{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.69300.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1383883"}},{"@id":"https://doi.org/10.1103/PhysRevD.92.072001","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2015","description":"CERN-LHC.  A search is presented for photonic signatures motivated by generalised models of gauge-mediated supersymmetry breaking. This search makes use of $20.3{\\rm fb}^{-1}$ of proton-proton collision data at $\\sqrt{s}=8$ TeV recorded by the ATLAS detector at the LHC, and explores models dominated by both strong and electroweak production of supersymmetric partner states. Four experimental signatures incorporating an isolated photon and significant missing transverse momentum are explored. These signatures include events with an additional photon, lepton, $b$-quark jet, or jet activity not associated with any specific underlying quark flavor. No significant excess of events is observed above the Standard Model prediction and model-dependent 95% confidence-level exclusion limits are set.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t1","@type":"Dataset","description":"Observed and expected exclusion limits in the gluino-bino mass plane, using the $\\rm{SR}^{\\gamma\\gamma}_{S-H}$ analysis for $m_{\\tilde{\\chi}_1^0}\\geq 800 {\\rm GeV}$ and...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t2","@type":"Dataset","description":"Observed and expected exclusion limits in the wino-bino mass plane, using the $\\rm{SR}^{\\gamma\\gamma}_{W-H}$ analysis for $m_{\\tilde{\\chi}_1^0}\\geq 350 {\\rm GeV}$ and...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t3","@type":"Dataset","description":"Observed exclusion limits in the gluino-neutralino mass plane, for the higgsino-bino GGM model with $\\mu < 0$, using the merged...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t4","@type":"Dataset","description":"Expected exclusion limits in the gluino-neutralino mass plane, for the higgsino-bino GGM model with $\\mu < 0$, using the merged...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t5","@type":"Dataset","description":"Observed exclusion limits in the $M_3$-$\\mu$ plane, for the higgsino-bino GGM model with $\\mu > 0$, using the merged $\\rm{SR}^{\\gamma...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t6","@type":"Dataset","description":"Expected exclusion limits in the $M_3$-$\\mu$ plane, for the higgsino-bino GGM model with $\\mu > 0$, using the merged $\\rm{SR}^{\\gamma...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t7","@type":"Dataset","description":"Contour of exclusion in wino production cross section from the photon+$\\ell$ analysis, as a function of the wino mass parameter...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t8","@type":"Dataset","description":"Numbers of selected data events at progressive stages of the selection, for each SR for the diphoton, photon+j and photon+$\\ell$...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t9","@type":"Dataset","description":"Expected number of signal events at progressive stages of the selection, shown for points in the parameter space that typify...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t10","@type":"Dataset","description":"Expected number of signal events at progressive stages of the $\\rm{SR}^{\\gamma b}_{H}$ selection, shown for data and signal Monte Carlo...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t11","@type":"Dataset","description":"Expected number of signal events at progressive stages of the $\\rm{SR}^{\\gamma b}_{L}$ selection, shown for data and signal Monte Carlo...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t12","@type":"Dataset","description":"$\\rm{SR}^{\\gamma\\gamma}_{S-H}$ and $\\rm{SR}^{\\gamma\\gamma}_{S-L}$ signal acceptance*efficiency across the strong-production parameter space, for $m_{\\tilde{g}}$ between 1550 and 1600 GeV.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t13","@type":"Dataset","description":"$\\rm{SR}^{\\gamma\\gamma}_{S-H}$ and $\\rm{SR}^{\\gamma\\gamma}_{S-L}$ signal acceptance*efficiency across the strong-production parameter space, for $m_{\\tilde{g}} = 1500$ GeV.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t14","@type":"Dataset","description":"$\\rm{SR}^{\\gamma\\gamma}_{S-H}$ and $\\rm{SR}^{\\gamma\\gamma}_{S-L}$ signal acceptance*efficiency across the strong-production parameter space, for $m_{\\tilde{g}}$ between 1350 and 1450 GeV.