{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.149851.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2766846"}},{"@id":"https://doi.org/10.1103/PhysRevLett.133.191902","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2024","description":"The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t1","@type":"Dataset","description":"The number of observed events as a function of the number of tracks in the SUEP candidate, for all CRs...","name":"Figure 2"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t2","@type":"Dataset","description":"The observed exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various $m_S$ values,...","name":"Figure 4 (observed)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t3","@type":"Dataset","description":"The expected exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various $m_S$ values,...","name":"Figure 4 (expected)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t4","@type":"Dataset","description":"The expected upper $68\\%$ exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various...","name":"Figure 4 (Upper 68)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t5","@type":"Dataset","description":"The expected lower $68\\%$ exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various...","name":"Figure 4 (Lower 68)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t6","@type":"Dataset","description":"The $95\\%$ CL observed upper limits on the cross section shown as a functions of $T_D$ and the pseudoscalar mass...","name":"Supplementary Figure 2 (top)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t7","@type":"Dataset","description":"The $95\\%$ CL observed upper limits on the cross section shown as a functions of $T_D$ and the pseudoscalar mass...","name":"Supplementary Figure 2 (middle)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t8","@type":"Dataset","description":"The $95\\%$ CL observed upper limits on the cross section shown as a functions of $T_D$ and the pseudoscalar mass...","name":"Supplementary Figure 2 (bottom)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t9","@type":"Dataset","description":"The observed exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various $m_S$ values,...","name":"Supplementary Figure 3 (observed)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t10","@type":"Dataset","description":"The expected exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various $m_S$ values,...","name":"Supplementary Figure 3 (expected)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t11","@type":"Dataset","description":"The expected upper $68\\%$ exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various...","name":"Supplementary Figure 3 (Upper 68)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t12","@type":"Dataset","description":"The expected lower $68\\%$ exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various...","name":"Supplementary Figure 3 (Lower 68)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t13","@type":"Dataset","description":"The observed exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various $m_S$ values,...","name":"Supplementary Figure 4 (observed)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t14","@type":"Dataset","description":"The expected exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various $m_S$ values,...","name":"Supplementary Figure 4 (expected)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t15","@type":"Dataset","description":"The expected upper $68\\%$ exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various...","name":"Supplementary Figure 4 (Upper 68)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t16","@type":"Dataset","description":"The expected lower $68\\%$ exclusions for the nominal $\\sigma$ cross section in the plane of $m_{\\phi}$ and $T_D$, for various...","name":"Supplementary Figure 4 (Lower 68)"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t17","@type":"Dataset","description":"For a selection of signal samples in era 2018 with $m_{\\phi} = T_D = 3$ GeV, the relative efficiencies and...","name":"Supplementary Table 4"},{"@id":"https://doi.org/10.17182/hepdata.149851.v2/t18","@type":"Dataset","description":"The $95\\%$ CL cross section limit for all values of $m_{A'}$, $T_D$, $m_{\\phi}$, and $m_S$ used in the scan.","name":"Full limits table"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2766846?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/149851"}],"inLanguage":"en","name":"Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2766846?version=2","version":2}
