{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.94261.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1796727"}},{"@id":"https://doi.org/10.1103/PhysRevD.102.072001","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2020","description":"A search is conducted for a low-mass charged Higgs boson produced        in a top quark decay and subsequently decaying into a charm and        a strange quark. The data sample was recorded in proton-proton        collisions at $\\sqrt{s}=13 TeV$ by the CMS experiment at the LHC        and corresponds to an integrated luminosity of 35.9/fb. The search        is performed in the process of top quark pair production,        where one top quark decays to a bottom quark and a charged Higgs        boson, and the other to a bottom quark and a W boson. With        the W boson decaying to a charged lepton (electron or muon) and a        neutrino, the final state comprises an isolated lepton, missing        transverse momentum, and at least four jets, of which two are tagged        as b jets. To enhance the search sensitivity, one of the jets        originating from the charged Higgs boson is required to satisfy a        charm tagging selection. No significant excess beyond standard model        predictions is found in the dijet invariant mass distribution. An        upper limit in the range 1.68--0.25% is set on the branching fraction        of the top quark decay to the charged Higgs boson and bottom quark for        a charged Higgs boson mass between 80 and 160 GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.94261.v1/t1","@type":"Dataset","description":"Expected and observed 95% CL exclusion limits in % on BR(t->H+ b) for the muon channel after the individual charm...","name":"Figure 4a"},{"@id":"https://doi.org/10.17182/hepdata.94261.v1/t2","@type":"Dataset","description":"Expected and observed 95% CL exclusion limits in % on BR(t->H+ b) for the electron channel after the individual charm...","name":"Figure 4b"},{"@id":"https://doi.org/10.17182/hepdata.94261.v1/t3","@type":"Dataset","description":"Expected and observed 95% CL exclusion limits in % on BR(t->H+ b) after the individual charm tagging categories and the...","name":"Figure 4c"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1796727?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/94261"}],"inLanguage":"en","name":"Search for a light charged Higgs boson in the H$^\\pm$ $\\to $ cs 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/ins1796727?version=1","version":1}