{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.85740.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1693614"}},{"@id":"https://doi.org/10.1140/epjc/s10052-018-6390-z","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t1","@type":"Dataset","description":"The $\\mathrm{J}/\\psi\\mathrm{K}^+$ invariant mass distribution in data","name":"Table 1: Data from Figure 1 (a)"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t2","@type":"Dataset","description":"The $\\mathrm{J}/\\psi\\mathrm{K}^{*0}$ invariant mass distribution in data","name":"Table 2: Data from Figure 1 (b)"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t3","@type":"Dataset","description":"The $\\mathrm{B}^+\\pi^-$ invariant mass distribution of the selected candidates in data","name":"Table 3:  Data from Figure 2 (b)"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t4","@type":"Dataset","description":"Invariant mass distribution of the selected $\\mathrm{B}^+\\mathrm{K}^-$ candidates in data","name":"Table 4:  Data from Figure 3 (a)"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t5","@type":"Dataset","description":"Invariant mass distribution of the selected $\\mathrm{B}^0 \\mathrm{K}^{0}_{\\mathrm{S}}$ candidates in data","name":"Table 5: Data from Figure 3 (b)"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t6","@type":"Dataset","description":"The observed signal yields ($N$), natural widths ($\\Gamma$), and mass differences from the fits to the $m_{\\mathrm{BK}}$ distributions in data,...","name":"Table 6: Data from Table 2 of the publication"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t7","@type":"Dataset","description":"The measured ratios of branching fractions","name":"Table 7: Results for the braching fraction ratios"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t8","@type":"Dataset","description":"The measured ratios of cross sections times branching fractions","name":"Table 8: Mesured cross sections times braching fraction ratios"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t9","@type":"Dataset","description":"The measured mass differences $M(\\mathrm{B}^{(*)0}_{\\mathrm{s1,2}})-M^{\\mathrm{PDG}}_{\\mathrm{B}}-M^{\\mathrm{PDG}}_{\\mathrm{K}}$","name":"Table 9: Results for the mass differences"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t10","@type":"Dataset","description":"The measured masses of $\\mathrm{B}^{*}_{\\mathrm{s2}}(5840)^0$ and $\\mathrm{B}_{\\mathrm{s1}}(5830)^0$ mesons","name":"Table 10: Results for the masses of P-wave B0s mesons"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t11","@type":"Dataset","description":"The measured mass differences between neutral and charged B mesons","name":"Table 11: Results for the mass differences"},{"@id":"https://doi.org/10.17182/hepdata.85740.v1/t12","@type":"Dataset","description":"The measured $\\mathrm{B}^{*}_{\\mathrm{s2}}(5840)^0$ natural width","name":"Table 12: Result for the Bs*2(5840)0 natural width"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1693614?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/85740"}],"inLanguage":"en","name":"Studies of B$^*_\\mathrm{s2}(5840)^0$ and B$_\\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\\mathrm{s2}(5840)^0\\to$ B$^0$K$_\\mathrm{S}^0$ decay in proton-proton collisions at $\\sqrt{s}=$8 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1693614?version=1","version":1}
