{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.94311.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1790250"}},{"@id":"https://doi.org/10.1140/epjc/s10052-020-8227-9","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2020","description":"Higgs boson properties are studied in the four-lepton decay channel (where lepton = $e$, $\\mu$) using 139 fb$^{-1}$ of proton--proton collision data recorded at $\\sqrt{s}$=13 TeV by the ATLAS experiment at the Large Hadron Collider.  The inclusive cross-section times branching ratio for $H\\to ZZ^*$ decay is measured to be $1.34 \\pm 0.12$ pb for a Higgs boson with absolute rapidity below 2.5, in good agreement with the Standard Model prediction of $1.33 \\pm 0.08$ pb. Cross-sections times branching ratio are measured for the main Higgs boson production modes in several exclusive phase-space regions. The measurements are interpreted in terms of coupling modifiers and of the tensor structure of Higgs boson interactions using an effective field theory approach. Exclusion limits are set on the CP-even and CP-odd 'beyond the Standard Model' couplings of the Higgs boson to vector bosons, gluons and top quarks.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t1","@type":"Dataset","description":"The expected number of SM Higgs boson events with a mass $m_{H}$= 125 GeV for an integrated luminosity of 139...","name":"Table 04 - Yields Higgs Production Mode "},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t2","@type":"Dataset","description":"The impact of the dominant systematic uncertainties (in percent) on the cross-sections in production bins of the Production Mode Stage...","name":"Table 06 - Uncertainties"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t3","@type":"Dataset","description":"The expected and the observed (post-fit) the four-lepton invariant mass distribution for the selected Higgs boson candidates, shown for an...","name":"Figure 05 - Distribution $m_{4l}$"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t4","@type":"Dataset","description":"The expected (pre-fit) and observed numbers of events for an integrated luminosity of 139 fb$^{-1}$ at $\\sqrt{s}$=13 TeV in the...","name":"Table 07 - Yields Results "},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t5","@type":"Dataset","description":"The expected and the observed (post-fit) the jet multiplicity distribution after the inclusive event selection for an integrated luminosity of...","name":"Figure 06a - Distribution $N_{jets}$"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t6","@type":"Dataset","description":"The expected and the observed (post-fit) the four-lepton transverse momentum distribution for events with zero jets, after the inclusive event...","name":"Figure 06b - Distribution $p_{T}^{4l}$ with $N_{jets}$=0"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t7","@type":"Dataset","description":"The expected and the observed (post-fit) the four-lepton transverse momentum distribution for events with one jet, after the inclusive event...","name":"Figure 06c - Distribution $p_{T}^{4l}$ with $N_{jets}$=1"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t8","@type":"Dataset","description":"The expected and the observed (post-fit) the four-lepton transverse momentum distribution for events with at least two jets, after the...","name":"Figure 06d - 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Distribution $NN_{VBF}$ in 1$j$-$p_{T}^{4l}$-Low"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t13","@type":"Dataset","description":"The expected and the observed $NN_{ZZ}$ output (post-fit) distribution in 1$j$-$p_{T}^{4l}$-Low category with $NN_{ZZ}$&gt;0.25 for an integrated luminosity of 139fb$^{-1}$...","name":"Figure 07d - Distribution $NN_{ZZ}$ in 1$j$-$p_{T}^{4l}$-Low"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t14","@type":"Dataset","description":"The expected and the observed $NN_{VBF}$ output (post-fit) distribution in 1$j$-$p_{T}^{4l}$-Med category with $NN_{ZZ}$&lt;0.25 for an integrated luminosity of 139fb$^{-1}$...","name":"Figure 07e - Distribution $NN_{VBF}$ in 1$j$-$p_{T}^{4l}$-Med"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t15","@type":"Dataset","description":"The expected and the observed $NN_{ZZ}$ output (post-fit) distribution in 1$j$-$p_{T}^{4l}$-Med category with $NN_{ZZ}$&gt;0.25 for an integrated luminosity of 139fb$^{-1}$...","name":"Figure 07f - 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Distribution $NN_{VBF}$ in 2$j$-BSM"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t20","@type":"Dataset","description":"The expected and the observed $NN_{ttH}$ output (post-fit) distribution in $ttH$-Had-enriched category with $NN_{tXX}$&lt;0.4 for an integrated luminosity of 139fb$^{-1}$...","name":"Figure 08d - Distribution $NN_{ttH}$ in $ttH$-Had"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t21","@type":"Dataset","description":"The expected and the observed $NN_{tXX}$ output (post-fit) distribution in $ttH$-Had-enriched category with $NN_{tXX}$&gt;0.4 for an integrated luminosity of 139fb$^{-1}$...","name":"Figure 08e - Distribution $NN_{tXX}$ in $ttH$-Had"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t22","@type":"Dataset","description":"The expected and the observed $NN_{ttH}$ output (post-fit) distribution in $VH$-Lep-enriched category for an integrated luminosity of 139fb$^{-1}$ at $\\sqrt{s}$=13TeV....","name":"Figure 08f - Distribution $NN_{ttH}$ in $VH$-Lep"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t23","@type":"Dataset","description":"The expected and the observed events in the categories where no NN discriminant is used for an integrated luminosity of...","name":"Figure 08g - 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The observed best fit value is the first value of the...","name":"Figure 11a - $ggF$vs.$VBF$ 68% CLs"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t29","@type":"Dataset","description":"Likelihood contours at 95% CLs in the (ggF,VBF) plane. The observed best fit value is the first value of the...","name":"Figure 11a - $ggF$vs.$VBF$ 95% CLs"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t30","@type":"Dataset","description":"Likelihood contours at 68% CLs in the (ggF,VH) plane. The observed best fit value is the first value of the...","name":"Figure 11b - $ggF$vs.$VH$ 68% CLs"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t31","@type":"Dataset","description":"Likelihood contours at 95% CLs in the (ggF,VH) plane. The observed best fit value is the first value of the...","name":"Figure 11b - $ggF$vs.$VH$ 95% CLs"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t32","@type":"Dataset","description":"Likelihood contours at 68% CLs in the (VBF,VH) plane. 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The observed best fit value is the first value of the...","name":"Figure 12 - $\\kappa_{V}$vs.$\\kappa_{F}$ 95% CLs"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t38","@type":"Dataset","description":"The expected signal yield ratio for chosen CP-even and CP-odd EFT parameter values together with the corresponding cross-section measurement in...","name":"Figure 15 - Signal yields for EFT parameters"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t39","@type":"Dataset","description":"The expected and observed confidence intervals at 68% and 95% CLs of the SMEFT Wilson coefficients for an integrated luminosity...","name":"Table 09 - SMEFT Wilson CLs"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t40","@type":"Dataset","description":"Expected 2D-fit likelihood curves at the 95% CLs for the $c_{HW}$ versus $c_{HB}$ coupling parameters at an integrated luminosity of...","name":"Figure 17a - $c_{HW}$vs.$c_{HB}$ Exp. 95% CLs"},{"@id":"https://doi.org/10.17182/hepdata.94311.v1/t41","@type":"Dataset","description":"Observed 2D-fit likelihood curves at the 95% CLs for the $c_{HW}$ versus $c_{HB}$ coupling parameters at an integrated luminosity of...","name":"Figure 17a - 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