:59.000Z

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

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

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

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

    2012-09-01T23:59:59.000Z

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

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

    E-Print Network [OSTI]

    ATLAS Collaboration

    2012-05-30T23:59:59.000Z

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

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

    SciTech Connect (OSTI)

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

    2012-02-01T23:59:59.000Z

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

  10. Search for the standard model Higgs boson produced in association with a Z boson in 7.9 fb[superscript ?1] of p[bar-over p] collisions at ?s = 1.96 TeV using the CDF II detector

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    We present a search for the standard model Higgs boson produced in association with a Z boson, using up to 7.9 fb[superscript ?1] of integrated luminosity from p[bar-over p] collisions collected with the CDF II detector. ...

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

    E-Print Network [OSTI]

    D0 Collaboration

    2013-01-07T23:59:59.000Z

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

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

    E-Print Network [OSTI]

    D0 Collaboration

    2013-01-22T23:59:59.000Z

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

  13. Combined CDF and Dzero Upper Limits on Standard Model Higgs Boson Production at High Mass (155-200 GeV/c2) with 3 fb-1 of data

    E-Print Network [OSTI]

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

    2008-08-05T23:59:59.000Z

    We combine results from CDF and DO searches for a standard model Higgs boson in ppbar collisions at the Fermilab Tevatron, at sqrt{s}=1.96 TeV. With 3.0 fb-1 of data analyzed at CDF, and at DO, the 95% C.L. upper limits on Higgs boson production are a factor of 1.2, 1.0 and 1.3 higher than the SM cross section for a Higgs boson mass of m_{H}=$165, 170 and 175 GeV, respectively. We exclude at 95% C.L. a standard model Higgs boson of m_H=170 GeV. Based on simulation, the ratios of the corresponding median expected upper limit to the Standard Model cross section are 1.2, 1.4 and 1.7. Compared to the previous Higgs Tevatron combination, more data and refined analysis techniques have been used. These results extend significantly the individual limits of each experiment and provide new knowledge on the mass of the standard model Higgs boson beyond the LEP direct searches.

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

    SciTech Connect (OSTI)

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

    2012-04-12T23:59:59.000Z

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

  15. Universitt Konstanz FB Informatik und Informationswissenschaft

    E-Print Network [OSTI]

    Reiterer, Harald

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

  16. y12 1950-55 FB

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

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

  17. Physics 214 Winter 2013 The Riemann-Lebesgue Lemma

    E-Print Network [OSTI]

    California at Santa Cruz, University of

    a f(t) eit dt = f(t) i eit b a - 1 i b a f (t) eit dt = eib f(b) - eia f(a) it - f (t) (i)2 eit b a + 1 (i)2 b a f (t) eit dt = N-1 n=0 (-1)n eib f(n) (b) - eia f(n) (a) (i)n+1 + O 1 N+1 , (4) #12;where

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

    SciTech Connect (OSTI)

    Nett, Jason Michael; /Wisconsin U., Madison

    2010-06-01T23:59:59.000Z

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

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

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

    Abazov, V M [Dubna, JINR; Abbott, B [Oklahoma U.; Acharya, B S [Tata Inst.; Adams, M [Illinois U., Chicago; Adams, T [Florida State U.; Alexeev, G D [Dubna, JINR; Alkhazov, G [St. Petersburg, INP; Alton, A [Augustana Coll., Sioux Falls; Michigan U.; Alverson, G [Northeastern U.; Alves, G A [Rio de Janeiro, CBPF; Ancu, L S [NIKHEF, Amsterdam; Fermilab

    2011-07-26T23:59:59.000Z

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

  20. PROBLEMS ENCOUNTERED DURING THE UP-GRADING TRANSFORMATION OF THE FN-TANDEM OF SACLAY

    E-Print Network [OSTI]

    Boyer, Edmond

    . There is no indication of any SF6 presence in both cases. (The insulating gas was N2 + C02 + SF6 mixture, with respective

  1. Photoelectron Spectroscopy of C60Fn- and C60Fm2-(n=17,33,35...

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

    Further reductive-defluorination of C60F47? in solution resulted in the selective generation of a new fluorofullerene, D2-C60F44, which was also characterized by mass...

  2. DYNAMIC STRUCTURE OF MATRICES OVER FINITE Given an endomorphism of a finite dimensional vector space Fn

    E-Print Network [OSTI]

    Ventura, Enric

    DYNAMIC STRUCTURE OF MATRICES OVER FINITE FIELDS E. Ventura March 1997 Abstract Given (Universitat Polit`ecnica de Catalunya). e-mail: ventura@ma3.upc.es #12;And a tree is a connected forest

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

    E-Print Network [OSTI]

    Diekmann, Martin

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

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

    E-Print Network [OSTI]

    Diekmann, Martin

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

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

    E-Print Network [OSTI]

    Diekmann, Martin

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

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

    E-Print Network [OSTI]

    Diekmann, Martin

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

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

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

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

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

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

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

  9. Fermilab Note: FN-0776-E A Large Liquid Argon Time Projection Chamber for Long-baseline, Off-Axis

    E-Print Network [OSTI]

    McDonald, Kirk

    . . . . . . . . . . . . . . . . . . . . . . . . 24 5.2 Argon Cooling, Supply, and Purification . . . . . . . . . . . . . . . . 27 5.3 Electronics

  10. Math 192r, Problem Set #1: Solutions 1. (a) Write and run a program to compute f(n) = n

    E-Print Network [OSTI]

    Propp, James

    . Every plus committee can be matched up with a minus committee, and vice versa, if one simply complements we are choosing a committee of size n from a group consisting of n men and n women, and where. Let's assume that the n men and n women are married in pairs, and that the couples are num- bered 1

  11. IntroductiontoProcessEngineering(PTG) 6. Fluid mechanics

    E-Print Network [OSTI]

    Zevenhoven, Ron

    ) forces: see Figure · Pressure (a scalar!) is defined as surface force / area, for example pb = Fb / (d·w) = p @ z = z1 Picture: KJ05 Fluid volume h·d·w with density and mass m = h·d·w· z = z1ProcessEngineering(PTG) VST rz13 4/96 Fluid statics, static pressure /2 · For the horizontal forces Fn+ Fs = 0 or - py·h·w

  12. 6. Fluid mechanics: fluid statics; fluid dynamics

    E-Print Network [OSTI]

    Zevenhoven, Ron

    Figure Pressure (a scalar!) is defined as surface force / area, for example pb = Fb / (d·w) = p @ z = z1 Picture: KJ05 Fluid volume h·d·w with density and mass m = h·d·w· z = z1 In engineering forces Fn+ Fs = 0 or - py·h·w + py·h·w = 0 py = 0 Similarly Fw+ Fe= 0 gives px = 0, There are three

  13. The Background to the Political Crisis in Ethiopia

    E-Print Network [OSTI]

    Gebeyehu, Asamenew G.W.

    1990-01-01T23:59:59.000Z

    The Government 0/ Ethiopia. (London: Faber and Faber, 1969),15. 3Donald L. Levine. Greater Ethiopia: The Evolution 01 aor thc peoples or Ethiopia. sec Levine abovc. GEBEYEHU

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

  18. Math 192r, Problem Set #1: Solutions 1. (a) Write and run a program to compute f(n) = P n

    E-Print Network [OSTI]

    Propp, James

    : n is odd. Every plus committee can be matched up with a minus committee, and vice versa, if one of signed counting, where we are choosing a committee of size n from a group consisting of n men and n women II: n is even, with n = 2m. Let's assume that the n men and n women are married in pairs

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

    E-Print Network [OSTI]

    Quigg, Chris

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

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

    SciTech Connect (OSTI)

    Quinn, Breese; /Mississippi U.

    2005-01-01T23:59:59.000Z

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

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

    E-Print Network [OSTI]

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

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

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

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

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

    E-Print Network [OSTI]

    Hein, Anke Marion

    2013-01-01T23:59:59.000Z

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

  4. Ethiopia and Eritrea During the Scramble for Africa: A Political Biography of Ras Alulá, 1875-1897

    E-Print Network [OSTI]

    Demissie, Fassil

    1983-01-01T23:59:59.000Z

    and Faber, London, 1974. Ethiopia and Eritrea During thediplomatic and military history of contemporary Ethiopia.this crucial juncture, Ethiopia faced three well organized

  5. ON SPECTRAL DISJOINTNESS OF POWERS FOR RANK-ONE TRANSFORMATIONS AND MOBIUS ORTHOGONALITY

    E-Print Network [OSTI]

    Boyer, Edmond

    ) of X which are Rokhlin towers for the transformation T , that is to say of the form {Fn, T Fn that the sequence (Pn) of Rokhlin towers is in- creasing, which means that for each n, Fn+1 Fn and the levels T i of refining constructions: At stage n 1 we have a Rokhlin tower Pn = {Fn, T Fn, . . . , T hn-1 Fn} whose base

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

    consists of installations requiring more than one wood pole and special poles, transformers, line extensions, non-standard fixtures and lamps, or underground service. The CIAC...

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

  3. Data:71fb7fd5-d384-4529-9590-9990446dae0d | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of North Little Rock, Arkansas (Utility Company) Effective date: 20120901 End date if known: Rate name:...

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

    Open Energy Info (EERE)

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

  5. '('()%0 1 243 57698A@CB(8EDGF24FB(8AHI8A24P

    E-Print Network [OSTI]

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

  9. A bibliography of James Joyce studies

    E-Print Network [OSTI]

    Deming, Robert H.

    1964-01-01T23:59:59.000Z

    : Faber & Faber, 1962.] 55 Kunitz, Stanley J. "James Joyce," in his Living Authors: A Boo\\ of Biographies. New York: H. W. Wilson, 1931, pp. 201-204. Br ici biographical study of Joyce. % Lennartz, Franz. "James Joyce," in his Ausländische Dichter und...

