27 results on '"B.J. KING"'
Search Results
2. Shelter type and birth number influence the birth and death sites of lambs and ewe movement around lambing time
- Author
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J.C. Broster, R.L. Dehaan, D.L. Swain, S.M. Robertson, B.J. King, and M.A. Friend
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Genetics ,Animal Science and Zoology ,General Medicine ,Food Science - Published
- 2017
- Full Text
- View/download PDF
3. Recent QCD results from NuTeV/CCFR Collaboration
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D. Buchholz, A. Romosan, V. Wu, D. Mason, J. E. Brau, G. P. Zeller, T. A. Bolton, F. J. Sculli, B.J. King, Jan Conrad, M. J. Lamm, S. R. Mishra, U. K. Yang, R. B. Drucker, P. Spentzouris, W. H. Smith, C. McNulty, S. Avvakumov, T. Kinnel, D. A. Harris, Joseph A. Formaggio, A. Vaitaitis, W. K. Sakumoto, A. Alton, Todd Adams, K. S. McFarland, H. Schellman, J. H. Kim, R. H. Bernstein, P. de Barbaro, W. G. Seligman, W. Marsh, M. Goncharov, A. O. Bazarko, C. G. Arroyo, S. Koutsoliotas, M. H. Shaevitz, D. Naples, E. G. Stern, R. A. Johnson, H. S. Budd, B. Tamminga, L. Bugel, R. Frey, L. de Barbaro, Jinhong Yu, P. Nienaber, A. Bodek, M. Vakili, and J. Goldman
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Physics ,Quantum chromodynamics ,Nuclear and High Energy Physics ,Particle physics ,Neutral current ,High Energy Physics::Phenomenology ,Nuclear Theory ,Deep inelastic scattering ,Atomic and Molecular Physics, and Optics ,Charm quark ,Nuclear physics ,High Energy Physics::Experiment ,Fermilab ,Charm (quantum number) ,Neutrino ,Nuclear Experiment ,Nucleon - Abstract
Fermilab experiments CCFR and its successor NuTeV study nucleon structure through deep inelastic scattering of neutrino beams off an iron target. We report on the most recent CCFR measurement of the νN differential cross section and resulting structure functions ΔxF 3 = xF ν 3 − xF ν 3 , and R long = σ L σ T , in the framework of massive charm quark. ΔxF3 in sensitive to strange and charm content of the nucleon. NuTeV's preliminary direct measurement of the strange sea, from dimuon charged-current production, and nucleon charm content probed by neutral-current νN interaction, are also presented.
- Published
- 2000
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4. A measurement of and R with the CCFR detector
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D. Naples, C. McNulty, W.C. Lefmann, D. Buchholz, D. Mason, W. G. Seligman, T. Kinnel, P. Nienaber, Jan Conrad, K. S. McFarland, L. de Barbaro, Jinhong Yu, G. P. Zeller, T. A. Bolton, U. K. Yang, L. Bugel, R. Frey, R. B. Drucker, H. Schellman, S.R. Mishra, C.G. Arroyo, A.O. Bazarko, P. de Barbaro, D. A. Harris, W. Marsh, J. E. Brau, W. K. Sakumoto, P. Spentzouris, A. Romosan, F. J. Sciulli, M. J. Lamm, A. Bodek, E. G. Stern, B.M. Tamminga, A. Alton, W. H. Smith, A. Vaitaitis, J. Goldman, M. Goncharov, Joseph A. Formaggio, B.J. King, R. A. Johnson, H. S. Budd, V. Wu, Todd Adams, M. H. Shaevitz, J. H. Kim, R. H. Bernstein, S. Avvakumov, S. Koutsoliotas, and M. Vakili
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Quantum chromodynamics ,Physics ,Scattering cross-section ,Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,High Energy Physics::Phenomenology ,Detector ,Atomic and Molecular Physics, and Optics ,Charm quark ,Nuclear physics ,High Energy Physics::Experiment ,Charm (quantum number) ,Nuclear Experiment ,Nucleon - Abstract
We report on a measurement of the neutrino-nucleon and antineutrino-nucleon differential cross sections in the CCFR detector. The measurement of the differential cross sections over a wide range of energies allows ΔχF 3 = χF 3 ν −χF 3 v and R to be extracted. ΔχF3 is related to the difference between the contributions of the strange and charm seas in the nucleon to production of massive charm quark. The results for ΔχF3 are compared to various massive charm NLO QCD models. The Q2 dependence of R for χ
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- 1999
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5. The Effect of Mandibular Fracture Treatment on Nutritional Status
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Brian J. Christensen and B.J. King
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Otorhinolaryngology ,business.industry ,Mandibular fracture ,Dentistry ,Medicine ,Surgery ,Nutritional status ,Oral Surgery ,business ,medicine.disease - Published
- 2016
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6. A study of the energy dependence of the mean, truncated mean, and most probable energy deposition of high-energy muons in sampling calorimeters
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P.Z. Quintas, A. O. Bazarko, W. G. Seligman, P. de Barbaro, P.H. Sandler, M. J. Lamm, D. D. Yovanovitch, F. Borcherding, W. H. Smith, W.C. Leung, H. E. Fisk, P. Auchincloss, M. Pillai, S. R. Mishra, W. K. Sakumoto, M. J. Oreglia, F. S. Merritt, S.A. Rabinowitz, W. Marsh, A. Bodek, B.J. King, C. Foudas, H. Schellman, C. G. Arroyo, E. Oltman, K.T. Bachmann, B.A. Schumm, R.E. Blair, T. Kinnel, W.C. Lefmann, F. J. Sciulli, H. S. Budd, F. Qun, M. H. Shaevitz, K. W. Merritt, R. H. Bernstein, and T. Bolton
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Range (particle radiation) ,Muon ,Large Hadron Collider ,Physics::Instrumentation and Detectors ,Hadron ,Tevatron ,Particle detector ,Calorimeter ,Nuclear physics ,High Energy Physics::Experiment ,Neutrino ,Instrumentation - Abstract
We have extracted the momentum dependence of the mean, the truncated mean and the most probable value of the energy deposited in a segmented, iron-scintillator, hadron calorimeter by high-energy muons. Data were drawn from a sample of momentum-analyzed, high-energy muons produced in charged-current neutrino interactions. The truncated mean energy deposition of high-energy muons traversing 20 calorimeter segments increases by approximately 16% per 100 GeV c increase in muon momentum over the range 25−125 GeV c ; the most probable energy deposition increases by approximately 7%. These results are important for experiments at high-energy colliders (e.g., Tevatron, SSC and LHC) which use the d E d x of high-energy muons to calibrate the response of electromagnetic and hadron calorimeters with tower geometry. The data are in qualitative agreement with GEANT3 (v3.15/308a) simulations.
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- 1994
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7. Hadron shower energy and direction measurements using drift chambers
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F. J. Sciulli, R. H. Bernstein, C. G. Arroyo, H. Schellman, A. Bodek, H. S. Budd, B.J. King, D. D. Yovanovitch, S. R. Mishra, K.T. Bachmann, K. W. Merritt, T. Kinnel, W. G. Seligman, P. de Barbaro, H. E. Fisk, W. Marsh, E. Oltman, F. S. Merritt, M. J. Lamm, W. K. Sakumoto, W.C. Lefmann, B.A. Schumm, S.A. Rabinowitz, W. H. Smith, C. Foudas, M. J. Oreglia, P.H. Sandler, W.C. Leung, P.Z. Quintas, A. O. Bazarko, T. Bolton, M. H. Shaevitz, and F. Borcherding
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Physics::Instrumentation and Detectors ,Astrophysics::High Energy Astrophysical Phenomena ,High Energy Physics::Phenomenology ,Hadron ,Astrophysics::Instrumentation and Methods for Astrophysics ,Tevatron ,Nuclear physics ,Shower ,Test beam ,Scintillation counter ,High Energy Physics::Experiment ,Fermilab ,Instrumentation ,Energy (signal processing) - Abstract
We report energy and angle resolutions for hadron showers produced in the CCFR iron target-calorimeter. The measurements were made using drift chambers instrumented with FADC readout; showers were produced using a momentum-analyzed hadron test beam from the Fermilab Tevatron at energies of 40, 70, 100, 150, and 200 GeV. Shower energy measurements are compared to measurements using scintillation counters in the same target.
