{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.165888.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/3083980"}},{"@id":"https://doi.org/10.1007/JHEP03(2026)189","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2025","description":"A search for signatures of a dark analog to quantum chromodynamics is performed. The analysis targets long-lived dark mesons that decay into standard-model particles, with a high branching fraction of the dark mesons decaying into muons. The dark mesons are formed by the hadronisation of dark partons, which are produced by a decay of the Higgs boson. The search is performed using a data set corresponding to an integrated luminosity of $41.6~\\textrm{fb}^{-1}$, which was collected in proton-proton collisions at $\\sqrt{s}=13~\\textrm{TeV}$ by the CMS experiment at the CERN LHC in 2018 using non-prompt muon triggers. The search is based on resonant muon pair signatures. Machine-learning techniques are employed in the analysis, utilising boosted decision trees to discriminate between signal and background. No significant excess is observed above the standard model expectation. Upper limits on the branching fraction of the Higgs boson decaying to dark partons are determined to be as low as $10^{-4}$ at 95% confidence level, surpassing and extending the existing limits on models with dark $\\tilde{\\omega}$ mesons for mean proper decay lengths of less than $500~\\textrm{mm}$ and for $\\tilde{\\omega}$ masses down to $0.3~\\textrm{GeV}$. First limits are set for extended dark-shower models with two dark flavours that contain dark photons, probing their masses down to $0.33~\\textrm{GeV}$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t1","@type":"Dataset","description":"Dimuon invariant mass distributions in mass windows around $0.67~\\textrm{GeV}$ in the single-vertex category with $1~\\textrm{cm}&lt;l_{xy}&lt;10~\\textrm{cm}$ and $\\textrm{pointing angle}&lt;0.2$. The background...","name":"Scenario A dimuon mass distribution at 0.67 GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t2","@type":"Dataset","description":"Dimuon invariant mass distributions in mass windows around $1.33~\\textrm{GeV}$ in the single-vertex category with $1~\\textrm{cm}&lt;l_{xy}&lt;10~\\textrm{cm}$ and $\\textrm{pointing angle}&lt;0.2$. The background...","name":"Scenario B1 dimuon mass distribution at 1.33 GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t3","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\omega}$ meson $c\\tau$ for $m_{\\tilde{\\omega}}=2~\\textrm{GeV}$...","name":"Vector portal limits, $m_{\\tilde{\\omega}}=2$GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t4","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\omega}$ meson $c\\tau$ for $m_{\\tilde{\\omega}}=5~\\textrm{GeV}$...","name":"Vector portal limits, $m_{\\tilde{\\omega}}=5$GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t5","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\omega}$ meson $c\\tau$ for $m_{\\tilde{\\omega}}=15~\\textrm{GeV}$...","name":"Vector portal limits, $m_{\\tilde{\\omega}}=15$GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t6","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\omega}$ meson $c\\tau$ for $m_{\\tilde{\\omega}}=20~\\textrm{GeV}$...","name":"Vector portal limits, $m_{\\tilde{\\omega}}=20$GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t7","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\textrm{A}'$ $c\\tau$ for $m_{\\tilde{\\pi}_{3}}=1~\\textrm{GeV}$ and...","name":"Scenario A limits, $m_{A'}=0.33$ GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t8","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\textrm{A}'$ $c\\tau$ for $m_{\\tilde{\\pi}_{3}}=4~\\textrm{GeV}$ and...","name":"Scenario A limits, $m_{A'}=0.4$ GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t9","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\textrm{A}'$ $c\\tau$ for $m_{\\tilde{\\pi}_{3}}=2~\\textrm{GeV}$ and...","name":"Scenario A limits, $m_{A'}=0.67$ GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t10","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\textrm{A}'$ $c\\tau$ for $m_{\\tilde{\\pi}_{3}}=4~\\textrm{GeV}$ and...","name":"Scenario A limits, $m_{A'}=1.33$ GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t11","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\pi}_{3}$ meson $c\\tau$ for $m_{\\tilde{\\pi}_{3}}=1~\\textrm{GeV}$...","name":"Scenario B1 limits, $m_{A'}=0.33$ GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t12","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\pi}_{3}$ meson $c\\tau$ for $m_{\\tilde{\\pi}_{3}}=2~\\textrm{GeV}$...","name":"Scenario B1 limits, $m_{A'}=0.4$ GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t13","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\pi}_{3}$ meson $c\\tau$ for $m_{\\tilde{\\pi}_{3}}=2~\\textrm{GeV}$...","name":"Scenario B1 limits, $m_{A'}=0.67$ GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t14","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\pi}_{3}$ meson $c\\tau$ for $m_{\\tilde{\\pi}_{3}}=4~\\textrm{GeV}$...","name":"Scenario B1 