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Search for Higgs boson pair production with one associated vector boson in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV

A. HayrapetyanYerevan Physics InstituteA. TumasyanUniversiteit Antwerpen, Antwerpen, BelgiumW. AdamYerevan Physics Institute, Yerevan, ArmeniaJ. W. AndrejkovicInstitut f ür Hochenergiephysik, Vienna, AustriaT. BergauerInstitut f ür Hochenergiephysik, Vienna, AustriaS. ChatterjeeIndian Institute of Technology MadrasK. DamanakisUniversiteit Antwerpen, Antwerpen, BelgiumM. DragicevicUniversiteit Antwerpen, Antwerpen, BelgiumA. Escalante Del ValleInstitut für HochenergiephysikPriya Sajid HussainInstitut für HochenergiephysikM. JeitlerYerevan Physics Institute, Yerevan, ArmeniaNatascha KrammerYerevan Physics Institute, Yerevan, ArmeniaD. LikoUniversiteit Antwerpen, Antwerpen, BelgiumI. MikulecYerevan Physics Institute, Yerevan, ArmeniaJ. SchieckUniversiteit Antwerpen, Antwerpen, BelgiumR. SchöfbeckInstitut für HochenergiephysikD. SchwarzInstitut f ür Hochenergiephysik, Vienna, AustriaM. SonawaneInstitut f ür Hochenergiephysik, Vienna, AustriaS. TemplInstitut für HochenergiephysikW. WaltenbergerUniversiteit Antwerpen, Antwerpen, BelgiumC.-E. WulzUniversiteit Antwerpen, Antwerpen, BelgiumM. R. DarwishYerevan Physics Institute, Yerevan, ArmeniaX. JanssenYerevan Physics Institute, Yerevan, ArmeniaP. Van MechelenInstitut f ür Hochenergiephysik, Vienna, AustriaE. S. BolsVrije Universiteit BrusselJ. D’HondtUniversiteit Antwerpen, Antwerpen, BelgiumSoumya DansanaUniversiteit Antwerpen, Antwerpen, BelgiumA. De MoorVrije Universiteit BrusselM. DelcourtYerevan Physics Institute, Yerevan, ArmeniaH. El FahamVrije Universiteit BrusselS. LowetteInstitut f ür Hochenergiephysik, Vienna, AustriaI. MakarenkoVrije Universiteit BrusselD. MüllerUniversiteit Antwerpen, Antwerpen, BelgiumA. R. SahasransuInstitut f ür Hochenergiephysik, Vienna, AustriaS. TavernierYerevan Physics Institute, Yerevan, ArmeniaM. TytgatInstitut f ür Hochenergiephysik, Vienna, AustriaS. Van PutteInstitut f ür Hochenergiephysik, Vienna, AustriaD. VanneromUniversiteit Antwerpen, Antwerpen, BelgiumB. ClerbauxUniversiteit Antwerpen, Antwerpen, BelgiumG. De LentdeckerUniversité Libre de BruxellesL. FavartYerevan Physics Institute, Yerevan, ArmeniaD. HohovUniversiteit Antwerpen, Antwerpen, BelgiumJ. JaramilloUniversité Libre de BruxellesA. KhalilzadehInstitut f ür Hochenergiephysik, Vienna, AustriaK. LeeKorea UniversityM. MahdavikhorramiInstitut f ür Hochenergiephysik, Vienna, AustriaA. MalaraUniversité Libre de BruxellesS. ParedesUniversiteit Antwerpen, Antwerpen, BelgiumL. PétréUniversiteit Antwerpen, Antwerpen, BelgiumN. PostiauUniversité Libre de BruxellesL. ThomasUniversité Libre de BruxellesM. Vanden BemdenUniversiteit Antwerpen, Antwerpen, BelgiumC. Vander VeldeInstitut f ür Hochenergiephysik, Vienna, AustriaP. VanlaerInstitut f ür Hochenergiephysik, Vienna, AustriaM. De CoenYerevan Physics Institute, Yerevan, ArmeniaD. DoburGhent UniversityY. HongYerevan Physics Institute, Yerevan, ArmeniaJ. KnolleInstitut f ür Hochenergiephysik, Vienna, AustriaLuka LambrechtGhent UniversityG. MestdachGhent UniversityCésar