  10. -Oak Ridge National l. oy [EFECT%W flHSUia-9PI gi)N~PCOEjJIR!.,o tS N9IN FN_RWiD)LCTH pgR^ s -

    E-Print Network [OSTI]

    Oak Ridge National Laboratory

    , and cooler) of a I maximum velocity of fluid based on cross- Stirling engine properly. Two major design goals occurring in a real Stirling engine. Irmiance of the GPU-3 and 41.3 enginoe is dii- The effects of pressure 7 ABSItA(I' For ;:Ipo flow Pressure-drop correltl ons for Stirling-en-- I nondimensional variable

  11. CLEAN-ROOM AND C02 -LASER PROCESSING OF ULTRA HIGH-PURITY AL2 0 3 P.A. Morris , R.H. French*, R.L. Coble*, F.N. Tebbe*, U. Chowdhry**

    E-Print Network [OSTI]

    Rollins, Andrew M.

    79 CLEAN-ROOM AND C02 -LASER PROCESSING OF ULTRA HIGH-PURITY AL2 0 3 P.A. Morris , R.H. French*ý, R of the material. The microstructure of a C02 - laser ultra high-purity A12 03 is illustrated. Densification with a C02 -laser. The microstructure of the laser fired ultra high purity A1 2 03 is discussed. Chemical

  12. fn{EE49F893-CA64-40D2-9A32-E9DA8936271E}EIMS+Content&dbwisle@srn.sandia.gov.vsd

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645U.S. DOE Office of ScienceandMesa del SolStrengtheningWildfires mayYuan T. Lee'sdefault Sign Inemc2Bubbles Errors and

  13. Flaggor A Akademiska Hus

    E-Print Network [OSTI]

    Uppsala Universitet

    Bulgarien Canada Chile Colombia Danmark Egypten England / Storbritannien Estland Etiopien EU Finland FN

  14. alamos geostationary orbit: Topics by E-print Network

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

    Websites Summary: PLANE CURVES WITH SMALL LINEAR ORBITS II Paolo Aluffi Carel Faber October 1999 Abstract. The linear orbit' of a plane curve of degree d is its orbit in P...

  15. at20ghz radio survey: Topics by E-print Network

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

    accretion-related emission. R. J. Ivison; S. C. Chapman; S. M. Faber; Ian Smail; A. D. Biggs; C. J. Conselice; G. Wilson; S. Salim; J. -S. Huang; S. P. Wilner 2006-07-12 31 The...

  16. all-wavelength extended groth: Topics by E-print Network

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

    accretion-related emission. R. J. Ivison; S. C. Chapman; S. M. Faber; Ian Smail; A. D. Biggs; C. J. Conselice; G. Wilson; S. Salim; J. -S. Huang; S. P. Wilner 2006-07-12 3 X-ray...

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

    5-657689fe1805 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information...

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    E-Print Network [OSTI]

    Choi, Woo-Young

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    E-Print Network [OSTI]

    Williams, John M.

    2013-01-01T23:59:59.000Z

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    E-Print Network [OSTI]

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

    matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Painesville, Ohio...

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

    Open Energy Info (EERE)

    12-bf96-c9dc6f6562f8 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic...

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

    All territories served by the Company. Definition: Distributed generation facilities are electricity generators owned by the customer, located R close to the point of energy...

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

    Open Energy Info (EERE)

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

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

    Open Energy Info (EERE)

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

  8. Data:0b0b963f-b6b0-41b4-b1b7-aab331be5afc | Open Energy Information

    Open Energy Info (EERE)

    date: 20090801 End date if known: Rate name: Residential:SINGLE PHASE EARTH(COUPLED HEAT PUMP SERVICE EXPERIMENTAL) Sector: Residential Description: This rate is applicable to...

  9. Data:2cac15b8-fb54-4701-8a31-18a7f4543add | Open Energy Information

    Open Energy Info (EERE)

    application to Company for service under this Rider, 3. Has applied for and received economic development assistance from State or local government or other public agency, 4....

  10. Data:C915ea5f-b581-42ae-abc9-a85634ae0b63 | Open Energy Information

    Open Energy Info (EERE)

    1-42ae-abc9-a85634ae0b63 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic...

  11. Data:547fb553-585c-48e3-80ad-9dd9a42e1f13 | Open Energy Information

    Open Energy Info (EERE)

    ad-9dd9a42e1f13 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information...

  12. Data:0695a8d3-4547-45fb-836a-4c9250b827ca | Open Energy Information

    Open Energy Info (EERE)

    under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information...

  13. Data:07595612-c315-4c8a-a671-9f77f7e0a4fb | Open Energy Information

    Open Energy Info (EERE)

    under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information...

  14. Data:80360d01-3f4d-418f-b6ff-9ee26559094f | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Rural Elec Coop Inc Effective date: End date if known: Rate name: 3 Phase...

  15. Data:2d57e112-efb2-4b70-bc8b-8fda9ae547fb | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp Effective date: 20081001 End date if known: Rate name:...

  16. Data:1f06c3a9-fb2c-4234-a83b-c527755c7472 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp Effective date: 20120101 End date if known: Rate name:...

  17. Data:B898c570-c83d-4d10-891e-6c9fb3ac7f72 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp Effective date: 20081001 End date if known: Rate name: Pole...

  18. Data:3e993494-ff87-4728-b8a9-e8fb7dedf5d3 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp (Tennessee) Effective date: 20140601 End date if known: Rate...

  19. Data:Fb7e7aa0-94fe-45dd-a02d-201fc2ee4bd0 | Open Energy Information

    Open Energy Info (EERE)

    Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp (Tennessee) Effective date: 20140601 End date if known: Rate...

  20. Data:26a0fca6-c8b2-43fb-995b-493e85981551 | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Indiana Michigan Power Co (Michigan) Effective date: 20130101 End date if known: Rate name: ECLS -...

  1. Data:437aab84-009f-4fb1-b666-ed5d43c9089f | Open Energy Information

    Open Energy Info (EERE)

    system. APPLICABLE: To firm point-to-point transmission service customers for which power and energy are supplied to the CRSP transmission system at points of interconnection...

  2. Data:C7e6667f-b670-45cf-9eb8-2cb4359e90e3 | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Indiana Michigan Power Co (Michigan) Effective date: 20130101 End date if known: Rate name: ECLS -...

  3. Data:4cf65e73-3ea7-4dff-a563-a52fb0797cbb | Open Energy Information

    Open Energy Info (EERE)

    rate is applicable for service that is supplied through new or rebuilt streetlight systems, including extension of streetlighting systems to additional locations where service...

  4. Data:6d6c822b-888c-423f-b8dc-11514e922c4d | Open Energy Information

    Open Energy Info (EERE)

    Parallel Generation (20 kW or less)- Net Energy Billing Customer-Owned Generation Systems (Greater than 20 kW) Source or reference: http:psc.wi.govapps40tariffs...

  5. Data:5fb276c4-1eb0-46bb-a17a-e2468acd697a | Open Energy Information

    Open Energy Info (EERE)

    rate is applicable for service that is supplied through new or rebuilt streetlight systems, including extension of streetlighting systems to additional locations where service...

  6. Data:55d52ef3-963f-45ad-9f06-c5a900c30fb1 | Open Energy Information

    Open Energy Info (EERE)

    buildings and lighting, sewage treatment facilities, grain elevators and see processors, commercial office buildings, lounges or night clubs, telephone microwave tower, pipeline...

  7. Data:Fb434813-28eb-44a4-ae2e-7b95e553e6e1 | Open Energy Information

    Open Energy Info (EERE)

    Parent: Comments If Company furnishes overhead or underground service to metal or concrete poles in residential subdivision, Customer pays a monthly charge of 1.94 or 3.93...

  8. Data:C7a0d59f-6269-4eb0-90f1-f79fb82efeab | Open Energy Information

    Open Energy Info (EERE)

    Parent: Comments If Company furnishes overhead or underground service to metal or concrete poles in residential subdivision, Customer pays a monthly charge of 1.94 or 3.93...

  9. Data:F5a39f92-e3fa-4974-b6d5-aed9fb6c14ac | Open Energy Information

    Open Energy Info (EERE)

    wood-street lighting standards. Those in subdivisions containing aluminum or concrete standards where the Company has received a contribution from developer or others...

  10. Data:61536f7d-df93-4115-8e79-156fb2e477c7 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc (New Mexico) Effective date: 20120901 End date if known: Rate name: 175 Watt MVL 75 kWh Street...

  11. Data:Fb788c4f-e589-4af0-aeab-8191994f64e7 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc (New Mexico) Effective date: 20120901 End date if known: Rate name: 100 Watt HPS 34 kWh Street...

  12. Data:A5464299-4fb1-49a6-86be-7b6c05c69f57 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Farmers' Electric Coop, Inc (New Mexico) Effective date: 20120501 End date if known: Rate name: Security Light Pole Only...

  13. Data:Ad4911fb-1ccb-4f96-921b-200c770e1d41 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc (New Mexico) Effective date: 20120801 End date if known: Rate name: Commercial and Industrial...

  14. Data:Cd3537d3-fd76-4fa7-9f3f-75d06fb2b0ba | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Tri-County Electric Coop, Inc (New Mexico) Effective date: 20131101 End date if known: Rate name: Industrial Service Rate 45...

  15. Data:Da10b869-2522-4b0f-b7b6-3127ac40ac6b | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Southwestern Electric Coop Inc (New Mexico) Effective date: 20070701 End date if known: Rate name: Commercial Lighting Service...

  16. Data:50bf8666-897e-420e-9296-bc0fb74c7ce2 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc (New Mexico) Effective date: 20120801 End date if known: Rate name: 250 Watt MVL 110 kWh...

  17. Data:95751d3f-b2bb-46c0-9950-b52b07b2d04d | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Tri-County Electric Coop, Inc (New Mexico) Effective date: 20131101 End date if known: Rate name: Public Street Lighting MV...

  18. Data:E5213578-0993-4bca-aaee-c3cfe1fb9d18 | Open Energy Information

    Open Energy Info (EERE)

    1 2 3 Next >> Basic Information Utility name: Navopache Electric Coop, Inc (New Mexico) Effective date: 20140109 End date if known: Rate name: Residential, Schools,...

