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AbstractAbstract
[en] This paper presents recent results in QCD and diffraction physics obtained by the DO experiment at the Fermilab Tevatron pp-bar collider at s=1.96 TeV. The data used correspond to an integrated luminosity up to 150 pb-1. The different measurements are jet inclusive and dijet cross sections, dijet azimuthal decorrelation, diffractively produced Z bosons and elastic scattering study
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DIFFRACTION 2004: International workshop on diffraction in high-energy physics; Cala Gonone, Sardinia (Italy); 18-23 Sep 2004; S0920-5632(05)00369-5; Copyright (c) 2005 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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AbstractAbstract
[en] A prospective analysis for the discovery of a light Higgs boson in the Compact Muon Solenoid (CMS) experiment at the Large Hadron Collider (LHC) is presented. The associated production channels WH and ZH of a Higgs boson decaying into a photon pair are studied using a full detector simulation. The method of analysis here employed should permit the utilization of real data once they become available in order to optimize the analysis performance and to estimate background rates. Minimizing in this way reliance on simulated data should allow a significant reduction in systematic errors. One year of LHC running at high luminosity (integrated luminosity of 100 fb-1) should allow an observation at 3σ of the Standard Model Higgs boson from the LEP lower limit of 114.4 GeV/c2 up to 146 GeV/c2. Three years of running at high luminosity should allow a 5σ discovery from the LEP lower limit up to 148 GeV/c2. In the context of supersymmetric models, the dominant gluon fusion Higgs boson production process could be strongly suppressed. This light Higgs gluophobic scenario could occur when the mixing in the stop sector is maximal. In such a case, the associated production channels WH and ZH may be recovery channels. (research note from collaboration)
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S0954-3899(07)34127-3; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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Journal of Physics. G, Nuclear and Particle Physics; ISSN 0954-3899; ; CODEN JPGPED; v. 34(4); p. N105-N131
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ACCELERATORS, BOSONS, CYCLIC ACCELERATORS, ELECTRIC COILS, ELECTRICAL EQUIPMENT, ELEMENTARY PARTICLES, ENERGY RANGE, EQUIPMENT, FERMIONS, FIELD THEORIES, GRAND UNIFIED THEORY, INTERMEDIATE BOSONS, INTERMEDIATE VECTOR BOSONS, LEPTONS, MASSLESS PARTICLES, MATHEMATICAL MODELS, MEASURING INSTRUMENTS, PARTICLE MODELS, POSTULATED PARTICLES, QUANTUM FIELD THEORY, SIMULATION, SPECTROMETERS, STORAGE RINGS, SYMMETRY, SYNCHROTRONS, UNIFIED GAUGE MODELS
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Abazov, V.M.; Abbott, B.; Abolins, M.; Acharya, B.S.; Adams, M.; Adams, T.; Agelou, M.; Agram, J.-L.; Ahn, S.H.; Ahsan, M.; Alexeev, G.D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G.A.; Anastasoaie, M.; Andeen, T.; Anderson, S.; Andrieu, B.; Anzelc, M.S.; Arnoud, Y.
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: US Department of Energy (United States)
arXiv e-print [ PDF ]2006
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: US Department of Energy (United States)
arXiv e-print [ PDF ]2006
AbstractAbstract
[en] The authors report a measurement of the Bs0 lifetime in the semileptonic decay channel Bs0 → Ds-μ+νX (and its charge conjugate), using approximately 0.4 fb-1 of data collected with the D0 detector during 2002-2004. They have reconstructed 5176 Ds- μ+ signal events, where the Ds- is identified via the decay Ds0 → φπ-, followed by φ → K+K-. Using these events, they have measured the Bs0 lifetime to be τ(Bs0) = 1.398 ± 0.044 (stat)-0.025+0.028(syst) ps. This is the most precise measurement of the Bs0 lifetime to date
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1 Apr 2006; 7 p; ARXIV EPRINT NUMBER HEP-EX/0604046; AC02-76CH03000; Available from http://lss.fnal.gov/cgi-bin/find_paper.pl?pub-06-085-E.pdf; PURL: https://www.osti.gov/servlets/purl/892507-mFnkfT/
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ANTILEPTONS, ANTIMATTER, ANTIPARTICLES, B MESONS, BEAUTY MESONS, BEAUTY PARTICLES, BOSONS, CHARM PARTICLES, CHARMED MESONS, D MESONS, DECAY, ELEMENTARY PARTICLES, FERMIONS, HADRONS, KAONS, LEPTONS, MASSLESS PARTICLES, MATTER, MESONS, MUONS, PARTICLE DECAY, PIONS, PSEUDOSCALAR MESONS, STRANGE MESONS, STRANGE PARTICLES, WEAK PARTICLE DECAY
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Abazov, V.M.; Abbott, B.; Abolins, M.; Acharya, B.S.; Adams, M.; Adams, T.; Agelou, M.; Agram, J.-L.; Ahn, S.H.; Ahsan, M.; Alexeev, G.D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G.A.; Anastasoaie, M.; Andeen, T.; Anderson, S.; Andrieu, B.; Anzelc, M.S.; Arnoud, Y.
