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Phys."],"abstract":"Abstract<\/jats:sc>\n <\/jats:title>\n An analysis of the production of a Higgs boson (H) in association with a top quark-antiquark pair (\n \n $$ \\textrm{t}\\overline{\\textrm{t}}\\textrm{H} $$<\/jats:tex-math>\n \n t<\/mml:mi>\n \n t<\/mml:mi>\n \u00af<\/mml:mo>\n <\/mml:mover>\n H<\/mml:mi>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>) or a single top quark (tH) is presented. The Higgs boson decay into a bottom quark-antiquark pair (H \u2192 \n \n $$ \\textrm{b}\\overline{\\textrm{b}} $$<\/jats:tex-math>\n \n b<\/mml:mi>\n \n b<\/mml:mi>\n \u00af<\/mml:mo>\n <\/mml:mover>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>) is targeted, and three different final states of the top quark decays are considered, defined by the number of leptons (electrons or muons) in the event. The analysis utilises proton-proton collision data collected at the CERN LHC with the CMS experiment at \n \n $$ \\sqrt{s} $$<\/jats:tex-math>\n \n \n s<\/mml:mi>\n <\/mml:msqrt>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> = 13 TeV in 2016\u20132018, which correspond to an integrated luminosity of 138 fb\n \u2212<\/jats:italic>1<\/jats:sup>. The observed \n \n $$ \\textrm{t}\\overline{\\textrm{t}}\\textrm{H} $$<\/jats:tex-math>\n \n t<\/mml:mi>\n \n t<\/mml:mi>\n \u00af<\/mml:mo>\n <\/mml:mover>\n H<\/mml:mi>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> production rate relative to the standard model expectation is 0.33 \u00b1 0.26 = 0.33 \u00b1 0.17(stat) \u00b1 0.21(syst). Additionally, the \n \n $$ \\textrm{t}\\overline{\\textrm{t}}\\textrm{H} $$<\/jats:tex-math>\n \n t<\/mml:mi>\n \n t<\/mml:mi>\n \u00af<\/mml:mo>\n <\/mml:mover>\n H<\/mml:mi>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> production rate is determined in intervals of Higgs boson transverse momentum. An upper limit at 95% confidence level is set on the tH production rate of 14.6 times the standard model prediction, with an expectation of \n \n $$ {19.3}_{-6.0}^{+9.2} $$<\/jats:tex-math>\n \n \n 19.3<\/mml:mn>\n \n \u2212<\/mml:mo>\n 6.0<\/mml:mn>\n <\/mml:mrow>\n \n +<\/mml:mo>\n 9.2<\/mml:mn>\n <\/mml:mrow>\n <\/mml:msubsup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>. Finally, constraints are derived on the strength and structure of the coupling between the Higgs boson and the top quark from simultaneous extraction of the \n \n $$ \\textrm{t}\\overline{\\textrm{t}}\\textrm{H} $$<\/jats:tex-math>\n \n t<\/mml:mi>\n \n t<\/mml:mi>\n \u00af<\/mml:mo>\n <\/mml:mover>\n H<\/mml:mi>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> and tH production rates, and the results are combined with those obtained in other Higgs boson decay channels.<\/jats:p>","DOI":"10.1007\/jhep02(2025)097","type":"journal-article","created":{"date-parts":[[2025,2,23]],"date-time":"2025-02-23T23:31:36Z","timestamp":1740353496000},"update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":5,"title":["Measurement of the $$ \\textrm{t}\\overline{\\textrm{t}}\\textrm{H} $$ and tH production rates in the H \u2192 $$ \\textrm{b}\\overline{\\textrm{b}} $$ decay channel using proton-proton collision data at $$ \\sqrt{s} $$ = 13 TeV"],"prefix":"10.1007","volume":"2025","author":[{"name":"The CMS collaboration","sequence":"first","affiliation":[]},{"given":"A.","family":"Hayrapetyan","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/00ad27c73","id-type":"ROR","asserted-by":"publisher"}],"name":"Yerevan Physics Institute"}]},{"given":"A.","family":"Tumasyan","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/00ad27c73","id-type":"ROR","asserted-by":"publisher"}],"name":"Yerevan Physics Institute"},{"id":[{"id":"https:\/\/ror.org\/00s8vne50","id-type":"ROR","asserted-by":"publisher"}],"name":"Yerevan State University"}]},{"given":"W.","family":"Adam","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/039shy520","id-type":"ROR","asserted-by":"publisher"}],"name":"Institut f\u00fcr Hochenergiephysik"}]},{"given":"J. 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