{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.77382.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1591328"}},{"@id":"https://doi.org/10.1140/epjc/s10052-017-4965-8","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"CERN-LHC. Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, exclusion limits in models where dark-matter candidates are pair-produced are determined. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750-1200 GeV for dark-matter candidate masses below 230-480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale $M_{*}$ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to $Z\\gamma$ and the $Z$ boson subsequently decays into neutrinos.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t1","@type":"Dataset","description":"Observed event yields in 36.1 fb$^{-1}$ of data compared to expected yields from SM backgrounds in all signal regions, as...","name":"Table 0"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t2","@type":"Dataset","description":"The observed 95% CL exclusion contour for a simplified model of dark-matter production involving an axial-vector operator, Dirac DM and...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t3","@type":"Dataset","description":"The expected 95% CL exclusion contour (+1$\\sigma$) for a simplified model of dark-matter production involving an axial-vector operator, Dirac DM...","name":"Table 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couplings...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t12","@type":"Dataset","description":"The expected 95% CL exclusion contour ($-1\\sigma$) for a simplified model of dark-matter production involving a vector operator with couplings...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t13","@type":"Dataset","description":"The expected 95% CL exclusion contour for a simplified model of dark-matter production involving a vector operator with couplings $g_{q}$...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t14","@type":"Dataset","description":"The observed 95% CL exclusion contour for a simplified model of dark-matter production involving for a vector operator with couplings...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t15","@type":"Dataset","description":"The expected 95% CL exclusion contour ($+1\\sigma$) for a simplified model of dark-matter production involving for a vector operator with...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t16","@type":"Dataset","description":"The expected 95% CL exclusion contour ($-1\\sigma$) for a simplified model of dark-matter production involving for a vector operator with...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t17","@type":"Dataset","description":"The expected 95% CL exclusion contour for a simplified model of dark-matter production involving for a vector operator with couplings...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t18","@type":"Dataset","description":"The 90% CL exclusion limit on the $\\chi$-proton scattering cross section in a simplifed model of dark-matter production involving an...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t19","@type":"Dataset","description":"The 90% CL exclusion limit on the $\\chi$-nucleon scattering cross section in a simplifed model of dark-matter production involving a...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t20","@type":"Dataset","description":"The observed and expected 95% CL limits on M* for a dimension-7 operator EFT model with a contact interaction of...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t21","@type":"Dataset","description":"The observed and expected limit at 95% CL on the production cross section of a $Z\\gamma$ resonance as a function...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t22","@type":"Dataset","description":"The observed 95% CL upper limits on signal strength $\\mu$, the ratio of the experimental limit to the predicted signal...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.77382.v1/t23","@type":"Dataset","description":"Acceptance, in %, for a simplified model of dark matter production involving an axial-vector operator, Dirac DM and couplings $g_{q}$=...","name":"Table 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