 | B CoxUniversity of Virginia, Charlottesville, USA | University of Virginia, Charlottesville, Virginia, U.S.A. | University of Virginia, Charlottesville, Virginia, USA. | University ... |
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B Cox:Expert Impact
Concepts for whichB Coxhas direct influence:Higgs boson,13 tev,Proton collisions,Integrated luminosity,Protonproton collisions,Transverse momentum,Cms detector,8 tev.
B Cox:KOL impact
Concepts related to the work of other authors for whichfor which B Cox has influence:Dark matter,Higgs boson,Atlas detector,Usepackagemathrsfs usepackageupgreek,Transverse momentum,Large hadron collider,Integrated luminosity.
KOL Resume for B Cox
| Year | |
|---|---|
| 2022 | University of Virginia, Charlottesville, USA |
| 2021 | University of Virginia, Charlottesville, Virginia 22904, USA Department of Microbiology, Royal Melbourne Hospital at The Peter Doherty Institute for Infection and Immunity, Melbourne, Vic, Australia |
| 2018 | University of Virginia, Charlottesville, Virginia USA |
| 2016 | Department of Geography and Environmental Science, University of Reading, UK University of Virginia, Charlottesville 22904, USA |
| 2015 | University of Virginia, Department of Physics, 382 McCormick Rd, Charlottesville, VA, 22904 |
| 2014 | University of Virginia, Charlottesville, United Kingdom |
| 2013 | University of Virginia, Charlottesville, Virgina, USA |
| 2012 | CERN, European Organization for Nuclear Research, Geneva, Switzerland |
| 2011 | The Department of Physics and Institute of Nuclear and Particle Physics, University of Virginia, Charlottesville, Virginia 22901, USA Department of Pharmacology, Manchester University, Manchester 13, U.K Centre for Nuclear Engineering, University of Toronto, Toronto, Ontario, Canada |
| 2009 | Dept. of Cognitive Sci., Univ. of California, Irvine, CA, USA University of Manchester, Manchester, United Kingdom |
| 2008 | University of Virginia, Charlottesville, Virginia 22901 Tanaka Business School, South Kensington Campus, Imperial College, SW7 2AZ, London, UK New Zealand Cancer Control Trust, Dunedin, New Zealand |
| 2006 | Protein Production, Procter and Gamble Pharmaceuticals, 8700 Mason-Montgomery Road, Mason, OH 45140, USA University of Manchester, Manchester, UK |
| 2005 | Centre for Nuclear Engineering, University of Toronto, Toronto, Ontario, Canada M5S 3E4 Radiation Oncology, Stanford University Medical Center, Stanford, CA |
| 2004 | Bilkei Consulting; Raubbühlstrasse 4 CH-8600 Dubendorf Switzerland |
| 2003 | Medicinal Chemistry, Respiratory Diseases Therapeutic Area, Novartis Pharma Research Centre, Horsham, United Kingdom |
| 2002 | The University of Virginia, Charlottesville, Virginia 22901 |
| 2001 | Hugh Adam Cancer Epidemiology Unit |
| 1999 | The Department of Physics and the Institute of Nuclear and Particle Physics, University of Virginia, Charlottesville, VA 22901, USA Centre for Nuclear Engineering, University of Toronto, 184 College St., Toronto, Ontario, M5S 3E4, Canada. |
| 1997 | Centre for Nuclear Engineering, University of Toronto, Toronto, Ont., Canada M5S 3E4 George Mason Univ., Fairfax, VA, USA |
| 1996 | The University of Virginia, Charlottesville, VA, USA |
| 1995 | Centre for Nuclear Engineering, Ontario, Canada M5S IA4 |
| 1994 | Shandong University, Jinan, People’s Republic of China McGill University, Montreal, PQ, Quebec, Canada H3A 2T8 Northwestern University, Evanston, Illinois 60208 Department of Medicine, Veterans Administration Medical Center, Milwaukee, Wisconsin. University of Virginia, VA, USA |
| 1993 | Bioscience II, ICI Pharmaceuticals, Macclesfield Shandong University, Jinan, Shandong, People’s Republic of China Centre for Nuclear Engineering, University of Toronto, Faculty of Applied Science & Engineering, 184 College Street, Toronto, Canada M5S 1A4 McGill University, Montreal, PQ, Canada H3A 2T8 |
| 1992 | University of Virginia, USA |
| 1990 | Centre for Nuclear Engineering, Department of Metallurgy and Materials Science, University of Toronto, Toronto, Ontario, Canada M5S 1A4 |
