{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.142036.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2684710"}},{"@id":"https://doi.org/10.1007/JHEP01(2024)173","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2023","description":"A measurement of the Higgs boson (H) production via vector boson fusion (VBF) and its decay into a bottom quark-antiquark pair ($\\mathrm{b\\bar{b}}$) is presented using proton-proton collision data recorded by the CMS experiment at $\\sqrt{s}$ = 13 TeV and corresponding to an integrated luminosity of 90.8 fb$^{-1}$. Treating the gluon-gluon fusion process as a background and constraining its rate to the value expected in the standard model (SM) within uncertainties, the signal strength of the VBF process, defined as the ratio of the observed signal rate to that predicted by the SM, is measured to be $\\mu^\\text{qqH}_\\mathrm{Hb\\bar{b}}$ = 1.01 $^{+0.55}_{-0.46}$. The VBF signal is observed with a significance of 2.4 standard deviations relative to the background prediction, while the expected significance is 2.7 standard deviations. Considering inclusive Higgs boson production and decay into bottom quarks, the signal strength is measured to be $\\mu^\\text{incl.}_\\mathrm{Hb\\bar{b}}$ = 0.99 $^{+0.48}_{-0.41}$, corresponding to an observed (expected) significance of 2.6 (2.9) standard deviations.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.142036.v1/t1","@type":"Dataset","description":"The mbb distribution after weighted combination of all categories in the analysis weighted with S/(S + B). where S is...","name":"S/(S+B) weighted mbb distribution"},{"@id":"https://doi.org/10.17182/hepdata.142036.v1/t2","@type":"Dataset","description":"The best fit values of the signal strength modifier for the different processes. The uncertainties, corresponding to one standard deviation...","name":"Best fit values of the signal strenght modifiers"},{"@id":"https://doi.org/10.17182/hepdata.142036.v1/t3","@type":"Dataset","description":"The best fit values of the signal strength modifier for the different processes by floating the VBF and ggH production...","name":"Signal strenght modifiers by floating both VBF and ggH processes"},{"@id":"https://doi.org/10.17182/hepdata.142036.v1/t4","@type":"Dataset","description":"Two dimensional observed likelihood profile scan as a function of mu_ggH and mu_qqH","name":"Observed 2D likelihood scan for the signal strenght modifiers"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2684710?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/142036"}],"inLanguage":"en","name":"Measurement of the Higgs boson production via vector boson fusion and its decay into bottom quarks 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/ins2684710?version=1","version":1}