  19. Data:B00670fb-e78f-4021-a814-a490e4d1677c | Open Energy Information

    Open Energy Info (EERE)

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

  20. Data:5220c34b-4017-4ef2-b1fb-c8a6b8d2cd4f | Open Energy Information

    Open Energy Info (EERE)

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

  1. Data:6a188798-a8fb-47e2-a28c-b02d550e3f84 | Open Energy Information

    Open Energy Info (EERE)

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

  2. Data:2f31aa69-c39e-462f-92fb-3b5c7475b93c | Open Energy Information

    Open Energy Info (EERE)

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

  3. Data:Ccda57a8-1a6c-455f-b4ca-cc019f0839dd | Open Energy Information

    Open Energy Info (EERE)

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

  4. Data:041ac1bb-63e3-40cf-a7f6-95aaa3fb3da1 | Open Energy Information

    Open Energy Info (EERE)

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

  5. Data:58d87638-1c49-486d-9f7f-b4fe230db159 | Open Energy Information

    Open Energy Info (EERE)

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

  6. Data:C2bfb777-23fe-43fb-817e-539a9942c888 | Open Energy Information

    Open Energy Info (EERE)

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

  7. Data:164c9b78-0248-4e1a-8760-fb9847e7671a | Open Energy Information

    Open Energy Info (EERE)

    the availability of replacement parts Source or reference: http:www.cmpco.comYourHomepricingpricingSchedulesdefault.html Source Parent: Comments Applicability Demand (kW)...

  8. Data:28c567a3-08e4-4fb3-806b-c40003a76e0c | Open Energy Information

    Open Energy Info (EERE)

    if known: Rate name: GSB Sector: Industrial Description: *Excessive over contract demand results in a charge of 16.45kw Source or reference: ISU Documentation Source Parent:...

  9. Data:99f9130f-d339-48c5-8078-430fb4e3041c | Open Energy Information

    Open Energy Info (EERE)

    or governmental authority where 120-volt service exists. The cost of service provides for electricity only from existing Northeastern REMC (Northeastern) facilities. Any investment...

  10. Data:155c5dea-18da-4430-b224-2c01c4b70fb9 | Open Energy Information

    Open Energy Info (EERE)

    be as stated in the applicable rate tariff. Under this rider, only the kWh charge for electricity delivered by the Customer is affected. The Customer will pay for all kWh...

  11. Data:Fb7f0ea2-ae62-4a86-b59e-aeebdae3b551 | Open Energy Information

    Open Energy Info (EERE)

    (including its appurtenances if served through the same meter), where the major use of electricity is for domestic purposes such as lighting, household appliances, and the...

  12. Data:3d46b2e1-fb0b-4c8d-a648-29fcad737e34 | Open Energy Information

    Open Energy Info (EERE)

    be as stated in the applicable rate tariff. Under this rider, only the kWh charge for electricity delivered by the Customer is affected. The Customer will pay for all kWh...

  13. Data:De1fb01f-d309-4e20-9694-97ded226814c | Open Energy Information

    Open Energy Info (EERE)

    will be determined by the Company. Where the Company deems it impractical to deliver electricity through one service, or where more than one meter has been installed for...

  14. Data:4539f4fd-2323-47e1-8beb-f4fb6df76d58 | Open Energy Information

    Open Energy Info (EERE)

    This schedule is available to separately metered and billed supply of alternating current electricity to any customer including a residential farm where the farm uses are not taken...

  15. Data:A442b48a-53fb-459d-8234-7a0d70af1dd6 | Open Energy Information

    Open Energy Info (EERE)

    net metering energy resource) Company shall measure the difference between the amount of electricity delivered by Company to Customer and the amount of electricity generated by...

  16. Data:1a7c1076-47ed-41c8-8fb4-3b06a99292ff | Open Energy Information

    Open Energy Info (EERE)

    available to new applicants after February 1, 2011. This rate is applicable to the use of electricity for water heating of any customer other than residential, except as noted...

  17. Data:1bd7fbd9-a0f4-457d-8ae7-0fcff075fb06 | Open Energy Information

    Open Energy Info (EERE)

    when all of Customer's service at one location is measured by one meter, and when electricity is used for space andor water heating. Source or reference: http:...

  18. Data:131d3b34-f521-4735-839f-1e0bc97fb1a9 | Open Energy Information

    Open Energy Info (EERE)

    voltage is available, the customer desires to furnish, install and maintain transformers and protective devices, a 2.5% discount will be allowed. All metering will be on...

  19. Data:73d34bb4-9b67-4ede-89da-e7fa254991fb | Open Energy Information

    Open Energy Info (EERE)

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

  20. Data:7361fb39-0c07-4e3d-95c3-9e4fbdb40fe9 | Open Energy Information

    Open Energy Info (EERE)

    adjustment. 1% reduction of total charge when metering is at primary voltage and transformers are owned by the City. Source or reference: http:www.cityofwayne.org...

  1. Data:A5b2284c-bb1a-4075-8aa3-7fb21d137e67 | Open Energy Information

    Open Energy Info (EERE)

    discount: Transformer Ownership Discount: Customers who own and maintain their own transformers or substations shall be given a credit of 0.25 per kW of distribution demand....

  2. Data:239dd8c3-2660-4fb5-a10f-200895eb226c | Open Energy Information

    Open Energy Info (EERE)

    ( 250W HPS - Shoebox ) Sector: Lighting Description: Additional fees for poles and transformers may apply Source or reference: ISU Documentation Source Parent: Comments Applicable...

  3. Data:5683ff7b-a387-45ac-b1e2-bf50b83fb3f9 | Open Energy Information

    Open Energy Info (EERE)

    is responsible for procuring, installing and maintaining all necessary wiring, transformers, switches, cut-outs and protection equipment beyond the point of delivery, with...

  4. Data:825019fb-1c94-43f8-8983-e99a01c5af6b | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Aspen, Colorado (Utility Company) Effective date: 20140101 End date if known: 20141231...

  5. Data:2ae66fb5-8162-47d9-b060-4c8b873ebfd6 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Aspen, Colorado (Utility Company) Effective date: 20140101 End date if known: 20141231...

  6. Search for resonant WZ to lvll production using 13 fb^{-1} in \\sqrt{s} = 8 TeV p-p collisions with the ATLAS detector

    E-Print Network [OSTI]

    Loscutoff, Peter Vladimir

    2013-01-01T23:59:59.000Z

    W ? ZZ WZ Rho600 m WZ T , eem [GeV] Events / 20 GeV Events /REGIONS WZ Invariant Mass (GeV) eem channel Entries/40 GeV

  7. Data:Ebcca88e-15be-40fb-af98-7dedc915d3db | Open Energy Information

    Open Energy Info (EERE)

    Public Service Co of NM Effective date: 20130301 End date if known: Rate name: 12 Cogeneration and Small Power Production Secondary Distribution (1A, 1B, 2A, 2B, 3B, 3C, 10A, &...

  8. Data:E229fb12-27d3-47a4-8a10-277f2f939016 | Open Energy Information

    Open Energy Info (EERE)

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

  9. Data:638bc389-fb01-4b31-96a5-0c12a8e0261b | Open Energy Information

    Open Energy Info (EERE)

    Sector: Commercial Description: Optional for non-Domestic Service where consumption of energy exceeds 3,500 kWh in any one month, where the Billing Demand is equal to or less...

  10. Data:9fb4ba6f-444e-4d67-a06a-be8f9b787c80 | Open Energy Information

    Open Energy Info (EERE)

    prices change. Power plants in the Midwest burn primarily coal as the fuel to generate electricity. When the market price changes for the coal they purchase, they pass that...

  11. Updated Combination of Searches for the Standard Model Higgs Boson at the D0 Experiment in 9.7 fb-1 of Data

    E-Print Network [OSTI]

    D0 Collaboration

    2012-07-02T23:59:59.000Z

    Searches for standard model Higgs boson production at the D0 experiment in ppbar collisions at sqrt(s)=1.96 TeV are carried out for Higgs boson masses (m_H) in the range 100Higgs boson. In absence of a significant excess above the background expectation, 95% confidence level upper limits are set on the production cross section for a standard model Higgs boson. The upper limits are found to be a factor of 2.11 (0.73) times the predicted standard model cross section for m_H=115 (165) GeV. Under the background-only hypothesis, the corresponding expected limit is 1.46 (0.72) times the standard model prediction. At the same confidence level, these analyses exclude a standard model Higgs boson with a mass in the range 159

  12. Data:0ac74409-f2ac-4fb5-89ca-2b93352f3c66 | Open Energy Information

    Open Energy Info (EERE)

    date: 20110315 End date if known: Rate name: MU-1 - a1b - 1000 watt MV Sector: Lighting Description: Lamps in enclosed fixtures, mounted on metal or fiberglass columns and...

  13. Data:B0993536-b649-466f-b2b7-92bd7d6d30f2 | Open Energy Information

    Open Energy Info (EERE)

    Company) Effective date: 20130701 End date if known: Rate name: Public Street Lighting Service - HPSV Pendant Lamp Fixtures - Ornamental Pole - Residential Sector: Lighting...

  14. Search for the standard model Higgs boson in associated $WH$ production in 9.7 fb$^{-1}$ of $p\\bar{p}$ collisions with the D0 detector

    E-Print Network [OSTI]

    The D0 Collaboration

    2012-09-21T23:59:59.000Z

    We present a search for the standard model Higgs boson in final states with a charged lepton (electron or muon), missing transverse energy, and two or three jets, at least one of which is identified as a $b$-quark jet. The search is primarily sensitive to $WH\\to\\ell\

  15. Type B Accident Investigation Board Report on the September 1, 1999, Plutonium Intakes at the Savannah River Site FB-Line

    Broader source: Energy.gov [DOE]

    This report is an independent product of the Type B Accident Investigation Board appointed by Greg Rudy, Manager, Savannah River Operations Office, U.S. Department of Energy.

  16. Data:F358e502-527d-49b0-b8e7-16ce8282b8fb | Open Energy Information

    Open Energy Info (EERE)

    a renewable or recurring basis, including dedicated energy crops, trees grown for energy production, wood waste and wood residues, plants (including aquatic plants, grasses, and...

  17. Data:53e191c2-04fb-4239-afd6-5e473bfeb11b | Open Energy Information

    Open Energy Info (EERE)

    are Eugene Code 9.6725 and all EWEB policies and procedures pertaining to light pollution, light trespass and glare. Source or reference: http:www.eweb.orgpublic...

  18. Data:A19a75cf-fea0-40fb-a873-890c6266b47a | Open Energy Information

    Open Energy Info (EERE)

    in all territory served by the Corporation to members who have Automated Metering Infrastructure (AMI), as a voluntary alternative to the Corporation's Schedule CS-14, subject to...