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- 1994
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8. A measurement of the Gross-Llewellyn Smith sum rule from the CCFR xF3 structure function
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B.A. Schumm, F. J. Sciulli, E. Oltman, S. R. Mishra, K. W. Merritt, K.T. Bachmann, R.E. Blair, D. D. Yovanovitch, W. Marsh, M. J. Lamm, H. S. Budd, H. E. Fisk, M. H. Shaevitz, W.C. Leung, P.Z. Quintas, W. H. Smith, F. S. Merritt, P. de Barbaro, B.J. King, R. H. Bernstein, W. G. Seligman, A. Bodek, W.C. Lefmann, W. K. Sakumoto, P.H. Sandler, S.A. Rabinowitz, C. Foudas, C. G. Arroyo, H. Schellman, M. J. Oreglia, and F. Borcherding
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Structure function ,Sum rule in quantum mechanics - Abstract
We report a measurement of the Gross-Llewellyn Smith sum rule: ∫( 1 x ) d x xF 3 (x, Q 2 =3 GeV 2 )=2.50±0.018( stat. ) ±0.078( syst. ) .
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- 1993
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9. Tests of perturbative QCD using CCFR data for measurements of nucleon structure functions
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W. G. Seligman, D. D. Yovanovitch, K. W. Merritt, F. J. Sciulli, M. J. Lamm, S.A. Rabinowitz, M. J. Oreglia, S. R. Mishra, A. Bodek, F. S. Merritt, C. Foudas, W.C. Lefmann, W.C. Leung, W. H. Smith, W. Marsh, H. S. Budd, K.T. Bachmann, R.E. Blair, P.H. Sandler, H. Schellman, W. K. Sakumoto, B.J. King, C. G. Arroyo, P.Z. Quintas, R. H. Bernstein, E. Oltman, B.A. Schumm, M. H. Shaevitz, H. E. Fisk, F. Borcherding, and P. de Barbaro
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Quantum chromodynamics ,Quark ,Physics ,Nuclear and High Energy Physics ,Particle physics ,High Energy Physics::Phenomenology ,Tevatron ,Perturbative QCD ,Parton ,Atomic and Molecular Physics, and Optics ,Nuclear physics ,High Energy Physics::Experiment ,Sum rule in quantum mechanics ,Fermilab ,Nucleon - Abstract
We present measurements of nucleon structure functions, F2(ϰ, Q2) and xFs(ϰ, Q2), from the high-statistics, high-energy neutrino-iron scattering experiment at the Fermilab Tevatron. The existing high-statistics xF3 determination by the CDHSW collaboration is compared to our data. The data presented here constitute the first corroboration of the QCD prediction of xF3 evolution at low-ϰ, and yields ΛMS=210±28±41 MeV, and a determination of the GLS sum rule at Q2 = 3 GeV2, SGLS = ∫ϰ1xFsϰ=2.50±0.018 (stat.)±0.078 (syst.). Our value of ΛMS yields α3(Mz) = .111 ± .002 ± .003 ± .003 (scale). Comparison of the neutrino determination of F2(ϰ, Q2) with that obtained from the charged-lepton (e or μ) scattering leads to a precise test of the mean-square charge prediction by the Quark Parton Model. The SLAC-CCFR and BCDMS structure function provide a consistent and precise set of structure functions over a large range of Q2.
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- 1993
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10. Precision measurement of sin2θ from vFe scattering at the Tevatron
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T. Bolton, K.T. Bachmann, F. S. Merritt, R.E. Blair, T. Kinnel, W.C. Leung, P.Z. Quintas, D. D. Yovanovitch, W. Marsh, F. J. Sciulli, R. H. Bernstein, B.A. Schumm, W.C. Lefmann, H. S. Budd, S. R. Mishra, C. G. Arroyo, W. G. Seligman, P.H. Sandler, H. Schellman, S.A. Rabinowitz, K. W. Merritt, F. Borcherding, C. Foudas, B.J. King, M. J. Oreglia, W. K. Sakumoto, A. Bodek, M. J. Lamm, W. H. Smith, M. H. Shaevitz, P. de Barbaro, H. E. Fisk, E. Oltman, and A. O. Bazarko
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Nuclear physics ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Physics::Instrumentation and Detectors ,Scattering ,Detector ,Tevatron ,High Energy Physics::Experiment ,Fermilab ,Neutrino ,Atomic and Molecular Physics, and Optics - Abstract
We present the results of a preliminary determination of sin 2 θ W from a study of vFe scattering in the Lab E detector at Fermilab. The analysis is based on a sample of 5 × 10 5 events with a mean neutrino energy of 166 GeV. Our result, sin 2 θ W = 0.2242 ± 0.0044 expt . ± 0.0047 model , is the highest energy high statistics determination of the weak mixing angle using neutrino data.
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- 1993
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11. Neutrino production of Dimuons at the Fermilab tevatron
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W.C. Lefmann, F. S. Merritt, M. J. Lamm, B.J. King, S.A. Rabinowitz, W. H. Smith, E. Oltman, H. Schellman, C. Foudas, F. J. Sciulli, K. W. Merritt, P.Z. Quintas, W. Marsh, D. D. Yovanovitch, W.C. Leung, F. Borcherding, K.T. Bachmann, W. K. Sakumoto, Arie Bodek, H. S. Budd, M. J. Oreglia, R.E. Blair, C. G. Arroyo, T. Kinnel, R. H. Bernstein, A. O. Bazarko, B.A. Schumm, W. G. Seligman, S. R. Mishra, P.H. Sandler, M. H. Shaevitz, H. E. Fisk, and P. de Barbaro
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Nuclear physics ,Physics ,Nuclear and High Energy Physics ,Strange quark ,Particle physics ,Muon ,Cabibbo–Kobayashi–Maskawa matrix ,Tevatron ,Fermilab ,Neutrino ,Strangeness ,Nucleon ,Atomic and Molecular Physics, and Optics - Abstract
Neutrino and antineutrino interactions with two muons in the final state have been studied by the CCFR collaboration in the Fermilab Tevatron neutrino beam. The rate of neutrino- and antineutrino-induced prompt same-sign dimuon production in steel was measured using a sample of 220 μ−μ− events and 15 μ+μ+ events with Pμ > 9 GeV/c, and energies between 30 GeV and 600 GeV. After background subtraction, the prompt rate of same-sign dimuon production is (0.53 ± 0.24) × 10−4 per νμ charged-current event and (0.52 ± 0.33) × 10 −4 per ν μ charged-current event. After demanding Pμ1 ≥ 9 GeV/c, Pμ2 ≥ 5 GeV/c and 30 ≤ Eν ≤ 600 GeV a sample of 5044 ν μ 1062 ν μ induced μ ∓ μ ± events are observed. The data support the slow rescaling model of charm production with a value of mc = 1.31 ± .24 GeV/c2. The CKM matrix element Vcd=.209±0.012 and the nucleon strangeness content, ηe=.064−0.00065+0.00075 are measured with the strange sea x distribution found to be softer than its non-strange counterpart. The first measurements of the Q2 dependence of the strange quark densities, ϰs(ϰ), are also presented.
