Constraints on anomalous Higgs boson couplings to vector bosons and fermions in its production and decay using the four-lepton final state

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Dharmaratna ,S Perriès ,Jonathan Guiang ,É Chapon ,S Sánchez Cruz ,K F Di Petrillo ,B R Yates ,Yuan Li ,A Rácz ,B B Tannenwald ,K M Black ,A Sánchez-Hernández ,I J Watson ,S M Silva Do Amaral ,Ian Reed ,C S Moon ,Silvia Goy López ,G A Alves ,G S F Stephans ,C M Kuo ,P K Netrakanti ,P Milenović ,V Veszprémi ,M Déjardin ,S P Ratti ,K H Lo ,F Canelli ,Anna Tsatsos ,D A Sanz Becerra ,Neha Rawal ,K W Bell ,F J M Geurts ,H A Weber ,Andres Mateus Vargas Hernandez ,P A Razis ,Laurits Tani ,C A Mondragon Herrera ,Shamik Ghosh ,B L Winer ,P R Pujahari ,R M Chatterjee ,K Özdemir ,D A Hangal ,Jay Mathew Lawhorn ,P C Tiwari ,W Y Sun ,J H Bhyun ,K Cankoçak ,M A Mahmoud ,M I Asghar ,Daniel Diaz ,J R Komaragiri ,Florian Eble ,M T Grippo ,J Molnár ,H R Hoorani ,G Martı́nez ,T A Gómez Espinosa ,A Çakır ,I D Reid ,M I Josa ,I González Caballero ,M A Ciocci ,J Königsberg ,V K Muraleedharan Nair Bindhu ,B Alvarez González ,D Ferenček ,Mohammad Hassan Hassanshahi ,W A Khan ,J Milošević ,Hevjin Yarar ,M S Kim ,D K Mishra ,C Peng ,J A Murillo Quijada ,Piero Giorgio Verdini ,J D Tapia ∋Takaki ,K Öcalan ,S M Etesami ,H S Kim ,E Pérez ,S C Eno ,D H Kim ,A C Marini ,G Hamel De Monchenault ,W T Ford ,T Csörgõ ,H J Simonis ,Kathryn Coldham ,B Işıldak ,K J Pena Rodriguez ,L I Estevez Banos ,M R Adams ,C Peña ,Janik Walter Andrejkovic ,M Besançon ,G P Van Onsem ,Attila József Rádl ,M M A Gadallah ,S Y Hoh ,R D Field ,Z Y You ,Margaret Eminizer ,E W Vaandering ,D S Lemos ,M M Baarmand ,P Maksimović ,E M Gregores ,K H M Kwok ,G W Wilson ,M P Rauch ,Viacheslav Bunichev ,C Hajdú ,Ž Antunović ,P H Chen ,J M Seixas ,G B Cerati ,S Argirò ,S C Schuler ,A V Gritsan ,B M Joshi ,Jaehoon Lim ,S R Wagner ,P C Bhat ,I C Park ,A A Bin Anuar ,Rafael Eduardo Sosa Ricardo ,Z Szillási ,V Lemaı̂tre ,D M Newbold ,C Işik ,M A Segura Delgado ,J W Gary ,J R Gonźalez Ferńandez ,J F Benitez ,Martha Nunez Ornelas ,F Siklér ,Khawla Jaffel ,V J Smith ,K Österberg ,H Oğul ,V Rodŕıguez Bouza ,H D Yoo ,C Martínez Rivero 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,Steffie Ann Thayil ,Eric Christian Chabert ,S Dubé ,P Martínez Ruiz Del Arbol ,S Đurić ,M Csanád ,P G Mercadante ,G P Heath ,Y D Oh ,M M Defranchis ,Leonardo Lunerti ,G M Chen ,T C Herwig ,S V Gleyzer ,F Colombina ,E M Da Costa ,H Castilla‐Valdez ,Arun Muthirakalayil Madhu ,K A Hahn ,G B Yu ,N J Hadley ,A T Meneguzzo ,M K Jayananda ,O Buchmüller ,Justin Anguiano ,Francesca Maria Addesa ,K T Lau ,H S Chen ,Mikko Lotti ,Tao Huang ,V Milošević ,Maciej Malawski ,J S Bonilla ,Alberto Orso Maria Iorio ,B Ristić ,Tamer Elkafrawy ,A G Delannoy ,K Ellis ,Hsin-Yeh Wu ,Dominic Stafford ,D U J Sonnadara ,Qiang Li ,R G Kellogg ,M Lipiński ,J R Vlimant ,Ashish Sehrawat ,J L Faure ,Oleg Filatov ,Stefan Wünsch ,F Ramírez ,L S Durkin ,I J Cabrillo ,U K Yang ,Diego Matos Figueiredo ,F Nessi‐Tedaldi ,Ravindra Kumar Verma ,Yechan Kang ,G Önengüt ,Claire Savard ,T Q Nguyen ,J J Brooke ,V D Elvira ,T Á Vámi ,Y Chào ,E A Yetkin ,V E Barnes ,M R Darwish ,R Y Zhu ,S Scarfì ,M R Di Domenico ,I S Donertas ,M Waßmer ,J B Singh ,C Tuvé ,J A Brochero Cifuentes ,I Hoş ,Grigorii B Pivovarov ,P H Butler ,Sanjeev Kumar ,Shaun Hogan ,Н Голубев ,S Czellár ,D M Raymond ,J F Schulte ,S S Yu ,Nicolaus Kratochwil ,J M Hernández ,Amandeep Singh Bakshi ,D Horváth ,A