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t15","@type":"Dataset","description":"$\\rm{SR}^{\\gamma\\gamma}_{S-H}$ and $\\rm{SR}^{\\gamma\\gamma}_{S-L}$ signal acceptance*efficiency across the strong-production parameter space, for $m_{\\tilde{g}}$ between 1250 and 1300 GeV.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t16","@type":"Dataset","description":"$\\rm{SR}^{\\gamma\\gamma}_{S-H}$ and $\\rm{SR}^{\\gamma\\gamma}_{S-L}$ signal acceptance*efficiency across the strong-production parameter space, for $m_{\\tilde{g}}$ between 1150 and 1200 GeV.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t17","@type":"Dataset","description":"$\\rm{SR}^{\\gamma\\gamma}_{S-H}$ and $\\rm{SR}^{\\gamma\\gamma}_{S-L}$ signal acceptance*efficiency across the strong-production parameter space, for $m_{\\tilde{g}}$ between 1000 and 1100 GeV.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t18","@type":"Dataset","description":"$\\rm{SR}^{\\gamma\\gamma}_{W-H}$ and $\\rm{SR}^{\\gamma\\gamma}_{W-L}$ signal acceptance*efficiency for $m_{\\tilde{W}}$ between 650 and 800 GeV.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t19","@type":"Dataset","description":"$\\rm{SR}^{\\gamma\\gamma}_{W-H}$ and $\\rm{SR}^{\\gamma\\gamma}_{W-L}$ signal acceptance*efficiency for $m_{\\tilde{W}}$ between 400 and 600 GeV.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t20","@type":"Dataset","description":"$\\rm{SR}^{\\gamma\\gamma}_{W-H}$ and $\\rm{SR}^{\\gamma\\gamma}_{W-L}$ signal acceptance*efficiency for $m_{\\tilde{W}}$ between 100 and 400 GeV.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t21","@type":"Dataset","description":"$\\rm{SR}^{\\gamma b}_{H}$ signal acceptance*efficiency for combined strong and weak production across the $\\mu<0$ higgsino-bino parameter space.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t22","@type":"Dataset","description":"$\\rm{SR}^{\\gamma b}_{L}$ signal acceptance*efficiency for combined strong and weak production across the $\\mu<0$ higgsino-bino parameter space.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t23","@type":"Dataset","description":"$\\rm{SR}^{\\gamma j}_{H}$ signal acceptance*efficiency for combined strong and weak production across the $\\mu>0$ higgsino-bino parameter space.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t24","@type":"Dataset","description":"$\\rm{SR}^{\\gamma j}_{L}$ signal acceptance*efficiency for combined strong and weak production across the $\\mu>0$ higgsino-bino parameter space.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t25","@type":"Dataset","description":"Acceptance-times-efficiency (a*e) for the photon+$\\ell$ analysis SRs.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t26","@type":"Dataset","description":"The total NLO+NLL strong production cross sections with uncertainties for GGM gluino-neutralino signal points for the diphoton and photon+b analyses....","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t27","@type":"Dataset","description":"The total NLO cross sections with uncertainties for GGM wino-bino signal points, for all final states, for the diphoton analysis....","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t28","@type":"Dataset","description":"The NLO gaugino pair production cross sections with relative uncertainties for GGM gluino-neutralino signal points for the photon+b analysis.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t29","@type":"Dataset","description":"The best signal region used for each signal point in the photon+b analysis.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t30","@type":"Dataset","description":"The total NLO+NLL cross sections with uncertainties for the strong production GGM signal grid for the photon+j analysis.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t31","@type":"Dataset","description":"The total NLO cross sections with uncertainties for the electroweak production GGM signal grid for the photon+j analysis.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.69300.v1/t32","@type":"Dataset","description":"The best signal region used for each signal point in the photon+j analysis.","name":"Table 32"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1383883?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/69300"}],"inLanguage":"en","name":"Search for photonic signatures of gauge-mediated supersymmetry in 8 TeV $pp$ collisions with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1383883?version=1","version":1}