{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.70527.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1362177"}},{"@id":"https://doi.org/10.1016/j.physletb.2015.07.010","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2016","description":"CERN-LHC.  Results are reported on a search for decays of a pseudoscalar A boson into a Z boson and a light scalar h boson, where the Z boson decays into a pair of oppositely-charged electrons or muons, and the h boson decays into b anti-b. The search is based on data from proton-proton collisions at a center-of-mass energy sqrt(s)=8 TeV collected with the CMS detector, corresponding to an integrated luminosity of 19.7 inverse femtobarns. The h boson is assumed to be the recently discovered standard model-like Higgs boson with a mass of 125 GeV. With no evidence for signal, upper limits are obtained on the product of the production cross section and the branching fraction of the A boson in the Zh channel. Results are also interpreted in the context of two Higgs doublet models.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t1","@type":"Dataset","description":"Observed and expected 95% CL upper limits on sigma A x B(A->Zh->llbb) as a function of mA in the narrow-width...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t2","@type":"Dataset","description":"Observed 95% CL upper limits on sigma A x B(A->Zh->llbb) as a function of mA and the A natural width...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t3","@type":"Dataset","description":"Expected 95% CL upper limits on sigma A x B(A->Zh->llbb) as a function of mA and the A natural width...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t4","@type":"Dataset","description":"Signal selection efficiency as a function of mA.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t5","@type":"Dataset","description":"Expected +2 sigma uncertainty band exclusion limit for Type-I models, as a function of tan beta and cos(beta-alpha).","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t6","@type":"Dataset","description":"Expected +1 sigma uncertainty band exclusion limit for Type-I models, as a function of tan beta and cos(beta-alpha).","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t7","@type":"Dataset","description":"Expected exclusion limit for Type-I models, as a function of tan beta and cos(beta-alpha).","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t8","@type":"Dataset","description":"Expected -1 sigma uncertainty band exclusion limit for Type-I models, as a function of tan beta and cos(beta-alpha).","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t9","@type":"Dataset","description":"Expected -2 sigma uncertainty band exclusion limit for Type-I models, as a function of tan beta and cos(beta-alpha).","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t10","@type":"Dataset","description":"Observed exclusion limit for Type-I models, as a function of tan beta and cos(beta-alpha).","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t11","@type":"Dataset","description":"Expected +2 sigma uncertainty band exclusion limit for Type-II models, as a function of tan beta and cos(beta-alpha).","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t12","@type":"Dataset","description":"Expected +1 sigma uncertainty band exclusion limit for Type-II models, as a function of tan beta and cos(beta-alpha).","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t13","@type":"Dataset","description":"Expected exclusion limit for Type-II models, as a function of tan beta and cos(beta-alpha).","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t14","@type":"Dataset","description":"Expected -1 sigma uncertainty band exclusion limit for Type-II models, as a function of tan beta and cos(beta-alpha).","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t15","@type":"Dataset","description":"Expected -2 sigma uncertainty band exclusion limit for Type-II models, as a function of tan beta and cos(beta-alpha).","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.70527.v1/t16","@type":"Dataset","description":"Observed exclusion limit for Type-II models, as a function of tan beta and cos(beta-alpha).","name":"Table 16"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1362177?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/70527"}],"inLanguage":"en","name":"Search for a pseudoscalar boson decaying into a Z boson and the 125 GeV Higgs boson in llbb final states","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1362177?version=1","version":1}