  19. Data:E5fb6d06-ca48-45c5-848c-8bfb3d23560d | Open Energy Information

    Open Energy Info (EERE)

    than 100KW and less than 1000KW as defined in the billing demand section of this tariff. 2. In the event that billing demand becomes permanently less than 100kW, the customer...

  20. Data:1e969327-8244-4db7-9c77-1fb5b2244bed | Open Energy Information

    Open Energy Info (EERE)

    greater than 30 KWs as defined in the determination of billing demand section of this tariff. 2. Average monthly energy consumption is equal to greater than 3,000KW based on the...

  1. Data:D80d58fb-40a7-49a9-9c18-62365ea596fd | Open Energy Information

    Open Energy Info (EERE)

    streets. Source or reference: https:www.burlingtonelectric.comELBOassetsTariff%20Sheets%20June%20262009%20revised-1.pdf Source Parent: Comments Applicability Demand...

  2. Data:F6fb5948-6080-45da-b55e-73808fcbb36d | Open Energy Information

    Open Energy Info (EERE)

    Commercial Description: Source or reference: http:www.pioneerelectric.coopdocumentstariff-schedules.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum...

  3. Data:45c71c2d-8c26-40fb-a7e0-fab503a49d1f | Open Energy Information

    Open Energy Info (EERE)

    Stillwater Utilities Authority Effective date: 20120101 End date if known: Rate name: ELECTRIC RATE GENERAL SERVICE Sector: Commercial Description: Production Cost Adjustment...

  4. Data:1fb310f8-db83-498b-b923-d5e0deaa9e09 | Open Energy Information

    Open Energy Info (EERE)

    Sector: Lighting Description: Source or reference: http:www.btes.netindex.phpelectricgeneral-electric-rates-oldlighting-service-rate-schedule Source Parent: Comments...

  5. Data:952ca314-1f91-4bf0-b704-e80630412fb4 | Open Energy Information

    Open Energy Info (EERE)

    entire requirements are taken through a single meter, for all uses excluding crop drying or irrigation. Demand Charge Purchased Power + Distribution Delivery Source or...

  6. Data:Aec094ea-a721-479f-b343-67fe5f637d52 | Open Energy Information

    Open Energy Info (EERE)

    entire requirements are taken through a single meter, for all uses excluding crop drying or irrigation. Demand Charge Purchased Power + Distribution Delivery Source or...

  7. Data:Da05fb7c-7f74-45c0-b1d2-dce609ef66f2 | Open Energy Information

    Open Energy Info (EERE)

    Valley Elec Coop Inc Effective date: End date if known: Rate name: Controlled Grain Drying - Off Season - Subject to Moderate Periods of Control Sector: Residential Description:...

  8. Data:97c39de8-7a02-4cbc-88fb-99fdd5889042 | Open Energy Information

    Open Energy Info (EERE)

    by the U. S. Army Corps of Engineers (Corps) as a precaution to prevent failure of the dams, Southeastern is not able to provide peaking capacity to these customers. Southeastern...

  9. Data:572eb4a7-39fb-45e6-98fd-7544a0fea433 | Open Energy Information

    Open Energy Info (EERE)

    20120101 End date if known: Rate name: RATE SCHEDULE NO. 99 LOAD FORECAST ADJUSTMENT Sector: Description: APPLICABILITY: All customers billed on rate schedules 14, 15, 16, and 85...

  10. Data:7146d5fb-ec7c-48ac-98a8-118f52ea32e2 | Open Energy Information

    Open Energy Info (EERE)

    charge calculated as follows: forecast capacity rate (1.87) + reactive supply (0.046) + regulation and frequency response (0.1897) Energy charge calculated as follows: forecast...

  11. Data:8c31dba9-331f-4d72-8d9b-7d63193fb4e8 | Open Energy Information

    Open Energy Info (EERE)

    B3PI Sector: Commercial Description: Note: 10.00 added to Fixed monthly charge if Remote Read Device is used. Source or reference: Rates Binder 1, Illinois State University...

  12. Data:3aca5136-67e4-4fb6-a05f-3cb32d2e6ccc | Open Energy Information

    Open Energy Info (EERE)

    3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Village of L'Anse, Michigan (Utility Company) Effective date: 20120201 End date if known: Rate name:...

  13. Data:8ddac2a0-3c8e-4fb7-9ff4-44308cdf0d45 | Open Energy Information

    Open Energy Info (EERE)

    power plant cost adjustment factor:0.01000 for all kWh, all service classes. State of Michigan P.A. 295, of Public Acts 2008, commonly referred to as the Clean, Renewable and...

  14. Data:16cc1788-21d0-4a0b-8df1-4c91f66fb14a | Open Energy Information

    Open Energy Info (EERE)

    base cost of power (U) is 0.0720 per kilowatt-hour. Parallel Generation (20 kW or less) Net Energy Billing - Available for single-phase and three-phase customers where a part or...

  15. Data:434682d3-1caf-49df-b1fb-06e5d91edec8 | Open Energy Information

    Open Energy Info (EERE)

    base cost of power (U) is 0.0785 per kilowatt-hour. Parallel Generation (20 kW or less) Net Energy Billing - Available for single-phase and three-phase customers where a part or...

  16. Data:4ce60f48-c2ac-449f-b745-9ab1009e8428 | Open Energy Information

    Open Energy Info (EERE)

    9am-9pm with Parallel Generation(20kW or less) Sector: Residential Description: Power Cost Adjustment Clause All metered rates shall be subject to a positive or negative power...

  17. Data:A1729943-9fb7-4246-9d3a-3e3e44e13410 | Open Energy Information

    Open Energy Info (EERE)

    To uses of electrical power on a continuous basis for seasonal agricultural irrigation pumping or agricultural drainage pumping. C. Character of Service: Sixty (60) hertz...

  18. Data:29dcf4eb-9ae8-4070-96b1-d655fb106e84 | Open Energy Information

    Open Energy Info (EERE)

    terminates, whichever occurs first. Fiberglass Pole Embededded Fixed Monthly Charge Steel Pole Foundation 39.89 Source or reference: http:www.duke-energy.compdfs...

  19. Data:773b7e72-2a29-4a09-b350-1d646e1824fb | Open Energy Information

    Open Energy Info (EERE)

    terminates, whichever occurs first. Fiberglass Pole Embededded Fixed Monthly Charge Steel Pole Foundation 39.26 Source or reference: http:www.duke-energy.compdfs...

  20. Data:Ca94fb47-d744-4b08-b999-6d27c8a05f7e | Open Energy Information

    Open Energy Info (EERE)

    250.00 16' Fiberglass (Black) 300.00 16' Fiberglass (Acorn, Black) 800.00 30' Steel & Sub Base 1325.00 30' Fiberglass with 6' Arm 625.00 30' Fiberglass with 2 - 6' Arm...

  1. Data:0e36e05e-8105-494f-b13f-a5fd48da93d6 | Open Energy Information

    Open Energy Info (EERE)

    250.00 16' Fiberglass (Black) 300.00 16' Fiberglass (Acorn, Black) 800.00 30' Steel & Sub Base 1325.00 30' Fiberglass with 6' Arm 625.00 30' Fiberglass with 2 - 6' Arm...

  2. Data:1cf1eec6-fb89-4f31-9cb0-aa3fae5bce04 | Open Energy Information

    Open Energy Info (EERE)

    250.00 16' Fiberglass (Black) 300.00 16' Fiberglass (Acorn, Black) 800.00 30' Steel & Sub Base 1325.00 30' Fiberglass with 6' Arm 625.00 30' Fiberglass with 2 - 6' Arm...

  3. Data:857c5962-cd32-43e6-b129-4d55e7fb4fcf | Open Energy Information

    Open Energy Info (EERE)

    date: 20130301 End date if known: Rate name: MVS - Closed Offerings - 400 Watt MV Steel Pole Sector: Lighting Description: Source or reference: https:www.swepco.com Source...

  4. Data:8e8569fb-812d-488a-85d7-010fac6de443 | Open Energy Information

    Open Energy Info (EERE)

    2.78 Standard Wood Pole with an Underground Feed, 30-35 feet: 4.24 Direct Burial Steel with an Underground Feed, 30 feet: 4.99 Source or reference: http:...

  5. Data:Fb56ea53-1506-48f1-a795-62ec14804dad | Open Energy Information

    Open Energy Info (EERE)

    250.00 16' Fiberglass (Black) 300.00 16' Fiberglass (Acorn, Black) 800.00 30' Steel & Sub Base 1325.00 30' Fiberglass with 6' Arm 625.00 30' Fiberglass with 2 - 6' Arm...

  6. Data:F3217065-46b0-4e77-b2cb-d45fa34046fb | Open Energy Information

    Open Energy Info (EERE)

    until their contract expires or this rate schedule terminates, whichever occurs first. Steel Pole Fixed Monthly Charge SteelAluminum Pole 42.61 Wood Pole 29.89 Additional...

  7. Data:52c1785f-1cda-4fb8-a8ac-98e3112e9493 | Open Energy Information

    Open Energy Info (EERE)

    date: End date if known: Rate name: Street Lighting ornamental, 400w mv, 30 ft steel pole Sector: Lighting Description: street lighting,ornamental mercury vapor 400 watt...

  8. Data:D3938799-e61a-4550-aaca-c3fb8724a8a7 | Open Energy Information

    Open Energy Info (EERE)

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

  9. Data:B0e9026d-17ec-4618-95e5-682d8e117fb7 | Open Energy Information

    Open Energy Info (EERE)

    pasturage at one Point of Delivery and through one meter. Water pumping or water delivery systems include, but are not limited to, irrigation pumps, pivots, fertilizer pumps,...

  10. Data:292737fc-1c21-4a71-8d84-878ca6e025fb | Open Energy Information

    Open Energy Info (EERE)

    http%3A%2F%2Fpsc.wi.gov%2Fapps40%2Ftariffs%2Fviewfile.aspx%3Ftype%3Delectric%26id%3D5940&eibLmEU9-kDIqSyATb34D4BA&usgAFQjCNHQszMM37DZ2RABeDOYr8qMUj5yA Source Parent: Comments...

