{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.150995.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2806818"}},{"@id":"https://doi.org/10.1007/JHEP12(2024)035","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2024","description":"A measurement is performed of Higgs bosons produced with high transverse momentum ($p_\\mathrm{T}$) via vector boson or gluon fusion in proton-proton collisions. The result is based on a data set with a center-of-mass energy of 13 TeV collected in 2016-2018 with the CMS detector at the LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. The decay of a high-$p_\\mathrm{T}$ Higgs boson to a boosted bottom quark-antiquark pair is selected using large-radius jets and employing jet substructure and heavy-flavor taggers based on machine learning techniques. Independent regions targeting the vector boson and gluon fusion mechanisms are defined based on the topology of two quark-initiated jets with large pseudorapidity separation. The signal strengths for both processes are extracted simultaneously by performing a maximum likelihood fit to data in the large-radius jet mass distribution. The observed signal strengths relative to the standard model expectation are 4.9 $^{+1.9}_{-1.6}$ and 1.6 $^{+1.7}_{-1.5}$ for the vector boson and gluon fusion mechanisms, respectively. A differential cross section measurement is also reported in the simplified template cross section framework.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.150995.v2/t1","@type":"Dataset","description":"Jet substructure SF, JMS SF, JMR","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.150995.v2/t2","@type":"Dataset","description":"All signal region bins of the signal strength fit","name":"Signal strength fit"},{"@id":"https://doi.org/10.17182/hepdata.150995.v2/t3","@type":"Dataset","description":"DDB scale factors","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.150995.v2/t4","@type":"Dataset","description":"Measured signal strengths","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.150995.v2/t5","@type":"Dataset","description":"Two-dimensional likelihood scan of the VBF and ggF signal strengths. The magnitude represents twice the negative log likelihood difference with...","name":"Two dimensional 2 Negative log likelihood"},{"@id":"https://doi.org/10.17182/hepdata.150995.v2/t6","@type":"Dataset","description":"ggF per-bin fit","name":"ggF per-bin fit"},{"@id":"https://doi.org/10.17182/hepdata.150995.v2/t7","@type":"Dataset","description":"VBF per-bin fit","name":"VBF per-bin fit"},{"@id":"https://doi.org/10.17182/hepdata.150995.v2/t8","@type":"Dataset","description":"ggF STXS","name":"ggF STXS"},{"@id":"https://doi.org/10.17182/hepdata.150995.v2/t9","@type":"Dataset","description":"VBF STXS","name":"VBF STXS"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2806818?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/150995"}],"inLanguage":"en","name":"Measurement of boosted Higgs bosons produced via vector boson fusion or gluon fusion in the H $\\to$$\\mathrm{b\\bar{b}}$ decay mode using LHC proton-proton collision data at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2806818?version=2","version":2}