{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.115995.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2072383"}},{"@id":"https://doi.org/10.1016/j.physletb.2022.137392","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"We search for new massive scalar particles X and Y through the resonant production process $X \\rightarrow YH \\rightarrow b\\bar{b} b\\bar{b}$, where H is the standard model Higgs boson. Data from CERN LHC proton-proton collisions are used, collected at a centre-of-mass energy of 13 TeV in 2016--2018 and corresponding to an integrated luminosity of 138 $\\mathrm{fb}^{-1}$. The search is performed in mass ranges of 0.9--4 TeV for X and 60--600 GeV for Y, where both Y and H are reconstructed as Lorentz-boosted single large-area jets. The results are interpreted in the context of the next-to-minimal supersymmetric standard model and also in an extension of the standard model with two additional singlet scalar fields. The 95% confidence level upper limits for the production cross section very between 0.1 and 150 fb depending on the X and Y masses, and represent a significant improvement over results from previous searches.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.115995.v2/t1","@type":"Dataset","description":"The $M_J^Y$ distribution for the number of observed events (black markers) compared with the estimated backgrounds (filled histograms) and their...","name":"Figure 2a"},{"@id":"https://doi.org/10.17182/hepdata.115995.v2/t2","@type":"Dataset","description":"The $M_{JJ}$ distribution for the number of observed events (black markers) compared with the estimated backgrounds (filled histograms) and their...","name":"Figure 2b"},{"@id":"https://doi.org/10.17182/hepdata.115995.v2/t3","@type":"Dataset","description":"The soft-drop mass distribution of the top quark candidate jets in the 2018 jets+lepton category, in the tight ParticleNet region,...","name":"Figure 3"},{"@id":"https://doi.org/10.17182/hepdata.115995.v2/t4","@type":"Dataset","description":"The 95% confidence level expected and observed upper limits on $\\sigma$(pp->X->YH->4b) for different values of $M_X$ and $M_Y$. The areas...","name":"Figure 4"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2072383?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/115995"}],"inLanguage":"en","name":"Search for a massive scalar resonance decaying to a light scalar and a Higgs boson in the four b quarks final state with boosted topology","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2072383?version=2","version":2}