{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.137886.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2023464"}},{"@id":"https://doi.org/10.1007/JHEP08(2022)027","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"A measurement of inclusive and differential fiducial cross-sections for the production of the Higgs boson decaying into two photons is performed using \\(139\\,\\text{fb}^{-1}\\) of proton--proton collision data recorded at \\(\\sqrt{s} = 13\\,\\text{TeV}\\) by the ATLAS experiment at the Large Hadron Collider. The inclusive cross-section times branching ratio, in a fiducial region closely matching the experimental selection, is measured to be \\(67\\pm 6\\) fb, which is in agreement with the state-of-the-art Standard Model prediction of \\(64\\pm 4\\) fb. Extrapolating this result to the full phase space and correcting for the branching ratio, the total cross-section for Higgs boson production is estimated to be \\(58\\pm 6\\) pb. In addition, the cross-sections in four fiducial regions sensitive to various Higgs boson production modes and differential cross-sections as a function of either one or two of several observables are measured. All the measurements are found to be in agreement with the Standard Model predictions. The measured transverse momentum distribution of the Higgs boson is used as an indirect probe of the Yukawa coupling of the Higgs boson to the bottom and charm quarks. In addition, five differential cross-section measurements are used to constrain anomalous Higgs boson couplings to vector bosons in the Standard Model effective field theory framework.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t1","@type":"Dataset","description":"Measured inclusive cross sections in the five fiducial regions. Each systematic uncertainty source is fully uncorrelated with the other sources.","name":"inclusive"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t2","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma}$. Each systematic uncertainty source is fully uncorrelated with...","name":"pT_yy"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t3","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $N_\\mathrm{jets}$. Each systematic uncertainty source is fully uncorrelated with...","name":"N_j_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t4","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $N$($b$-jets). Each systematic uncertainty source is fully uncorrelated with...","name":"catXS_nbjet"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t5","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{j1}$. Each systematic uncertainty source is fully uncorrelated with...","name":"pT_j1_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t6","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma} (N_\\mathrm{jets}^{p_T>30\\ \\mathrm{GeV}}=0)$. Each systematic uncertainty source is fully...","name":"pT_yy_JV_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t7","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $m_{jj}$. Each systematic uncertainty source is fully uncorrelated with...","name":"m_jj_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t8","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $\\Delta\\phi_{jj}$. Each systematic uncertainty source is fully uncorrelated with...","name":"Dphi_j_j_30_signed"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t9","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma}$ in bins of $|y_{\\gamma\\gamma}|$. Each systematic uncertainty source...","name":"pT_yy_vs_yAbs_yy"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t10","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $\\Delta\\phi_{jj}$ in the VBF fiducial region. Each systematic uncertainty...","name":"VBF_Dphi_j_j_30_signed"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t11","@type":"Dataset","description":"Observed statistical correlations, evaluated with a bootstrapping technique, between $p_\\mathrm{T}^{\\gamma\\gamma}$, $N_\\mathrm{jets}$, $m_{jj}$, $\\Delta\\phi_{jj}$, and $p_\\mathrm{T}^{j1}$","name":"EFT_var_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t12","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma}$.","name":"pT_yy_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t13","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $N_\\mathrm{jets}$.","name":"N_j_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t14","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $N$($b$-jets).","name":"catXS_nbjet_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t15","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{j1}$.","name":"pT_j1_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t16","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma} (N_\\mathrm{jets}^{p_T>30\\ \\mathrm{GeV}}=0)$.","name":"pT_yy_JV_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t17","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $m_{jj}$.","name":"m_jj_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t18","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $\\Delta\\phi_{jj}$.","name":"Dphi_j_j_30_signed_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t19","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $\\Delta\\phi_{jj}$ in the VBF fiducial region.","name":"VBF_Dphi_j_j_30_signed_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t20","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma}$ in bins of $|y_{\\gamma\\gamma}|$. The bins...","name":"pT_yy_vs_yAbs_yy_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t21","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma1}/m_{\\gamma\\gamma}$. Each systematic uncertainty source is fully uncorrelated with...","name":"rel_pT_y1"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t22","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma1}/m_{\\gamma\\gamma}$.","name":"rel_pT_y1_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t23","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma2}/m_{\\gamma\\gamma}$. Each systematic uncertainty source is fully uncorrelated with...","name":"rel_pT_y2"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t24","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma2}/m_{\\gamma\\gamma}$.","name":"rel_pT_y2_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t25","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $|y_{\\gamma\\gamma}|$. Each systematic uncertainty source is fully uncorrelated with...","name":"yAbs_yy"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t26","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $|y_{\\gamma\\gamma}|$.","name":"yAbs_yy_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t27","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $m_{\\gamma\\gamma j}$. Each systematic uncertainty source is fully uncorrelated...","name":"m_yyj_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t28","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $m_{\\gamma\\gamma