{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.146900.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2809450"}},{"@id":"https://doi.org/10.1007/JHEP02(2025)040","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2024","description":"A search is presented for the resonant production of a pair of the standard model-like Higgs bosons using data from proton-proton collisions at a centre-of-mass energy of 13 TeV, collected by the CMS experiment at the CERN LHC in 2016--2018, corresponding to an integrated luminosity of 138 $\\mathrm{fb}^{-1}$. The final state consists of two b quark-antiquark pairs. The search is conducted in the region of phase space where at least one of the pairs is highly Lorentz-boosted and is reconstructed as a single large-area jet. The other pair may be either similarly merged or resolved, the latter reconstructed using two b-tagged jets. The data is found to be consistent with the measured standard model processes and are interpreted as 95% confidence level upper limits on the product of the cross sections and the branching fractions of the spin-0 radion and the spin-2 bulk graviton in warped extradimensional models. The limits set are in the range 9.74--0.29 fb and 4.94--0.19 fb for a narrow radion and a graviton, respectively, with a mass between 1 and 3 TeV. For a 10%-width radion and a bulk graviton, the limits are in the range 12.5--0.35 fb and 8.23--0.23 fb, respectively, for the same masses.  These limits result in the exclusion of the narrow-width graviton with a mass below 1.2 TeV, and of the narrow and 10%-width radion with masses below 2.6 TeV, and 2.8 TeV, respectively, an improvement of $\\approx$1 TeV over the previous CMS measurement.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t1","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the LL pass region, projected onto the plane...","name":"Figure 2 (upper left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t2","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the LL pass region, projected onto the plane...","name":"Figure 2 (middle left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t3","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the LL pass region, projected onto the plane...","name":"Figure 2 (lower left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t4","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the TT pass region, projected onto the plane...","name":"Figure 3 (upper left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t5","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the TT pass region, projected onto the plane...","name":"Figure 3 (middle left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t6","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the TT pass region, projected onto the plane...","name":"Figure 3 (lower left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t7","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the LL pass region, projected onto the plane...","name":"Figure 2 (upper right)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t8","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the LL pass region, projected onto the plane...","name":"Figure 2 (middle right)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t9","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the LL pass region, projected onto the plane...","name":"Figure 2 (lower right)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t10","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the TT pass region, projected onto the plane...","name":"Figure 3 (upper right)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t11","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the TT pass region, projected onto the plane...","name":"Figure 3 (middle right)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t12","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the TT pass region, projected onto the plane...","name":"Figure 3 (lower right)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t13","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the semi-resolved pass region, projected onto the plane...","name":"Figure 4 (upper right)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t14","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the semi-resolved pass region, projected onto the plane...","name":"Figure 4 (middle right)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t15","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the semi-resolved pass region, projected onto the plane...","name":"Figure 4 (lower right)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t16","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the semi-resolved pass region, projected onto the plane...","name":"Figure 4 (upper left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t17","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the semi-resolved pass region, projected onto the plane...","name":"Figure 4 (middle left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t18","@type":"Dataset","description":"Slices of 2D distributions of observed events and the post-fit templates in the semi-resolved pass region, projected onto the plane...","name":"Figure 4 (lower left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t19","@type":"Dataset","description":"The observed (solid black line) and expected (dashed black line) upper limits at 95% CL on $\\sigma$(pp-&gt;X)B(X-&gt;HH-&gt;4b) for the narrow...","name":"Figure 5 (left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t20","@type":"Dataset","description":"The observed (solid black line) and expected (dashed black line) upper limits at 95% CL on $\\sigma$(pp-&gt;X)B(X-&gt;HH-&gt;4b) for the narrow...","name":"Figure 5 (right)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t21","@type":"Dataset","description":"The observed (solid black line) and expected (dashed black line) upper limits at 95% CL on $\\sigma$(pp-&gt;X)B(X-&gt;HH-&gt;4b) for the 10%-width...","name":"Figure 6 (left)"},{"@id":"https://doi.org/10.17182/hepdata.146900.v1/t22","@type":"Dataset","description":"The observed (solid black line) and expected (dashed black line) upper limits at 95% CL on $\\sigma$(pp-&gt;X)B(X-&gt;HH-&gt;4b) for the 10%-width...","name":"Figure 6 (right)"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2809450?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/146900"}],"inLanguage":"en","name":"Search for resonant pair production of Higgs bosons in the $\\mathrm{b\\bar{b}b\\bar{b}}$ final state using large-area jets 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/ins2809450?version=1","version":1}
