{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.89370.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1717495"}},{"@id":"https://doi.org/10.1007/JHEP04(2019)093","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2019","description":"CERN-LHC.  Measurement of the ratio of cross sections for inclusive isolated-photon production in proton-proton collisions at a centre-of-mass energy of 13 TeV over 8 TeV. Measurement is also presented of the double ratio of the ratio above to the ratio of the fiducial cross sections for Z boson production at 13 TeV and 8 TeV using the decay channels Z into an electron-positron pair and Z into a muon-antimuon pair.\n \nThe ratio of cross sections for inclusive isolated-photon production is denoted by Rgamma13/8. The ratio of fiducial cross sections for Z boson production is denoted by RZ13/8. The double ratio (Rgamma13/8)/(RZ13/8) is denoted by Dgamma/Z13/8.\n\nThe photon is required to have a transverse energy above 125 GeV and absolute value of pseudorapity |etaGamma|<2.37, excluding the region 1.37<|etaGamma|<1.56. The photon isolation is ensured by requiring the transverse energy around a cone of radius R=0.4 around the photon to be less than (4.8 + 0.0042 * ETGamma) [GeV]. At particle level it is the sum of transverse energy from all particles, except for muons, neutrinos and the photon itself. At parton level it is the sum of energy from all coloured partons.\n  \nThe fiducial cross section for Z boson production at a given centre-of-mass energy is defined as the production cross section of a Z boson times the branching ratio into a lepton pair of flavour l+l- = e+e- or mu+mu- within the following phase space: the lepton transverse momentum pT> 25 GeV, the lepton pseudorapidity |eta|<2.5 and the dilepton invariant mass 66 < mll < 116 GeV. Measurements of the fiducial cross sections were made using the decay channels Z into e+e- and Z into mu+mu-, and combined for the final result. The measured RZ13/8 is 1.537 +- 0.001 (stat.) +- 0.010 (syst.) +- 0.044 (lumi.).\n\nPredictions for Rgamma13/8 are given at NLO QCD from the program Jetphox using the MMHT2014 NLO PDF set. Predictions for Dgamma/Z13/8 are obtained from the predictions of Rgamma13/8 at NLO QCD from Jepthox using the MMHT2014 NNLO PDF set and the predictions of RZ13/8 at NNLO QCD from Dyturbo using the MMHT2014 NNLO PDF set.\n\nInformation about the bin-to-bin correlation of the systematic uncertainties of Rgamma13/8. The following uncertainties are to be treated as uncorrelated bin-to-bin:  sysEnergyResolution13, sysEnergyResolution8, sysPhotonID13, sysPhotonID8, sysBackgroundIsolation13, sysBackgroundIsolation8, sysBackgroundIsolationUpperLimit13, sysBackgroundID13, sysBackgroundID8, sysIsolationMC13 and sysMCstats13. The systematic uncertainty due to the photon energy scale (sysEnergyScale) is partially correlated bin-to-bin; the table shows just the total systematic uncertainty due to the photon energy scale (separately for the up and down contributions). In order to take into account properly the correlations due to the photon energy scale, see the information provided below.\n\nThe systematic uncertainty due to the photon energy scale (GES) is decomposed into 25 independent components. Each file (see below) contains 50 lines since for each independent component there are two variations (up and down). Each variation is to be treated as fully correlated bin-to-bin. The relative changes in the ratio Rgamma13/8 of the differential cross sections due to each variation are given in the following files.\n\nFor the ratio Rgamma13/8 as a function of ETGamma for the range |etaGamma|<0.6 is in the file decompositionsystematicuncertaintygesratio1stetabin.txt\n\nFor the ratio Rgamma13/8 as a function of ETGamma for the range 0.6<|etaGamma|<1.37 is in the file decompositionsystematicuncertaintygesratio2ndetabin.txt\n\nFor the ratio Rgamma13/8 as a function of ETGamma for the range 1.56<|etaGamma|<1.81 is in the file decompositionsystematicuncertaintygesratio3rdetabin.txt\n\nFor the ratio Rgamma13/8 as a function of ETGamma for the range 1.81<|etaGamma|<2.37 is in the file decompositionsystematicuncertaintygesratio4thetabin.txt\n\nEach file contains 50 lines and each line contains the relative changes in the ratio Rgamma13/8 of the differential cross sections for each bin of ETGamma: 14 bins for the 1st region in etaGamma, 13 bins for the 2nd region in etaGamma, 10 bins for the 3rd region in etaGamma and 10 bins for the 4th region in etaGamma. It should be noted that RELATIVE CHANGES are quoted in the files and that the relative changes are SIGNED. It should also be noted that the relative changes in the ratio Rgamma13/8 of the differential cross sections induced by the up and down variations of a given component are not necessarily symmetric. All the txt files are included in the gzipped tar file files_with_decompositionsystematicuncertaintyges.tar.gz that can be accessed in the resources.