  11. Data:8a6072d5-dbda-47fb-a54e-7eb1eb932b74 | Open Energy Information

    Open Energy Info (EERE)

    2 3 Next >> Basic Information Utility name: Slash Pine Elec Member Corp Effective date: 19970201 End date if known: Rate name: Outdoor Lighting 250 Watt HPS Security Light...

  12. Data:Fc63ad02-f0fb-4ded-a90a-32612313be85 | Open Energy Information

    Open Energy Info (EERE)

    Single-phase, 60-cycles, and where available, three-phase, 60 cycles, at available secondary voltages. For prepay accounts, the facilities charge will be increased by 5.00...

  13. Data:54adb3ff-c362-4574-b14b-8b9c0fd2f8fb | Open Energy Information

    Open Energy Info (EERE)

    Power Supply Cost Recovery Factor, Fixed Charge Customer Charge + Energy Optimization. kWh << Previous 1 2 3 Next >> Category:Categories Retrieved from "http:...

  14. Data:0fb798a6-a6bb-45c1-a0f6-6f6727504b4a | Open Energy Information

    Open Energy Info (EERE)

    1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 Comments Fixed charge is facilities charge, energy optimization, and renewable energy standard charge multiplied by 36512. Energy charge is energy...

  15. Data:E00fc87e-6fb1-459c-b964-8747a495d7fe | Open Energy Information

    Open Energy Info (EERE)

    1 1 1 1 1 1 1 1 Dec 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 Comments Energy Optimization: .001780 added onto adjustments. kWh << Previous 1 2 3 Next >>...

  16. Data:F1d01087-996f-41c3-8ffa-e628e4fb6f61 | Open Energy Information

    Open Energy Info (EERE)

    Pole (NLA) 20.85 1220 &When consumer chooses URD service to the light where OH is the EMC preferred method of service. Additional Charges: Street Light Arms and Fixtures A. ARMS...

  17. Data:C1bb69c9-96f2-4d2f-b939-1755bc17809f | Open Energy Information

    Open Energy Info (EERE)

    Energy << Previous 1 2 3 Next >> Basic Information Utility name: Whitewater Valley Rural EMC Effective date: 20110101 End date if known: Rate name: Schedule GS - General Service...

  18. Data:8fd9d4ef-688a-48e0-88fb-3e93108c11d1 | Open Energy Information

    Open Energy Info (EERE)

    2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Wild Rice Electric Coop, Inc Effective date: 20120318 End date if known: Rate name:...

  19. Data:Fb4e97fa-6eca-42de-a38f-01fc44fa31f9 | Open Energy Information

    Open Energy Info (EERE)

    within 30 days following the due date, a charge will be assessed. Any customer on a budget or leveled payment plan shall not be assessed for a late payment amount provided that...

  20. Data:Fb19a4b3-1bef-46cb-95e3-015a2272ad0d | Open Energy Information

    Open Energy Info (EERE)

    Effective date: 20090601 End date if known: Rate name: External interraptible service EIS-16 Sector: Industrial Description: Source or reference: Source Parent: Comments...

  1. Data:0e162bce-fb0e-4b37-9243-3fa48ccfb7a1 | Open Energy Information

    Open Energy Info (EERE)

    to either residential or commercial customers for the operation of storage type electric water heaters of standard make and design when used in conjunction with other regular...

  2. Data:Fc1fb8cb-2413-4f2a-bedf-27d0e7dd65b1 | Open Energy Information

    Open Energy Info (EERE)

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

  3. Data:7da9fb6d-395e-466f-8865-016e956e7d1e | Open Energy Information

    Open Energy Info (EERE)

    Street Lighting- 400 Watt Sector: Lighting Description: Source or reference: *ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):...

  4. Data:90eb1d4f-b204-4b5a-9d73-f04224bf00de | Open Energy Information

    Open Energy Info (EERE)

    name: Street Lighting- D150 Sector: Lighting Description: Source or reference: *ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):...

  5. Data:C2f657fb-1bf4-43a7-bab8-35adf4b59fa0 | Open Energy Information

    Open Energy Info (EERE)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page onYou are now leaving Energy.gov You are now leaving Energy.gov You are being directedAnnualPropertyd8c-a9ae-f8521cbb8489 No revision has been approved for this page.adf4b59fa0 No

  6. Data:Ffe2fb55-352f-473b-a2dd-50ae8b27f0a6 | Open Energy Information

    Open Energy Info (EERE)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page onYou are now leaving Energy.gov You are now leaving Energy.gov You are being directedAnnualPropertyd8c-a9ae-f8521cbb8489 No revision hasda62829c05b No revision has

  7. Local Power Functions of Tests for Double Unit Roots

    E-Print Network [OSTI]

    Haldrup, Niels Prof.; Lildholdt, Peter

    2000-01-01T23:59:59.000Z

    U! i)|it|t S 2 S  f H S e D fD f fbe fb. ff fbH fbb fff.S f.H fb fHH fb fb. fbe fb. fbb feS fe2 fDH fS2 fS f.SfS fSf fS2 fDe fDf fbS fbS fbe fb fb2 fbf fb fbf fHH fbf

  8. alpha3 laminin subunit: Topics by E-print Network

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

    (FN), suggesting that cell surface Con A binding proteins could be involved in 8 d CEF spreading on a LM substrate. The interaction of Con A spreading on LM but not on FN....

  9. Simulations of Vibrational Frequencies of Carbon

    E-Print Network [OSTI]

    Adler, Joan

    analytical model ­ Euler-Bernoulli theory Frequencies of the modes of the lateral vibration 8 fn ~ 1/L2 fn close to global or local buckling instabilities. 19 · The results of this study are relevant fo

  10. Recent Developments in Quantum White Noise Calculus: Quantum White Noise Derivatives and Implementation Problem

    E-Print Network [OSTI]

    Obata, Nobuaki

    ) is defined by . . (H) = { = (fn) ; fn Hn , 2 = n=0 n!|fn|2 0 ) ), respectively. (The pair {at, a t ; t T } is called the quantum white noise on T .) Definition Given l,m (E(l+m,m (E(l+m) ) , where the right-hand side converges

  11. Errata sheet to dissertation: Aristotle's Contribution to Scholarly Communication 5/8/09

    E-Print Network [OSTI]

    Bales, Stephen

    2009-05-08T23:59:59.000Z

    . ------------------------------------------------------------------------------------------------------------ 27. FN 14. Add ?trans. Seux? to citation. 31. FN 26. Change page numbers from 1023 to 1023-1024. Add ?trans. R?mer? 62. line 20 ADD FN: Kenyon, Books and Readers, 60. Kenyon?s description of Roman filing systems is correctly cited on pg. 99, FN... 40, betraying the order in which the diss. chapters were written. 71. line 9. Change ?Ptolemies? to ?Ptolemaic kings? 101. line 4. Insert ?Table 2? in the brackets 136. FN 12. In addition to Lamberton, to recent works that address the topic...

  12. J. Number Theory 130(2010), no. 4, 930935. SOME CURIOUS CONGRUENCES MODULO PRIMES

    E-Print Network [OSTI]

    Sun, Zhi-Wei

    2010-01-01T23:59:59.000Z

    + 2 S2 - S3 + S4 - 2 S5 =S0 - S3 - (S1 - S4) + (-1 - )(S2 - S5) =S0 - S3 - S2 + S5 - (S1 + S2 - S4 - S5). Similarly, Fn(-2 ) = S0 - S3 - S2 + S5 - 2 (S1 + S2 - S4 - S5). Thus Fn(-) + Fn(-2 ) =2(S0 - S2 - S3 + S5) + S1 + S2 - S4 - S5 =2S0 + S1 - S2 - 2S3 - S4 + S5 and Fn(-) - Fn(-2 ) = (2 - )(S1 + S2 - S

  13. GRADO EN INGENIERA DE TECNOLOGAS Y SERVICIOS DE TELECOMUNICACIN

    E-Print Network [OSTI]

    Autonoma de Madrid, Universidad

    Semestre 18462 ANÁLISIS MATEMÁTICO I 6 FB 1 18463 ALGEBRA LINEAL 6 FB 1 18464 PROGRAMACI�N I 6 FB 1 18465 FUNDAMENTOS DE SISTEMAS INFORMÁTICOS 6 FB 18474 SISTEMAS LINEALES 6 FB 18475 FUNDAMENTOS DE TRANSMISI�N Y

  14. Search for a standard model Higgs boson in the H?ZZ??[superscript +]?[subscript ?]?[bar over ?] decay channel using 4.7 fb[superscript -1] of ?s = 7 TeV data with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for a Standard Model Higgs boson decaying via H?ZZ??[superscript +]?[superscript ?]?[bar over ?], where ? represents electrons or muons, is presented. It is based on proton–proton collision data at ?s = 7 TeV, ...

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

    E-Print Network [OSTI]

    Taylor, Frank E.

    This Letter presents a search for the Standard Model Higgs boson in the decay channel H?ZZ(*)??[superscript +]?[superscript ?]??[superscript +]??[superscript ?], where ?,?? = e or ?, using proton–proton collisions at ?s = ...

  16. Data:Fb6b6dbc-e7c2-4d4c-8c18-e0cf9d99c8ca | Open Energy Information

    Open Energy Info (EERE)

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

  17. Search for direct pair production of a chargino and a neutralino decaying to the 125 GeV Higgs boson with 20.3 fb$^{-1}$ of 8 TeV pp collisions using the ATLAS detector

    E-Print Network [OSTI]

    Gignac, Matthew; The ATLAS collaboration

    2015-01-01T23:59:59.000Z

    A search is presented for the direct pair production of a chargino and a neutralino $pp$ $\\rightarrow$ $\\tilde{\\chi}^{\\pm}_{1}$$\\tilde{\\chi}^{0}_{2}$, where the chargino decays to the lightest neutralino and the $W$ boson, $\\tilde{\\chi}^{\\pm}_{1}$ $\\rightarrow$ $\\tilde{\\chi}^{0}_{1}$ $(W^{\\pm}\\to\\ell^{\\pm}\

  18. A search for the Standard Model Higgs boson in the process $ZH \\rightarrow \\ell^{+} \\ell^{-} b \\bar{b}$ in $4.1\\unit{fb^{-1}}$ OF CDF~II DATA}

    SciTech Connect (OSTI)

    Shalhout, Shalhout Zaki; /Wayne State U.