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: US Department of Energy (United States)
arXiv e-print [ PDF ]2006
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: US Department of Energy (United States)
arXiv e-print [ PDF ]2006
AbstractAbstract
[en] We present a search for electroweak production of single top quarks in the s-channel (p(bar p) → t(bar b) + X) and t-channel (p(bar p) → tq(bar b) + X) modes. We have analyzed 230 pb-1 of data collected with the D0 detector at the Fermilab Tevatron collider at a center-of-mass energy of √s = 1.96 TeV. Two separate analysis methods are used: neural networks and a cut-based analysis. No evidence for a single top quark signal is found. We set 95% confidence level upper limits on the production cross sections using Bayesian statistics, based on event counts and binned likelihoods formed from the neural network output. The limits from the neural network (cut-based) analysis are 6.4 pb (10.6 pb) in the s-channel and 5.0 pb (11.3 pb) in the t-channel
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1 Apr 2006; 28 p; ARXIV EPRINT NUMBER HEP-EX--0604020; AC02-76CH03000; Available from http://lss.fnal.gov/cgi-bin/find_paper.pl?pub-06-069-E.pdf; PURL: https://www.osti.gov/servlets/purl/892398-bFKW4M/
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AbstractAbstract
No abstract available
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(c) 2008 The American Physical Society; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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Abazov, V. M.; Abbott, B.; Abolins, M.; Acharya, B. S.; Adams, M.; Adams, T.; Agelou, M.; Agram, J.-L.; Ahn, S. H.; Ahsan, M.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; Anastasoaie, M.; Andeen, T.; Anderson, S.; Andrieu, B.; Arnoud, Y.
D0 Collaboration
arXiv e-print [ PDF ]2008
D0 Collaboration
arXiv e-print [ PDF ]2008
AbstractAbstract
No abstract available
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(c) 2008 The American Physical Society; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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Abazov, V. M.; Abbott, B.; Abolins, M.; Acharya, B. S.; Adams, M.; Adams, T.; Agelou, M.; Agram, J.-L.; Ahn, S. H.; Ahsan, M.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; Anastasoaie, M.; Anderson, S.; Andrieu, B.; Arnoud, Y.; Askew, A.
D0 Collaboration
arXiv e-print [ PDF ]2008
D0 Collaboration
arXiv e-print [ PDF ]2008
AbstractAbstract
No abstract available
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(c) 2008 The American Physical Society; Country of input: International Atomic Energy Agency (IAEA)
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Agram, J.-L.; Angarano, M.M.; Assouak, S.; Bergauer, T.; Bilei, G.M.; Borrello, L.; Brianzi, M.; Civinini, C.; Dierlamm, A.; Dinu, N.; Demaria, N.; Feld, L.; Focardi, E.; Fontaine, J.-C.; Forton, E.; Furgeri, A.; Gregoire, Gh.; Hartmann, F.; Honma, A.; Juillot, P.; Kartashov, D.; Krammer, M.; Macchiolo, A.; Mannelli, M.; Messineo, A.; Migliore, E.; Militaru, O.; Piasecki, C.; Santinelli, R.; Sentenac, D.; Servoli, L.; Starodumov, A.; Tonelli, G.; Wang, J., E-mail: krammer@hephy.oeaw.ac.at2004
AbstractAbstract
[en] The Compact Muon Solenoid (CMS) is one of the experiments at the Large Hadron Collider (LHC) under construction at CERN. Its inner tracking system consist of the world largest Silicon Strip Tracker (SST). In total it implements 24,244 silicon sensors covering an area of 206 m2. To construct a large system of this size and ensure its functionality for the full lifetime of 10 years under LHC condition, the CMS collaboration developed an elaborate design and a detailed quality assurance program. This paper describes the strategy and shows first results on sensor qualification
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S0168900203026512; Copyright (c) 2003 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment; ISSN 0168-9002; ; CODEN NIMAER; v. 517(1-3); p. 77-93
