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Measurement of the $$ \textrm{t}\overline{\textrm{t}}\textrm{H} $$ and tH production rates in the H → $$ \textrm{b}\overline{\textrm{b}} $$ decay channel using proton-proton collision data at $$ \sqrt{s} $$ = 13 TeV

Aram HayrapetyanYerevan Physics InstituteA. TumasyanYerevan Physics InstituteW. AdamInstitut für HochenergiephysikJanik Walter AndrejkovicInstitut für HochenergiephysikT. BergauerInstitut für HochenergiephysikS. ChatterjeeIndian Institute of Technology MadrasK. DamanakisInstitut für HochenergiephysikM. DragicevicInstitut für HochenergiephysikPriya Sajid HussainInstitut für HochenergiephysikM. JeitlerInstitut für HochenergiephysikNatascha KrammerInstitut für HochenergiephysikA. LiInstitut für HochenergiephysikD. LikoInstitut für HochenergiephysikI. MikulecInstitut für HochenergiephysikJ. SchieckInstitut für HochenergiephysikR. SchöfbeckInstitut für HochenergiephysikD. SchwarzInstitut für HochenergiephysikM. SonawaneInstitut für HochenergiephysikS. TemplInstitut für HochenergiephysikW. WaltenbergerInstitut für HochenergiephysikC.-E. WulzInstitut für HochenergiephysikM. R. DarwishArab Academy for Science, Technology and Maritime TransportX. JanssenUniversiteit AntwerpenP. Van MechelenUniversiteit AntwerpenNordin BreugelmansVrije Universiteit BrusselJ. D’HondtVrije Universiteit BrusselSoumya DansanaVrije Universiteit BrusselA. De MoorVrije Universiteit BrusselM. DelcourtVrije Universiteit BrusselFelix HeyenVrije Universiteit BrusselS. LowetteVrije Universiteit BrusselI. MakarenkoVrije Universiteit BrusselD. MüllerVrije Universiteit BrusselS. TavernierVrije Universiteit BrusselM. TytgatGhent UniversityG. P. Van OnsemVrije Universiteit BrusselS. Van PutteVrije Universiteit BrusselD. VanneromVrije Universiteit BrusselB. BilinUniversité Libre de BruxellesB. ClerbauxUniversité Libre de BruxellesAshok DasUniversity of Notre DameG. De LentdeckerUniversité Libre de BruxellesHugues EvardUniversité Libre de BruxellesL. FavartUniversité Libre de BruxellesP. GianneiosUniversité Libre de BruxellesJ. JaramilloUniversité Libre de BruxellesA. KhalilzadehUniversité Libre de BruxellesFakhri Alam KhanUniversité Libre de BruxellesK. LeeKorea UniversityM. MahdavikhorramiUniversité Libre de BruxellesA. MalaraUniversité Libre de BruxellesS. ParedesUniversité Libre de BruxellesM. A. ShahzadUniversité Libre de BruxellesL. ThomasUniversité Libre de BruxellesM. Vanden BemdenUniversité Libre de BruxellesC. Vander VeldeUniversité Libre de BruxellesP. VanlaerUniversité Libre de BruxellesM. De CoenGhent UniversityD. DoburGhent UniversityG. GökbulutGhent UniversityY. HongGhent UniversityJ. KnolleGhent UniversityLuka LambrechtGhent UniversityDavid MarckxGhent UniversityK. Mota AmariloGhent UniversityA. SamalanGhent UniversityK. SkovpenGhent UniversityN. Van Den BosscheGhent UniversityJan van der LindenGhent UniversityLiam WezenbeekGhent UniversityA. BeneckeUniversité Catholique de LouvainA. BethaniUniversité Catholique de LouvainG. BrunoUniversité Catholique de LouvainC. CaputoUniversité Catholique de LouvainJ. De Favereau De JeneretUniversité Catholique de LouvainC. DelaereUniversité Catholique de LouvainI. S. DonertasUniversité Catholique de LouvainA. GiammancoUniversité Catholique de LouvainAhmet Oguz GuzelUniversité Catholique de LouvainSa. JainUniversité Catholique de LouvainV. LemaitreUniversité Catholique de LouvainPaola MastrapasquaUniversité Catholique de LouvainT. T. TranUniversité Catholique de LouvainS. WertzUniversité Catholique de LouvainG. A. AlvesCentro Brasileiro de Pesquisas FisicasM. Alves Gallo PereiraCentro Brasileiro de Pesquisas FisicasE. CoelhoCentro Brasileiro de Pesquisas FisicasG. Correia SilvaCentro Brasileiro de Pesquisas FisicasC. HenselCentro Brasileiro de Pesquisas FisicasT. Menezes De OliveiraCentro Brasileiro de Pesquisas FisicasA. MoraesCentro Brasileiro de Pesquisas FisicasP. Rebello TelesCentro Brasileiro de Pesquisas FisicasM. SoeiroCentro Brasileiro de Pesquisas FisicasA. Vilela PereiraCentro Brasileiro de Pesquisas FisicasW. L. Aldá JúniorUniversidade do Estado do Rio de JaneiroM. Barroso Ferreira FilhoUniversidade do Estado do Rio de JaneiroH. Brandao MalbouissonUniversidade do Estado do Rio de JaneiroW. CarvalhoUniversidade do Estado do Rio de JaneiroJ. ChinellatoUniversidade Estadual de Campinas
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Abstract

A bstract An analysis of the production of a Higgs boson (H) in association with a top quark-antiquark pair ( $$ \textrm{t}\overline{\textrm{t}}\textrm{H} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>H</mml:mi> </mml:math> ) or a single top quark (tH) is presented. The Higgs boson decay into a bottom quark-antiquark pair (H → $$ \textrm{b}\overline{\textrm{b}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>b</mml:mi> <mml:mover> <mml:mi>b</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> ) 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 $$ \sqrt{s} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msqrt> <mml:mi>s</mml:mi> </mml:msqrt> </mml:math> = 13 TeV in 2016–2018, which correspond to an integrated luminosity of 138 fb − 1 . The observed $$ \textrm{t}\overline{\textrm{t}}\textrm{H} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>H</mml:mi> </mml:math> production rate relative to the standard model expectation is 0.33 ± 0.26 = 0.33 ± 0.17(stat) ± 0.21(syst). Additionally, the $$ \textrm{t}\overline{\textrm{t}}\textrm{H} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>H</mml:mi> </mml:math> 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 $$ {19.3}_{-6.0}^{+9.2} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mn>19.3</mml:mn> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>6.0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>9.2</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> . 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 $$ \textrm{t}\overline{\textrm{t}}\textrm{H} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>H</mml:mi> </mml:math> and tH production rates, and the results are combined with those obtained in other Higgs boson decay channels.

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