    2010-05-01T23:59:59.000Z

    The standard model of particle physics provides a detailed description of a universe in which all matter is composed of a small number of fundamental particles, which interact through the exchange of force - carrying gauge bosons (the photon, W{sup {+-}}, Z and gluons). The organization of the matter and energy in this universe is determined by the effects of three forces; the strong, weak, and electromagnetic. The weak and electromagnetic forces are the low energy manifestations of a single electro-weak force, while the strong force binds quarks into protons and neutrons. The standard model does not include gravity, as the effect of this force on fundamental particles is negligible. Four decades of experimental tests, spanning energies from a few electron-volts (eV) up to nearly two TeV, confirm that the universe described by the standard model is a reasonable approximation of our world. For example, experiments have confirmed the existence of the top quark, the W{sup {+-}} and the Z bosons, as predicted by the standard model. The latest experimental averages for the masses of the top quark, W{sup {+-}} and Z are respectively 173.1 {+-} 0.6(stat.) {+-} 1.1(syst.), 80.399 {+-} 0.023 and 91.1876 {+-} 0.0021 GeV/c{sup 2}. The SM is a gauge field theory of zero mass particles. However, the SM is able to accommodate particles with non-zero mass through the introduction of a theoretical Higgs field which permeates all of space. Fermions gain mass through interactions with this field, while the longitudinal components of the massive W{sup {+-}} and Z are the physical manifestations of the field itself. Introduction of the Higgs field, directly leads to the predicted existence of an additional particle, the Higgs boson. The Higgs boson is the only particle of the standard model that has not been observed, and is the only unconfirmed prediction of the theory. The standard model describes the properties of the Higgs boson in terms of its mass, which is a free parameter in the theory. Experimental evidence suggests that the Higgs mass has a value between 114.4 and 186 GeV/c{sup 2}. Particles with a mass in this range can be produced in collisions of less massive particles accelerated to near the speed of light. Currently, one of only a few machines capable of achieving collision energies large enough to potentially produce a standard model Higgs boson is the Tevatron proton-antiproton collider located at Fermi National Accelerator Laboratory in Batavia, Illinois. This dissertation describes the effort to observe the standard model Higgs in Tevatron collisions recorded by the Collider Detector at Fermilab (CDF) II experiment in the ZH {yields} {ell}{sup +}{ell}{sup -}b{bar b} production and decay channel. In this process, the Higgs is produced along with a Z boson which decays to a pair of electrons or muons (Z {yields} {ell}{sup +}{ell}{sup -}), while the Higgs decays to a bottom anti-bottom quark pair (H {yields} b{bar b}). A brief overview of the standard model and Higgs theory is presented in Chapter 2. Chapter 3 explores previous searches for the standard model Higgs at the Tevatron and elsewhere. The search presented in this dissertation expands upon the techniques and methods developed in previous searches. The fourth chapter contains a description of the Tevatron collider and the CDF II detector. The scope of the discussion in Chapter 4 is limited to the experimental components relevant to the current ZH {yields} {ell}{sup +}{ell}{sup -}b{bar b} search. Chapter 5 presents the details of object reconstruction; the methods used to convert detector signals into potential electrons, muons or quarks. Chapter six describes the data sample studied for the presence of a ZH {yields} {ell}{sup +}{ell}{sup -}b{bar b} signal and details the techniques used to model the data. The model accounts for both signal and non-signal processes (backgrounds) which are expected to contribute to the observed event sample. Chapters 7 and 8 summarize the event selection applied to isolate ZH {yields} {ell}{sup +}{ell}{sup -}b{bar b} candidate events

  19. Measurements of top quark pair production cross section in proton anti-proton collisions at s**(1/2) = 1.96 TeV in the tau + jets final state using 1 inv fb of data

    SciTech Connect (OSTI)

    Hossain, Sohrab; /Oklahoma U.

    2009-12-01T23:59:59.000Z

    This dissertation presents a new measurement of p{bar p} {yields} t{bar t}X production at {radical}s = 1.96 TeV using 974.2 pb{sup -1} of data collected with the D0 detector between 2002 and 2006. We focus on the final state where the W boson from one of the top quarks decays into a {tau} lepton and its associated neutrino, while the other W boson decays into a quark-antiquark pair. We aim to select those events in which the {tau} lepton subsequently decays hadronically, meaning to one or three charged hadrons, zero or more neutral hadrons and a tau neutrino (the charge conjugate processes are implied in all of the above). The observable signature thus consists of a narrow calorimeter shower with associated track(s) characteristic of a hadronic tau decay, four or more jets, of which two are initiated by b quarks accompanying the W's in the top quark decays, and a large net missing momentum in the transverse plane due to the energetic neutrino-antineutrino pair that leave no trace in the detector media. The preliminary result for the measured cross section is: {sigma}(t{bar t}) = 6.9{sub -1.2}{sup +1.2}(stat){sub -0.7}{sup +0.8}(syst) {+-} 0.4 (lumi) pb. This indicates that our finding is consistent with the Standard Model prediction.

  20. Data:B03f35f5-3d19-42b6-94fb-ab65c5a6f1b4 | Open Energy Information

    Open Energy Info (EERE)

    htdocstariffswyhwe1hwe.pdf Source Parent: http:psc.state.wy.ushtdocsWyUtilityTariffsnew.htm Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History...

  1. OC$78@MU%3!<%Q%9$N7ABVAG2r@O Fb85 @65. y LnH* <~ y ;3ED FF y 4X:, Ao z 0f:486 6Q y

    E-Print Network [OSTI]

    Sekine, Satoshi

    $rkJ}K! (Nc$($P (3) $J$I) $G$"$j!"$b$&0l$D$O L$CN8l$G$b2r@O$G$­$k$h$&$J%b%G%k$r:n@.$9$kJ}K! (Nc$( $P (4, 5) $J$I) $G$"$k!#$3$3$G!"A0

  2. Data:46e648d5-2bc6-4fb2-8b00-5c2216a349f3 | Open Energy Information

    Open Energy Info (EERE)

    Effective date: 20130701 End date if known: Rate name: Rate 27 - Small Time-Of-Day General Electric Service (Distribution Service Transmission Voltage Delivery Allowance)...

  3. Search for neutral Higgs bosons in the multi-b -jet topology in 5.5 fb-1 of pp-bar collisions at sqrt(s)=1.96 TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Carrasco-Lizarraga, M. A.; Chen, G.; Clutter, Justace Randall; McGivern, Carrie Lynne; Sekaric, Jadranka; Wilson, Graham Wallace; D0 Collaboration; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.

    2011-04-04T23:59:59.000Z

    Data recorded by the D0 experiment at the Fermilab Tevatron Collider are analyzed to search for neutral Higgs bosons produced in association with b quarks. The search is performed in the three-b -quark channel using multijet-triggered events...

  4. Data:5cbae07c-1d28-4b0d-aa5f-b62b5f3cdde8 | Open Energy Information

    Open Energy Info (EERE)

    rate is applicable for service that is supplied through new or rebuilt streetlight systems, including extension of streetlighting systems to additional locations where service...

  5. Data:4cd454f2-4c17-4d9d-a055-1fb33f8dd5ce | Open Energy Information

    Open Energy Info (EERE)

    case the registrations of the two meters shall be added for billing under this rate. All electricity delivered hereunder shall be for the exclusive use of the customer and shall...

  6. Data:9b275f4a-aa5f-451f-b5a0-d5f9f462f550 | Open Energy Information

    Open Energy Info (EERE)

    voltage of the transmission or distribution line serving the customer through transformers owned by the customer. Customers with a demand less than 500 kW may enter into an...

  7. Data:B43e359d-3de2-4f6f-a13f-b18ae46dd24a | Open Energy Information

    Open Energy Info (EERE)

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

  8. Data:E23a3d26-3e21-4baf-a1f5-74c2f4b230fb | Open Energy Information

    Open Energy Info (EERE)

    and maintain an overhead street lighting system in conjunction with and as a part of its general overhead electric distribution system, and the REMC will furnish all electric...

  9. Data:A5c990b6-1bc0-4ba5-85c1-954a40fb9b0e | Open Energy Information

    Open Energy Info (EERE)

    (Nebraska) Effective date: 20140101 End date if known: Rate name: Grain Storage and Drying Sector: Industrial Description: Source or reference: http:www.hea.coopBilling...

  10. Data:Ff0ec6e9-1a3b-492f-b7fa-358f6fd609d1 | Open Energy Information

    Open Energy Info (EERE)

    Generation Rider Sector: Commercial Description: *Customers requesting interconnection and parallel operation of Distributed Generation("DG") shall complete the...

  11. Data:9a87e30d-b106-4fb8-81d6-2cd201f57d69 | Open Energy Information

    Open Energy Info (EERE)

    base cost of power (U) is 0.0720 per kilowatt-hour. Parallel Generation (20 kW or less) Net Energy Billing - Available for single-phase and three-phase customers where a part or...

  12. Data:C5aab511-9af0-4c9f-b2cd-aa8e3df15f9f | Open Energy Information

    Open Energy Info (EERE)

    in addition to charges in Option 2, there is a charge of .333% per month for return on investment (plant original cost). Source or reference: http:www.subutil.comfiles...

  13. Data:Cc0acc3a-fb58-4bdd-8e1d-f7e0d6b32e6e | Open Energy Information

    Open Energy Info (EERE)

    Inc Effective date: 20090201 End date if known: Rate name: SL- 250 Watt HPS 106 kWh (Steel Pole Overhead) Sector: Lighting Description: Source or reference: http:...

  14. Data:0fb2a9e9-d1e7-40b6-bb23-de5d53c9f0e3 | Open Energy Information

    Open Energy Info (EERE)

    midwestmidwest2cur.pdf Source Parent: http:www.teammidwest.com Comments Energy Optimization Charge 1.76 per month Power Cost Recovery 0.00596 Applicability Demand (kW)...

  15. Search for Direct Top Squark Pair Production in Final States with One Isolated Lepton, Jets, and Missing Transverse Momentum in ?s=7??TeV pp Collisions Using 4.7??fb[superscript -1] of ATLAS Data

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search is presented for direct top squark pair production in final states with one isolated electron or muon, jets, and missing transverse momentum in proton-proton collisions at ?s=7??TeV. The measurement is based on ...

