1994/07/26 by J. Ohnemus · 2 citations
Computer Science · Physics and Astronomy · #Computational Physics and Python Applications #Cosmology and Gravitation Theories #Particle physics theoretical and experimental studies #hep-ph
paper · pdf · doi:10.1103/physrevd.51.1068
published as Phys.Rev. D51 (1995) 1068-1076 · 16 pages + 9 figures, UCD-94-29. A postscript version and 9 postscript figures are available via anonymous ftp to UCDHEP.UCDAVIS.EDU in the directory [.ohnemus.ucd-94-29]
arxiv created 1994/07/26 · openalex publication_date 1995/02/01 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28
The process pp^(\mathrm\ensuremath-)\ensuremath→Z\ensuremathγ+X\ensuremath→l^\mathrm\ensuremath-l+\ensuremathγ+X, where l denotes a lepton, is calculated to O(\mathrm\ensuremathαs). Total and differential cross sections, with acceptance cuts imposed on the leptons and photon, are given for the Fermilab Tevatron and CERN LHC center-of-mass energies. In general, invariant mass and angular distributions are simply scaled up in magnitude by the QCD radiative corrections, whereas in transverse momentum distributions, the QCD radiative corrections increase with the transverse momentum.