A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of √𝑠 =8 TeV is presented. The results are based on an integrated luminosity of 20.2 fb−1 recorded by the ATLAS detector at the Large Hadron Collider. The measurement considers photons with pseudorapidities satisfying |𝜂𝛾| <1.37 or 1.56<|𝜂𝛾|<2.37 and transverse energies of respectively 𝐸𝛾 T,1>40 GeV and 𝐸𝛾 T,2>30 GeV for the two leading photons ordered in transverse energy produced in the interaction. The background due to hadronic jets and electrons is subtracted using data-driven techniques. The fiducial cross sections are corrected for detector effects and measured differentially as a function of six kinematic observables. The measured cross section integrated within the fiducial volume is 16.8 ±0.8 pb. The data are compared to fixed-order QCD calculations at next-to-leading-order and next-to-next-to-leading-order accuracy as well as next-to-leading-order computations including resummation of initial-state gluon radiation at next-to-next-to-leading logarithm or matched to a parton shower, with relative uncertainties varying from 5% to 20%.
Measurements of integrated and differential cross sections for isolated photon pair production in 𝑝𝑝 collisions at √𝑠=8 TeV with the ATLAS detector
Bruscino NMembro del Collaboration Group
;Spanò FMembro del Collaboration Group
;
2017-01-01
Abstract
A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of √𝑠 =8 TeV is presented. The results are based on an integrated luminosity of 20.2 fb−1 recorded by the ATLAS detector at the Large Hadron Collider. The measurement considers photons with pseudorapidities satisfying |𝜂𝛾| <1.37 or 1.56<|𝜂𝛾|<2.37 and transverse energies of respectively 𝐸𝛾 T,1>40 GeV and 𝐸𝛾 T,2>30 GeV for the two leading photons ordered in transverse energy produced in the interaction. The background due to hadronic jets and electrons is subtracted using data-driven techniques. The fiducial cross sections are corrected for detector effects and measured differentially as a function of six kinematic observables. The measured cross section integrated within the fiducial volume is 16.8 ±0.8 pb. The data are compared to fixed-order QCD calculations at next-to-leading-order and next-to-next-to-leading-order accuracy as well as next-to-leading-order computations including resummation of initial-state gluon radiation at next-to-next-to-leading logarithm or matched to a parton shower, with relative uncertainties varying from 5% to 20%.| File | Dimensione | Formato | |
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PhysRevD.95.112005.pdf
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