{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.115024.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1984855"}},{"@id":"https://doi.org/10.1007/JHEP05(2022)005","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2021","description":"A search for new heavy resonances decaying to a pair of Higgs bosons (HH) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. Data were collected with the CMS detector at the LHC in 2016--2018, corresponding to an integrated luminosity of 138 $\\mathrm{fb}^{-1}$. Resonances with a mass between 0.8 and 4.5 TeV are considered using events in which one Higgs boson decays into a bottom quark pair and the other into final states with either one or two charged leptons. Specifically, the single-lepton decay channel $\\mathrm{HH} \\to \\mathrm{b}\\bar{\\mathrm{b}} \\mathrm{WW}^* \\to \\mathrm{b}\\bar{\\mathrm{b}} \\ell \\nu \\mathrm{q}\\bar{\\mathrm{q}}'$ and the dilepton decay channels $\\mathrm{HH} \\to \\mathrm{b}\\bar{\\mathrm{b}} \\mathrm{WW}^* \\to \\mathrm{b}\\bar{\\mathrm{b}} \\ell \\nu \\ell \\nu$ and $\\mathrm{HH} \\to \\mathrm{b}\\bar{\\mathrm{b}} \\tau\\tau \\to \\mathrm{b}\\bar{\\mathrm{b}} \\ell \\nu \\nu \\ell \\nu \\nu$ are examined, where $\\ell$ in the final state corresponds to an electron or muon. The signal is extracted using a two-dimensional maximum likelihood fit of the $\\mathrm{H}\\to\\mathrm{b}\\bar{\\mathrm{b}}$ jet mass and HH invariant mass distributions. No significant excess above the standard model expectation is observed in data. Model-independent exclusion limits are placed on the product of the cross section and branching fraction for narrow spin-0 and spin-2 massive bosons decaying to HH. The results are also interpreted in the context of radion and bulk graviton production in models with a warped extra spatial dimension. The results provide the most stringent limits to date for $\\mathrm{X}\\to\\mathrm{HH}$ signatures with final-state leptons and at some masses provide the most sensitive limits of all $\\mathrm{X}\\to\\mathrm{HH}$ searches.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.115024.v1/t1","@type":"Dataset","description":"Exclusion limits on the product of the production cross section and the branching fraction for a new spin-0 resonance produced...","name":"Figure 7a"},{"@id":"https://doi.org/10.17182/hepdata.115024.v1/t2","@type":"Dataset","description":"Exclusion limits on the product of the production cross section and the branching fraction for a new spin-2 resonance produced...","name":"Figure 7b"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1984855?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/115024"}],"inLanguage":"en","name":"Search for heavy resonances decaying to a pair of Lorentz-boosted Higgs bosons in final states with leptons and a bottom quark pair at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1984855?version=1","version":1}