- Published
- 1993
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12. Neutrino production of same-sign dimuons at the Fermilab Tevatron
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F. Borcherding, W. G. Seligman, W.C. Lefmann, K.T. Bachmann, R.E. Blair, T. Kinnel, M. J. Lamm, P. de Barbaro, W. H. Smith, B.J. King, P.Z. Quintas, M. H. Shaevitz, P.H. Sandler, W.C. Leung, M. J. Oreglia, W. K. Sakumoto, A. Bodek, H. Schellman, S.A. Rabinowitz, C. Foudas, R. H. Bernstein, W. Marsh, F. J. Sciulli, H. S. Budd, B.A. Schumm, S. R. Mishra, D. D. Yovanovitch, and F. S. Merritt
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Physics ,Particle physics ,Muon ,Physics and Astronomy (miscellaneous) ,Meson ,Astrophysics::High Energy Astrophysical Phenomena ,High Energy Physics::Phenomenology ,Tevatron ,Nuclear physics ,Pair production ,Neutrino detector ,High Energy Physics::Experiment ,Fermilab ,Neutrino ,Nuclear Experiment ,Engineering (miscellaneous) ,Lepton - Abstract
The rate of neutrino- and antineutrino-induced prompt same-sign dimuon production in steel was measured using a sample of μ−μ− events and 25 μ+μ+ events withPμ>9 GeV/c, produced in 1.5 millionvμ and 0.3 million\(\overline {v_\mu }\) induced charged-current events with energies between 30 GeV and 600 GeV. The data were obtained with the Chicago-Columbia-Fermilab-Rochester (CCFR) neutrino detector in the Fermilab Tevatron Quadrupole Triplet Neutrino Beam during experiments E 744 and E 770. After background subtraction, the prompt rate of same-sign dimuon production is (0.53±0.24)×10−4 pervμ charged-current event and (0.52±0.33)×10−4 per\(\overline {v_\mu }\) charged-current event. The kinematic distributions of the same-sign dimuon events after background subtraction are consistent with those of the non-prompt background due to meson decays in the hadron shower of a charged-current event. Calculations ofc\(\bar c\) gluon bremsstrahlung, based on improved measurements of the charm mass parameter and nucleon structure functions by the CCFR collaboration, yield a prompt rate of (0.09±0.39)×10−4 pervμ charged-current event. In this case,c\(\bar c\) gluon bremsstrahlung is probably not an observable source of prompt same-sign dimuons.
- Published
- 1993
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13. Comparison of hadronic shower punchthrough and TeV muon dE/dx with calculation
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F. S. Merritt, H. E. Fisk, F. Borcherding, E. Oltman, M. J. Lamm, S.A. Rabinowitz, D. D. Yovanovitch, W. G. Seligman, W. H. Smith, B.A. Schumm, C. Foudas, S. R. Mishra, A. Bodek, K.T. Bachmann, B.J. Kim, R.E. Blair, P. de Barbaro, P.Z. Quintas, W.C. Lefmann, B.J. King, C. G. Arroyo, P.H. Sandler, H. Schellman, W. K. Sakumoto, W.C. Leung, P. A. Rapidis, K. W. Merritt, W. Marsh, F. J. Sciulli, R. H. Bernstein, H. S. Budd, M. H. Shaevitz, and M. J. Oreglia
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Physics ,Nuclear and High Energy Physics ,High energy ,Particle physics ,Muon ,Calorimeter (particle physics) ,Physics::Instrumentation and Detectors ,Astrophysics::High Energy Astrophysical Phenomena ,High Energy Physics::Phenomenology ,Hadron ,Detector ,Monte Carlo method ,Atomic and Molecular Physics, and Optics ,Nuclear physics ,Shower ,Neutrino detector ,High Energy Physics::Experiment - Abstract
We have measured the longitudinal particle punchthrough probability from shower cascades produced by hadrons incident on the iron-scintillator calorimeter of the CCFR neutrino detector and have compared them to a Monte Carlo simulation. Measurements of the dE/dx energy loss iron of high energy cosmic ray muons (up to 1 TeV) incident on the same detector are presented and are compared against calculations.
- Published
- 1991
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14. Measuring muon momenta with the CCFR neutrino detector
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M. J. Lamm, S.R. Mishra, W.C. Lefmann, K. W. Merritt, Arie Bodek, Wesley H Smith, R. H. Bernstein, F. S. Merritt, Mark Oreglia, William L. Marsh, P.H. Sandler, D. D. Yovanovitch, P.Z. Quintas, F. J. Sciulli, S.A. Rabinowitz, H. Schellman, Michael H. Shaevitz, C. G. Arroyo, W.C. Leung, C. Foudas, B.A. Schumm, W. K. Sakumoto, B.J. King, F.O. Borcherding, K.T. Bachmann, R.E. Blair, P. de Barbaro, H. E. Fisk, H. S. Budd, W.G. Seligman, and E. Oltman
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Muon ,Spectrometer ,Physics::Instrumentation and Detectors ,High Energy Physics::Phenomenology ,Nuclear physics ,Neutrino detector ,Muon spectrometer ,Muon collider ,Calibration ,Physics::Accelerator Physics ,High Energy Physics::Experiment ,Neutrino ,Nuclear Experiment ,Instrumentation - Abstract
We report on muon spectrometry at the CCFR neutrino detector. The muon spectrometer and momentum-fitting analysis code are described, and results presented from the calibration of the spectrometer with test beams of momentum-analyzed muons.
- Published
- 1991
- Full Text
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15. Nucleon structure functions from νμ-Fe scattering at the Tevatron
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C. G. Arroyo, P. de Barbaro, F. Borcherding, S. R. Mishra, W. Marsh, P.H. Sandler, H. E. Fisk, M. J. Lamm, W.C. Leung, M. J. Oreglia, K.T. Bachmann, B.A. Schumm, W. H. Smith, E. Oltman, F. J. Sciulli, H. Schellman, R.E. Blair, D. D. Yovanovitch, F. S. Merritt, W. K. Sakumoto, S.A. Rabinowitz, C. Foudas, H. S. Budd, B.J. King, M. H. Shaevitz, K. W. Merritt, R. H. Bernstein, W. G. Seligman, A. Bodek, W.C. Lefmann, and P.Z. Quintas
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Physics ,Nuclear physics ,Nuclear and High Energy Physics ,Particle physics ,Scattering ,Structure function ,Tevatron ,Nucleon ,Atomic and Molecular Physics, and Optics ,Charged current - Abstract
Preliminary measurements of structure functions have been made from a sample of 1,281,000 ν μ and 270,000 ν μ charged current events with 30 GeV σ( ν μ )/σ(ν μ ) = .511 ± .002 ( stat ) ± .005 ( syst ) , and an analysis of the Q2 evolution of xF3.
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- 1991
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16. Inverse muon decay, ν+e→μ−+νe, at the Fermilab Tevatron
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D. D. Yovanovitch, F. S. Merritt, B.J. King, F. J. Sciulli, M. H. Shaevitz, W. Marsh, W.C. Lefmann, P. de Barbaro, S.A. Rabinowitz, M. J. Oreglia, C. Foudas, K. W. Merritt, H. E. Fisk, K.T. Bachmann, R.E. Blair, H. Schellman, H. S. Budd, M. J. Lamm, W. K. Sakumoto, P.Z. Quintas, A. Bodek, B. G. Seligman, B.A. Schumm, W.C. Leung, R. H. Bernstein, S. R. Mishra, W. H. Smith, F. Borcherding, and E. Oltman
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Physics ,Nuclear physics ,Nuclear and High Energy Physics ,Particle physics ,Sterile neutrino ,Muon ,Tevatron ,High Energy Physics::Experiment ,Fermilab ,Neutrino ,Neutrino oscillation ,Charged current ,Lepton - Abstract
We report an improved measurement of the inverse muon decay process, νμ+e→μ−+νe, at the Fermilab Tevatron. The rate of this reaction with respect to the νμ-N charged current interaction is measured to be (0.1245±0.0057(stat.)±0.0031 (sys.)) × 10−2. The measurement confirms the standard model predictions for the Lorentz structure of the weak current, the helicity of the neutrino, and the energy dependence of the cross section.