| 1989 | E. I. du Pont de Nemours and Co., Central Research and Development and Fibers Departments, Experimental Station, PO Box 80356, Wilmington, DE 19880-0356, USA |
| 1988 | University of Michigan, Ann Arbor, Michigan 48109 Fermilab Fermi National Accelerator Laboratory Batavia, Illinois 60510 |
| 1987 | Atomic Energy of Canada Limited, Chalk River Nuclear Laboratories, Chalk River, Ontario KOJ 1JO, Canada |
| 1986 | Rockwell International Science Center, 1049 Camino Dos Rios, 91366, Thousand Oaks, CA, USA |
| 1984 | Fermi National Accelerator Laboratory, P.O. Box 500, Batavia, Illinois 60510 |
| 1983 | Bioscience II Department, I.C.I. Pharmaceuticals Division, Alderly Park, Macclesfield, Cheshire SK10 4TG |
| 1982 | Bioscience Department II, Imperial Chemical Industries Ltd., Pharmaceuticals Division, Alderley Park, Macclesfield, Cheshire SK10 4TG, U.K. |
| 1981 | Biology (Research) Dept., I.C.I. Pharmaceuticals Division, Alderley Park, Macclesfield, Cheshire SK10 4TG Department of Pharmacology Materia Medica and Therapeutics, Manchester University, Medical School, Manchester M13 9PT, England |
| 1980 | Department of Pharmacology, Materia Medica & Therapeutics, Manchester University Medical School, Manchester M13 9PT |
| 1976 | Fermi National Accelerator Laboratory, Batavia, Illinois 60510, U.S.A.∗∗Operated by Universties Research Association Inc. under contract with the U.S. Energy Research and Development Administration. |
| 1974 | Department of Medicine, Guy's Hospital Medical School, London SE1, United Kingdon |
| 1973 | Nuclear Division, Union Carbide Corp., P. O. Box P, Oak Ridge, Tenn. |
| 1972 | Department of Pharmacology, Manchester University, Manchester, M13 9PL, U.K. |
| 1969 | U.S. Army Nuclear Defense Laboratory, Edgewood Arsenal, Maryland, U.S.A. |
| 1968 | Atomic Energy of Canada Ltd., Chalk River, Ont., Canada. |
| 1963 | Chemistry Division, U.K. Atomic Energy Research Establishment, Harwell, Didcot, Berks. Great Britain |
| 1961 | United Kingdom Atomic Energy Authority, Atomic Energy Research Establishment, Harwell, Didcot, Berkshire, England |
| Concept | World rank |
|---|---|
| large aperture spectrometer | #1 |
| differences pore structures | #1 |
| zirconium alloy corrosion | #1 |
| zrliner | #1 |
| zircaloy2 evidence | #1 |
| zirconia reactor | #1 |
| beam extraction studies | #1 |
| nb nucleon | #1 |
| pci failures | #1 |
| canlubgraphite | #1 |
| 0625 methysergide | #1 |
| proton west | #1 |
| jψ ψ′ production | #1 |
| e537 | #1 |
| mechanisms reactor | #1 |
| p¯n π | #1 |
| serotonin tryptamines cyproheptadine | #1 |
| 5htinduced hypothermia | #1 |
| 02 contrast | #1 |
| gluon structure functions | #1 |
| hypothesis nodular corrosion | #1 |
| ≌10 | #1 |
| p¯n | #1 |
| cyproheptadine 25 | #1 |
| environmentallyinduced cracking | #1 |
| zircaloy2 zr25 | #1 |
| zr matrix zirconia | #1 |
| fe spps | #1 |
| reactors pci failures | #1 |
| methergoline 0625 | #1 |
| breakdown zirconium | #1 |
| 25 methergoline | #1 |
| fluoroferrates | #1 |
| corrosion zirconium | #1 |
| p¯ π | #1 |
| rats 20 degrees | #1 |
| xgx110±0101x120±020 | #1 |
| methysergide 02 | #1 |
| spps zr matrix | #1 |
| oxide films zircaloy2 | #1 |
| zircaloys hypothesis | #1 |
| contrast methergoline | #1 |
| zirconium alloy fuel | #2 |
| πw | #2 |
| χ1 χ2 states | #2 |
| fermilab e771 spectrometer | #2 |
| χ2 states | #2 |
| drell–yan events | #2 |
| 125 gev | #2 |
| skin cancer england | #2 |
| Sign-in to see all concepts, it's free! | |
Prominent publications by B Cox
Combined ATLAS and CMS measurements of the Higgs boson production and decay rates, as well as constraints on its couplings to vector bosons and fermions, are presented. The combination is based on the analysis of five production processes, namely gluon fusion, vector boson fusion, and associated production with a W or a Z boson or a pair of top quarks, and of the six decay modes H → ZZ, W W , γγ, ττ, bb, and μμ. All results are reported assuming a value of 125.09 GeV for the Higgs boson ...