j}$.","name":"m_yyj_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t29","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma j}$. Each systematic uncertainty source is fully uncorrelated...","name":"pT_yyj_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t30","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma j}$.","name":"pT_yyj_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t31","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $H_{T}$. Each systematic uncertainty source is fully uncorrelated with...","name":"HT_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t32","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $H_{T}$.","name":"HT_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t33","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $\\tau_{C,j1}$. Each systematic uncertainty source is fully uncorrelated with...","name":"maxTau_yyj_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t34","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $\\tau_{C,j1}$.","name":"maxTau_yyj_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t35","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $\\sum\\tau_{C,j}$. Each systematic uncertainty source is fully uncorrelated with...","name":"sumTau_yyj_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t36","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $\\sum\\tau_{C,j}$.","name":"sumTau_yyj_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t37","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma} (N_\\mathrm{jets}^{p_T>40\\ \\mathrm{GeV}}=0)$. Each systematic uncertainty source is fully...","name":"pT_yy_JV_40"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t38","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma} (N_\\mathrm{jets}^{p_T>40\\ \\mathrm{GeV}}=0)$.","name":"pT_yy_JV_40_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t39","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma} (N_\\mathrm{jets}^{p_T>50\\ \\mathrm{GeV}}=0)$. Each systematic uncertainty source is fully...","name":"pT_yy_JV_50"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t40","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma} (N_\\mathrm{jets}^{p_T>50\\ \\mathrm{GeV}}=0)$.","name":"pT_yy_JV_50_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t41","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma} (N_\\mathrm{jets}^{p_T>60\\ \\mathrm{GeV}}=0)$. Each systematic uncertainty source is fully...","name":"pT_yy_JV_60"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t42","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma} (N_\\mathrm{jets}^{p_T>60\\ \\mathrm{GeV}}=0)$.","name":"pT_yy_JV_60_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t43","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $\\pi - |\\Delta\\phi_{\\gamma\\gamma,jj}|$. Each systematic uncertainty source is fully...","name":"Dphi_yy_jj_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t44","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $\\pi - |\\Delta\\phi_{\\gamma\\gamma,jj}|$.","name":"Dphi_yy_jj_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t45","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma jj}$. Each systematic uncertainty source is fully uncorrelated...","name":"pT_yyjj_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t46","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma jj}$.","name":"pT_yyjj_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t47","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma}$ in bins of $p_{T}^{\\gamma\\gamma j}$. Each systematic uncertainty...","name":"pT_yy_vs_pT_yyj_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t48","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma}$ in bins of $p_{T}^{\\gamma\\gamma j}$. The...","name":"pT_yy_vs_pT_yyj_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t49","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma}$ in bins of $\\tau_{C,j1}$. Each systematic uncertainty source...","name":"pT_yy_vs_maxTau_yyj_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t50","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma}$ in bins of $\\tau_{C,j1}$. The bins...","name":"pT_yy_vs_maxTau_yyj_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t51","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $(p_{T}^{\\gamma1}-p_{T}^{\\gamma2})/m_{\\gamma\\gamma}$ in bins of $(p_{T}^{\\gamma1}+p_{T}^{\\gamma2})/m_{\\gamma\\gamma}$. Each systematic uncertainty source...","name":"rel_DpT_y_y_vs_rel_sumpT_y_y"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t52","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $(p_{T}^{\\gamma1}-p_{T}^{\\gamma2})/m_{\\gamma\\gamma}$ in bins of $(p_{T}^{\\gamma1}+p_{T}^{\\gamma2})/m_{\\gamma\\gamma}$. The bins...","name":"rel_DpT_y_y_vs_rel_sumpT_y_y_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t53","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $|\\eta^*|$ in the VBF fiducial region. Each systematic uncertainty...","name":"VBF_abs_Zepp"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t54","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $|\\eta^*|$ in the VBF fiducial region.","name":"VBF_abs_Zepp_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t55","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{\\gamma\\gamma jj}$ in the VBF fiducial region. Each systematic...","name":"VBF_pT_yyjj_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t56","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{\\gamma\\gamma jj}$ in the VBF fiducial region.","name":"VBF_pT_yyjj_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t57","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{j1}$ in the VBF fiducial region. Each systematic uncertainty...","name":"VBF_pT_j1_30"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t58","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{j1}$ in the VBF fiducial region.","name":"VBF_pT_j1_30_corr"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t59","@type":"Dataset","description":"Measured differential cross section with associated uncertainties as a function of $p_{T}^{j1}$ in bins of $\\Delta\\phi_{jj}$ in the VBF fiducial...","name":"VBF_pT_j1_30_vs_Dphi_j_j_30_signed"},{"@id":"https://doi.org/10.17182/hepdata.137886.v2/t60","@type":"Dataset","description":"Post-fit correlation matrix for the differential cross section measured as a function of $p_{T}^{j1}$ in bins of $\\Delta\\phi_{jj}$ in the...","name":"VBF_pT_j1_30_vs_Dphi_j_j_30_signed_corr"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2023464?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/137886"}],"inLanguage":"en","name":"Measurements of the Higgs boson inclusive and differential fiducial cross-sections in the diphoton decay channel with $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2023464?version=2","version":2}