{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.89938.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1735729"}},{"@id":"https://doi.org/10.1103/PhysRevLett.123.131802","@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 light charged Higgs boson ($\\mathrm{H^{+}}$) decaying to a W boson and a CP-odd Higgs boson (A) in final states with $\\mathrm{e}\\mu\\mu$ or $\\mu\\mu\\mu$ is performed using data from pp collisions at $\\sqrt{s}=13$ TeV, recorded by the CMS detector at the LHC and corresponding to an integrated luminosity of 35.9 fb$^{-1}$. In this search, it is assumed that the $\\mathrm{H}^{+}$ boson is produced in decays of top quarks, and the A boson decays to two opposite-charge muons. The presence of signals for $\\mathrm{H}^{+}$ boson masses between 100 and 160 GeV and A boson masses between 15 and 75 GeV is investigated. No evidence for the production of the $\\mathrm{H^{+}}$ boson is found. Upper limits at 95% confidence level are obtained on the combined branching fraction for the decay chain, $\\mathrm{t}\\to\\mathrm{bH^{+}}\\to\\mathrm{bW^{+}A}\\to\\mathrm{bW^{+}}\\mu^{+}\\mu^{-}$, of $1.9\\times10^{-6}$ to $8.6\\times10^{-6}$, depending on the masses of the $\\mathrm{H^{+}}$ and A bosons. These are the first limits for these decay modes of the $\\mathrm{H^{+}}$ and A bosons.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.89938.v2/t1","@type":"Dataset","description":"Expected and observed upper limits at 95% CL on $\\mathcal{B}_{sig}=\\mathcal{B}(\\mathrm{t}\\to\\mathrm{b}\\mathrm{H^{+}})\\mathcal{B}(\\mathrm{H^{+}}\\to\\mathrm{W^{+}}\\mathrm{A})\\mathcal{B}(\\mathrm{A}\\to\\mu^{+}\\mu^{-})$ for the A boson masses ($\\mathit{m}_{\\mathrm{A}}$). The $\\mathrm{H^{+}}$ boson mass...","name":"Figure 2a"},{"@id":"https://doi.org/10.17182/hepdata.89938.v2/t2","@type":"Dataset","description":"Expected and observed upper limits at 95% CL on $\\mathcal{B}_{sig}=\\mathcal{B}(\\mathrm{t}\\to\\mathrm{b}\\mathrm{H^{+}})\\mathcal{B}(\\mathrm{H^{+}}\\to\\mathrm{W^{+}}\\mathrm{A})\\mathcal{B}(\\mathrm{A}\\to\\mu^{+}\\mu^{-})$ for the A boson masses ($\\mathit{m}_{\\mathrm{A}}$). The $\\mathrm{H^{+}}$ boson mass...","name":"Figure 2b"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1735729?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/89938"}],"inLanguage":"en","name":"Search for a light charged Higgs boson decaying to a W boson and a CP-odd Higgs boson in final states with e$\\mu\\mu$ or $\\mu\\mu\\mu$ 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/ins1735729?version=2","version":2}