limits, $m_{A'}=1.33$ GeV"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t15","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\omega}$ meson mass for $c\\tau=10~\\textrm{mm}$...","name":"Vector portal limits, $c\\tau=10$mm"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t16","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\omega}$ meson mass for $c\\tau=100~\\textrm{mm}$...","name":"Vector portal limits, $c\\tau=100$mm"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t17","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\to\\psi\\overline{\\psi}\\right)$ as a function of the $\\mathrm{A}'$ mass in Scenario A,...","name":"Scenario A limits, $m_{\\tilde{\\pi}_{3}}=10m_{A'}$, $c\\tau=10$mm"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t18","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\to\\psi\\overline{\\psi}\\right)$ as a function of the $\\mathrm{A}'$ mass in Scenario A,...","name":"Scenario A limits, $m_{\\tilde{\\pi}_{3}}=3m_{A'}$, $c\\tau=10$mm"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t19","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\to\\psi\\overline{\\psi}\\right)$ as a function of the $\\mathrm{A}'$ mass in Scenario A,...","name":"Scenario A limits, $m_{\\tilde{\\pi}_{3}}=10m_{A'}$, $c\\tau=100$mm"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t20","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\to\\psi\\overline{\\psi}\\right)$ as a function of the $\\mathrm{A}'$ mass in Scenario A,...","name":"Scenario A limits, $m_{\\tilde{\\pi}_{3}}=3m_{A'}$, $c\\tau=100$mm"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t21","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\to\\psi\\overline{\\psi}\\right)$ as a function of the $\\mathrm{A}'$ mass in Scenario B1,...","name":"Scenario B1 limits, $m_{\\tilde{\\pi}_{3}}=10m_{A'}$, $c\\tau=10$mm"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t22","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\to\\psi\\overline{\\psi}\\right)$ as a function of the $\\mathrm{A}'$ mass in Scenario B1,...","name":"Scenario B1 limits, $m_{\\tilde{\\pi}_{3}}=3m_{A'}$, $c\\tau=10$mm"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t23","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\to\\psi\\overline{\\psi}\\right)$ as a function of the $\\mathrm{A}'$ mass in Scenario B1,...","name":"Scenario B1 limits, $m_{\\tilde{\\pi}_{3}}=10m_{A'}$,$c\\tau=100$mm"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t24","@type":"Dataset","description":"Upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\to\\psi\\overline{\\psi}\\right)$ as a function of the $\\mathrm{A}'$ mass in Scenario B1,...","name":"Scenario B1 limits, $m_{\\tilde{\\pi}_{3}}=3m_{A'}$,$c\\tau=100$mm"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t25","@type":"Dataset","description":"Observed upper limits at 95% CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as a function of the $\\tilde{\\omega}$ meson mass and...","name":"Vector portal 2D limits"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t26","@type":"Dataset","description":"Observed upper limits at $95\\%$ CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as functions of the $\\textrm{A}'$ mass and $c\\tau$ for...","name":"Scenario A 2D limits, $m_{\\tilde{\\pi}_{3}}=10m_{A'}$"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t27","@type":"Dataset","description":"Observed upper limits at $95\\%$ CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as functions of the $\\textrm{A}'$ mass and $c\\tau$ for...","name":"Scenario A 2D limits, $m_{\\tilde{\\pi}_{3}}=3m_{A'}$"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t28","@type":"Dataset","description":"Observed upper limits at $95\\%$ CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as functions of the $\\textrm{A}'$ mass and $c\\tau$ for...","name":"Scenario B1 2D limits, $m_{\\tilde{\\pi}_{3}}=10m_{A'}$"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t29","@type":"Dataset","description":"Observed upper limits at $95\\%$ CL on the branching fraction $\\mathcal{B}\\left(\\textrm{H}\\rightarrow\\psi\\overline{\\psi}\\right)$ as functions of the $\\textrm{A}'$ mass and $c\\tau$ for...","name":"Scenario B1 2D limits, $m_{\\tilde{\\pi}_{3}}=3m_{A'}$"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t30","@type":"Dataset","description":"Cutflow efficiencies for representative signal model points in the vector portal.","name":"Vector portal cutflow efficiencies"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t31","@type":"Dataset","description":"Cutflow efficiencies for representative signal model points in Scenario A.","name":"Scenario A cutflow efficiencies"},{"@id":"https://doi.org/10.17182/hepdata.165888.v1/t32","@type":"Dataset","description":"Cutflow efficiencies for representative signal model points in Scenario B1.","name":"Scenario B1 cutflow efficiencies"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins3083980?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/165888"}],"inLanguage":"en","name":"Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins3083980?version=1","version":1}
