The NNLO QCD corrections to Z boson production at large transverse momentum

被引:84
|
作者
Ridder, A. Gehrmann-De [1 ,2 ,3 ]
Gehrmann, T. [2 ,3 ]
Glover, E. W. N. [4 ]
Huss, A. [1 ]
Morgan, T. A. [4 ]
机构
[1] ETH, Inst Theoret Phys, CH-8093 Zurich, Switzerland
[2] Univ Zurich, Dept Phys, CH-8057 Zurich, Switzerland
[3] Univ Calif Santa Barbara, Kavli Inst Theoret Phys, Santa Barbara, CA USA
[4] Univ Durham, Inst Particle Phys Phenomenol, Dept Phys, Durham DH1 3LE, England
来源
基金
美国国家科学基金会; 瑞士国家科学基金会; 英国科学技术设施理事会;
关键词
QCD Phenomenology; DRELL-YAN PROCESSES; TO-LEADING ORDER; ONE-LOOP AMPLITUDES; HADRON COLLIDERS; ELECTROWEAK CORRECTIONS; CROSS-SECTION; W-BOSON; RESUMMATION; DIS; JET;
D O I
10.1007/JHEP07(2016)133
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
The transverse momentum distribution of massive neutral vector bosons can be measured to high accuracy at hadron colliders. The transverse momentum is caused by a partonic recoil, and is determined by QCD dynamics. We compute the single and double-differential transverse momentum distributions for fully inclusive Z/gamma* production including leptonic decay to next-to-next-to-leading order (NNLO) in perturbative QCD. We also compute the same distributions normalised to the cross sections for inclusive Z/gamma* production, i.e. integrated over the transverse momentum of the lepton pair. We compare our predictions for the fiducial cross sections to the 8TeV data set from the ATLAS and CMS collaborations, which both observed a tension between data and NLO theory predictions, using the experimental cuts and binning. We find that the inclusion of the NNLO QCD effects does not fully resolve the tension with the data for the unnormalised p(T)(Z) distribution. However, we observe that normalising the NNLO Z-boson transverse momentum distribution by the NNLO Drell-Yan cross section substantially improves the agreement between experimental data and theory, and opens the way for precision QCD studies of this observable.
引用
收藏
页数:19
相关论文
共 50 条
  • [1] The NNLO QCD corrections to Z boson production at large transverse momentum
    A. Gehrmann-De Ridder
    T. Gehrmann
    E.W.N. Glover
    A. Huss
    T.A. Morgan
    Journal of High Energy Physics, 2016
  • [2] NNLO QCD corrections to Higgs boson production at large transverse momentum
    X. Chen
    J. Cruz-Martinez
    T. Gehrmann
    E. W. N. Glover
    M. Jaquier
    Journal of High Energy Physics, 2016
  • [3] NNLO QCD corrections to Higgs boson production at large transverse momentum
    Chen, X.
    Cruz-Martinez, J.
    Gehrmann, T.
    Glover, E. W. N.
    Jaquier, M.
    JOURNAL OF HIGH ENERGY PHYSICS, 2016, (10): : 1 - 30
  • [4] NNLO soft-gluon corrections for the Z boson and W boson transverse momentum distributions
    Kidonakis, Nikolaos
    Gonsalves, Richard J.
    PHYSICAL REVIEW D, 2014, 89 (09):
  • [5] NNLO soft function for electroweak boson production at large transverse momentum
    Becher, Thomas
    Bell, Guido
    Marti, Stefanie
    JOURNAL OF HIGH ENERGY PHYSICS, 2012, (04):
  • [6] NNLO soft function for electroweak boson production at large transverse momentum
    Thomas Becher
    Guido Bell
    Stefanie Marti
    Journal of High Energy Physics, 2012
  • [7] Electroweak-boson hadroproduction at large transverse momentum: factorization, resummation, and NNLO corrections
    Kidonakis, N
    Del Duca, V
    PHYSICS LETTERS B, 2000, 480 (1-2) : 87 - 96
  • [8] QCD RADIATIVE-CORRECTIONS TO ELECTROWEAK-BOSON PRODUCTION AT LARGE TRANSVERSE-MOMENTUM IN HADRON-COLLISIONS
    GONSALVES, RJ
    PAWLOWSKI, J
    WAI, CF
    PHYSICAL REVIEW D, 1989, 40 (07): : 2245 - 2268
  • [9] NNLO mixed EW-QCD corrections to single vector boson production
    Bonciani, Roberto
    Buccioni, Federico
    Rana, Narayan
    Vicini, Alessandro
    14TH INTERNATIONAL SYMPOSIUM ON RADIATIVE CORRECTIONS, RADCOR2019, 2020,
  • [10] Combining QED and QCD transverse-momentum resummation for Z boson production at hadron colliders
    Cieri, Leandro
    Ferrera, Giancarlo
    Sborlini, German F. R.
    JOURNAL OF HIGH ENERGY PHYSICS, 2018, (08):