| Known for Higgs Boson Production | Decay Rates | Cms Analysis | Constraints Couplings | Gluon Fusion |
Combined measurements of the production and decay rates of the Higgs boson, as well as its couplings to vector bosons and fermions, are presented. The analysis uses the LHC proton–proton collision data set recorded with the CMS detector in 2016 at ...
| Known for Combined Measurements | Higgs Boson | Usepackagemathrsfs Usepackageupgreek | Proton Collisions | Setlength Oddsidemargin69pt |
Measurement of prompt and nonprompt J/ψ production in pp and pPb collisions at sNN=5.02TeV
[ PUBLICATION ]
This paper reports the measurement of J/ψ\documentclass[12pt]{minimal}
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\begin{document}$$\mathrm{J}/{\psi }$$\end{document} meson production in proton–proton ...
| Known for Usepackagemathrsfs Usepackageupgreek | Setlength Oddsidemargin69pt | Ψ Production | Ppb Collisions | Begindocument Mathrm |
Measurement of the inclusive W and Z production cross sections in pp collisions at TeV with the CMS experiment
[ PUBLICATION ]
A measurement of inclusive W and Z production cross sections in pp collisions at \documentclass[12pt]{minimal}
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\begin{document}$ \sqrt {s} = 7 $\end{document} TeV is presented. The electron and muon decay channels are analyzed in a data sample collected with the CMS ...
| Known for Cms Experiment | Syst ± | Production Cross | Collisions Tev | Setlength Oddsidemargin69pt |
Search for heavy resonances decaying to two Higgs bosons in final states containing four b quarks
[ PUBLICATION ]
A search is presented for narrow heavy resonances X decaying into pairs of Higgs bosons (H\documentclass[12pt]{minimal}
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\begin{document}$${\mathrm{H}}$$\end{document}) in proton-proton collisions collected by the CMS experiment at the LHC at ...
| Known for Higgs Bosons | Begindocument Text | Heavy Resonances | Usepackagemathrsfs Usepackageupgreek | Setlength Oddsidemargin69pt |
Search for resonances and quantum black holes using dijet mass spectra in proton-proton collisions at s=8 TeV
[ PUBLICATION ]
A search for resonances and quantum black holes is performed using the dijet mass spectra measured in proton-proton collisions at s=8 TeV with the CMS detector at the LHC. The data set corresponds to an integrated luminosity of 19.7 fb−1. In a search for narrow resonances that couple to quark-quark, quark-gluon, or gluon-gluon pairs, model-independent upper limits, at 95% confidence level, are obtained on the production cross section of resonances, with masses above 1.2 TeV. When ...
| Known for Quantum Black Holes | Proton Collisions | Resonances Masses | Excited Quarks | S8 Tev |
Search for invisible decays of a Higgs boson produced through vector boson fusion in proton-proton collisions at s = 13 TeV
[ PUBLICATION ]
A search for invisible decays of a Higgs boson is performed using proton-proton collision data collected with the CMS detector at the LHC in 2016 at a center-of-mass energy s = 13 TeV , corresponding to an integrated luminosity of 35.9 fb − 1 . The search targets the production of a Higgs boson via vector boson fusion. The data are found to be in agreement with the background contributions from standard model processes. An observed (expected) upper limit of 0.33(0.25), at 95% confidence ...
| Known for Higgs Boson | Invisible Decays | 13 Tev | Branching Fraction | 95 Confidence Level |
Search for invisible decays of Higgs bosons in the vector boson fusion and associated ZH production modes
[ PUBLICATION ]
A search for invisible decays of Higgs bosons is performed using the vector boson fusion and associated ZH production modes. In the ZH mode, the Z boson is required to decay to a pair of charged leptons or a [Formula: see text] quark pair. The searches use the 8 [Formula: see text] pp collision dataset collected by the CMS detector at the LHC, corresponding to an integrated luminosity of up to 19.7 [Formula: see text]. Certain channels include data from 7 [Formula: see text] collisions ...
