{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.140529.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2664553"}},{"@id":"https://doi.org/10.1016/j.scib.2024.06.003","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"Results from a wide range of searches targeting different experimental signatures with and without missing transverse momentum ($E_{\\mathrm{T}}^{\\mathrm{miss}}$) are used to constrain a Two-Higgs-Doublet Model (2HDM) with an additional pseudo-scalar mediating the interaction between ordinary and dark matter (2HDM+$a$). The analyses use up to 139 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy $\\sqrt{s}=13$ TeV recorded with the ATLAS detector at the Large Hadron Collider during 2015-2018. The results from three of the most sensitive searches are combined statistically. These searches target signatures with large $E_{\\mathrm{T}}^{\\mathrm{miss}}$ and a leptonically decaying $Z$ boson; large $E_{\\mathrm{T}}^{\\mathrm{miss}}$ and a Higgs boson decaying to bottom quarks; and production of charged Higgs bosons in final states with top and bottom quarks, respectively. Constraints are derived for several common and new benchmark scenarios in the 2HDM+$a$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t1","@type":"Dataset","description":"Observed combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\\theta$ = 0.35.","name":"Figure 4a (Observed)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t2","@type":"Dataset","description":"Expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\\theta$ = 0.35.","name":"Figure 4a (Expected)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t3","@type":"Dataset","description":"1 sigma band of expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\\theta$ =...","name":"Figure 4a (Expected 1 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t4","@type":"Dataset","description":"2 sigma band of expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\\theta$ =...","name":"Figure 4a (Expected 2 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t5","@type":"Dataset","description":"Observed combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\\theta$ = 0.7.","name":"Figure 4b (Observed)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t6","@type":"Dataset","description":"Expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\\theta$ = 0.7.","name":"Figure 4b (Expected)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t7","@type":"Dataset","description":"1 sigma band of expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\\theta$ =...","name":"Figure 4b (Expected 1 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t8","@type":"Dataset","description":"2 sigma band of expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\\theta$ =...","name":"Figure 4b (Expected 2 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t9","@type":"Dataset","description":"Observed limits of H(inv) at 95% CL in the $(m_{a},m_{\\chi})$ plane under the assumption of $m_{A}$ = 1.2 TeV, $tan\\beta$...","name":"Figure 9 (H(inv) Observed limits)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t10","@type":"Dataset","description":"Expected limits of H(inv) at 95% CL in the $(m_{a},m_{\\chi})$ plane under the assumption of $m_{A}$ = 1.2 TeV, $tan\\beta$...","name":"Figure 9 (H(inv) Expected limits)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t11","@type":"Dataset","description":"Observed limits of monoh(bb) at 95% CL in the $(m_{a},m_{\\chi})$ plane under the assumption of $m_{A}$ = 1.2 TeV, $tan\\beta$...","name":"Figure 9 (monoh(bb) Observed limits)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t12","@type":"Dataset","description":"Expected limits of monoh(bb) at 95% CL in the $(m_{a},m_{\\chi})$ plane under the assumption of $m_{A}$ = 1.2 TeV, $tan\\beta$...","name":"Figure 9 (monoh(bb) Expected limits)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t13","@type":"Dataset","description":"Observed limits of $h\\to aa \\to \\mu\\mu\\tau\\tau$ at 95% CL in the $(m_{a},m_{\\chi})$ plane under the assumption of $m_{A}$ =...","name":"Figure 9 (mumutautau channel, Observed limits)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t14","@type":"Dataset","description":"Observed limits of $h\\to aa \\to bbbb$ at 95% CL in the $(m_{a},m_{\\chi})$ plane under the assumption of $m_{A}$ =...","name":"Figure 9 (4 b channel, Observed limits)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t15","@type":"Dataset","description":"Observed limits of $h\\to aa \\to bb\\mu\\mu$ at 95% CL in the $(m_{a},m_{\\chi})$ plane under the assumption of $m_{A}$ =...","name":"Figure 9 (bbmumu channel, Observed limits)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t16","@type":"Dataset","description":"Observed limits of $h\\to aa \\to 4 \\mu$ at 95% CL in the $(m_{a},m_{\\chi})$ plane under the assumption of $m_{A}$...","name":"Figure 9 (4 mu channel, 2015-2016, Observed limits)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t17","@type":"Dataset","description":"Observed limits of $h\\to aa \\to 4 \\mu$ at 95% CL in the $(m_{a},m_{\\chi})$ plane under the assumption of $m_{A}$...","name":"Figure 9 (4 mu channel, 2015-2018, Observed limits, 1st part)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t18","@type":"Dataset","description":"Observed