\n  \nInformation about the bin-to-bin correlation of the systematic uncertainties of Dgamma/Z13/8. The following uncertainties are to be treated as uncorrelated bin-to-bin:  sysEnergyResolution13, sysEnergyResolution8, sysPhotonID13, sysPhotonID...","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t1","@type":"Dataset","description":"Measured ratio of cross sections for inclusive isolated-photon production as a function of $E_{\\rm T}^{\\gamma}$ for $|\\eta^{\\gamma}|<0.6$.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t2","@type":"Dataset","description":"Predicted ratio of cross sections for inclusive isolated-photon production as a function of $E_{\\rm T}^{\\gamma}$ for $|\\eta^{\\gamma}|<0.6$.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t3","@type":"Dataset","description":"Measured ratio of cross sections for inclusive isolated-photon production as a function of $E_{\\rm T}^{\\gamma}$ for $0.6<|\\eta^{\\gamma}|<1.37$.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t4","@type":"Dataset","description":"Predicted ratio of cross sections for inclusive isolated-photon production as a function of $E_{\\rm T}^{\\gamma}$ for $0.6<|\\eta^{\\gamma}|<1.37$.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t5","@type":"Dataset","description":"Measured ratio of cross sections for inclusive isolated-photon production as a function of $E_{\\rm T}^{\\gamma}$ for $1.56<|\\eta^{\\gamma}|<1.81$.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t6","@type":"Dataset","description":"Predicted ratio of cross sections for inclusive isolated-photon production as a function of $E_{\\rm T}^{\\gamma}$ for $1.56<|\\eta^{\\gamma}|<1.81$.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t7","@type":"Dataset","description":"Measured ratio of cross sections for inclusive isolated-photon production as a function of $E_{\\rm T}^{\\gamma}$ for $1.81<|\\eta^{\\gamma}|<2.37$.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t8","@type":"Dataset","description":"Predicted ratio of cross sections for inclusive isolated-photon production as a function of $E_{\\rm T}^{\\gamma}$ for $1.81<|\\eta^{\\gamma}|<2.37$.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t9","@type":"Dataset","description":"Measured double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\\rm T}^{\\gamma}$ for...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t10","@type":"Dataset","description":"Predicted double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\\rm T}^{\\gamma}$ for...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t11","@type":"Dataset","description":"Measured double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\\rm T}^{\\gamma}$ for...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t12","@type":"Dataset","description":"Predicted double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\\rm T}^{\\gamma}$ for...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t13","@type":"Dataset","description":"Measured double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\\rm T}^{\\gamma}$ for...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t14","@type":"Dataset","description":"Predicted double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\\rm T}^{\\gamma}$ for...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t15","@type":"Dataset","description":"Measured double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\\rm T}^{\\gamma}$ for...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.89370.v1/t16","@type":"Dataset","description":"Predicted double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\\rm T}^{\\gamma}$ for...","name":"Table 16"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1717495?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/89370"}],"inLanguage":"en","name":"Measurement of the ratio of cross sections for inclusive isolated-photon production in $pp$ collisions at $\\sqrt s = 13$ and $8$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1717495?version=1","version":1}