  16. Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using 4.7??fb?1 of ?s=7??TeV proton-proton collision data

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for squarks and gluinos in final states containing jets, missing transverse momentum and no high-pT electrons or muons is presented. The data represent the complete sample recorded in 2011 by the ATLAS experiment ...

  17. Molina A., Panetto H., Chen D., Whitman L., Chapurlat V., Vernadat F.B. (2007). Enterprise Integration and Networking: Challenges and Trends. Studies in Informatics and Control. 16/4. December, Informatics

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    Interoperability · Validation, Verification, Qualification and Accreditation of Enterprise Models · Model Reuse Supplier on time % - + + - + + + + - + - - + + + ++ + - + + · Process definition, execution and tracking Validation, Verification, Qualification and Accreditation of Enterprise Models Research Challenges Model

  18. Data:D0b1be3f-6d90-470f-b82a-1fc113e7fa82 | Open Energy Information

    Open Energy Info (EERE)

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

  19. Data:B485777c-c4fb-42b3-8d2a-3da95f7c7c10 | Open Energy Information

    Open Energy Info (EERE)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page onYou are now leaving Energy.gov You are now leaving Energy.gov You are being directedAnnualPropertyd8c-a9ae-f8521cbb8489 No revision has been approved for this page. It is

  20. Crack-based analysis of concrete with brittle reinforcement

    E-Print Network [OSTI]

    Burgoyne, Chris

    { FaberMaunsell Ltd; University of Cambridge Brittle reinforcement (such as fibre-reinforced plastic to the surround- ing concrete, at a crack surface sL=sR s on the left/right side of a crack u increase in unbonded

  1. Journal self-citations -analysing the JIF mechanism

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    1 Journal self-citations - analysing the JIF mechanism Tove Faber Frandsen1 tff@db.dk Department investigates the mechanism of the Journal Impact Factor (JIF). Although created as a journal selection tool the indicator is probably the central quantitative indicator for measuring journal quality. The focus is journal

  2. Journal interaction A bibliometric analysis of economics journals

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    1 Journal interaction A bibliometric analysis of economics journals Tove Faber Frandsen1 Royal journals. The proposed method controls for the different characteristics of the journals as well Author manuscript, published in "Journal of Documentation 61, 3 (2005) 385-401" #12;2 economics

  3. INTERFACING AUTOCAD WITH MAGNETIC DESIGN

    E-Print Network [OSTI]

    Sorin, M.

    2010-01-01T23:59:59.000Z

    more procedures, namely, fbI, fbll, eatblank, car4str, andwritten by Michael Helm. fbI finds the next blank in theprocedures car4str, cdr4str, fbI, fbll, and eatblank (which

  4. 11601. For any prime p and positive integer n, let N(p, n) denote the dif-ference between the number of p's appearing as factors in the denominator

    E-Print Network [OSTI]

    Karaivanov, Borislav

    11601. For any prime p and positive integer n, let N(p, n) denote the dif- ference between the number of p's appearing as factors in the denominator of Fn and the number of those appearing in the numerator of Fn. Clearly, Fn is an integer if and only if N(p, n) 0 for all primes p. The idea of the proof

  5. The EIIIA domain from astrocyte-derived fibronectin mediates proliferation of oligodendrocyte progenitor cells following CNS demyelination

    E-Print Network [OSTI]

    Stoffels, Josephine M. J.; Hoekstra, Dick; Franklin, Robin J. M.; Baron, Wia; Zhao, Chao

    2014-08-25T23:59:59.000Z

    an alternative mechanism.This mechanism may involve other domains of Fn, since alternative splicing of Fn can change the conformation of Fn, affecting the presentation of binding sequences and exposing cryptic binding sites(Pickford and Campbell, 2004; Ventura... -EDA promotes survival and prevents adverse remodeling and heart function deterioration after myocardial infarction. Circ Res 108:582-592. Balza E, Sassi F, Ventura E, Parodi A, Fossati S, Blalock W, Carnemolla B, Castellani P, Zardi L, Borsi L (2009) A...

  6. An Analysis of the Impacts of British Transport Reforms on Transit Integration in the Metropolitan Areas

    E-Print Network [OSTI]

    Rivasplata, Charles Richard

    2006-01-01T23:59:59.000Z

    and C. Nash, 1995. Bus deregulation: ten years on, TransportFN Spon. ________, 1996. Deregulation and privatization: theand N. Topham (Eds. ), Bus Deregulation and Privatisation,

  7. Microstructural and solidification cracking evaluation of electron beam welds in 304L

    SciTech Connect (OSTI)

    Sturgill, P.L.; Campbell, R.D.; Henningsen, J.L.

    1991-01-01T23:59:59.000Z

    Weld hot cracking of stainless steels is a major materials-related problem in the welding industry. This present investigation evaluates the crack susceptibility of highly-constrained EB welds made in materials whose DeLong ferrite potentials range from zero to nine FN. In addition, the effect of piece part strength level on cracking is examined. This study has revealed that these deep penetration EB welds have regions that solidify as primary austenite, even when the DeLong ferrite potential is as high as 9 FN. This points out the critical role that solidification rate plays in the crack susceptibility of these highly restrained welds. In addition, 0 FN to 0 FN welds had primarily transverse cracks while 6 FN to 0 FN welds had primarily centerline cracks. Of particular interest is the observation that cracks still occur if a high ferrite (greater than 6 FN) component is welded to a zero FN component. Cracking is always associated with regions which solidify as primary austenite and these cracks occur because there are areas in the weld which do not mix. Thus it is not a recommended production practice to compensate for low ferrite in one piece part with high ferrite in its mate. Finally, it is shown that a DeLong FN threshold of 4 to prevent cracking in EB welds in not valid. 21 refs., 16 figs.

  8. DOS HAYZELE Members of a workshop at Yugntruf Yidish-Vokh 8/1996, Copake, NY

    E-Print Network [OSTI]

    Finkel, Raphael

    - ze - le shteyt ley - dik zin - gen fey - gel - ekh nit mer 2. teg, zey loy - fn, yo - rn gey - en, un

  9. CSC 378 Lecture 12 August 2, 2001

    E-Print Network [OSTI]

    Penn, Gerald

    (', *) and M. Winterhalter (2) (~) Freie Unlversitat Berlin, FB Physik, WE2, Amimallee 14, 1000 Berlin 33

  10. Advanced Data Structures Jan-Apr 2012 Lecture NUMBER --DATE, 2012

    E-Print Network [OSTI]

    Raman, Venkatesh

    ) Freie Universitat Berlin~ FB Physik~ Institut fur Theoretische Physik, WE 2~ Amimallee 14~ 1000 Berlin

  11. Algebra Lineal 1 Un problema de la Tarea num. 12 (Por entregar el miercoles, 21 de mayo, 2003)

    E-Print Network [OSTI]

    Bor, Gil

    Algebra Lineal 1 ­ Un problema de la Tarea num. 12 (Por entregar el miercoles, 21 de mayo, 2003) Sean Av = b y A v = b dos sistemas de m ecuaciones lineales con n incognitas con coeficientes en un campo F, donde v Fn , b, b Fm y A, A son tranformaciones lineales Fn Fm (matrices m × n). Hemos

  12. Some application of Malliavin calculus to SPDE and convergence of densities

    E-Print Network [OSTI]

    Lu, Fei

    2013-05-31T23:59:59.000Z

    to the fourth moment theorem is provided by Nourdin and Peccati [34] (see also Nourdin and Peccati [35]). Bringing together Stein’s 5 method with Malliavin calculus, they proved a bound for the total variation distance, dTV (Fn,N) := sup B?B(R) |P(Fn ? B...

  13. Syllabus Analyse B2 door T. H. Koornwinder

    E-Print Network [OSTI]

    Wiegerinck, Jan

    , 1990. [5] W. Rudin, Principles of mathematical analysis, McGraw-Hill, Third ed., 1976. [6] W. Walter functierij (fn) n=1 convergeert puntsgewijs op X naar een limietfunctie f op X als voor elke x X geldt dat als er voor elke > 0 een natuurlijk getal N bestaat zo dat voor alle n N geldt dat |f(x) - fn

  14. fur Mathematik in den Naturwissenschaften

    E-Print Network [OSTI]

    in Quantum Information Geometry (revised version: August 2002) by Nihat Ay and Wilderich Tuschmann Preprint no.: 69 2002 #12;#12;DUALITY VERSUS DUAL FLATNESS IN QUANTUM INFORMATION GEOMETRY NIHAT AY as to pure state estimation theory (cf. [FN1], [FN2], [Mats]). Date: August 15, 2002. 1 #12;2 NIHAT AY

  15. Max-Planck-Institut f ur Mathematik

    E-Print Network [OSTI]

    Flatness in Quantum Information Geometry (revised version: August 2002) by Nihat Ay and Wilderich Tuschmann Preprint no.: 69 2002 #12; #12; DUALITY VERSUS DUAL FLATNESS IN QUANTUM INFORMATION GEOMETRY NIHAT AY as to pure state estimation theory (cf. [FN1], [FN2], [Mats]). Date: August 15, 2002. 1 #12; 2 NIHAT AY

  16. Carrier recombination mechanisms and efficiency droop in GaInN/GaN light-emitting diodes

    SciTech Connect (OSTI)

    Dai, Qi; Shan, Qifeng; Wang, Jing; Chhajed, Sameer; Cho, Jaehee; Schubert, E. Fred; Crawford, Mary H.; Koleske, Daniel D.; Kim, Min-Ho; Park, Yongjo

    2010-01-01T23:59:59.000Z

    We model the carrier recombination mechanisms in GaInN/GaN light-emitting diodes as R=An+Bn{sup 2} +Cn{sup 3} +f(n) , where f(n) represents carrier leakage out of the active region. The term f(n) is expanded into a power series and shown to have higher-than-third-order contributions to the recombination. The total third-order nonradiative coefficient (which may include an f(n) leakage contribution and an Auger contribution) is found to be 8×10{sup ?29} ?cm{sup 6} ?s{sup ?1} . Comparison of the theoretical ABC+f(n) model with experimental data shows that a good fit requires the inclusion of the f(n) term.