limits of $h\\to aa \\to 4 \\mu$ at 95% CL in the $(m_{a},m_{\\chi})$ plane under the assumption of $m_{A}$...","name":"Figure 9 (4 mu channel, 2015-2018, Observed limits, 2nd part)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t19","@type":"Dataset","description":"Observed combination limits at 95% CL in the $(m_{A},tan\\beta)$ plane under the assumption of $sin\\theta$ = 0.35.","name":"Auxiliary Figure 3a (Observed)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t20","@type":"Dataset","description":"Expected combination limits at 95% CL in the $(m_{A},tan\\beta)$ plane under the assumption of $sin\\theta$ = 0.35.","name":"Auxiliary Figure 3a (Expected)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t21","@type":"Dataset","description":"1 sigma band of expected combination limits at 95% CL in the $(m_{A},tan\\beta)$ plane under the assumption of $sin\\theta$ =...","name":"Auxiliary Figure 3a (Expected 1 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t22","@type":"Dataset","description":"2 sigma band of expected combination limits at 95% CL in the $(m_{A},tan\\beta)$ plane under the assumption of $sin\\theta$ =...","name":"Auxiliary Figure 3a (Expected 2 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t23","@type":"Dataset","description":"Observed combination limits at 95% CL in the $(m_{A},tan\\beta)$ plane under the assumption of $sin\\theta$ = 0.7.","name":"Auxiliary Figure 3b (Observed)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t24","@type":"Dataset","description":"Expected combination limits at 95% CL in the $(m_{A},tan\\beta)$ plane under the assumption of $sin\\theta$ = 0.7.","name":"Auxiliary Figure 3b (Expected)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t25","@type":"Dataset","description":"1 sigma band of expected combination limits at 95% CL in the $(m_{A},tan\\beta)$ plane under the assumption of $sin\\theta$ =...","name":"Auxiliary Figure 3b (Expected 1 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t26","@type":"Dataset","description":"2 sigma band of expected combination limits at 95% CL in the $(m_{A},tan\\beta)$ plane under the assumption of $sin\\theta$ =...","name":"Auxiliary Figure 3b (Expected 2 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t27","@type":"Dataset","description":"Observed combination limits at 95% CL in the $(m_{a},tan\\beta)$ plane under the assumption of $sin\\theta$ = 0.35.","name":"Auxiliary Figure 4a (Observed)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t28","@type":"Dataset","description":"Expected combination limits at 95% CL in the $(m_{a},tan\\beta)$ plane under the assumption of $sin\\theta$ = 0.35.","name":"Auxiliary Figure 4a (Expected)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t29","@type":"Dataset","description":"1 sigma band of expected combination limits at 95% CL in the $(m_{a},tan\\beta)$ plane under the assumption of $sin\\theta$ =...","name":"Auxiliary Figure 4a (Expected 1 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t30","@type":"Dataset","description":"2 sigma band of expected combination limits at 95% CL in the $(m_{a},tan\\beta)$ plane under the assumption of $sin\\theta$ =...","name":"Auxiliary Figure 4a (Expected 2 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t31","@type":"Dataset","description":"Observed combination limits at 95% CL in the $(m_{a},tan\\beta)$ plane under the assumption of $sin\\theta$ = 0.7.","name":"Auxiliary Figure 4b (Observed)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t32","@type":"Dataset","description":"Expected combination limits at 95% CL in the $(m_{a},tan\\beta)$ plane under the assumption of $sin\\theta$ = 0.7.","name":"Auxiliary Figure 4b (Expected)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t33","@type":"Dataset","description":"1 sigma band of expected combination limits at 95% CL in the $(m_{a},tan\\beta)$ plane under the assumption of $sin\\theta$ =...","name":"Auxiliary Figure 4b (Expected 1 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t34","@type":"Dataset","description":"2 sigma band of expected combination limits at 95% CL in the $(m_{a},tan\\beta)$ plane under the assumption of $sin\\theta$ =...","name":"Auxiliary Figure 4b (Expected 2 sigma band)"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t35","@type":"Dataset","description":"Observed and expected combination limits at 95% CL as a function of $sin\\theta$ for the low-mass hypothesis $m_{A}$ = 0.6...","name":"Auxiliary Figure 5a"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t36","@type":"Dataset","description":"Observed and expected combination limits at 95% CL as a function of $sin\\theta$ for the high-mass hypothesis $m_{A}$ = 1...","name":"Auxiliary Figure 5b"},{"@id":"https://doi.org/10.17182/hepdata.140529.v1/t37","@type":"Dataset","description":"Observed and expected combination limits at 95% CL as a function of $m_{\\chi}$ following the parameter choices of $m_{A}$ =...","name":"Auxiliary Figure 6"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2664553?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/140529"}],"inLanguage":"en","name":"Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb$^{-1}$ of $\\sqrt{s} = 13$ TeV $pp$ collision data","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2664553?version=1","version":1}
