{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.57987.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/930002"}},{"@id":"https://doi.org/10.1016/j.physletb.2012.02.051","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2011","description":"CERN-LHC. Study of events having final states with no leptons, jets and missing  transverse momentum, and with no reconstructed electrons or muons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. Data are selected with various cuts and criteria to enhance different  physics regions as described in the text of the paper. Exclusion limits on gluino and squark masses  in SUSY models are presented for a simplified model (described in the paper) together with limits on  m_0 and m_1/2 in MSUGRA/CMSSM models. The data sample has a total integrated luminosity of 1.04 FB-1  and shows no excess above the Standard Model background.     Additional model interpretations are given in the Conference Note.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.57987.v1/t1","@type":"Dataset","description":"The distribution in Meff (scalar sum of the missing transverse momentum and the transverse momenta of the two highest pT...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.57987.v1/t2","@type":"Dataset","description":"The distribution in Meff (scalar sum of the missing transverse momentum and the transverse momenta of the three highest pT...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.57987.v1/t3","@type":"Dataset","description":"The distribution in Meff (scalar sum of the missing transverse momentum and the transverse momenta of the four highest pT...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.57987.v1/t4","@type":"Dataset","description":"The distribution in Meff for the higher jet Pt cut (&gt; 80 GeV) (scalar sum of the missing transverse momentum...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.57987.v1/t5","@type":"Dataset","description":"95% CL exclusion limit in the (Mgluino,Msquark) plane for the simplified model described in the paper. The gluino mass and...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.57987.v1/t6","@type":"Dataset","description":"95% CL exclusion limit in the Squark-Gluino model, as in the previous table, but for a lightest neutralino assigned mass...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.57987.v1/t7","@type":"Dataset","description":"95% CL exclusion limit in the Squark-Gluino model, as in the previous table, but for a lightest neutralino assigned mass...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.57987.v1/t8","@type":"Dataset","description":"95% CL exclusion limit in M(0) and M(1/2) in the tan(beta)=10, A0=0, MU&gt;0 slice of MSUGRA/CMSSM.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.57987.v1/t9","@type":"Dataset","description":"95% CL exclusion limit in the Universal Extra Dimensions model in 1/R v Lambda*R space.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.57987.v1/t10","@type":"Dataset","description":"95% CL exclusion limit in the Universal Extra Dimensions model in m_{g_KK} vs (m_{g_KK}-m_{gamma_KK}) space.","name":"Table 10"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins930002?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/57987"}],"inLanguage":"en","name":"Search for squarks and gluinos using final states with jets and missing transverse momentum with the ATLAS detector in sqrt(s) = 7 TeV proton-proton collisions","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins930002?version=1","version":1}
