{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.86538.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1678088"}},{"@id":"https://doi.org/10.1007/JHEP11(2018)152","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2019","description":"A search for a Higgs boson decaying into a pair of electrons or muons and a photon is described. Higgs boson decays to a Z boson and a photon $(H\\rightarrow Z\\gamma\\rightarrow ll\\gamma, l = e \\text{ or } \\mu)$, or to two photons, one of which has an internal conversion into a muon pair $(H\\rightarrow\\gamma^{*}\\gamma\\rightarrow\\mu\\mu\\gamma)$ were considered. The analysis is performed using a data set recorded by the CMS experiment at the LHC from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. No significant excess above the background prediction has been found. Limits are set on the cross section for a standard model Higgs boson decaying to opposite-sign electron or muon pairs and a photon. The observed limits on cross section times the corresponding branching fractions vary between 1.4 and 4.0 (6.1 and 11.4) times the standard model cross section for $H\\rightarrow\\gamma^{*}\\gamma\\rightarrow\\mu\\mu\\gamma$ $(H\\rightarrow Z\\gamma\\rightarrow ll\\gamma)$ in the 120-130 GeV mass range of the $ll\\gamma$ system. The $H\\rightarrow\\gamma^{*}\\gamma\\rightarrow\\mu\\mu\\gamma$ and $H\\rightarrow Z\\gamma\\rightarrow ll\\gamma$ analyses are combined for $m_{H} = 125$ GeV, obtaining an observed (expected) 95% condifence level upper limit of 3.9 (2.0) times the standard model cross section.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.86538.v1/t1","@type":"Dataset","description":"Exclusion limit, at 95% CL, on the cross section of the $H \\rightarrow \\gamma^{*}\\gamma \\rightarrow \\mu\\mu\\gamma$ process relative to the...","name":"Figure 6a ($H\\rightarrow\\gamma^{*}\\gamma$ Limits)"},{"@id":"https://doi.org/10.17182/hepdata.86538.v1/t2","@type":"Dataset","description":"Exclusion limit, at 95% CL, on the cross section of the $H \\rightarrow Z\\gamma \\rightarrow ll\\gamma$ process relative to the...","name":"Figure 6b ($H\\rightarrow Z\\gamma$ Limits)"},{"@id":"https://doi.org/10.17182/hepdata.86538.v1/t3","@type":"Dataset","description":"Exclusion limit, at 95% CL, on the cross section of the $H \\rightarrow ll\\gamma$ relative to the SM prediction, for...","name":"Figure 7 ($H\\rightarrow ll\\gamma$ Limits)"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1678088?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/86538"}],"inLanguage":"en","name":"Search for the decay of a Higgs boson in the $\\ell\\ell\\gamma$ channel in proton-proton collisions at $\\sqrt{s}=$ 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1678088?version=1","version":1}