  17. Measurement of sin(2)?(?)(eff) and Z-light quark couplings using the forward-backward charge asymmetry in pp-bar?Z/?*?e(+)e(?) events with L=5.0??fb(?1) at s?=1.96??TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Carrasco-Lizarraga, M. A.; Clutter, Justace Randall; McGivern, Carrie Lynne; Sekaric, Jadranka; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.

    2011-07-26T23:59:59.000Z

    -Institute NIKHEF and University of Amsterdam/NIKHEF, Amsterdam, The Netherlands 34Radboud University Nijmegen/NIKHEF, Nijmegen, The Netherlands 35Joint Institute for Nuclear Research, Dubna, Russia 36Institute for Theoretical and Experimental Physics, Moscow..., Russia 37Moscow State University, Moscow, Russia 38Institute for High Energy Physics, Protvino, Russia 39Petersburg Nuclear Physics Institute, St. Petersburg, Russia 40Institucio´ Catalana de Recerca i Estudis Avanc¸ats (ICREA) and Institut de F?´sica d...

  18. 10/1/2014 Micro-windmill research encourages innovation -The Shorthorn : News http://www.theshorthorn.com/news/micro-windmill-research-encourages-innovation/article_d477da18-48fb-11e4-a7ee-001a4bcf6878.html?mode=print 1/2

    E-Print Network [OSTI]

    Chiao, Jung-Chih

    once offered her and the rest of his students to fabricate a 3D windmill from silicon in his advanced6878.html?mode=print 1/2 Micro-windmill research encourages innovation By Benjamin Owens, The Shorthorn-windmill, which could change the way humans harness energy in the future, they hope to see students inspired

  19. 2/1/2014 Tinywindmills mayone daypower cell phones http://www.eetindia.co.in/articleLogin.do?artId=8800694132&fromWhere=/ART_8800694132_1800008_NT_36244fb4.HTM&catId=1800008&newsType=NT&pag... 1/3

    E-Print Network [OSTI]

    Chiao, Jung-Chih

    perfect sound experience Researchers study graphene photodetectors Wearable energy storage devices power Hydrogen fuel cells yet to take off ... Microgrids to generate $20B revenue ... Posted: 15 Jan 2014 Print Comment on "Tiny windmills may one day power cel..." Username: Visitor0126(To avoid code verification

  20. 10/1/2014 Micro-windmill research encourages innovation -The Shorthorn : News http://www.theshorthorn.com/news/micro-windmill-research-encourages-innovation/article_d477da18-48fb-11e4-a7ee-001a4bcf6878.html 1/3

    E-Print Network [OSTI]

    Chiao, Jung-Chih

    their patents through the office may save the money they would have spent employing a patent lawyer separately vehicle Mavericks report to fall training Oozeball serves up dirty competition J.R. Bentley's needs $50K

  1. Search for R-Parity Violating Decays of Sneutrinos to e?, ??, and e? Pairs in pp? Collisions at ?s=1.96??TeV

    E-Print Network [OSTI]

    Bauer, Gerry P.

    We present a search for supersymmetric neutrino ?˜ production using the Tevatron pp? collision data collected with the CDF II detector and corresponding to an integrated luminosity of 1??fb-1 [fb superscript -1]. We focus ...

  2. RoboCup 2004 Thomas Rofer

    E-Print Network [OSTI]

    Stryk, Oskar von

    RoboCup 2004 Thomas R¨ofer Tim Laue Center for Computing Technology, FB 3 Informatik, Universit Stefan Uhrig Fachgebiet Simulation und Systemoptimierung, FB 20 Informatik, Technische Universit

  3. On Optimal Slicing of Parallel Programs Markus Muller-Olm

    E-Print Network [OSTI]

    Müller-Olm, Markus

    On Optimal Slicing of Parallel Programs Markus M¨uller-Olm Universit¨at Dortmund, FB Informatik, LS

  4. Combining Synthetic Data with Subsampling to Create Public Use Microdata Files for Large

    E-Print Network [OSTI]

    Reiter, Jerome P.

    of monomial ideals Klaus Altmanna , Bernd Sturmfelsb, aFB Mathematik und Informatik, WE2, Freie Universität

  5. Discrete Mathematics and Theoretical Computer Science DMTCS vol. 14:1, 2012, 120 Vertex-colouring edge-weightings with two

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    of experimental results M. M. Ko~ov (I, *) and M. Winterhalter (2) (') Freie Unlversitat Berlin, FB Physik, WE2

  6. When queens were dissected after the start of oviposition, an average of 1 million

    E-Print Network [OSTI]

    Boyer, Edmond

    (Poly- techn Gesselschaft) Fb Biologie der JW Goethe-Universität Frankfurt, Karl-von- Frisch-Weg 2, D

  7. Development of a Biomarker and Clay Based Remediation Strategy for Populations at Risk for Fumonisin Toxicosis

    E-Print Network [OSTI]

    Robinson, Abraham

    2012-07-16T23:59:59.000Z

    the toxin using established in vitro techniques; 2) evaluate urinary FB1 as a biomarker of exposure from a fumonisin contaminated diet; 3) utilize urinary FB1 as a diagnostic tool to evaluate the efficacy of NS in reducing biomarkers of FB1 bioavailability...

  8. Outgoing-Pltze 2015/16 (Stand: 19.11.2014) Fachbereich

    E-Print Network [OSTI]

    Haller-Dintelmann, Robert

    University Englisch B2 FB 01 Ungarn Budapesti Mszaki és Gazdaságtudományi Egyetem English B2 Hungarian B2 FB 01 Ungarn University of Pannonia F English B1 FB 02 Sprachwissenschaften Finnland �bo Akademi

  9. EVALUATION OF COMPLEMENTARITY TECHNIQUES FOR MINIMAL COORDINATE CONTACT DYNAMICS

    E-Print Network [OSTI]

    -Marquardt Algorithm PLM Projected Levenberg-Marquardt Algorithm MLCP-FB-RLM Contact dynamics solver, where the dynam function, and solved with the help of the RLM algorithm MLCP-FB-PLM Similar to the MLCP-FB-RLM solver ex- cept that the PLM algorithm is used to tackle the optimization problem MLCP-PATH Contact dynamics

  10. Results and prospects for Y(5S) running at B-factories

    E-Print Network [OSTI]

    A. Drutskoy

    2008-07-24T23:59:59.000Z

    Recent results and future prospects for Y(5S) running at B-factories are discussed. The first Belle measurements with 23.6 fb-1 of data taken at the Y(5S) energy are reported. Eligibility of potential measurements expected with 100 fb-1 and 1000 fb-1 of data at the Y(5S) is estimated.

  11. acid mononucleotide adenylyltransferase: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 14 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  12. acids syn anti-1-amino-3-2-iodoethenyl-cyclobutane-1-carboxylic...

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 43 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  13. aminoadipic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  14. aminocaproic acid eaca: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  15. ariab acidic min-influenced: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  16. acid hydrazone dpktch: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 11 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  17. acids povedenie monatsita: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  18. aminolevulinic acid dehydratase: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 18 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  19. acid-dependent ribonucleic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 40 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  20. acid docosahexaenoic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 38 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  1. aminobutyric acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 36 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  2. acid controls expression: Topics by E-print Network

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

    12 13 14 15 16 17 18 19 20 21 22 23 24 25 Next Page Last Page Topic Index 1 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  3. acid permease aap6: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 14 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  4. acid aspartic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 20 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  5. asparagic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 8 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  6. acroleic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  7. alkenoic acids: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  8. acid caffeic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 11 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  9. acidic meglcua xylotetrasaccharide: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  10. acid dicamba dicloran: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 10 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  11. aminolevulinic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 12 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  12. acid riboside salvage: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 30 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  13. acid sulfites: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 18 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  14. acid hydroperoxide lyase1: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 25 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  15. anf 4-hydroxyhomocitric acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 15 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  16. acid dioxygenase hpd: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 37 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  17. acid propionic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 19 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  18. acid sorbic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 9 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  19. acid ascorbyl palmitate: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 27 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  20. amoxicillin clavulanic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 13 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  1. acid dehydratase alad: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 15 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  2. acetoacetic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 8 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  3. acidic pathogenesis-related pr-1: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 23 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  4. acid benzoic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 24 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  5. acetylsalicylic acid aspirin: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 29 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  6. acid nda 22-562: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 17 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  7. acid vliyanie sernoj: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  8. azo barbituric acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 35 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  9. acephate cacodylic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 9 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  10. acid lna taqman: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 46 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  11. acid desaturase sfat-1-transgenic: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 34 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  12. amygdalic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 8 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  13. acid phytases paphy: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 18 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  14. acid 3-np-induced neurotoxicity: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 30 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  15. acid propanoic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 9 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  16. arachidic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 30 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  17. acid phenylmethyl eater: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 14 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  18. acid phosphoribosyltransferase 1-deficient: Topics by E-print...

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 19 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  19. acid desaturases fad2: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 35 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  20. adipic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 11 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  1. alpha-amino-isobutyric acid aib: Topics by E-print Network

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

    12 13 14 15 16 17 18 19 20 21 22 23 24 25 Next Page Last Page Topic Index 21 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  2. acid dmsa renography: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 8 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  3. acid methoxyacetic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  4. anthranilic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 10 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  5. acid hiryusan hasseigata: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  6. ameliorates subsoil acidity: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 32 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  7. aminocaproic acids: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  8. aldehydo acids: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  9. acid eicosapentaenoic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 18 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  10. acids eicosapentaenoic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 18 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  11. air-spun polyl-lactic acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  12. alkylphosphonic acid ehehpa-pc: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 8 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  13. acid ehehpa-pc 88a: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 12 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  14. arundic acid ono-2506: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 7 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  15. acid glycosaminoglycan mucopolysaccharide: Topics by E-print...

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 34 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  16. acid o-methyltransferase activity1: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 39 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  17. alpha-oxo acid decarboxylase: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 32 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  18. anti-psoriatic fumaric acid: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 15 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  19. acidic oligosaccharides paos: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 40 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...

  20. acid anhydrases: Topics by E-print Network

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

    by USDA and U of I researchers Illinois at Urbana-Champaign, University of 42 Controlling acid rain MIT - DSpace Summary: High concentrations of sulfuric and nitric acid in raTn fn...