{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.156777.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2846106"}},{"@id":"https://doi.org/10.1007/JHEP02(2025)143","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2025","description":"This article presents a search for a heavy charged Higgs boson produced in association with a top quark and a bottom quark, and decaying into a \ud835\udc4a boson and a 125 GeV Higgs boson \u210e. The search is performed in final states with one charged lepton, missing transverse momentum, and jets using proton\u2013proton collision data at \u221a\ud835\udc60 = 13 TeV recorded with the ATLAS detector during Run 2 of the LHC at CERN. This data set corresponds to a total integrated luminosity of 140 fb\u22121. The search is conducted by examining the reconstructed invariant mass distribution of the \ud835\udc4a \u210e candidates for evidence of a localised excess in the charged Higgs boson mass range from 250 GeV to 3 TeV . No significant excess is observed and 95% confidence-level upper limits between 2.8 pb and 1.2 fb are placed on the production cross-section times branching ratio for charged Higgs bosons decaying into \ud835\udc4a \u210e.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.156777.v1/t1","@type":"Dataset","description":"Upper limit at the 95% CL on the product of the cross-section for the $pp \\rightarrow tb H^{\\pm}$ process and...","name":"Limit resolved category"},{"@id":"https://doi.org/10.17182/hepdata.156777.v1/t2","@type":"Dataset","description":"Upper limit at the 95% CL on the product of the cross-section for the $pp \\rightarrow tb H^{\\pm}$ process and...","name":"Limit merged category"},{"@id":"https://doi.org/10.17182/hepdata.156777.v1/t3","@type":"Dataset","description":"Product of acceptance and efficiency for pp->tbH(->Wh) as function of the charged Higgs boson mass for the resolved qqbb low-purity...","name":"Signal efficiency resolved Low pur qqbb"},{"@id":"https://doi.org/10.17182/hepdata.156777.v1/t4","@type":"Dataset","description":"Product of acceptance and efficiency for pp->tbH(->Wh) as function of the charged Higgs boson mass for the resolved qqbb signal...","name":"Signal efficiency resolved SR qqbb"},{"@id":"https://doi.org/10.17182/hepdata.156777.v1/t5","@type":"Dataset","description":"Product of acceptance and efficiency for pp->tbH(->Wh) as function of the charged Higgs boson mass for the resolved lvbb signal...","name":"Signal efficiency resolved SR lvbb"},{"@id":"https://doi.org/10.17182/hepdata.156777.v1/t6","@type":"Dataset","description":"Product of acceptance and efficiency for pp->tbH(->Wh) as function of the charged Higgs boson mass for the merged lvbb signal...","name":"Signal efficiency merged lvbb"},{"@id":"https://doi.org/10.17182/hepdata.156777.v1/t7","@type":"Dataset","description":"Product of acceptance and efficiency for pp->tbH(->Wh) as function of the charged Higgs boson mass for the merged qqbb signal...","name":"Signal efficiency merged qqbb"},{"@id":"https://doi.org/10.17182/hepdata.156777.v1/t8","@type":"Dataset","description":"Distributions of the mWh observable in the low-purity signal regions of the resolved qqbb 5jex3bex event categories. 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