{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.90834.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1753215"}},{"@id":"https://doi.org/10.1140/epjc/s10052-019-7493-x","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2023","description":"Two related searches for phenomena beyond the standard model (BSM) are performed using events with hadronic jets and significant transverse momentum imbalance. The results are based on a sample of proton-proton collisions at a center-of-mass energy of 13 TeV, collected by the CMS experiment at the LHC in 2016--2018 and corresponding to an integrated luminosity of 137 fb$^{-1}$. The first search is inclusive, based on signal regions defined by the hadronic energy in the event, the jet multiplicity, the number of jets identified as originating from bottom quarks, and the value of the kinematic variable $M_\\mathrm{T2}$ for events with at least two jets. For events with exactly one jet, the transverse momentum of the jet is used instead. The second search looks in addition for disappearing tracks produced by BSM long-lived charged particles that decay within the volume of the tracking detector. No excess event yield is observed above the predicted standard model background. This is used to constrain a range of BSM models that predict the following: the pair production of gluinos and squarks in the context of supersymmetry models conserving $R$-parity, with or without intermediate long-lived charginos produced in the decay chain; the resonant production of a colored scalar state decaying to a massive Dirac fermion and a quark; or the pair production of scalar and vector leptoquarks each decaying to a neutrino and a top, bottom, or light-flavor quark. In most of the cases, the results obtained are the most stringent constraints to date.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t1","@type":"Dataset","description":"Definitions of super signal regions, along with predictions, observed data, and the observed 95% CL upper limits on the number...","name":"Table 6 (SSRs)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t2","@type":"Dataset","description":"Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks ($\\tilde{g}\\to q\\bar{q}\\tilde{\\chi}_1^0$). Signal...","name":"Figure 11 (T1qqqq)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t3","@type":"Dataset","description":"Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks and either a...","name":"Figure 11 (T5qqqqVV)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t4","@type":"Dataset","description":"Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks and a $\\tilde{\\chi}_1^\\pm$...","name":"Figure 11 (T5qqqqWW)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t5","@type":"Dataset","description":"Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to bottom quarks ($\\tilde{g}\\to b\\bar{b}\\tilde{\\chi}_1^0$). Signal...","name":"Figure 12 (T1bbbb)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t6","@type":"Dataset","description":"Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to top quarks ($\\tilde{g}\\to t\\bar{t}\\tilde{\\chi}_1^0$). Signal...","name":"Figure 12 (T1tttt)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t7","@type":"Dataset","description":"Exclusion limits at 95% CL for light-flavor squark pair production, where the squarks decay to $q\\tilde{\\chi}_1^0$. Signal cross sections are...","name":"Figure 13 (T2qq)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t8","@type":"Dataset","description":"Exclusion limits at 95% CL for bottom squark pair production, where the squarks decay to $b\\tilde{\\chi}_1^0$. Signal cross sections are...","name":"Figure 13 (T2bb)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t9","@type":"Dataset","description":"Exclusion limits at 95% CL for top squark pair production, where the squarks decay to $t\\tilde{\\chi}_1^0$. Signal cross sections are...","name":"Figure 13 (T2tt)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t10","@type":"Dataset","description":"Exclusion limits at 95% CL for top squark pair production, where the squarks decay to $b\\tilde{\\chi}_1^\\pm$ and the $\\tilde{\\chi}_1^0$ decay...","name":"Figure 14 (T2bW)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t11","@type":"Dataset","description":"Exclusion limits at 95% CL for top squark pair production, where the squarks decay either to $b\\tilde{\\chi}_1^\\pm\\to bW^\\pm\\tilde{\\chi}_1^0$ or to...","name":"Figure 14 (T2bt)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t12","@type":"Dataset","description":"Exclusion limits at 95% CL for top squark pair production, where the squarks decay to $c\\tilde{\\chi}_1^0$. Signal cross sections are...","name":"Figure 14 (T2cc)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t13","@type":"Dataset","description":"Exclusion limits at 95% CL for the mono-$\\phi$ model, in which a resonantly-produced colored scalar decays to a massive Dirac...","name":"Figure 15 (mono-$\\phi$)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t14","@type":"Dataset","description":"Cross section limits for $\\mathrm{LQ}\\to\\mathrm{q}\\nu$, where $q=u,\\,d,\\,s,\\,\\mathrm{or}\\,c$. Limits are at the 95% confidence level. Theory cross sections are LO for...","name":"Figure 16 ($\\mathrm{LQ}\\to\\mathrm{q}\\nu$)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t15","@type":"Dataset","description":"Cross section limits for $\\mathrm{LQ}\\to\\mathrm{b}\\nu$. Limits are at the 95% confidence level. Theory cross sections are LO for vector LQ,...","name":"Figure 16 ($\\mathrm{LQ}\\to\\mathrm{b}\\nu$)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t16","@type":"Dataset","description":"Cross section limits for $\\mathrm{LQ}\\to\\mathrm{t}\\nu$. Limits are at the 95% confidence level. Theory cross sections are LO for vector LQ,...","name":"Figure 16 ($\\mathrm{LQ}\\to\\mathrm{t}\\nu$)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t17","@type":"Dataset","description":"Predictions and observations for monojet signal regions","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t18","@type":"Dataset","description":"Predictions and observations for signal regions with $250 \\leq H_\\mathrm{T} < 450$ GeV","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t19","@type":"Dataset","description":"Predictions and observations for signal regions with $450 \\leq H_\\mathrm{T} < 575$ GeV and $N_\\mathrm{j}<7$","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t20","@type":"Dataset","description":"Predictions and observations for signal regions with $450 \\leq H_\\mathrm{T} < 575$ GeV and $N_\\mathrm{j}\\geq7$","name":"Table 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decay to either a top and the...","name":"Figure 21 (T2bt Max Chargino Exclusion)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t45","@type":"Dataset","description":"Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks and either the...","name":"Figure 22 (T1qqqq Fixed Masses)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t46","@type":"Dataset","description":"Exclusion limits at 95% CL for direct squark pair production, where the squarks decay to light-flavor quarks and either the...","name":"Figure 22 (T2qq Fixed Masses)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t47","@type":"Dataset","description":"Exclusion limits at 95% CL for direct stop pair production, where the stops decay to either a top and the...","name":"Figure 22 (T2bt Fixed Masses)"},{"@id":"https://doi.org/10.17182/hepdata.90834.v1/t48","@type":"Dataset","description":"Predictions and observations for 2016 disappearing track signal 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