- Published
- 1990
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17. Calibration of the CCFR target calorimeter
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H. Schelman, S.A. Rabinowitz, D. D. Yovanovitch, R.E. Blaie, C. Foudas, Wesley H Smith, K.T. Bachmann, W.C. Lefmann, Mark Oreglia, W.G. Seligman, W. K. Sakumoto, B.J. King, P.H. Sandler, F. J. Sciulli, M. J. Lamm, W.C. Leung, P. A. Rapidis, Frank Merritt, B.A. Schumm, P.Z. Quintas, William L. Marsh, H. S. Budd, B.J. Kim, M.H. Saevitz, H. E. Fisk, E. Oltman, P. de Barbaro, F.O. Borcherding, R. H. Bernstein, K. W. Merritt, Arie Bodek, and S.R. Mishra
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Physics ,Nuclear and High Energy Physics ,Range (particle radiation) ,Particle physics ,Muon ,Calorimeter (particle physics) ,Physics::Instrumentation and Detectors ,Hadron ,Electron ,Ionizing radiation ,Nuclear physics ,Calibration ,High Energy Physics::Experiment ,Nuclear Experiment ,Instrumentation ,Energy (signal processing) - Abstract
The techniques used to calibrate and monitor the energy response of the CCFR (Lab E) iron-scintillator target calorimeter for a precision measurement of shower energies are described. Measurements on the energy response of the calorimeter to hadrons, electrons, and minimum ionizing muons (from range outs) are presented. The calorimeter's energy response and resolution for hadrons and electrons are obtained using a test beam with energies between 15 and 450 GeV.
- Published
- 1990
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18. Studies for muon collider parameters at center-of-mass energies of 10 TeV and 100 TeV
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B.J. King
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Physics ,Particle physics ,Muon ,Large Hadron Collider ,Meson ,Physics::Instrumentation and Detectors ,Astrophysics::High Energy Astrophysical Phenomena ,High Energy Physics::Phenomenology ,Electron ,Accelerators and Storage Rings ,law.invention ,Nuclear physics ,Muon collider ,law ,Physics::Accelerator Physics ,High Energy Physics::Experiment ,Center of mass ,Neutrino ,Collider - Abstract
Parameter lists are presented for speculative muon colliders at center-of-mass energies of 10 TeV and 100 TeV. The technological advances required to achieve the given parameters are itemized and discussed, and a discussion is given of the design goals and constraints. An important constraint for multi-TeV muon colliders is the need to minimize neutrino radiation from the collider ring.
- Published
- 2003
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19. Design study for 20 T 15 cm bore hybrid magnet with radiation-resistant insert for pion capture
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C.E. Pearson, B.J. King, and R.J. Weggel
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Nuclear physics ,Physics ,Muon ,Electromagnet ,Muon collider ,law ,Electromagnetic coil ,Magnet ,Neutrino Factory ,Superconducting magnet ,Accelerators and Storage Rings ,law.invention ,Conductor - Abstract
To capture pions the Neutrino Factory and Muon Collider Collaboration needs a field of /spl sim/20 T throughout a cylinder 15 cm in diameter and 60 cm long, falling over the next 18 m to 1.25 T, while the bore increases fourfold inversely as the square root of the field. We propose a hybrid system. The superconducting magnet is of world-class parameters, storing 600 MJ and including a coil to generate 14 T in a bore of /spl sim/1.3 m. Intercoil forces reach 100 MN. For high radiation resistance, the insert coil is of mineral-insulated hollow conductor, as developed for the Japan Hadron Facility; it would require 12 MW to generate 6 T. Needed is research to develop a more efficient hollow conductor or radiation-resistant insulator for a Bitter coil.
- Published
- 2002
- Full Text
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20. The R&D program for targetry at a neutrino factory
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Kirk T. McDonald, N.V. Mokhov, S.A. Kahn, G. A. Greene, Bernie Riemer, H. Ludewig, P. Thieberger, A. Fabich, H. Wang, Y. Fukui, R.J. Weggel, D.M. Gassner, B.J. King, J. Scaduto, A. L. Hanson, T. Tsang, A.F. Pendzick, N. Simos, A. Bernadon, R. Samulyak, J.R. Haines, R. Prigl, C.C. Tsai, H. Ravn, C.C. Finfrock, M.C. Cates, R.B. Palmer, J. Lettry, C.D. Johnson, K.A. Brown, Harold Kirk, A. Zeller, and D.L. Beshears
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Physics ,Particle physics ,Muon ,Physics::Instrumentation and Detectors ,Particle accelerator ,Superconducting magnet ,Linear particle accelerator ,law.invention ,Nuclear physics ,law ,Muon collider ,Physics::Accelerator Physics ,High Energy Physics::Experiment ,Neutrino Factory ,Neutrino ,Beam (structure) - Abstract
The need for intense muon beams for muon colliders and for neutrino factories based on muon storage rings leads to a concept of 1-4 MW proton beams incident a moving target that is inside a 20-T solenoid magnet, with a mercury jet as a preferred example. Novel technical issues for such a system include disruption of the mercury jet by the proton beam and distortion of the jet on entering the solenoid, as well as more conventional issues of materials lifetime and handling of activated materials in an intense radiation environment. As part of the R&D program of the Neutrino Factory and Muon Collider Collaboration, R&D effort related to targetry is being performed within the context of BNL E951, first results of which are discussed here and in other contributions to this conference.
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- 2002
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21. A ROTATING INCONEL BAND TARGET FOR PION PRODUCTION AT A NEUTRINO FACTORY, USING STUDY II PARAMETERS
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B.J. KING, N.P. SIMOS, R.V. WEGGEL, and N.V. MOKHOV
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- 2001
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22. The Primary Target Facility for a Neutrino Factory Based on Muon Beams
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G. Naumovitch, M.A. Green, J.R. Miller, E.J. Prebys, S.A. Kahn, Roman Samulyak, Peter Thieberger, K.T. McDonald, A. Hassenein, J.R. Haines, A. Zeller, C.E. Pearson, H. Ludewig, N.V. Mokhov, N. Simos, R.B. Palmer, Y. Fukui, T.A. Gabriel, C. Lu, I. Stumer, H. Ravn, B.J. King, C.D. Johnson, L.L. Reginato, S. Childress, P.T. Spampinato, P. Hwang, Harold Kirk, and R.J. Weggel
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Physics ,Particle physics ,Physics::Instrumentation and Detectors ,Astrophysics::High Energy Astrophysical Phenomena ,Solar neutrino ,Accelerators and Storage Rings ,Nuclear physics ,Neutrino detector ,Muon collider ,Physics::Accelerator Physics ,Measurements of neutrino speed ,High Energy Physics::Experiment ,Neutrino Factory ,Neutrino ,Neutrino oscillation ,Lepton - Abstract
Neutrino beams from the decay of muons in a storage ring offer the prospect of very high flux, well-understood spectra, and equal numbers of electron and muon neutrinos, as desirable for detailed exploration of neutrino oscillations via long baseline detectors. Such beams require large numbers of muons, and hence a high performance target station at which a 1-4 MW proton beam of 16-24 GeV impinges on a compact target, all inside a high field solenoid channel to capture as much of the phase volume of soft pions as possible. A first concept was based on a carbon target, as reported in 2000 the Neutrino Factory Study-I. A higher performance option based on a free mercury jet has been studied in 2001 as part of the Neutrino Factory Feasibility Study-II. An overview of a mercury jet target facility is presented here, including requirements, design concept and summaries of simulated performance. Further details are presented in related papers at this conference.
