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Search for Higgs boson pair production in the $$ \textrm{b}\overline{\textrm{b}}{\textrm{W}}^{+}{\textrm{W}}^{-} $$ decay mode in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV

A. HayrapetyanYerevan Physics InstituteA. TumasyanYerevan Physics InstituteW. AdamUniversiteit Antwerpen, Antwerpen, BelgiumJ. W. AndrejkovicUniversiteit Antwerpen, Antwerpen, BelgiumT. BergauerInstitut für HochenergiephysikS. ChatterjeeUniversiteit Antwerpen, Antwerpen, BelgiumK. DamanakisYerevan Physics Institute, Yerevan, ArmeniaM. DragicevicUniversiteit Antwerpen, Antwerpen, BelgiumA. Escalante Del ValleInstitut für HochenergiephysikPriya Sajid HussainInstitut f ür Hochenergiephysik, Vienna, AustriaM. JeitlerInstitut für HochenergiephysikNatascha KrammerYerevan Physics Institute, Yerevan, ArmeniaD. LikoInstitut f ür Hochenergiephysik, Vienna, AustriaI. MikulecInstitut f ür Hochenergiephysik, Vienna, AustriaJ. SchieckInstitut für HochenergiephysikR. SchöfbeckInstitut für HochenergiephysikD. SchwarzUniversiteit Antwerpen, Antwerpen, BelgiumM. SonawaneInstitut für HochenergiephysikS. TemplInstitut f ür Hochenergiephysik, Vienna, AustriaW. WaltenbergerInstitut f ür Hochenergiephysik, Vienna, AustriaC.-E. WulzTU WienM. R. DarwishInstitut f ür Hochenergiephysik, Vienna, AustriaX. JanssenYerevan Physics Institute, Yerevan, ArmeniaP. Van MechelenYerevan Physics Institute, Yerevan, ArmeniaE. S. BolsInstitut f ür Hochenergiephysik, Vienna, AustriaJ. D’HondtYerevan Physics Institute, Yerevan, ArmeniaSoumya DansanaInstitut f ür Hochenergiephysik, Vienna, AustriaA. De MoorVrije Universiteit BrusselM. DelcourtYerevan Physics Institute, Yerevan, ArmeniaH. El FahamUniversiteit Antwerpen, Antwerpen, BelgiumS. LowetteInstitut f ür Hochenergiephysik, Vienna, AustriaI. MakarenkoUniversiteit Antwerpen, Antwerpen, BelgiumD. MüllerInstitut f ür Hochenergiephysik, Vienna, AustriaA. R. SahasransuVrije Universiteit BrusselS. TavernierYerevan Physics Institute, Yerevan, ArmeniaM. TytgatYerevan Physics Institute, Yerevan, ArmeniaS. Van PutteYerevan Physics Institute, Yerevan, ArmeniaD. VanneromInstitut f ür Hochenergiephysik, Vienna, AustriaB. ClerbauxYerevan Physics Institute, Yerevan, ArmeniaG. De LentdeckerUniversiteit Antwerpen, Antwerpen, BelgiumL. FavartYerevan Physics Institute, Yerevan, ArmeniaD. HohovUniversiteit Antwerpen, Antwerpen, BelgiumJ. JaramilloUniversiteit Antwerpen, Antwerpen, BelgiumA. KhalilzadehUniversiteit Antwerpen, Antwerpen, BelgiumK. LeeUniversiteit Antwerpen, Antwerpen, BelgiumM. MahdavikhorramiUniversité Libre de BruxellesA. MalaraUniversité Libre de BruxellesS. ParedesInstitut f ür Hochenergiephysik, Vienna, AustriaL. PétréInstitut f ür Hochenergiephysik, Vienna, AustriaN. PostiauInstitut f ür Hochenergiephysik, Vienna, AustriaL. ThomasInstitut f ür Hochenergiephysik, Vienna, AustriaM. Vanden BemdenYerevan Physics Institute, Yerevan, ArmeniaC. Vander VeldeYerevan Physics Institute, Yerevan, ArmeniaP. VanlaerUniversité Libre de BruxellesM. De CoenInstitut f ür Hochenergiephysik, Vienna, AustriaD. DoburGhent UniversityY. HongUniversiteit Antwerpen, Antwerpen, BelgiumJ. KnolleUniversiteit Antwerpen, Antwerpen, BelgiumLuka LambrechtYerevan Physics Institute, Yerevan, ArmeniaG. MestdachYerevan Physics Institute, Yerevan, ArmeniaCésar