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Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Journal , Other literature type 01 Jan 2017Embargo end date: 01 Jan 2018 United Kingdom, Italy, United Kingdom, South Africa, United Kingdom, United Kingdom, United Kingdom, United Kingdom, Turkey, Italy, Italy, Switzerland, Germany, Italy, Germany, South Africa, Italy, Turkey, Germany, Italy, Italy, United Kingdom, France, Italy, Italy, Italy Publisher:arXivJournal:Physics Letters B (issn: 0370-2693, Copyright policy )Funded by:GSRI | unidentified
Authors: Jeannine Wagner-kuhr; Juraj Bracinik; Yoichi Ninomiya; Pavel Starovoitov; Alexander Khanov; David Martin Bjergaard; Alberto Gascon Bravo; +193 Authors

doi: 10.48550/arxiv.1801.00112 , 10.3204/pubdb-2018-00059 , 10.3204/pubdb-2018-01922

arXiv: http://arxiv.org/abs/1801.00112 , 1801.00112

handle: 2434/587256 , 20.500.11770/304349 , 11390/1131440 , 2108/200863 , 11590/337685 , 11573/1216320 , 11367/72188 , 11568/947245 , 11568/1164402 , 11571/1271006 , 10210/287612

Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

Abstract

The dynamics of isolated-photon production in association with a jet in proton–proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of 3.2 $fb^{−1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R = 0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon–jet invariant mass and the scattering angle in the photon–jet centre-of-mass system. Tree-level plus parton-shower predictions from Sherpa and Pythia as well as next-to-leading-order QCD predictions from Jetphox and Sherpa are compared to the measurements.

Physics letters / B 780, 578 - 602 (2018). doi:10.1016/j.physletb.2018.03.035

Published by North-Holland Publ., Amsterdam

Countries
United Kingdom, Italy, United Kingdom, South Africa, United Kingdom, United Kingdom, United Kingdom, United Kingdom, Turkey, Italy, Italy, Switzerland, Germany, Italy, Germany, South Africa, Italy, Turkey, Germany, Italy, Italy, United Kingdom, France, Italy, Italy, Italy
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Keywords

13000 GeV-cms, transverse energy [photon], jet: transverse momentum, transverse momentum dependence, transverse momentum [jet], Settore FIS/04 - Fisica Nucleare e Subnucleare, High Energy Physics - Experiment, High Energy Physics - Experiment (hep-ex), scattering [p p], [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], Settore ING-INF/07 - Misure Elettriche e Elettroniche, photon: transverse energy, Physics, ddc:530, Settore FIS/01 - Fisica Sperimentale, Particle physics, higher-order: 1, Monte Carlo [numerical calculations], ATLAS, Settore FIS/01 - FISICA SPERIMENTALE, CERN LHC Coll, associated production [photon], PYTHIA, hadroproduction [jet], colliding beams [p p], numerical calculations: Monte Carlo, Particle Physics - Experiment, 1 [higher-order], perturbation theory [quantum chromodynamics], Nuclear and High Energy Physics, p p: scattering, [PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex], QC1-999, FOS: Physical sciences, Hadron-collisions; fragmentation; dynamics, 530, info:eu-repo/classification/ddc/500.2, energy dependence, HADRON-COLLISIONS; FRAGMENTATION; DYNAMICS, differential cross section: measured, measured [differential cross section], tree approximation, High energy physics, quantum chromodynamics: perturbation theory, hep-ex, 500, jet: hadroproduction, 541, photon: associated production, anti-kT algorithm, p p: colliding beams, experimental results, ddc: ddc:500.2, ddc: ddc:530

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