Meaurement of the incluive iolated-photon cro ection in pp colliion at $$ \qrt{} $$ = 13 TeV uing 36 fb−1 of ATLAS data

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Zenin,Tibor Ženiš,Dirk Zerwas,Miha Zgubic,Dengfeng Zhang,Fusuo Zhang,Guang-Ping Zhang,Hai-Feng Zhang,J. Zhang,Lijun Zhang,Matt Zhang,Ren-You Zhang,X.Y. Zhang,Y. H. Zhang,Zhidong Zhang,Pingchuan Zhao,Yong Zhao,Z. G. Zhao,Alexey Zhemchugov,Zhi Zheng,Dewen Zhong,B. Zhou,Chen Zhou,Mingliang Zhou,Maosen Zhou,Ning Zhou,You Zhou,C. G. Zhu,Heling Zhu,Hongsheng Zhu,Ji Zhu,Y. C. Zhu,Xuai Zhuang,Konstantin Zhukov,Vladimir Zhulanov,Vladimir Zhulanov,Daria Zieminska,Nikolai Zimine,Stephanie Zimmermann,Zinonas Zinonos,Michael Ziolkowski,Lidija Zivkovic,Georg Zobernig,Antonio Zoccoli,Knut Zoch,Theodoros Georgio Zorbas,Rui Zou,Lukasz Zwalinski

Meaurement of the incluive iolated-photon cro ection in pp colliion at $$ \qrt{} $$ = 13 TeV uing 36 fb−1 of ATLAS data

2019

The differential cross section for isolated-photon production in pp collisions is measured at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC using an integrated luminosity of 36.1 fb−1. The differential cross section is presented as a function of the photon transverse energy in different regions of photon pseudorapidity. The differential cross section as a function of the absolute value of the photon pseudorapidity is also presented in different regions of photon transverse energy. Next-to-leading-order QCD calculations from Jetphox and Sherpa as well as next-to-next-to-leading-order QCD calculations from Nnlojet are compared with the measurement, using several parameterisations of the proton parton distribution functions. The predictions provide a good description of the data within the experimental and theoretical uncertainties.

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