| Known for Invisible Decays | Higgs Bosons | Vector Boson Fusion | Text Formula Text | Integrated Luminosity |
A search for an exotic decay of the Higgs boson to a pair of light pseudoscalar bosons is performed for the first time in the final state with two b quarks and two τ leptons. The search is motivated in the context of models of physics beyond the standard model (SM), such as two Higgs doublet models extended with a complex scalar singlet (2HDM + S), which include the next-to-minimal supersymmetric SM (NMSSM). The results are based on a data set of proton–proton collisions corresponding ...
| Known for Higgs Boson | 13 Tev | Exotic Decay | Light Pseudoscalars | Branching Fraction |
Search for top squarks and dark matter particles in opposite-charge dilepton final states at s=13 TeV
[ PUBLICATION ]
A search for new physics is presented in final states with two oppositely charged leptons (electrons or muons), jets identified as originating from b quarks, and missing transverse momentum (pTmiss). The search uses proton-proton collision data at s=13 TeV amounting to 35.9 fb-1 of integrated luminosity collected using the CMS detector in 2016. Hypothetical signal events are efficiently separated from the dominant tt¯ background with requirements on pTmiss and transverse-mass variables. ...
| Known for Dark Matter | Lightest Neutralino | Search Squarks | Exclusion Limits | S13 Tev |
Search for dark matter produced with an energetic jet or a hadronically decaying W or Z boson at s=13 TeV
[ PUBLICATION ]
A search for dark matter particles is performed using events with large missing transverse momentum, at least one energetic jet, and no leptons, in proton-proton collisions at s=13\documentclass[12pt]{minimal}
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\begin{document}$$ \sqrt{s}=13 $$\end{document} TeV collected ...
| Known for Energetic Jet | Dark Matter | Pseudoscalar Mediator | Higgs Boson | Integrated Luminosity |
Long-range two-particle correlations of strange hadrons with charged particles in pPb and PbPb collisions at LHC energies
[ PUBLICATION ]
Measurements of two-particle angular correlations between an identified strange hadron (KS0 or Λ/Λ¯) and a charged particle, emitted in pPb collisions, are presented over a wide range in pseudorapidity and full azimuth. The data, corresponding to an integrated luminosity of approximately 35 nb−1, were collected at a nucleon–nucleon center-of-mass energy (sNN) of 5.02 TeV with the CMS detector at the LHC. The results are compared to semi-peripheral PbPb collision data at sNN=2.76 TeV, ...
| Known for Pbpb Collisions | Charged Particles | Strange Hadrons | Particle Correlations | V2 V3 |
Measurements are presented of the associated production of a W boson and a charm-quark jet (W + c) in pp collisions at a center-of-mass energy of 7 TeV. The analysis is conducted with a data sample corresponding to a total integrated luminosity of 5 fb−1, collected by the CMS detector at the LHC. W boson candidates are identified by their decay into a charged lepton (muon or electron) and a neutrino. The W + c measurements are performed for charm-quark jets in the kinematic region ...
| Known for Charm Production | 7 Tev | Usepackagemathrsfs Usepackageupgreek | Setlength Oddsidemargin69pt | Measurements Lhc |
Properties of the Higgs boson with mass near 125[Formula: see text] are measured in proton-proton collisions with the CMS experiment at the LHC. Comprehensive sets of production and decay measurements are combined. The decay channels include [Formula: see text], [Formula: see text], [Formula: see text], [Formula: see text], [Formula: see text], and [Formula: see text] pairs. The data samples were collected in 2011 and 2012 and correspond to integrated luminosities of up to 5.1[Formula: ...
| Known for Higgs Boson | Proton Collisions | Standard Model Predictions | Decay Channels | Measured Mass |
A search for supersymmetry in final states with jets and missing transverse energy is performed in pp collisions at a centre-of-mass energy of \documentclass[12pt]{minimal}
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\begin{document}$ \sqrt{s}=7 $\end{document} TeV. The data sample corresponds to an integrated ...
| Known for Transverse Energy | States Jets | Variable Αt | Search Supersymmetry | Simplified Models |
