{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.157577.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2915441"}},{"@id":"https://doi.org/10.1007/JHEP09(2025)070","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2025","description":"Inclusive and differential cross sections for the Higgs boson production in proton-proton collisions at a centre-of-mass energy of 13.6 TeV are measured. The data set was collected with the CMS detector at the LHC in 2022 and corresponds to an integrated luminosity of $34.7~\\mathrm{fb}^{-1}$. Events with the diphoton final state are selected, and the measured inclusive fiducial cross section is $\\sigma_{fid} = 74 \\pm 11~\\text{(stat)}^{+5}_{\u22124}~\\text{(syst)}~\\mathrm{fb}$, in agreement with the standard model prediction of $67.8 \\pm 3.8~\\mathrm{fb}$$. Differential cross sections are measured as functions of several observables: the Higgs boson transverse momentum and rapidity, the number of associated jets, and the transverse momentum of the leading jet in the event. The differential cross sections also agree with the standard model predictions within the uncertainties.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.157577.v1/t1","@type":"Dataset","description":"Differential fiducial cross sections for pT of the Higgs boson","name":"Figure 7"},{"@id":"https://doi.org/10.17182/hepdata.157577.v1/t2","@type":"Dataset","description":"Example description","name":"Figure 7 correlation matrix"},{"@id":"https://doi.org/10.17182/hepdata.157577.v1/t3","@type":"Dataset","description":"Differential fiducial cross sections for rapidity of the Higgs boson","name":"Figure 8"},{"@id":"https://doi.org/10.17182/hepdata.157577.v1/t4","@type":"Dataset","description":"Example description","name":"Figure 8 correlation matrix"},{"@id":"https://doi.org/10.17182/hepdata.157577.v1/t5","@type":"Dataset","description":"Differential fiducial cross sections for the number of jets","name":"Figure 9"},{"@id":"https://doi.org/10.17182/hepdata.157577.v1/t6","@type":"Dataset","description":"Example description","name":"Figure 9 correlation matrix"},{"@id":"https://doi.org/10.17182/hepdata.157577.v1/t7","@type":"Dataset","description":"Differential fiducial cross sections for the leading jet pT","name":"Figure 10"},{"@id":"https://doi.org/10.17182/hepdata.157577.v1/t8","@type":"Dataset","description":"Example description","name":"Figure 10 correlation matrix"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2915441?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/157577"}],"inLanguage":"en","name":"Measurements of inclusive and differential Higgs boson production cross sections at $\\sqrt{s}$ = 13.6 TeV in the H $\\to$$\u03b3\u03b3$ decay channel","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2915441?version=1","version":1}