{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.68783.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1343107"}},{"@id":"https://doi.org/10.1140/epjc/s10052-015-3517-3","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2015","description":"CERN-LHC.  Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb$^{-1}$ of $\\sqrt{s}=8$ TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with $p_T > 120$ GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between $E_T^{miss} > 150$ GeV and $E_T^{miss} > 700$ GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with large extra spatial dimensions, pair production of weakly interacting dark matter candidates, and production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presented.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t1","@type":"Dataset","description":"Distributions of the measured transverse mass distribution of the identified muon in the $W\\mu\\nu$+jets control region for the inclusive SR1...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t2","@type":"Dataset","description":"Measured $E_{T}^{miss}$ distribution in the $W\\mu\\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t3","@type":"Dataset","description":"Measured leading jet $p_{T}$ distribution in the $W\\mu\\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations....","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t4","@type":"Dataset","description":"Measured jet multiplicity distribution in the $W\\mu\\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t5","@type":"Dataset","description":"Measured dilepton invariant mass distribution in the $Z\\mu\\mu$+jets control region for the inclusive SR1 selection, compared to the background expectations....","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t6","@type":"Dataset","description":"Measured $E_{T}^{miss}$ distribution in the $Z\\mu\\mu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t7","@type":"Dataset","description":"Measured leading jet $p_{T}$ distribution in the $Z\\mu\\mu$+jets control region for the inclusive SR1 selection, compared to the background expectations....","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t8","@type":"Dataset","description":"Measured jet multiplicity distribution in the $Z\\mu\\mu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t9","@type":"Dataset","description":"Measured transverse mass distribution in the $We\\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t10","@type":"Dataset","description":"Measured $E_{T}^{miss}$ distribution in the $We\\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t11","@type":"Dataset","description":"Measured leading jet $p_{T}$ distribution in the $We\\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations....","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t12","@type":"Dataset","description":"Measured jet multiplicity distribution in the $We\\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t13","@type":"Dataset","description":"Measured dilepton invariant mass distribution in the $Zee$+jets control region for the inclusive SR1 selection, compared to the background expectations....","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t14","@type":"Dataset","description":"Measured $E_{T}^{miss}$ distribution in the $Zee$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t15","@type":"Dataset","description":"Measured leading jet $p_{T}$ distribution in the $Zee$+jets control region for the inclusive SR1 selection, compared to the background expectations....","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t16","@type":"Dataset","description":"Measured jet multiplicity distribution in the $Zee$+jets control region for the inclusive SR1 selection, compared to the background expectations. The...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t17","@type":"Dataset","description":"Measured distribution of the jet multiplicity for the SR1 selection compared to the SM expectations. The $Z\\nu\\nu$+jets contribution is shown...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t18","@type":"Dataset","description":"Measured distribution of $E_{T}^{miss}$ for the SR1 selection compared to the SM expectations. The $Z\\nu\\nu$+jets contribution is shown as constrained...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t19","@type":"Dataset","description":"Measured distribution of leading jet $p_{T}$ for the SR1 selection compared to the SM expectations. The $Z\\nu\\nu$+jets contribution is shown...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t20","@type":"Dataset","description":"Measured distribution of the leading jet $p_{T}$ to $E_{T}^{miss}$ ratio for the SR1 selection compared to the SM expectations. The...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t21","@type":"Dataset","description":"Measured distribution of the jet multiplicity for SR7 selection compared to the SM expectations. The $Z\\nu\\nu$+jets contribution is shown as...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t22","@type":"Dataset","description":"Measured distribution of the jet multiplicity for SR7 selection compared to the SM expectations. The $Z\\nu\\nu$+jets contribution is shown as...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t23","@type":"Dataset","description":"Measured distribution of the leading jet $p_T$ for SR7 selection compared to the SM expectations. The $Z\\nu\\nu$+jets contribution is shown...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t24","@type":"Dataset","description":"Measured distribution of the leading jet $p_T$ for SR9 selection compared to the SM expectations. The $Z\\nu\\nu$+jets contribution is shown...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t25","@type":"Dataset","description":"Measured distribution of the leading jet $p_T$ to $E_{T}^{miss}$ ratio for SR7 selection compared to the SM expectations. The $Z\\nu\\nu$+jets...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t26","@type":"Dataset","description":"Measured distribution of the leading jet $p_T$ to $E_{T}^{miss}$ ratio for SR9 selection compared to the SM expectations. The $Z\\nu\\nu$+jets...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t27","@type":"Dataset","description":"Observed and expected 95$\\%$ CL limit on the fundamental Planck scale in $4+n$ dimensions, $M_D$, as a function of the...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t28","@type":"Dataset","description":"Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t29","@type":"Dataset","description":"Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t30","@type":"Dataset","description":"Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t31","@type":"Dataset","description":"Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t32","@type":"Dataset","description":"Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t33","@type":"Dataset","description":"Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t34","@type":"Dataset","description":"Observed 95% CL limits on the suppression scale M* as a function of the mediator mass Mmed, assuming a Z'-like...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t35","@type":"Dataset","description":"Observed 95% CL upper limits on the product of couplings of the simplified model vertex in the plane of mediator...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t36","@type":"Dataset","description":"Upper limits at 90% C.L. on the WIMP-nucleon scattering cross section as a function of m_chi for spin-independent interactions, for...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t37","@type":"Dataset","description":"Upper limits at 90% C.L. on the WIMP-nucleon scattering cross section as a function of m_chi for spin-dependent interactions, for...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t38","@type":"Dataset","description":"Upper limits at 90% C.L. on the WIMP-nucleon annihilation cross section as a function of m_chi, for a coupling strength...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t39","@type":"Dataset","description":"95$\\%$ CL lower limits on the gravitino mass $m_{\\tilde{G}}$ as a function of the squark mass $m_{\\tilde{q}}$ for degenerate squark/gluino...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t40","@type":"Dataset","description":"95$\\%$ CL lower limits on the gravitino mass $m_{\\tilde{G}}$ as a function of the squark mass $m_{\\tilde{q}}$ for non-degenerate squark/gluino...","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t41","@type":"Dataset","description":"95$\\%$ CL lower limits on the gravitino mass $m_{\\tilde{G}}$ as a function of the squark mass $m_{\\tilde{q}}$ for non-degenerate squark/gluino...","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t42","@type":"Dataset","description":"95$\\%$ CL lower limits on the gravitino mass $m_{\\tilde{G}}$ as a function of the squark mass $m_{\\tilde{q}}$ for non-degenerate squark/gluino...","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t43","@type":"Dataset","description":"95$\\%$ CL lower limits on the gravitino mass $m_{\\tilde{G}}$ as a function of the squark mass $m_{\\tilde{q}}$ for non-degenerate squark/gluino...","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t44","@type":"Dataset","description":"Observed and expected 95$\\%$ CL upper limit on $\\sigma \\times {\\rm{BR}}(H \\to {\\rm{invisible}})$ as a function of the Higgs boson...","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.68783.v1/t45","@type":"Dataset","description":"Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the...","name":"Table 45"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1343107?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/68783"}],"inLanguage":"en","name":"Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at $\\sqrt{s}=8$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1343107?version=1","version":1}