{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.145687.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2745376"}},{"@id":"https://doi.org/10.1007/JHEP10(2024)130","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2024","description":"A search for a new heavy boson produced via gluon-fusion in the four-lepton channel with missing transverse momentum or jets is performed. The search uses proton-proton collision data equivalent to an integrated luminosity of 139 fb$^{-1}$ at a centre-of-mass energy of 13 TeV collected by the ATLAS detector between 2015 and 2018 at the Large Hadron Collider. This study explores the decays of heavy bosons: $R\\to SH$ and $A\\to ZH$, where $R$ is a CP-even, $A$ is a CP-odd boson, $H$ is a CP-even boson, and $S$ is considered to decay into invisible particles that are candidates for dark matter. In these processes, $S\\to \\text{invisible}$ and $H\\to ZZ$. The $Z$ boson associated with the heavy scalar boson $H$ decays into all decay channels of the $Z$ boson. The mass range under consideration is 390-1300 (320-1300) GeV for the $R$ ($A$) boson and 220-1000 GeV for the $H$ boson. No significant deviation from the Standard Model backgrounds is observed. The results are interpreted as upper limits at a 95% confidence level on the cross-section times the branching ratio of the heavy resonances.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t1","@type":"Dataset","description":"Observed and expected distributions of the invariant mass of the four-lepton system in the $R\\to SH\\to 4\\ell+E^{\\textrm{miss}}_{\\textrm{T}}$ search for SR1...","name":"Post-fit $m_{4\\ell}$ in SR1 for $R\\to SH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t2","@type":"Dataset","description":"Observed and expected distributions of the invariant mass of the four-lepton system in the $R\\to SH\\to 4\\ell+E^{\\textrm{miss}}_{\\textrm{T}}$ search for SR2...","name":"Post-fit $m_{4\\ell}$ in SR2 for $R\\to SH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t3","@type":"Dataset","description":"Observed and expected distributions of the invariant mass of the four-lepton system in the $R\\to SH\\to 4\\ell+E^{\\textrm{miss}}_{\\textrm{T}}$ search for SR3...","name":"Post-fit $m_{4\\ell}$ in SR3 for $R\\to SH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t4","@type":"Dataset","description":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR1...","name":"Post-fit $m_{4\\ell}$ in SR1 for $A\\to ZH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t5","@type":"Dataset","description":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR2...","name":"Post-fit $m_{4\\ell}$ in SR2 for $A\\to ZH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t6","@type":"Dataset","description":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR3...","name":"Post-fit $m_{4\\ell}$ in SR3 for $A\\to ZH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t7","@type":"Dataset","description":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR4...","name":"Post-fit $m_{4\\ell}$ in SR4 for $A\\to ZH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t8","@type":"Dataset","description":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR5...","name":"Post-fit $m_{4\\ell}$ in SR5 for $A\\to ZH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t9","@type":"Dataset","description":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR6...","name":"Post-fit $m_{4\\ell}$ in SR6 for $A\\to ZH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t10","@type":"Dataset","description":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR7...","name":"Post-fit $m_{4\\ell}$ in SR7 for $A\\to ZH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t11","@type":"Dataset","description":"Local p0-values in the $(m_{H}, m_{R})$ plane for the $R\\to SH\\to 4\\ell+E^{\\textrm{miss}}_{\\textrm{T}}$ search with $m_{S} = 160$ GeV.","name":"Observed local $p_{0}$-value for the $R\\to SH$ search"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t12","@type":"Dataset","description":"Local p0-values in the $(m_{H}, m_{A})$ plane for the $A\\to ZH\\to 4\\ell+X$ search.","name":"Observed local $p_{0}$-value the $A\\to ZH$ search"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t13","@type":"Dataset","description":"The observed upper limits at 95% confidence level on $\\sigma(gg\\to R)\\times \\mathcal{B}(R\\to SH)\\times (H\\to ZZ)$ across the $(m_{H}, m_{R})$ plane...","name":"Observed upper limit on the cross-section for the $R$ production"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t14","@type":"Dataset","description":"The expected upper limits at 95% confidence level on $\\sigma(gg\\to R)\\times \\mathcal{B}(R\\to SH)\\times (H\\to ZZ)$ across the $(m_{H}, m_{R})$ plane...","name":"Expected upper limit on the cross-section for the $R$ production"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t15","@type":"Dataset","description":"The observed upper limits at 95% confidence level on $\\sigma(gg\\to A)\\times \\mathcal{B}(A\\to ZH)\\times (H\\to ZZ)$ across the $(m_{H}, m_{A})$ plane...","name":"Observed upper limit on the cross-section for the $A$ production"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t16","@type":"Dataset","description":"The expected upper limits at 95% confidence level on $\\sigma(gg\\to A)\\times \\mathcal{B}(A\\to ZH)\\times (H\\to ZZ)$ across the $(m_{H}, m_{A})$ plane...","name":"Expected upper limit on the cross-section for $A$ production"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t17","@type":"Dataset","description":"Cut-flow of the raw events at each selection stage for the $R\\rightarrow SH\\rightarrow 4\\ell + E^{\\textrm{miss}}_{\\textrm{T}}$ signal with a mass...","name":"Cut-flow table for the $R\\to SH$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t18","@type":"Dataset","description":"Cut-flow of the raw events at each selection stage for the $A\\rightarrow Z(\\rightarrow jj/\\ell^+\\ell^-/\\textrm{invisible})H(\\rightarrow 4\\ell)$ signal with a mass point...","name":"Cut-flow for the $A\\to Z(jj/2\\ell/\\rm invisible)H(4\\ell)$ signal"},{"@id":"https://doi.org/10.17182/hepdata.145687.v1/t19","@type":"Dataset","description":"Cut-flow of the raw events at each selection stage for the $A\\rightarrow Z(\\rightarrow 2\\ell)H(\\rightarrow 2\\ell+jj/\\textrm{invisible})$ signal with a mass point...","name":"Cut-flow for the $A\\to Z(2\\ell)H(2\\ell/jj/\\rm invisible)$ signal"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2745376?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/145687"}],"inLanguage":"en","name":"Search for heavy resonances in final states with four leptons and missing transverse momentum or jets in $pp$ collisions 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/ins2745376?version=1","version":1}