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- 2001
23. High Energy Muon Colliders
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B.J. King
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Physics ,Particle physics ,Muon ,Large Hadron Collider ,Meson ,Physics::Instrumentation and Detectors ,Astrophysics::High Energy Astrophysical Phenomena ,High Energy Physics::Phenomenology ,Hadron ,Particle accelerator ,Accelerators and Storage Rings ,law.invention ,Nuclear physics ,law ,Muon collider ,Physics::Accelerator Physics ,High Energy Physics::Experiment ,Collider ,Very Large Hadron Collider - Abstract
A plausible "straw-man" scenario and collider ring parameter sets are presented for future energy frontier muon colliders in symbiotic facilities with e/sup +/e/sup -/ and hadron colliders: 1.6-10 TeV "mu-linear colliders" (mu-LC) where the muons are accelerated in the linacs of a TeV-scale linear e/sup +/e/sup c/ollider, and a 100 TeV Very Large Muon Collider (VLMC) that shares a facility with a 200 TeV Very Large Hadron Collider (VLHC) and a 140 TeV muon-proton collider.
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- 2001
24. New Measurements of Nucleon Structure Functions from CCFR/NuTeV
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M. Vakili, P. Nienaber, S.R. Mishra, F. J. Sciulli, S. Koutsoliotas, W. Marsh, W. G. Seligman, G. P. Zeller, A. Bodek, U. K. Yang, R. B. Drucker, B. T. Fleming, L. de Barbaro, P. Spentzouris, Todd Adams, J. E. Brau, C.G. Arroyo, Jinhong Yu, D. Buchholz, M. J. Lamm, R. A. Johnson, H. S. Budd, A. Vaitaitis, J. Goldman, M. Goncharov, M. H. Shaevitz, W. H. Smith, D. A. Harris, L. Bugel, Joseph A. Formaggio, W. K. Sakumoto, B.J. King, R. Frey, H. Schellman, T. Kinnel, N. Suwonjandee, E. D. Zimmerman, C. McNulty, A.O. Bazarko, K. S. McFarland, J. H. Kim, R. H. Bernstein, D. Naples, S. Avvakumov, A. Romoson, Jan Conrad, P. de Barbaro, E. G. Stern, D. Mason, A. Alton, and T. Boltoen
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Physics ,High Energy Physics - Experiment (hep-ex) ,Nuclear and High Energy Physics ,Particle physics ,Scattering ,Structure function ,FOS: Physical sciences ,Astronomy and Astrophysics ,Charm (quantum number) ,Nucleon ,Atomic and Molecular Physics, and Optics ,High Energy Physics - Experiment - Abstract
We report on the extraction of the structure functions F_2 and Delta xF_3 = xF_3nu-xF_3nub from CCFR neutrino-Fe and antineutrino-Fe differential cross sections. The extraction is performed in a physics model independent (PMI) way. This first measurement for Delta xF_3, which is useful in testing models of heavy charm production, is higher than current theoretical predictions. Within 5% the F_2 (PMI) values measured in neutrino and muon scattering are in agreement with the predictions of Next-to-Leading-Order PDFs (using massive charm production schemes), thus resolving the long-standing discrepancy between the two measurements., 3 pages, Presented by Arie Bodek at DPF2000 Conference, Columbus, Ohio, Aug. 2000
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- 2000
25. THE POTENTIAL FOR NEUTRINO PHYSICS AT MUON COLLIDERS AND DEDICATED HIGH CURRENT MUON STORAGE RINGS
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I. BIGI, T. BOLTON, J. FORMAGGIO, D. HARRIS, J. MORFIN, P. SPENTZOURIS, J. YU, B. KAYSER, B.J. KING, K. MCFARLAND, A. PETROV, H. SCHELLMAN, M. VELASCO, and R. SHROCK
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Physics ,Particle physics ,Physics::Instrumentation and Detectors ,Astrophysics::High Energy Astrophysical Phenomena ,Solar neutrino ,High Energy Physics::Phenomenology ,Solar neutrino problem ,Nuclear physics ,Neutrino detector ,Muon collider ,Physics::Accelerator Physics ,Measurements of neutrino speed ,High Energy Physics::Experiment ,Neutrino astronomy ,Neutrino ,Neutrino oscillation - Abstract
Conceptual design studies are underway for both muon colliders and high-current non-colliding muon storage rings that have the potential to become the first true neutrino factories. Muon decays in long straight sections of the storage rings would produce uniquely intense and precisely characterized two-component neutrino beams--muon neutrinos plus electron antineutrinos from negative muon decays and electron neutrinos plus muon antineutrinos from positive muons. This article presents a long-term overview of the prospects for these facilities to greatly extend the capabilities for accelerator-based neutrino physics studies for both high rate and long baseline neutrino experiments. As the first major physics topic, recent experimental results involving neutrino oscillations have motivated a vigorous design effort towards dedicated neutrino factories that would store muon beams of energies 50 GeV or below. These facilities hold the promise of neutrino oscillation experiments with baselines up to intercontinental distances and utilizing well understood beams that contain, for the first time, a substantial component of multi-GeV electron-flavored neutrinos. In deference to the active and fast-moving nature of neutrino oscillation studies, the discussion of long baseline physics at neutrino factories has been limited to a concise general overview of the relevant theory, detector technologies, beam properties, experimental goals and potential physics capabilities. The remainder of the article is devoted to the complementary high rate neutrino experiments that would study neutrino-nucleon and neutrino-electron scattering and would be performed at high performance detectors placed as close as is practical to the neutrino production straight section of muon storage rings in order to exploit beams with transverse dimensions as small as a few tens of centimeters.
