Production of γγ+2 jets from double parton scattering in proton-proton collisions at the LHC

Cross sections for the production of pairs of photons plus two additional jets produced from double parton scattering in high-energy proton-proton collisions at the LHC are calculated for the first time. The estimates are based on the theoretical perturbative QCD predictions for the productions of γ...

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Published inChinese physics C Vol. 39; no. 12; pp. 1 - 6
Main Author 陶军全 张思靓 沈玉乔 范嘉伟 陈国明 陈和生
Format Journal Article
LanguageEnglish
Published 01.12.2015
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ISSN1674-1137
2058-6132
0254-3052
DOI10.1088/1674-1137/39/12/121001

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Summary:Cross sections for the production of pairs of photons plus two additional jets produced from double parton scattering in high-energy proton-proton collisions at the LHC are calculated for the first time. The estimates are based on the theoretical perturbative QCD predictions for the productions of γγ at next-to-next-to-leading-order, jet+jet and γ+jet at next-to-leading-order, for their corresponding single-scattering cross sections. The cross sections and expected event rates for γγ+2 jets from double parton scattering, after typical acceptance and selections, are given for proton-proton collisions with the collision energy s=13 TeV and integrated luminosity of 100 fb-1 planned for the following years, and also s=14 TeV with 3000 fb 1 of integrated luminosity as the LHC design.
Bibliography:γγ+2 jets production, double parton scattering, QCD
11-5641/O4
Cross sections for the production of pairs of photons plus two additional jets produced from double parton scattering in high-energy proton-proton collisions at the LHC are calculated for the first time. The estimates are based on the theoretical perturbative QCD predictions for the productions of γγ at next-to-next-to-leading-order, jet+jet and γ+jet at next-to-leading-order, for their corresponding single-scattering cross sections. The cross sections and expected event rates for γγ+2 jets from double parton scattering, after typical acceptance and selections, are given for proton-proton collisions with the collision energy s=13 TeV and integrated luminosity of 100 fb-1 planned for the following years, and also s=14 TeV with 3000 fb 1 of integrated luminosity as the LHC design.
TAO dun-Quan, ZHANG Si-Jing,SHEN Yu-Qiao, FAN Jia-Wei, CHEN Guo-Ming, CHEN He-Sheng (1 Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China 2 University of Chinese Academy of Sciences, Beijing 100049, China)
ISSN:1674-1137
2058-6132
0254-3052
DOI:10.1088/1674-1137/39/12/121001