RendónUniversiteit Antwerpen, Antwerpen, BelgiumA. SamalanGhent UniversityK. SkovpenGhent UniversityN. Van Den BosscheInstitut f ür Hochenergiephysik, Vienna, AustriaLiam WezenbeekYerevan Physics Institute, Yerevan, ArmeniaA. BeneckeInstitut f ür Hochenergiephysik, Vienna, AustriaG. BrunoYerevan Physics Institute, Yerevan, ArmeniaC. CaputoUniversité Catholique de LouvainC. DelaereInstitut f ür Hochenergiephysik, Vienna, AustriaI. S. DonertasYerevan Physics Institute, Yerevan, ArmeniaA. GiammancoYerevan Physics Institute, Yerevan, ArmeniaK. JaffelYerevan Physics Institute, Yerevan, ArmeniaSa. JainUniversiteit Antwerpen, Antwerpen, BelgiumV. LemaitreUniversiteit Antwerpen, Antwerpen, BelgiumPaola MastrapasquaInstitut f ür Hochenergiephysik, Vienna, AustriaK. MondalUniversiteit Antwerpen, Antwerpen, BelgiumT. T. TranUniversiteit Antwerpen, Antwerpen, BelgiumS. WertzInstitut f ür Hochenergiephysik, Vienna, AustriaG. 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 TelesInstitut f ür Hochenergiephysik, Vienna, AustriaM. SoeiroYerevan Physics Institute, Yerevan, ArmeniaW. L. Aldá JúniorUniversidade do Estado do Rio de JaneiroM. Alves Gallo PereiraUniversiteit Antwerpen, Antwerpen, BelgiumM. Barroso Ferreira FilhoYerevan Physics Institute, Yerevan, ArmeniaH. Brandao MalbouissonYerevan Physics Institute, Yerevan, ArmeniaW. CarvalhoInstitut f ür Hochenergiephysik, Vienna, AustriaJ. ChinellatoYerevan Physics Institute, Yerevan, ArmeniaE. M. Da CostaUniversiteit Antwerpen, Antwerpen, BelgiumG. G. Da SilveiraUniversiteit Antwerpen, Antwerpen, BelgiumD. De Jesus DamiãoInstitut f ür Hochenergiephysik, Vienna, AustriaS. Fonseca De SouzaUniversiteit Antwerpen, Antwerpen, BelgiumJ. MartinsUFMSC. Mora HerreraYerevan Physics Institute, Yerevan, ArmeniaK. Mota AmariloUniversidade do Estado do Rio de JaneiroL. MundimUniversiteit Antwerpen, Antwerpen, Belgium
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A bstract A search for Higgs boson pair (HH) production in association with a vector boson V (W or Z boson) is presented. The search is based on proton-proton collision data at a center-of-mass energy of 13 TeV, collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 138 fb − 1 . Both hadronic and leptonic decays of V bosons are used. The leptons considered are electrons, muons, and neutrinos. The HH production is searched for in the $$ \textrm{b}\overline{\textrm{b}}\textrm{b}\overline{\textrm{b}} $$ <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:mi>b</mml:mi> <mml:mover> <mml:mi>b</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> decay channel. An observed (expected) upper limit at 95% confidence level of VHH production cross section is set at 294 (124) times the standard model prediction. Constraints are also set on the modifiers of the Higgs boson trilinear self-coupling, k λ , assuming k 2V = 1, and vice versa on the coupling of two Higgs bosons with two vector bosons, k 2V . The observed (expected) 95% confidence intervals of these coupling modifiers are − 37.7 &lt; k λ &lt; 37.2 ( − 30.1 &lt; k λ &lt; 28.9) and − 12.2 &lt; k 2V &lt; 13.5 ( − 7.2 &lt; k 2V &lt; 8.9), respectively.

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