Study of forward Z + jet production in pp collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \sqrt{s} $\end{document} = 7 TeV

被引:0
作者
R. Aaij
B. Adeva
M. Adinolfi
C. Adrover
A. Affolder
Z. Ajaltouni
J. Albrecht
F. Alessio
M. Alexander
S. Ali
G. Alkhazov
P. Alvarez Cartelle
A. A. Alves
S. Amato
S. Amerio
Y. Amhis
L. Anderlini
J. Anderson
R. Andreassen
M. Andreotti
J. E. Andrews
R. B. Appleby
O. Aquines Gutierrez
F. Archilli
A. Artamonov
M. Artuso
E. Aslanides
G. Auriemma
M. Baalouch
S. Bachmann
J. J. Back
A. Badalov
C. Baesso
V. Balagura
W. Baldini
R. J. Barlow
C. Barschel
S. Barsuk
W. Barter
V. Batozskaya
Th. Bauer
A. Bay
J. Beddow
F. Bedeschi
I. Bediaga
S. Belogurov
K. Belous
I. Belyaev
E. Ben-Haim
G. Bencivenni
机构
[1] Centro Brasileiro de Pesquisas Físicas (CBPF),Center for High Energy Physics
[2] Universidade Federal do Rio de Janeiro (UFRJ),Fakultät Physik
[3] Tsinghua University,School of Physics
[4] LAPP,Institute of Nuclear Physics
[5] Université de Savoie,Physik
[6] CNRS/IN2P3,Institut
[7] Clermont Université,H.H. Wills Physics Laboratory
[8] Université Blaise Pascal,Cavendish Laboratory
[9] CNRS/IN2P3,Department of Physics
[10] LPC,School of Physics and Astronomy
[11] CPPM,School of Physics and Astronomy
[12] Aix-Marseille Université,Oliver Lodge Laboratory
[13] CNRS/IN2P3,School of Physics and Astronomy
[14] LAL,Department of Physics
[15] Université Paris-Sud,Institut für Physik
[16] CNRS/IN2P3,P.N. Lebedev Physical Institute
[17] LPNHE,LIFAELS, La Salle
[18] Université Pierre et Marie Curie,undefined
[19] Université Paris Diderot,undefined
[20] CNRS/IN2P3,undefined
[21] Technische Universität Dortmund,undefined
[22] Max-Planck-Institut für Kernphysik (MPIK),undefined
[23] Physikalisches Institut,undefined
[24] Ruprecht-Karls-Universität Heidelberg,undefined
[25] University College Dublin,undefined
[26] Sezione INFN di Bari,undefined
[27] Sezione INFN di Bologna,undefined
[28] Sezione INFN di Cagliari,undefined
[29] Sezione INFN di Ferrara,undefined
[30] Sezione INFN di Firenze,undefined
[31] Laboratori Nazionali dell’INFN di Frascati,undefined
[32] Sezione INFN di Genova,undefined
[33] Sezione INFN di Milano Bicocca,undefined
[34] Sezione INFN di Padova,undefined
[35] Sezione INFN di Pisa,undefined
[36] Sezione INFN di Roma Tor Vergata,undefined
[37] Sezione INFN di Roma La Sapienza,undefined
[38] Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences,undefined
[39] AGH - University of Science and Technology,undefined
[40] Faculty of Physics and Applied Computer Science,undefined
[41] National Center for Nuclear Research (NCBJ),undefined
[42] Horia Hulubei National Institute of Physics and Nuclear Engineering,undefined
[43] Petersburg Nuclear Physics Institute (PNPI),undefined
[44] Institute of Theoretical and Experimental Physics (ITEP),undefined
[45] Moscow State University (SINP MSU),undefined
[46] Institute for Nuclear Research of the Russian Academy of Sciences (INR RAN),undefined
[47] Budker Institute of Nuclear Physics (SB RAS) and Novosibirsk State University,undefined
[48] Institute for High Energy Physics (IHEP),undefined
[49] Universitat de Barcelona,undefined
[50] Universidad de Santiago de Compostela,undefined
关键词
Hadron-Hadron Scattering;
D O I
10.1007/JHEP01(2014)033
中图分类号
学科分类号
摘要
A measurement of the Z(→ μ+μ−) + jet production cross-section in pp collisions at a centre-of-mass energy \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \sqrt{s} $\end{document} = 7 TeV is presented. The analysis is based on an integrated luminosity of 1.0 fb−1 recorded by the LHCb experiment. Results are shown with two jet transverse momentum thresholds, 10 and 20 GeV, for both the overall cross-section within the fiducial volume, and for six differential cross-section measurements. The fiducial volume requires that both the jet and the muons from the Z boson decay are produced in the forward direction (2.0 < η < 4.5). The results show good agreement with theoretical predictions at the second-order expansion in the coupling of the strong interaction. [graphic not available: see fulltext]
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共 63 条
[1]  
Hautmann F(2012)Inclusive W and Z production in the forward region at JHEP 06 058-undefined
[2]  
Hentschinski M(2013) = 7 TeV JHEP 02 106-undefined
[3]  
Jung H(2013)Measurement of the cross-section for Z → e JHEP 01 111-undefined
[4]  
Arnold PB(2013)e JHEP 07 032-undefined
[5]  
Reno MH(2013) production in pp collisions at Phys. Lett. B 722 238-undefined
[6]  
Giele W(2012) = 7 TeV Nucl. Phys. B 865 54-undefined
[7]  
Glover EN(1989)A study of the Z production cross-section in pp collisions at Nucl. Phys. B 319 37-undefined
[8]  
Kosower DA(1993) = 7 TeV using tau final states Nucl. Phys. B 403 633-undefined
[9]  
Anastasiou C(2004)Measurement of the production cross section of jets in association with a Z boson in pp collisions at Phys. Rev. D 69 094008-undefined
[10]  
Dixon LJ(2011) = 7 TeV with the ATLAS detector Comput. Phys. Commun. 182 2388-undefined