Combined measurements of Higgs boson couplings in proton\u2013proton collisions at sqrt{s}=13,text {Te}text {V}

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Quero,A Canepa,Jaehoon Lim ,P Kontaxakis,M Aldaya Martin,Wolfram Dietrich Zeuner ,F M Stober,J Hoß ,D Soldi,A Baden,E De La Cruz-Burelo,G Pásżtor ,K Höepfner ,M Naimuddin,C Scharf,A Di Florio,Peter Hansen ,Mehmet Özgür Sahin ,A Bornheim,G Bauer,A Kayis Topaksu,S Afanasiev,G Grenier,A Di Mattia,B Penning,Joaquin Emilo Siado ,В Сулимов ,Arun Kumar,A De Wit,M I Nagy,Jesús Puerta Pelayo ,Reddy Pratap Gandrajula ,B Ujvári ,R G Kellogg,А Калинин ,A Meyer,A Benecke,Alberto Sánchez Hernández ,V Bunichev,H Lee,G Cucciati,C De Oliveira Martins ,J S Wood ,P E Karchin,R Sharma,T Weiler,S Goy Lopez,T Tabarelli De Fatis,J Andreä ,G Paspalaki,O Hlushchenko,J A Brochero Cifuentes,M De Mattia,D Doḿınguez Damiani ,P Milenović ,K Cankoçak ,G M Dallavalle,E Eskandari Tadavani,L S Durkin,M Schmitt ,M P Rauch,Antônio Rossi ,L F Chaparro Sierra,M Mohammadi Najafabadi,G Mäggi ,F Dölek ,R López-Fernández ,Tao Huang ,M I Asghar,P Chang,R B Garg,А Спиридонов ,I González Caballero ,H Wei,G P Van Onsem,T Maënpaä ,A Calderón ,J D Ruiz Alvarez,G B Mohanty,R Del Burgo,P Rebello Teles,J Duarte Campderros,P Van Hove,P Bloch,F Pauß ,M Franco Sevilla,R Granier De Cassagnac,M C Duran-Osuna,S Carrillo Moreno,B Wysłouch ,John Michael Marraffino ,N De Filippis,G B Yu,H Castilla‐Valdez ,J R Gonźalez Ferńandez ,P Kyberd,G De Lentdecker,T Mitchell,V Myronenko,A Çelik ,F Özok ,E Belchior Batista Das Chagas,M Guchait,E A De Wolf,S Czellár ,K W Bell,F Simonetto,Michael Benjamin Andrews ,B Işıldak ,T Y Ling,T R Fernandez Perez Tomei,A Di Crescenzo,P C Tiwari,P Van Mulders,W Ji,J Suarez Gonzalez,G G Da Silveira,C Oropeza Barrera,P De Castro Manzano,K Wichmann,N Van Remortel,R Gonzalez Suarez,Feng Liu ,Q N Xu ,E Clément ,Thea Klaeboe Aarrestad ,J A Murillo Quijada,Mohd Adli Bin Ali ,R Démina ,E Pérez ,D Ferenček ,Р Тенчини ,М Фингер ,K H M Kwok,O Zenaiev,A García-Bellido ,A Polatöz ,V Dūdėnas ,R Teixeira De Lima,V Monaco,C Vander Velde,Sh Jain,J S H Lee,S Banerjee,A Di Francesco,N Zaganidis,C S Moon,H Van 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Herrera,E Di Marco,P Das,M Lipiński ,C Tuvé ,C A Carrillo Montoya,I Babounikau,I De Bruyn,В Качанов ,Sanjeev Kumar ,W T Hung,G L Pinna Angioni,Yuan Li ,R Bhattacharya,C F Gonźalez Herńandez ,Kin Ho Lo ,S Abu Zeid,V Brigljević ,S Slabospitskii,C Madrid,U K Yang,Deepak Kumar Sahoo ,Y Güler ,C Wissing,E M Da Costa,D Kotliński ,F Mohamad Idris,J M Vizan Garcia,W Van Doninck,M Csanád ,S Özkorucuklu ,H S Chen,Y Choi,S Petrushanko,V Veszprémi ,O Behnke,G Gökbulut ,A Escalante Del Valle,O González López ,M Kröhn ,D Ćutts ,M Ramírez-García ,M Barrio Luna,J Almond,S Somalwar,A A Abdelalim,M R Adams,M Grünewald ,R Vilar Cortabitarte,K Sandeep,C Ávila ,C Martínez Rivero ,Mara Senghi Soares ,D A Sanz Becerra,M Besançon ,G Correia Silva,S M A Ghiasi Shirazi,U Bhawandeep,S Roy Chowdhury ,S Lacaprara,Y Chào ,É Chapon ,P Major,M Vidal Marono,A K Virdi,Yang Yu ,F Nessi‐Tedaldi ,S Bheesette,T Lenzi,A Rizzi,J M Hernández ,E Carrera Jarrin,F De Guio,R Taus,D Blöch ,D De Jesus Damião ,S Kaur,A Rácz ,W De Boer,F Torres Da Silva De Araujo,D Matos Figueiredo,M Jones,S Bhattacharya,S Williamson,H W Wulsin,M A Segura Delgado,Zainol Abidin Ibrahim ,J Malclès ,I Dumanoğlu ,J Fernández Menéndez

