{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.150033.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2812281"}},{"@id":"https://doi.org/10.1007/JHEP12(2024)172","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2024","description":"This analysis (HIG-21-004 [2017+2018 CMS data]) is an extenstion to the search (HIG-18-003 [2016 data]) for new light bosons decaying into muon pairs using data sample corresponding to an integrated luminosity of 35.9 fb^{\u22121}.\nThis analysis HIG-21-004 [2017+2018 CMS data] - explores a larger parameter space, dimuon mass from 0.21-60 GeV (was from 0.25-8.5 GeV for HIG-18-003 [2016 data]), with 0 < c\u03c4 < 100 mm. - increases luminosity to 60\u2013137 fb^{\u22121} (was 36 fb^{\u22121} for HIG-18-003 [2016 data]). - covers a range of 10E\u22122 > \u03b5 > 10E\u22128 for kinetic mixing in the dark sector, which is complementary to others (EXO-20-014 and EXO-21-006, 10E\u22125 > \u03b5 > 10E\u22129). - expanded fiducial volume benefit from phase-1 pixel upgrade. - interprets four bench mark models using model-independent limits - Axion-like particle (ALP) - Vector portal - NMSSM - Dark SUSY\nAnalysis strategy of this analysis - Data-driven background (BKG) estimation method - Below \u03a5; Template method [1] - 1DBKGtemplate; TI(\u00b5\u00b51) and TII(\u00b5\u00b52) - 2DBKGtemplate; TI(\u00b5\u00b51)\u2297TII(\u00b5\u00b52) - Above \u03a5; Gaussian kernel-density estimate (KDE) method","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t1","@type":"Dataset","description":"The model-independent 95\\% \\CL expected and observed upper limits set on ${\\sigma(\\PP\\to 2\\Pa+\\PX)\\mathcal{B}^2(\\Pa\\to 2\\PGm)\\alphaGen}$ over the range $0.21 < \\MPa...","name":"Panel 1"},{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t2","@type":"Dataset","description":"The model-independent 95\\% \\CL expected and observed upper limits set on ${\\sigma(\\PP\\to 2\\Pa+\\PX)\\mathcal{B}^2(\\Pa\\to 2\\PGm)\\alphaGen}$ over the range $0.21 < \\MPa...","name":"Panel 2"},{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t3","@type":"Dataset","description":"The model-independent 95\\% \\CL expected and observed upper limits set on ${\\sigma(\\PP\\to 2\\Pa+\\PX)\\mathcal{B}^2(\\Pa\\to 2\\PGm)\\alphaGen}$ over the range $0.21 < \\MPa...","name":"Panel 3"},{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t4","@type":"Dataset","description":"The model-independent 95\\% \\CL expected and observed upper limits set on ${\\sigma(\\PP\\to 2\\Pa+\\PX)\\mathcal{B}^2(\\Pa\\to 2\\PGm)\\alphaGen}$ over the range $0.21 < \\MPa...","name":"Panel 4"},{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t5","@type":"Dataset","description":"The 95\\% \\CL observed upper limits on the effective coupling $\\CahLambda$ of the ALP to the SM Higgs assuming the...","name":"Panel 5"},{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t6","@type":"Dataset","description":"The 95\\% \\CL observed upper limits on the effective coupling $\\cll/\\Lambda$ of the ALP to the SM leptons. The orange...","name":"Panel 6"},{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t7","@type":"Dataset","description":"The 95\\% \\CL observed upper limits on $\\varepsilon^{2} \\mathcal{B}(\\ZDark \\to \\sDark \\overline{\\sDark}) \\mathcal{B}^{2}(\\sDark \\rightarrow 2\\PGm)$ for the vector portal model...","name":"Panel 7"},{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t8","@type":"Dataset","description":"The 95\\% \\CL observed upper limits for $\\sigma(\\PP\\to\\PhOneTwo\\to 2\\PaOne) \\mathcal{B}^2(\\PaOne\\to 2\\PGm)$ for the NMSSM as a function of $\\MPaOne$ for...","name":"Panel 8"},{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t9","@type":"Dataset","description":"The 95\\% \\CL observed upper limits for $\\sigma(\\PP\\to\\PhOneTwo\\to 2\\PaOne) \\mathcal{B}^2(\\PaOne\\to 2\\PGm)$ for the NMSSM as a function of $\\MPaOne$ for...","name":"Panel 9"},{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t10","@type":"Dataset","description":"The 95\\% \\CL observed upper limits for $\\sigma(\\PP\\to\\PhOneTwo\\to 2\\PaOne) \\mathcal{B}^2(\\PaOne\\to 2\\PGm)$ for the NMSSM as a function of $\\MPaOne$ for...","name":"Panel 10"},{"@id":"https://doi.org/10.17182/hepdata.150033.v1/t11","@type":"Dataset","description":"The 95\\% \\CL observed upper limits (black solid curves) from this search as interpreted in the dark SUSY scenario for...","name":"Panel 11"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2812281?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/150033"}],"inLanguage":"en","name":"Model-independent search for pair production of new bosons decaying into muons 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/ins2812281?version=1","version":1}