论文信息 - Measurements of integrated and differential cross sections for isolated photon pair production in pp collisions at ﬃﬃ s p = 8 TeV with the ATLAS detector

Measurements of integrated and differential cross sections for isolated photon pair production in pp collisions at ﬃﬃ s p = 8 TeV with the ATLAS detector

A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of root s = 8 TeV is presented. The results are based on an integrated ...

[1] A. S. Mete,et al. Topological cell clustering in the ATLAS calorimeters and its performance in LHC Run 1 , 2017, The European Physical Journal C.

[2] F. Siegert. A practical guide to event generation for prompt photon production with Sherpa , 2016, 1611.07226.

[3] S. M. Etesami,et al. Search for Resonant Production of High-Mass Photon Pairs in Proton-Proton Collisions at sqrt[s]=8 and 13 TeV. , 2016, Physical review letters.

[4] A. S. Mete,et al. Measurement of the photon identification efficiencies with the ATLAS detector using LHC Run-1 data , 2016, The European Physical Journal C.

[5] P. Catastini,et al. Measurement of the transverse momentum and $$\phi ^*_{\eta }$$ϕη∗ distributions of Drell–Yan lepton pairs in proton–proton collisions at $$\sqrt{s}=8$$s=8 TeV with the ATLAS detector , 2016, The European physical journal. C, Particles and fields.

[6] J. Campbell,et al. Predictions for diphoton production at the LHC through NNLO in QCD , 2016, 1603.02663.

[7] D. Florian,et al. Diphoton production at hadron colliders: transverse-momentum resummation at next-to-next-to-leading logarithmic accuracy , 2015, 1505.03162.

[8] J. Latorre,et al. Parton distributions for the LHC run II , 2014, 1410.8849.

[9] J. T. Childers,et al. Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector , 2014, 1408.7084.

[10] J. T. Childers,et al. Measurements of fiducial and differential cross sections for Higgs boson production in the diphoton decay channel at √s = 8 TeV with ATLAS , 2014, 1407.4222.

[11] J. T. Childers,et al. Electron and photon energy calibration with the ATLAS detector using LHC Run 1 data , 2014, 1407.5063.

[12] V. M. Ghete,et al. Observation of the diphoton decay of the Higgs boson and measurement of its properties , 2014, The European physical journal. C, Particles and fields.

[13] A. Korytov,et al. Les Houches 2013: Physics at TeV Colliders: Standard Model Working Group Report , 2014, 1405.1067.

[14] D. Whiteson,et al. Measurement of the cross section for prompt isolated diphoton production using the full CDF run II data sample. , 2013, Physical review letters.

[15] J. Jia. TeV with the ATLAS Detector , 2013 .

[16] F. Siegert,et al. QCD matrix elements + parton showers. The NLO case , 2012, Journal of High Energy Physics.

[17] F Cascioli,et al. Scattering amplitudes with open loops. , 2011, Physical review letters.

[18] G. Aad. Measurement of the isolated diphoton cross section in pp collisions at ffiffi s p 1⁄4 7 TeV with the ATLAS detector , 2012 .

[19] W. Marsden. I and J , 2012 .

[20] J. T. Childers,et al. Performance of the ATLAS Trigger System in 2010 , 2012 .

[21] R. K. Shivpuri,et al. Precise study of the Z/γ* boson transverse momentum distribution in pp collisions using a novel technique. , 2010, Physical review letters.

[22] P. Waller,et al. Optimisation of variables for studying dilepton transverse momentum distributions at hadron colliders , 2010, 1009.1580.

[23] G. Aad. Measurement of the inclusive isolated prompt photon cross section in pp collisions , 2011 .

[24] Abdallah. Measurement of the inclusive isolated prompt photon cross section in pp collisions at ffiffi s p 1⁄4 7 TeV with the ATLAS detector , 2011 .

[25] J. T. Childers,et al. The ATLAS Simulation Infrastructure , 2010, 1005.4568.

[26] J. Huston,et al. New parton distributions for collider physics , 2010, 1007.2241.

[27] E. Re,et al. A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX , 2010, 1002.2581.

[28] M. Cacciari,et al. On the characterisation of the underlying event , 2009, 0912.4926.

[29] Frank Siegert,et al. QCD matrix elements and truncated showers , 2009, 0903.1219.

[30] T. Wyatt,et al. A Novel Technique for Studying the Z Boson Transverse Momentum Distribution at Hadron Colliders , 2008, 0807.4956.

[31] A. Goshaw. The ATLAS Experiment at the CERN Large Hadron Collider , 2008 .

[32] P. Nason,et al. Matching NLO QCD computations with Parton Shower simulations: the POWHEG method , 2007, 0709.2092.

[33] S. Schumann,et al. A Parton shower algorithm based on Catani-Seymour dipole factorisation , 2007, 0709.1027.

[34] E. Berger,et al. Gluon-gluon contributions to the production of continuum diphoton pairs at hadron colliders , 2007, hep-ph/0702003.

[35] J. T. Physik. Fakultt fr Physik und Astronomie , 2007 .

[36] Z. Was,et al. PHOTOS Monte Carlo: a precision tool for QED correctionsin Z and W decays , 2005, hep-ph/0506026.

[37] P. Nason. A new method for combining NLO QCD with shower Monte Carlo algorithms , 2004, hep-ph/0409146.

[38] A. Dell'Acqua,et al. Geant4 - A simulation toolkit , 2003 .

[39] J. Huston,et al. New generation of parton distributions with uncertainties from global QCD analysis , 2002, hep-ph/0201195.

[40] G. Soff,et al. AMEGIC++ 1.0: A Matrix element generator in C++ , 2001, hep-ph/0109036.

[41] K. Cranmer,et al. Kernel estimation in high-energy physics , 2000, hep-ex/0011057.

[42] J. Guillet,et al. A full next-to-leading order study of direct photon pair production in hadronic collisions , 1999, hep-ph/9911340.

[43] S. Frixione. ISOLATED PHOTONS IN PERTURBATIVE QCD , 1998, hep-ph/9801442.

[44] G. D'Agostini,et al. A Multidimensional unfolding method based on Bayes' theorem , 1995 .

[45] Yuan,et al. Nonperturbative regime in QCD resummation for gauge boson production at hadron colliders. , 1993, Physical review. D, Particles and fields.

[46] D. Soper,et al. Angular distribution of dileptons in high-energy hadron collisions , 1977 .