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- 2000
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26. Erratum to 'Hadron shower energy and direction measurements using drift chambers' [Nucl. Instr. and Meth. A 340 (1994) 474–484]
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T.S. Kinnel, P.H. Sandler, W.H. Smith, C. Arroyo, K.T. Bachmann, A.O. Bazarko, T. Bolton, C. Foudas, B.J. King, W.C. Lefmann, W.C. Leung, S.R. Mishra, E. Oltman, P.Z. Quintas, S.A. Rabinowitz, F.J. Sciulli, W.G. Seligman, M.H. Shaevitz, F.S. Merritt, M.J. Oreglia, B.A. Schumm, R.H. Bernstein, F.O. Borcherding, H.E. Fisk, M.J. Lamm, W. Marsh, K.W.B. Merritt, H. Schellman, D.D. Yovanovitch, A. Bodek, H.S. Budd, P. de Barbaro, and W.K. Sakumoto
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Nuclear and High Energy Physics ,Instrumentation - Published
- 1995
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27. Precision electroweak measurements on the Z resonance
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Schael, S, Barate, R, Bruneliere, R, Buskulic, D, Bonis, De, Decamp, I, Ghez, D, Goy, P, Jezequel, C, Lees, S, Lucotte, Jp, Martin, A, Merle, F, Minard, E, Nief, Mn, Odier, Jy, Pietrzyk, P, Trocme, B, Bravo, B, Casado, S, Chmeissani, Mp, Comas, M, Crespo, P, Fernandez, Jm, E, Fernandez, Bosman, Garrido, M, Grauges, L, Juste, E, Martinez, A, Merino, M, Miquel, G, Mir, R, Orteu, Lm, Pacheco, S, Park, A, Perlas, Ic, Riu, J, Ruiz, I, Sanchez, H, Colaleo, F, Creanza, A, D, Filippis, De, N, Palma, De, Iaselli, M, Maggi, G, Nuzzo, M, Ranieri, S, Raso, A, Ruggieri, G, Selvaggi, F, Silvestris, G, Tempesta, L, Tricomi, P, Zito, A, Huang, G, Lin, X, Ouyang, J, Wang, Q, Xie, T, Xu, Y, Xue, R, Zhang, S, Zhang, J, Zhao, L, Abbaneo, W, Bazarko, D, Becker, A, Boix, U, Bird, G, Blucher, F, Bonvicini, E, B, Bright, Thomas, Barklow, P, Buchmuller, T, Cattaneo, O, Cerutti, M, Ciulli, F, Clerbaux, V, Drevermann, B, Forty, H, Frank, Rw, Greening, M, Hagelberg, Tc, Halley, R, Gianotti, Aw, Girone, F, Hansen, M, Harvey, Jb, Jacobsen, J, Hutchcroft, R, Janot, De, Jost, R, Knobloch, B, Kado, J, Lehraus, M, Lazeyras, I, Maley, P, Mato, R, May, P, Moutussi, J, A, Pepe, Altarelli, Ranjard, M, Rolandi, F, Schlatter, L, Schmitt, D, Schneider, B, Tejessy, O, Teubert, W, Tomalin, F, Tournefier, Ir, Veenhof, E, Valassi, R, Wiedenmann, A, Wright, W, Ajaltouni, Ae, Badaud, Z, Chazelle, F, Deschamps, G, Dessagne, O, Falvard, S, Ferdi, A, Fayolle, C, Gay, D, Guicheney, P, Henrard, C, Jousset, P, Michel, J, Monteil, B, Montret, S, Pallin, Jc, Pascolo, D, Perret, Jm, Podlyski, P, Bertelsen, F, Fernley, H, Hansen, T, Hansen, Jd, Hansen, Jr, Kraan, Ph, Lindahl, Ac, Mollerud, A, Nilsson, R, Rensch, Bs, Waananen, B, Daskalakis, A, Kyriakis, G, Markou, A, Simopoulou, C, Siotis, E, Vayaki, I, Zachariadou, A, Blondel, K, Bonneaud, A, Brient, G, Machefert, Jc, Rouge, E, Rumpf, A, Swynghedauw, M, Tanaka, M, Verderi, R, Videau, M, Focardi, H, Parrini, E, Corden, G, Georgiopoulos, M, Antonelli, C, Antonelli, A, Bencivenni, M, Bologna, G, Bossi, G, Campana, F, Capon, P, Chiarella, G, Felici, V, Laurelli, G, Mannocchi, P, Murtas, G, Passalacqua, Gp, Picchi, L, Colrain, P, P, Ten, Have, Hughes, I, Kennedy, Is, Knowles, J, Lynch, Ig, Morton, Jg, Negus, Wt, Oshea, P., Raine, V, Reeves, C, Scarr, P, Smith, Jm, Thompson, K., Turnbull, As, Wasserbaech, Rm, Cavanaugh, S, Dhamotharan, R, Geweniger, S, Hanke, C, Hansper, P, Hepp, G, Kluge, V, Putzer, Ee, Sommer, A, Stenzel, J, Tittel, H, Werner, K, Wunsch, W, Beuselinck, M, Binnie, R, Cameron, Dm, Davies, W, Dornan, G, Goodsir, Pj, Marinelli, S, Martin, N, Nash, Eb, Nowell, J, Rutherford, J, Sedgbeer, Sa, Thompson, Jk, White, Jc, Williams, R, Ghete, Md, Girtler, Vm, Kneringer, P, Kuhn, E, Rudolph, D, G, Bouhova, Thacker, Bowdery, E, Buck, Ck, Clarke, Pg, Ellis, Dp, Finch, G, Foster, Aj, Hughes, F, Jones, G, Rwl, Keemer, Pearson, Nr, Robertson, Mr, Sloan, Na, Smizanska, T, Snow, M, Williams, Sw, van der Aa, Delaere, O, Leibenguth, C, Lemaitre, G, Bauerdick, V, Lat, Blumenschein, U, Van, Gemmeren, Giehl, P, Holldorfer, I, Jakobs, F, Kasemann, K, Kayser, M, Kleinknecht, F, Muller, K, Quast, As, Renk, G, Rohne, B, Sander, E, Schmeling, Hg, Wachsmuth, S, Wanke, H, Zeitnitz, R, Ziegler, C, Aubert, T, Benchouk, Jj, Bonissent, C, Carr, A, Coyle, J, Curtil, P, Ealet, C, Etienne, A, Fouchez, F, Motsch, D, Payre, F, Rousseau, P, Tilquin, D, Talby, A, Thulasides, M, Aleppo, M, Ragusa, M, Buscher, F, David, V, Dietl, A, Ganis, H, Huttmann, G, Lutjens, K, Mannert, G, Manner, C, Moser, W, Settles, Hg, Seywerd, R, Villegas, H, Wolf, M, Azzurri, G, Boucrot, P, Callot, J, Chen, O, Cordier, S, Davier, A, Duflot, M, Grivaz, L, Heusse, Jf, Jacholkowska, P, Diberder, Le, Lefrancois, F, Mutz, J, Schune, Am, Serin, Mh, Veillet, L, Videau, Jj, Zerwas, I, Bagliesi, D, Bettarini, G, Boccali, S, Bozzi, T, Calderini, C, Dellorso, G, Fantechi, R, Ferrante, R, Fidecaro, I, Foa, F, Giammanco, L, Giassi, A, Gregorio, A, Ligabue, A, Lusiani, F, Marrocchesi, PIER SIMONE, Messineo, Ps, Palla, A, Rizzo, F, Sanguinetti, G, Sciaba, G, Sguazzoni, A, Spagnolo, G, Steinberger, P, Tenchini, J, Venturi, R, Vannini, A, Verdini, C, Awunor, Pg, Blair, O, Cowan, Ga, Garcia, Bellido, Green, A, Medcalf, Mg, Misiejuk, T, Strong, A, Teixeira, Dias, Botterill, P, Clifft, Dr, Edgecock, Rw, Edwards, Tr, Haywood, M, Norton, Sj, Ward, Pr, Bloch, Devaux, Boumediene, B, Colas, D, Emery, P, Fabbro, S, Kozanecki, B, Lancon, W, Lemaire, E, Locci, Mc, Perez, E, Rander, P, Renardy, J, Roussarie, Jf, Schuller, A, Schwindling, Jp, Tuchming, J, Vallage, B, Black, B, Dann, Sn, Kim, Jh, Konstantinidis, Hy, Litke, N, Mcneil, Am, Taylor, Ma, Booth, G, Cartwright, Cn, Combley, S, Hodgson, F, Lehto, Pn, Thompson, M, Affholderbach, Lf, Barberio, K, Bohrer, E, Brandt, A, Burkhardt, S, Feigl, H, Grupen, E, Hess, C, Lutters, J, Meinhard, G, H, Minguet, Rodriguez, Mirabito, J, Neugebauer, L, Ngac, E, Prange, A, Rivera, G, Saraiva, F, Schafer, P, Sieler, U, Smolik, U, Stephan, L, Trier, F, Apollonio, H, Borean, M, Bosisio, C, L, Della, Marina, Giannini, R, Gobbo, G, Musolino, B, Pitis, G, He, L, Kim, H, Putz, H, Rothberg, J, Armstrong, J, Bellantoni, Sr, Berkelman, L, Cinabro, K, Conway, D, Cranmer, Js, Elmer, K, Feng, P, Ferguson, Z, Dps, Gao, Gonzalez, Y, Grahl, S, Harton, J, Hayes, Jl, Hu, Oj, Jin, H, Johnson, S, Kile, Rp, Mcnamara, J, Nielsen, Pa, Orejudos, J, Pan, W, Saadi, Y, Scott, Y, Sharma, Ij, Walsh, V, Walsh, Am, Wear, J, J, von