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Neutrino production of dimuons
Authors:K Lang  A Bodek  F Borcherding  N Giokaris  I E Stockdale  P Auchincloss  R Blair  C Haber  S Mishra  E Oltman  M Ruiz  F J Sciulli  M Shaevitz  W H Smith  R Zhu  Y K Chu  D B MacFarlane  R L Messner  D B Novikoff  M V Purohit  D Garfinkle  F S Merritt  M Oreglia  P Reutens  R Coleman  H E Fisk  Y Fukushima  O Kerns  B Jin  D Levinthal  T Kondo  W Marsh  P A Rapidis  S Segler  R Stefanski  D Theriot  H B White  D Yovanovitch  O Fackler  K Jenkins
Institution:1. University of Rochester, 14627, Rochester, NY, USA
6. Columbia University, 10027, New York, NY, USA
10. California Institute of Technology, 91125, Pasadena, CA, USA
14. Enrico Fermi Institute and Physics Department, University of Chicago, 60637, Chicago, IL, USA
15. Fermi National Accelerator Laboratory, 60510, Batavia, IL, USA
18. Rockefeller University, 10021, New York, NY, USA
Abstract:Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10?4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 \(\bar v_\mu \) opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: \(\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-0em} {c^2 }}} \right)}}} \right. \kern-0em} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-0em} {c^2 }}} \right)}}\) using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e ? collisions and neutrino emulsion data.
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