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Abazov, V.M.; Abbott, B.; Abolins, M.; Acharya, B.S.; Adams, D.L.; Adams, M.; Adams, T.; Agelou, M.; Agram, J.-L.; Ahmed, S.N.; Ahn, S.H.; Ahsan, M.; Alexeev, G.D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G.A.; Anastasoaie, M.; Andeen, T.; Anderson, J.T.; Anderson, S.; Buenos Aires U., Rio de Janeiro, CBPF, Sao Paulo, IFT, Alberta U., Simon Fraser U., York U., Canada, McGill U., Beijing, Inst. High Energy Phys., Hefei, CUST, Andes U., Bogota, Charles U., Prague, Tech. U., Prague, Inst. Phys., San Francisco de Quito U., Clermont-Ferrand U., LPSC, Grenoble, Marseille, CPPM, Orsay, LAL, Paris U., VI-VII, DAPNIA, Saclay, Strasbourg, IReS
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: US Department of Energy (United States)
arXiv e-print [ PDF ]2005
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: US Department of Energy (United States)
arXiv e-print [ PDF ]2005
AbstractAbstract
[en] The D0 experiment enjoyed a very successful data-collection run at the Fermilab Tevatron collider between 1992 and 1996. Since then, the detector has been upgraded to take advantage of improvements to the Tevatron and to enhance its physics capabilities. We describe the new elements of the detector, including the silicon microstrip tracker, central fiber tracker, solenoidal magnet, preshower detectors, forward muon detector, and forward proton detector. The uranium/liquid-argon calorimeters and central muon detector, remaining from Run I, are discussed briefly. We also present the associated electronics, triggering, and data acquisition systems, along with the design and implementation of software specific to D0
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1 Jul 2005; 142 p; ARXIV EPRINT NUMBER PHYSICS/0507191; AC02-76CH03000; Available from OSTI as DE15020158; PURL: https://www.osti.gov/servlets/purl/15020158-IN30F6/
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Abazov, V.M.; Abbott, B.; Abolins, M.; Acharya, B.S.; Adams, M.; Adams, T.; Agelou, M.; Agram, J.-L.; Ahn, S.H.; Ahsan, M.; Alexeev, G.D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G.A.; Anastasoaie, M.; Andeen, T.; Anderson, S.; Andrieu, B.; Anzelc, M.S.; Arnoud, Y.; Buenos Aires U.; Rio de Janeiro, CBPF; Rio de Janeiro State U.; Sao Paulo, IFT; Alberta U.; Simon Fraser U.; York U., Canada; McGill U.; Beijing, Inst. High Energy Phys.; Hefei, CUST; Andes U., Bogota; Charles U.; Prague, Tech. U.; Prague, Inst. Phys.; San Francisco de Quito U.; Clermont-Ferrand U.; LPSC, Grenoble; Marseille, CPPM; Orsay, LAL; Paris U., VI-VII; DAPNIA, Saclay
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: US Department of Energy (United States)
arXiv e-print [ PDF ]2006
Fermi National Accelerator Lab., Batavia, IL (United States). Funding organisation: US Department of Energy (United States)
arXiv e-print [ PDF ]2006
AbstractAbstract
[en] A search for the production of neutral Higgs bosons Φ decaying into τ+τ- final states in p(bar p) collisions at a center-of-mass energy of 1.96 TeV is presented. The data, corresponding to an integrated luminosity of approximately 325 pb-1, were collected by the D0 experiment at the Fermilab Tevatron Collider. Since no excess compared to the expectation from standard model processes is found, limits on the production cross section times branching ratio are set. The results are combined with those obtained from the D0 search for Φb((bar b)) → b(bar b)b((bar b)) and are interpreted in the minimal supersymmetric standard model
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1 May 2006; 7 p; ARXIV EPRINT NUMBER HEP-EX/0605009; AC02-76CH03000; Available from http://lss.fnal.gov/cgi-bin/find_paper.pl?pub-06-092.pdf; PURL: https://www.osti.gov/servlets/purl/892432-GMv89H/
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