Wimmersperg Toeller, Wu, Jh, Wu, J, Wu, Sl, Yamartino, X, Zobernig, Jm, Dissertori, G, Abdallah, G, Abreu, J, Adam, P, Adye, W, Adzic, T, Ajinenko, P, Albrecht, I, Alderweireld, T, Alekseev, T, Alemany, Fernandez, Allmendinger, R, Allport, T, Almehed, Pp, Amaldi, S, Amapane, U, Amato, N, Anashkin, S, Anassontzis, E, Andersson, Eg, Andreazza, P, Andringa, A, Anjos, S, Antilous, N, Apel, P, Arnoud, Wd, Ask, Y, Asman, S, Augustin, B, Augustinus, Je, Baillon, A, Ballestrero, P, Bambade, A, Barao, P, Barbiellini, F, Barbier, G, Bardin, R, Barker, D, Baroncelli, G, Battaglia, A, Baubillier, M, Becks, M, Begalli, Kh, Behrmann, M, Beilliere, A, Belokopytov, P, Belous, Y, K, Ben, Haim, Benekos, E, Benvenuti, N, Berat, A, Berggren, C, Berntzon, M, Bertini, L, Bertrand, D, Besancon, D, Besson, M, Bianchi, N, Bigi, F, Bilenky, M, Bizouard, Ms, Bloch, Ma, Blom, D, Bluj, M, Bonesini, M, Bonivento, M, Boonekamp, W, Booth, M, Psl, Borgland, Borisov, Aw, Bosio, G, Botner, C, Boudinov, O, Bouquet, E, Bourdarios, B, Bowcock, C, Tjv, Boyko, Bozovic, I, Bozzo, I, Bracko, M, Branchini, M, Brenke, P, Brenner, T, Brodet, R, Bruckman, E, Brunet, P, Bugge, Jm, Buran, L, Burgsmueller, T, Buschbeck, T, Buschmann, B, Cabrera, P, Caccia, S, Calvi, M, Rozas, M, Ajc, Camporesi, Canale, T, Canepa, V, Carena, M, Carroll, F, Caso, L, Gimenez, C, Mvc, Castro, Cattai, N, Cavallo, A, Cerruti, F, Chabaud, C, Chapkin, V, Charpentier, M, Chaussard, P, Checchia, L, Chelkov, P, Chen, Ga, Chierici, M, Chliapnikov, R, Chochula, R, Chorowicz, P, Chudoba, V, Chung, J, Cieslik, Su, Collins, K, Colomer, P, Contri, M, Cortina, R, Cosme, E, Cossuti, G, Costa, F, Cowell, Mj, Crawley, Jh, Crennell, Hb, Crepe, D, Crosetti, S, Cuevas, G, Czellar, J, Dhondt, S, Dalmagne, J, Dalmau, B, Damgaard, J, Davenport, G, M, Silva, Da, T, Deghorain, W, Della, Ricca, Delpierre, G, Demaria, P, Angelis, De, Boer, De, W, Brabandere, De, S, Clercq, De, C, Lotto, De, Maria, De, Min, De, Paula, De, Dijkstra, L, Ciaccio, Di, Diodato, Di, Simone, Di, Djannati, A, Dolbeau, A, Doroba, J, Dracos, K, Drees, M, Drees, J, Dris, Ka, Duperrin, M, Durand, A, Ehret, Jd, Eigen, R, Ekelof, G, Ekspong, T, Ellert, G, Elsing, M, Engel, M, Erzen, Jp, Santo, B, Mce, Falk, Fanourakis, E, Fassouliotis, G, Fayot, D, Feindt, J, Fenyuk, M, Fernandez, A, Ferrari, J, Ferrer, P, Ferrer, Ribas, Ferro, E, Fichet, F, Firestone, S, Fischer, A, Flagmeyer, Pa, Foeth, U, Fokitis, H, Fontanelli, E, Franek, F, Frodesen, B, Fruhwirth, Ag, R, Fulda, Quenzer, Fuster, F, Galloni, J, Gamba, A, Gamblin, D, Gandelman, S, Garcia, M, Garcia, C, Gaspar, J, Gaspar, C, Gasparini, M, Gavillet, U, Gazis, P, Gele, E, Gerber, D, Gerdyukov, Jp, Ghodbane, L, Gil, N, Glege, I, Gokieli, F, Golob, R, Gomez, Ceballos, Goncalves, G, Caballero, P, Gopal, Ig, Gorn, G, Gorski, L, Gouz, M, Gracco, Y, Graziani, V, Green, E, Grefrath, C, Grimm, A, Gris, Hj, Grosdidier, P, Grzelak, G, Gunther, K, Guy, M, Haag, J, Hahn, C, Hahn, F, Hallgren, S, Hamacher, A, Hamilton, K, Hansen, K, Harris, J, Haug, Fj, Hauler, S, Hedberg, F, Heising, V, Hennecke, S, Henriques, M, Hernandez, R, Herquet, Jj, Herr, P, Hessing, H, Heuser, Tl, Higon, Jm, Hoffman, E, Holmgren, J, Holt, So, Holthuizen, Pj, Hoorelbeke, D, Houlden, S, Hrubec, Ma, Huber, J, Huet, M, Hughes, K, Hultqvist, Gj, Jackson, K, Jacobsson, Jn, Jalocha, R, Janik, P, Jarlskog, R, Jarlskog, C, Jarry, G, Jean, Marie, Jeans, B, Johansson, D, Johansson, Ek, Jonsson, Pd, Joram, P, Juillot, C, Jungermann, P, Kapusta, L, Karafasoulis, F, Katsanevas, K, 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Thaler, Fe, Thom, Jj, Trandafir, J, Turk, Ai, Usher, Jd, Vavra, T, Vella, J, Venuti, E, Verdier, Jp, Wagner, R, Waite, Sr, Walston, Ap, Wang, S, Watts, J, Weidemann, Sj, Weiss, Aw, Whitaker, Er, White, Js, Wickens, Sl, Williams, Fj, Williams, Da, Williams, Dc, Willocq, Sh, Wilson, S, Wisniewski, Rj, Wittlin, Wj, Woods, Jl, Word, M, Wright, Gb, Wyss, Tr, Yamamoto, J, Yang, Rk, Yashima, Xq, Yellin, J, Young, Sj, Yuta, Cc, Zapalac, H, Zdarko, G, Zeitlin, Rw, Zhou, C, Blondel, Alain, Schael, S, Barate, R, Bruneliere, R, Spagnolo, Stefania Antonia, S., Schael, Aloisio, Alberto, Alviggi, Mariagrazia, Canale, Vincenzo, Chiefari, Giovanni, DELLA VOLPE, Domenico, Merola, Leonardo, Napolitano, Marco, Patricelli, Sergio, Sciacca, Crisostomo, Lista, Luca, Laboratoire d'Annecy de Physique des Particules (LAPP), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Corpusculaire - Clermont-Ferrand (LPC), Université Blaise Pascal - Clermont-Ferrand 2 (UBP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Théorique et Astroparticules (LPTA), Université Montpellier 2 - Sciences et Techniques (UM2)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire Leprince-Ringuet (LLR), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique des Particules de Marseille (CPPM), Aix Marseille Université (AMU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de l'Accélérateur Linéaire (LAL), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Nucléaire et de Hautes Énergies (LPNHE), Université Pierre et Marie Curie - Paris 6 (UPMC)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire de Lyon (IPNL), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches Subatomiques (IReS), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Cancéropôle du Grand Est-Université Louis Pasteur - Strasbourg I-Centre National de la Recherche Scientifique (CNRS), Physique Corpusculaire et Cosmologie - Collège de France (PCC), Collège de France (CdF (institution))-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), ALEPH, DELPHI, L3, OPAL, SLD, BARBIELLINI AMIDEI, Guido, Bosisio, Luciano, DELLA RICCA, Giuseppe, Giannini, Gianrossano, Gregorio, Anna, Lanceri, Livio, Poropat, Paolo, Vitale, Lorenzo, Buskulic, D, De Bonis, I, Decamp, D, Ghez, P, Goy, C, Jezequel, S, Lees, J, Lucotte, A, Martin, F, Merle, E, Minard, M, Nief, J, Odier, P, Pietrzyk, B, Trocme, B, 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SZUMILO, T. TAKAHASHI, F.E. TAYLOR, J.J. THALER, J. THOM, E. TORRENCE, A.I. TRANDAFIR, J.D. TURK, T. USHER, J. VA