High Pt [p Subscript T] Nonphotonic Electron Production in P+p Collisions at S=200[square Root of S=200] Gev Accessed Terms of Use Detailed Terms

نویسندگان

  • J. Alford
  • B. D. Anderson
  • C. D. Anson
  • D. Arkhipkin
  • G. S. Averichev
  • J. Balewski
  • D. R. Beavis
  • N. K. Behera
  • R. Bellwied
  • M. J. Betancourt
  • R. R. Betts
  • T. P. Burton
  • X. Z. Cai
  • H. Caines
  • P. Chaloupka
  • S. Chattopadhyay
  • H. F. Chen
  • J. H. Chen
  • J. Y. Chen
  • L. Chen
  • J. Cheng
  • M. Cherney
  • A. Chikanian
  • K. E. Choi
  • H. J. Crawford
  • S. Dash
  • A. Davila Leyva
  • L. C. De Silva
  • R. R. Debbe
  • T. G. Dedovich
  • D. J. Hofman
  • B. Huang
  • H. Z. Huang
  • T. J. Humanic
  • J. H. Lee
  • W. Leight
  • M. J. LeVine
چکیده

Citation Agakishiev, H. et al. (STAR Collaboration) "High pT nonphotonic electron production in p+p collisions at s=200GeV" Phys. Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. High p T nonphotonic electron production in p þ p collisions at ffiffi ffi s p ¼ 200 GeV We present the measurement of nonphotonic electron production at high transverse momentum (p T > 2:5 GeV=c) in p þ p collisions at ffiffi ffi s p ¼ 200 GeV using data recorded during 2005 and 2008 by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The measured cross sections from the two runs are consistent with each other despite a large difference in photonic background levels due to different detector configurations. We compare the measured nonphotonic electron cross sections with previously published RHIC data and perturbative quantum chromodynamics H. AGAKISHIEV et al. calculations. Using the relative contributions of B and D mesons to nonphotonic electrons, we determine the integrated cross sections of electrons (e þ þe À 2) at 3 GeV=c < p T < 10 GeV=c from bottom and charm meson decays to be ½ðd ðB!eÞþðB!D!eÞ Þ=ðdy e ފ y e ¼0 ¼ 4:0 AE 0:5ðstatÞ AE 1:1ðsystÞ nb and ½ðd D!e Þ=ðdy e ފ y e ¼0 ¼ 6:2 AE 0:7ðstatÞ AE 1:5ðsystÞ nb, respectively.

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تاریخ انتشار 2011