{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.81626.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1654357"}},{"@id":"https://doi.org/10.1103/PhysRevD.97.092006","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"A search is presented for photonic signatures, motivated by generalized models of gauge-mediated supersymmetry breaking. This search makes use of proton-proton collision data at $\\sqrt{s}$ = 13 TeV corresponding to an integrated luminosity of 36.1 fb$^{\u22121}$ recorded by the ATLAS detector at the LHC, and explores models dominated by both strong and electroweak production of supersymmetric partner states. Experimental signatures incorporating an isolated photon and significant missing transverse momentum are explored. These signatures include events with an additional photon or additional jet activity not associated with any specific underlying quark flavor. No significant excess of events is observed above the Standard Model prediction, and 95% confidence-level upper limits of between 0.083 fb and 0.32 fb are set on the visible cross section of contributions from physics beyond the Standard Model. These results are interpreted in terms of lower limits on the masses of gluinos, squarks, and gauginos in the context of generalized models of gauge-mediated supersymmetry, which reach as high as 2.3 TeV for strongly produced and 1.3 TeV for weakly produced supersymmetric partner pairs.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t1","@type":"Dataset","description":"Distribution of the total visible transverse energy $H_{\\mathrm{T}}$ for selected diphoton events, after requiring $\\Delta\\phi_{\\mathrm{min}} (\\mathrm{jet}, E_{\\mathrm{T}}^{\\mathrm{miss}}) > 0.5$ but...","name":"Distribution 1"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t2","@type":"Dataset","description":"Distribution of $R_{\\mathrm{T}}^{4}$ for the sample satisfying all $\\mathrm{SR}^{\\gamma j}_{L}$ selection criteria except the $R_{\\mathrm{T}}^{4}$ requirement itself, but with a...","name":"Distribution 2"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t3","@type":"Dataset","description":"Comparisons between expected and observed content of the validation and signal regions for the diphoton analysis. The uncertainties in the...","name":"Distribution 3"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t4","@type":"Dataset","description":"Distribution of the missing transverse momentum $E_{\\mathrm{T}}^{\\mathrm{miss}}$ for the sample satisfying all requirements of the $\\mathrm{SR}^{\\gamma\\gamma}_{W-L}$ selection except the $E_{\\mathrm{T}}^{\\mathrm{miss}}$...","name":"Distribution 4"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t5","@type":"Dataset","description":"Distribution of the missing transverse momentum $E_{\\mathrm{T}}^{\\mathrm{miss}}$ for the sample satisfying all requirements of the $\\mathrm{SR}^{\\gamma\\gamma}_{W-H}$ selection except the $E_{\\mathrm{T}}^{\\mathrm{miss}}$...","name":"Distribution 5"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t6","@type":"Dataset","description":"Comparisons between expected and observed content of the validation and signal regions for the photon+jets analysis. The uncertainties in the...","name":"Distribution 6"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t7","@type":"Dataset","description":"Distribution of the missing transverse momentum $E_{\\mathrm{T}}^{\\mathrm{miss}}$ for the sample satisfying all requirements of the $\\mathrm{SR}^{\\gamma j}_{H}$ selection except the...","name":"Distribution 7"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t8","@type":"Dataset","description":"Distribution of the missing transverse momentum $E_{\\mathrm{T}}^{\\mathrm{miss}}$ for the sample satisfying all requirements of the $\\mathrm{SR}^{\\gamma j}_{L}$ or $\\mathrm{SR}^{\\gamma j}_{L200}$...","name":"Distribution 8"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t9","@type":"Dataset","description":"Expected exclusion limits in the gluino-bino mass plane, using the $\\mathrm{SR}^{\\gamma\\gamma}_{S-H}$ analysis for $m_{\\tilde{\\chi}^{0}_{1}} > 1600$ GeV and the $\\mathrm{SR}^{\\gamma\\gamma}_{S-L}$...","name":"Exclusion contour (expected) 1"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t10","@type":"Dataset","description":"Observed exclusion limits in the gluino--bino mass plane, using the $\\mathrm{SR}^{\\gamma\\gamma}_{S-H}$ analysis for $m_{\\tilde{\\chi}^{0}_{1}} > 1600$ GeV and the $\\mathrm{SR}^{\\gamma\\gamma}_{S-L}$...","name":"Exclusion contour (observed) 2"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t11","@type":"Dataset","description":"Expected exclusion limit in the squark-bino mass plane, using the $\\mathrm{SR}^{\\gamma\\gamma}_{S-H}$ analysis for $m_{\\tilde{\\chi}^{0}_{1}} > 900$ GeV and the $\\mathrm{SR}^{\\gamma\\gamma}_{S-L}$...","name":"Exclusion contour (expected) 3"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t12","@type":"Dataset","description":"Observed exclusion limit in the squark--bino mass plane, using the $\\mathrm{SR}^{\\gamma\\gamma}_{S-H}$ analysis for $m_{\\tilde{\\chi}^{0}_{1}} > 900$ GeV and the $\\mathrm{SR}^{\\gamma\\gamma}_{S-L}$...","name":"Exclusion contour (observed) 4"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t13","@type":"Dataset","description":"Expected exclusion limit in the wino-bino mass plane, using the $\\mathrm{SR}^{\\gamma\\gamma}_{W-H}$ analysis for $m_{\\tilde{\\chi}^{0}_{1}} > 400$ GeV and the $\\mathrm{SR}^{\\gamma\\gamma}_{W-L}$...","name":"Exclusion contour (expected) 5"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t14","@type":"Dataset","description":"Observed exclusion limit in the wino-bino mass plane, using the $\\mathrm{SR}^{\\gamma\\gamma}_{W-H}$ analysis for $m_{\\tilde{\\chi}^{0}_{1}} > 400$ GeV and the $\\mathrm{SR}^{\\gamma\\gamma}_{W-L}$...","name":"Exclusion contour (observed) 6"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t15","@type":"Dataset","description":"Expected exclusion limits for the $\\mu > 0$ higgsino-bino GGM model explored by the photon+jets analysis.","name":"Exclusion contour (expected) 7"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t16","@type":"Dataset","description":"Observed exclusion limits for the $\\mu > 0$ higgsino-bino GGM model explored by the photon+jets analysis.","name":"Exclusion contour (observed) 8"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t17","@type":"Dataset","description":"Distribution of the transverse momentum $p_{\\mathrm{T}} (\\ell\\gamma\\gamma)$ of events in the $\\ell\\gamma\\gamma$ control region (except without a cut on $p_{\\mathrm{T}}...","name":"Distribution 9"},{"@id":"https://doi.org/10.17182/hepdata.81626.v1/t18","@type":"Dataset","description":"Distribution of $E_{\\mathrm{T}}^{\\mathrm{miss}}$ for diphoton events in a validation region defined by a requirement of $H_{\\mathrm{T}} > 1750$ GeV. 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