VRA, C. VANNINI, E. VELLA, J.P. VENUTI, R. VERDIER, P.G. VERDINI, D.L. WAGNER, S.R. WAGNER, A.P. WAITE, S. WALSTON, J. WANG, S.J. WATTS, A.W. WEIDEMANN, E.R. WEISS, J.S. WHITAKER, S.L. WHITE, F.J. WICKENS, D.A. WILLIAMS, D.C. WILLIAMS, S.H. WILLIAMS, S. WILLOCQ, R.J. WILSON, W.J. WISNIEWSKI, J.L. WITTLIN, M. WOODS, G.B. WORD, T.R. WRIGHT, J. WYSS, R.K. YAMAMOTO, J.M. YAMARTINO, X.Q. YANG, J. YASHIMA, S.J. YELLIN, C.C.YOUNG, H.YUTA, G. ZAPALAC, R.W. ZDARKO, C. ZEITLIN, J. ZHOU, Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Centre National de la Recherche Scientifique (CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Pierre et Marie Curie - Paris 6 (UPMC), Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Joseph Fourier - Grenoble 1 (UJF)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Laboratoire d'Annecy de Physique des Particules (LAPP/Laboratoire d'Annecy-le-Vieux de Physique des Particules), Centre National de la Recherche Scientifique (CNRS)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Aix Marseille Université (AMU), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA), Collège de France (CdF)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), GRUNEVALD M, NEWALD M, SCHAEL S, BARATE R, BRUNELIE, RE R, BUSKULIC D, DE BONIS I, DECAMP D, GHEZ P, GOY C, JE, ZE, QUEL S, LEES J, LUCOTTE A, MARTIN M, MERLE E, MINARD M, NIEF J, ODIER P, PIETRZYK B, TROCME, BRAVO S, CASADO MP, CHMEISSANI M, COMAS P, CRESPO JM, FERNANDEZ E, FERNANDEZ-BOSMAN M, GARRIDO L, GRAUGES E, JUSTE A, MARTINEZ M, MERINO G, MIQUEL R, MIR LM, ORTEU S, PACHECO A, PARK IC, PERLAS J, RIU I, RUIZ H, SANCHEZ F, COLALEO A, CREANZA D, DE FILIPPIS N, DE PALMA M, IASELLI G, MAGGI G, MAGGI M, NUZZO S, RANIERI, A, RASO, G, RUGGIERI F, SELVAGGI, G, SILVESTRIS L, TEMPESTA P, TRICOMI A, ZITO G, HUANG X, LIN J, OUYANG Q, WANG T, XIE Y, XU R, XUE S, ZHANG J, ZHANG L, ZHAO W, ABBANEO D, BAZARKO A, BECKER U, BOIX G, BIRD F, BLUCHER E, BONVICINI B, BRIGHT-THOMAS P, BARKLOW T, BUCHMU, LLER O, CATTANEO M, CERUTTI F, CIULLI V, CLERBAUX B, DREVERMANN H, FORTY RW, FRANK M, GREENING TC, HAGELBERG R, HALLEY AW, GIANOTTI F, GIRONE M, HANSEN JB, HARVEY J, JACOBSEN J, HUTCHCROFT DE, JANOT P, JOST B, KNOBLOCH J, KADO M, LEHRAUS I, LAZEYRAS P, and MALEY P
- Subjects
Top quark ,FORWARD-BACKWARD ASYMMETRY ,PARTICLE PHYSICS ,LARGE ELECTRON POSITRON COLLIDER ,ALEPH ,DELPHI ,L3 ,OPAL ,General Physics and Astronomy ,01 natural sciences ,7. Clean energy ,High Energy Physics - Experiment ,Settore FIS/04 - Fisica Nucleare e Subnucleare ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,electron-positron physics ,[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex] ,Electroweak interaction ,Physics ,Quantum chromodynamics ,Electron–positron physics ,Electroweak interactions ,Decays of heavy intermediate gauge bosons ,Fermion–antifermion production ,Precision measurements at the Z resonance ,Tests of the Standard Model ,Radiative corrections ,Effective coupling constants ,Neutral weak current ,Z boson ,W boson ,Higgs boson ,Particle physics - Experiment ,Settore FIS/01 - Fisica Sperimentale ,FERMION-PAIR PRODUCTION ,HADRONIC-Z-DECAYS ,TOP-QUARK MASS ,ANGLE BHABHA SCATTERING ,W-BOSON MASS ,CROSS-SECTION ASYMMETRY ,Z-LINE-SHAPE ,SEMILEPTONIC BRANCHING RATIOS ,CARLO EVENT GENERATOR ,decays of heavy intermediate gauge bosons ,effective coupling constants ,electroweak interactions ,fermion-antifermion production ,higgs boson ,neutral weak current ,precision measurements at the z resonance ,radiative corrections ,tests of the standard model ,top quark ,w boson ,z boson ,Radiative correction ,High Energy Physics - Phenomenology ,FIS/01 - FISICA SPERIMENTALE ,Física nuclear ,Neutrino ,Particle physics ,FOS: Physical sciences ,ddc:500.2 ,Elementary particle physics ,LEP ,electroweak ,Decays of heavy intermediate gauge boson ,Effective coupling constant ,Partícules (Física nuclear) ,Standard Model ,electroweak theory, Z boson, DELPHI, ALEPH, OPAL, L3 ,0103 physical sciences ,010306 general physics ,Coupling constant ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,Fermion ,FORWARD-BACKWARD ASYMMETRY, FERMION-PAIR PRODUCTION, HADRONIC-Z-DECAYS, TOP-QUARK MASS, ANGLE BHABHA SCATTERING, W-BOSON MASS, CROSS-SECTION ASYMMETRY, Z-LINE-SHAPE, SEMILEPTONIC BRANCHING RATIOS, CARLO EVENT GENERATOR ,[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph] ,Experimental High Energy Physics ,Electron–positron physic ,High Energy Physics::Experiment ,FIS/04 - FISICA NUCLEARE E SUBNUCLEARE - Abstract
We report on the final electroweak measurements performed with data taken at the Z resonance by the experiments operating at the electron-positron colliders SLC and LEP. The data consist of 17 million Z decays accumulated by the ALEPH, DELPHI, L3 and OPAL experiments at LEP, and 600 thousand Z decays by the SLD experiment using a polarised beam at SLC. The measurements include cross-sections, forward-backward asymmetries and polarised asymmetries. The mass and width of the Z boson, $\MZ$ and $\GZ$, and its couplings to fermions, for example the $\rho$ parameter and the effective electroweak mixing angle, are precisely measured. The number of light neutrino species is determined to be 2.9840+/-0.0082. The results are compared to the predictions of the Standard Model. Electroweak radiative corrections beyond the running of the QED and QCD coupling constants are observed with a significance of five standard deviations, and in agreement with the Standard Model. Of the many Z-pole measurements, the forward-backward asymmetry in b-quark production shows the largest difference with respect to its Standard Model expectation, at the level of 2.8 standard deviations. Through radiative corrections evaluated in the framework of the Standard Model, the masses of the top quark and the W Boson are predicted. These indirect constraints are compared to the direct measurements, providing a stringent test of the Standard Model. Using in addition the direct measurements of $\Mt$ and $\MW$, the mass of the as yet unobserved Standard Model Higgs boson is predicted., Comment: 302 pages, v2: minor corrections and updates of references. Accepted for publication by Physics Reports, v3: further small corrections and journal version
- Published
- 2006
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