doi:10.1140/epjc/s10052-019-6909-y

Abstract

Combined measurements of the production and decay rates of the Higgs boson, as well as its couplings to vector bosons and fermions, are presented. The analysis uses the LHC proton–proton collision data set recorded with the CMS detector in 2016 at sqrt{s}=13,text {Te}text {V} , corresponding to an integrated luminosity of 35.9{,text {fb}^{-1}} . The combination is based on analyses targeting the five main Higgs boson production mechanisms (gluon fusion, vector boson fusion, and associated production with a mathrm {W} or mathrm {Z} boson, or a top quark-antiquark pair) and the following decay modes: mathrm {H} rightarrow gamma gamma , mathrm {Z}mathrm {Z}, mathrm {W}mathrm {W}, mathrm {tau }mathrm {tau }, mathrm {b} mathrm {b} , and mathrm {mu }mathrm {mu }. Searches for invisible Higgs boson decays are also considered. The best-fit ratio of the signal yield to the standard model expectation is measured to be mu =1.17pm 0.10, assuming a Higgs boson mass of 125.09,text {Ge}text {V} . Additional results are given for various assumptions on the scaling behavior of the production and decay modes, including generic parametrizations based on ratios of cross sections and branching fractions or couplings. The results are compatible with the standard model predictions in all parametrizations considered. In addition, constraints are placed on various two Higgs doublet models.

Highlights

Higgs boson mass is near the electroweak scale, since it is not protected in the standard model (SM) from large quantum corrections [15–19]
A set of combined measurements of Higgs boson production and decay rates has been presented, along with the consequential constraints placed on its couplings to standard model (SM) particles, and on the parameter spaces of several beyond the standard model (BSM) scenarios
The combination is based on analyses targeting the gluon fusion and vector boson fusion production modes, and associated production with a vector boson or a pair of top quarks

Summary

Introduction

Higgs boson mass is near the electroweak scale, since it is not protected in the SM from large quantum corrections [15–. Leading-order Feynman b, , diagrams for Higgs boson decays in the H → bb, H → τ τ , and H → μμ (upper left); H. q g t t q to the five main production processes, the contributions due to Higgs boson production in association with a single top quark (tH) and either a W boson (tHW) or a quark (tHq), as shown, are included in the analyses that have some sensitivity to them. The tH cross section is small in the SM, being approximately 14% of the ttH cross section, due to the destructive interference between the diagrams shown, which involve the coupling of the Higgs boson to W bosons (tHW process) and top quarks (tHq process). The ATLAS and CMS Collaborations have published combined measurements of Higgs √boson production rates, decay rates, and couplings with the s = 7 and 8 TeV LHC Run 1 data [54,55].

The CMS detector

Analyses included in the combination

Statistical uncertainties in simulation

Theoretical uncertainties in gluon fusion

Combination procedure

Systematic uncertainties

Signal strength and cross section fits

Stage 0 simplified template cross sections

Measurements of Higgs boson couplings

Generic model within κ-framework assuming resolved loops

Generic model within κ-framework with effective loops

Generic model with effective loops and coupling modifier ratios

Fits of vector boson and fermion coupling modifiers

Compatibility of measurements with the SM

Findings

10 Summary

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Journal: Zeitschrift für Physik C: Particles and Fields	Publication Date: May 1, 2019
Citations: 317	License type: open-access

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Combined measurements of Higgs boson couplings in proton\u2013proton collisions at sqrt{s}=13,text {Te}text {V}

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