RendónGhent UniversityA. SamalanGhent UniversityK. SkovpenUniversiteit Antwerpen, Antwerpen, BelgiumN. Van Den BosscheYerevan Physics Institute, Yerevan, ArmeniaLiam WezenbeekUniversiteit Antwerpen, Antwerpen, BelgiumA. BeneckeUniversiteit Antwerpen, Antwerpen, BelgiumG. BrunoYerevan Physics Institute, Yerevan, ArmeniaC. CaputoUniversiteit Antwerpen, Antwerpen, BelgiumC. DelaereInstitut f ür Hochenergiephysik, Vienna, AustriaI. S. DonertasInstitut f ür Hochenergiephysik, Vienna, AustriaA. GiammancoYerevan Physics Institute, Yerevan, ArmeniaK. JaffelInstitut f ür Hochenergiephysik, Vienna, AustriaSa. JainInstitut f ür Hochenergiephysik, Vienna, AustriaV. LemaitreUniversiteit Antwerpen, Antwerpen, BelgiumPaola MastrapasquaUniversiteit Antwerpen, Antwerpen, BelgiumK. MondalYerevan Physics Institute, Yerevan, ArmeniaT. T. TranYerevan Physics Institute, Yerevan, ArmeniaS. WertzUniversiteit Antwerpen, Antwerpen, BelgiumG. A. AlvesInstitut f ür Hochenergiephysik, Vienna, AustriaE. CoelhoInstitut f ür Hochenergiephysik, Vienna, AustriaC. HenselInstitut f ür Hochenergiephysik, Vienna, AustriaT. Menezes De OliveiraYerevan Physics Institute, Yerevan, ArmeniaA. MoraesInstitut f ür Hochenergiephysik, Vienna, AustriaP. Rebello TelesUniversiteit Antwerpen, Antwerpen, BelgiumM. SoeiroYerevan Physics Institute, Yerevan, ArmeniaW. L. Aldá JúniorUniversidade do Estado do Rio de JaneiroM. Alves Gallo PereiraUniversiteit Antwerpen, Antwerpen, BelgiumM. Barroso Ferreira FilhoUniversidade do Estado do Rio de JaneiroH. Brandao MalbouissonUniversidade do Estado do Rio de JaneiroW. CarvalhoYerevan Physics Institute, Yerevan, ArmeniaJ. ChinellatoYerevan Physics Institute, Yerevan, ArmeniaE. M. Da CostaYerevan Physics Institute, Yerevan, ArmeniaG. G. Da SilveiraUniversity of Rio Grande and Rio Grande Community CollegeD. De Jesus DamiaoYerevan Physics Institute, Yerevan, ArmeniaS. Fonseca De SouzaInstitut f ür Hochenergiephysik, Vienna, AustriaJ. MartinsUFMSC. Mora HerreraInstituto Politécnico NacionalK. Mota AmariloYerevan Physics Institute, Yerevan, ArmeniaL. MundimYerevan Physics Institute, Yerevan, Armenia
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A bstract A search for Higgs boson pair (HH) production with one Higgs boson decaying to two bottom quarks and the other to two W bosons are presented. The search is done using proton-proton collisions data at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb − 1 recorded by the CMS detector at the LHC from 2016 to 2018. The final states considered include at least one leptonically decaying W boson. No evidence for the presence of a signal is observed and corresponding upper limits on the HH production cross section are derived. The limit on the inclusive cross section of the nonresonant HH production, assuming that the distributions of kinematic observables are as expected in the standard model (SM), is observed (expected) to be 14 (18) times the value predicted by the SM, at 95% confidence level. The limits on the cross section are also presented as functions of various Higgs boson coupling modifiers, and anomalous Higgs boson coupling scenarios. In addition, limits are set on the resonant HH production via spin-0 and spin-2 resonances within the mass range 250–900 GeV.

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