{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83009.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1641268"}},{"@id":"https://doi.org/10.1007/JHEP03(2018)095","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"Measurement of the Higgs boson coupling properties in the H-&gt;ZZ*-&gt;4l decay channel at sqrt{s} = 13 TeV with the ATLAS detector","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t1","@type":"Dataset","description":"The expected number of SM Higgs boson events with a mass mH= 125.09 GeV in the mass range 118 &lt;...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t2","@type":"Dataset","description":"The observed and expected numbers of signal and background events in the four-lepton decay channels for an integrated luminosity of...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t3","@type":"Dataset","description":"The expected and observed numbers of signal events in reconstructed event categories for an integrated luminosity of 36.1/fb at sqrt(s)=...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t4","@type":"Dataset","description":"The observed values of Sigma*BR(H-&gt;ZZ*), the SM expected cross section sBRsm and their ratio Sigma*BR/(Sigma*BR)_SM for the inclusive production and...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t5","@type":"Dataset","description":"Signal acceptance obtained as the ratio of the number of simulated signal events satisfying the event selection criteria in each...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t6","@type":"Dataset","description":"Signal acceptance obtained as the ratio of the number of simulated signal events satisfying the event selection criteria in each...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t7","@type":"Dataset","description":"The signal strengths mu for the inclusive production and in each Stage-0 and reduced Stage-1 production bin for an integrated...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t8","@type":"Dataset","description":"Signal acceptance (in percent) obtained as the ratio of the number of simulated signal events satisfying the event selection criteria...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t9","@type":"Dataset","description":"Number of expected ggF Higgs boson events for an integrated luminosity of $\\mathcal L=36.1 \\text{fb}^{-1}$ and at $\\sqrt{\\mathrm{s}}=13$ TeV, as...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t10","@type":"Dataset","description":"Number of expected VBF and VH Higgs boson events for an integrated luminosity of $\\mathcal L=36.1 \\text{fb}^{-1}$ and at $\\sqrt{\\mathrm{s}}=13$...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t11","@type":"Dataset","description":"Expected Correlation Matrix for Stage 0","name":"Stage 0 Expected Correlation Matrix"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t12","@type":"Dataset","description":"Observed Correlation Matrix for Stage 0. As upper limits are derived for ttH and VH POIs using the observed data,...","name":"Stage 0 Observed Correlation Matrix"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t13","@type":"Dataset","description":"Expected Correlation Matrix for Reduced Stage 1","name":"Reduced Stage 1 Expected Correlation Matrix"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t14","@type":"Dataset","description":"Observed Correlation Matrix for Reduced Stage 1. As upper limits are derived for ttH and VH POIs using the observed...","name":"Reduced Stage 1 Observed Correlation Matrix"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t15","@type":"Dataset","description":"Expected Covariance Matrix for Stage 0","name":"Stage 0 Expected Covariance Matrix"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t16","@type":"Dataset","description":"Observed Covariance Matrix for Stage 0. As upper limits are derived for ttH and VH POIs using the observed data,...","name":"Stage 0 Observed Covariance Matrix"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t17","@type":"Dataset","description":"Expected Covariance Matrix for Reduced Stage 1","name":"Reduced Stage 1 Expected Covariance Matrix"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t18","@type":"Dataset","description":"Observed Covariance Matrix for Reduced Stage 1. As upper limits are derived for ttH and VH POIs using the observed...","name":"Reduced Stage 1 Observed Covariance Matrix"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t19","@type":"Dataset","description":"Likelihood contours at 68% CL in the (Sigma_ggF*B , Sigma_VBF*B ) plane","name":"Figure 8a - 68%CLs"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t20","@type":"Dataset","description":"Likelihood contours at 95% CL in the (Sigma_ggF*B , Sigma_VBF*B ) plane","name":"Figure 8a - 95%CLs"},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t21","@type":"Dataset","description":"Expected two-dimensional negative log-likelihood scans for $\\kappa_{HVV}$ versus $\\kappa_{AVV}$ coupling parameters using $\\mathcal L=36.1 \\text{fb}^{-1}$ of data and at $\\sqrt{\\mathrm{s}}=13$...","name":"Figure 10a - Expected 95%CLs "},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t22","@type":"Dataset","description":"Observed two-dimensional negative log-likelihood scans for $\\kappa_{HVV}$ versus $\\kappa_{AVV}$ coupling parameters using $\\mathcal L=36.1 \\text{fb}^{-1}$ of data and at $\\sqrt{\\mathrm{s}}=13$...","name":"Figure 10a - Observed 95%CLs "},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t23","@type":"Dataset","description":"Expected two-dimensional negative log-likelihood scans for $\\kappa_{HVV}$ versus $\\kappa_{AVV}$ coupling parameters using $\\mathcal L=36.1 \\text{fb}^{-1}$ of data and at $\\sqrt{\\mathrm{s}}=13$...","name":"Figure 10b - Expected 95%CLs "},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t24","@type":"Dataset","description":"Observed two-dimensional negative log-likelihood scans for $\\kappa_{HVV}$ versus $\\kappa_{AVV}$ coupling parameters using $\\mathcal L=36.1 \\text{fb}^{-1}$ of data and at $\\sqrt{\\mathrm{s}}=13$...","name":"Figure 10b - Observed 95%CLs "},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t25","@type":"Dataset","description":"Expected two-dimensional negative log-likelihood scans for $\\kappa_{HVV}$ versus $\\kappa_{SM}$ coupling parameters using $\\mathcal L=36.1 \\text{fb}^{-1}$ of data and at $\\sqrt{\\mathrm{s}}=13$...","name":"Figure 21a - Expected 95%CLs "},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t26","@type":"Dataset","description":"Observed two-dimensional negative log-likelihood scans for $\\kappa_{HVV}$ versus $\\kappa_{SM}$ coupling parameters using $\\mathcal L=36.1 \\text{fb}^{-1}$ of data and at $\\sqrt{\\mathrm{s}}=13$...","name":"Figure 21a - Observed 95%CLs "},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t27","@type":"Dataset","description":"Expected two-dimensional negative log-likelihood scans for $\\kappa_{AVV}$ versus $\\kappa_{SM}$ coupling parameters using $\\mathcal L=36.1 \\text{fb}^{-1}$ of data and at $\\sqrt{\\mathrm{s}}=13$...","name":"Figure 21b - Expected 95%CLs "},{"@id":"https://doi.org/10.17182/hepdata.83009.v1/t28","@type":"Dataset","description":"Observed two-dimensional negative log-likelihood scans for $\\kappa_{AVV}$ versus $\\kappa_{SM}$ coupling parameters using $\\mathcal L=36.1 \\text{fb}^{-1}$ of data and at $\\sqrt{\\mathrm{s}}=13$...","name":"Figure 21b - Observed 95%CLs "}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1641268?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/83009"}],"inLanguage":"en","name":"Measurement of the Higgs boson coupling properties in the $H\\rightarrow ZZ^{*} \\rightarrow 4\\ell$ decay channel at $\\sqrt{s}$ = 13 TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1641268?version=1","version":1}