Calderón ,S F Novaes ,Michael Benjamin Andrews ,Wing Yan Wong ,C A Salazar González ,S Webb ,Evan Koenig ,Arun Kumar ,M E Dinardo ,Balaji Venkat Sathia Narayanan ,P Adžić ,I S Zorbakir ,S J Qian ,J R Patterson ,Byung Hun Oh ,Г Тамулайтис ,Maksym Titov ,Ram Krishna Dewanjee ,M A Iqbal ,Z L Trócsányi ,M S Ryu ,P T Cox ,Clemencia Mora Herrera ,M A Wadud ,Konstantin Shchablo ,B S Yuldashev ,A Vaitkevičius ,Д Педрини ,Da Young Kang ,B C Choudhary ,T J Kim ,J G Branson ,A C Mignerey ,T Šuša ,G Pásżtor ,S I Cooper ,S Lökòs ,O González López ,I O Atakisi ,S W Lee ,F García ,Matteo Pisano ,R López-Fernández ,A Rinkevičius ,Abbas Hassani ,Stephen Trembath-Reichert ,Federica Maria Simone ,K F Chen ,Y Güler ,Minseok Oh ,Z H Lin ,R M Harris ,Р Тенчини ,W L Aldá Júnior ,J Kašpar ,N V Tran ,G M Dallavalle ,L A T Bauerdick ,J Fernández Menéndez ,S Consuegra Rodŕıguez ,Lucas Wiens ,D D C Wickramarathna ,K A Wozniak ,E A De Wolf ,Suzanne Rosenzweig ,E Eşkut ,Sitong An ,D Kotliński ,K Höepfner ,C Fernandez Bedoya ,P K Behera ,S Özkorucuklu ,J L Dulemba ,M Aguilar-Benı́tez ,G G Da Silveira ,Francesco Carnevali ,S Çerçi ,N Z Jomhari ,Joaquin Emilo Siado ,Antonello Pellecchia ,B C Radburn-Smith ,H Aarup Petersen ,A K Virdi ,J K Heikkilä ,Ralf Florian Von Cube ,V R Tavolaro ,J P Fernández Ramos ,Michal Bluj ,Adam Jackson Parker ,S S Chhibra ,Álvaro Navarro Tobar ,Amanda Sarkar ,S I Pak ,Д Сеитова ,В Сулимов ,K Buńkowski ,K J R Cormier ,U G Tok ,G M Bilei ,M T Lucchini ,H Flächer ,M Ramírez-García ,Peter Hansen ,A W Jung ,J P Cumalat ,S Gianì ,D H Moon ,W A T Wan Abdullah ,M W Arenton ,H B Newman ,Siqi Yuan ,A E Simsek ,T Krämer ,A K Kalsi ,J Królikowski ,T Novák ,B Wysłouch ,S B Beri ,G Köpp ,M Roguljić ,D M Morse ,Kang Li ,D Giljanović ,C H Shepherd-Themistocleous ,Pablo Matorras Cuevas ,M Kröhn ,A A Abdelalim ,Michael Henry Schmitt ,S K Park ,Moisés León Coello ,D De Jesus Damião ,J Andreä ,G Gómez ,E Clément ,V Brigljević ,K S Lee ,Krisztián Farkas ,Diwakar Vats ,Aashaq Shah ,J P Chou ,D Ćutts ,H Malbouisson ,H C Kaestli ,I R Tomalin ,N Raičević ,Claudia-Elisabeth Wulz ,A García-Bellido ,J H Kim ,Chiara Aimè ,Sushrut Karmarkar ,C E Gerber ,P J Fernández Manteca ,Jonas Rübenach ,M T Meinhard ,Jesús Puerta Pelayo ,R Démina ,Tu Thong Tran

doi:10.1103/physrevd.104.052004

Abstract

Studies of $CP$ violation and anomalous couplings of the Higgs boson to vector bosons and fermions are presented. The data were acquired by the CMS experiment at the LHC and correspond to an integrated luminosity of 137 fb$^{-1}$ at a proton-proton collision energy of 13 TeV. The kinematic effects in the Higgs boson's four-lepton decay H $\to$ 4$\ell$ and its production in association with two jets, a vector boson, or top quarks are analyzed, using a full detector simulation and matrix element techniques to identify the production mechanisms and to increase sensitivity to the Higgs boson tensor structure of the Higgs boson interactions. A simultaneous measurement is performed of up to five Higgs boson couplings to electroweak vector bosons (HVV), two couplings to gluons (Hgg), and two couplings to top quarks (Htt). The $CP$ measurement in the Htt interaction is combined with the recent measurement in the H $\to$ $\gamma\gamma$ channel. The results are presented in the framework of anomalous couplings and are also interpreted in the framework of effective field theory, including the first study of $CP$ properties of the Htt and effective Hgg couplings from a simultaneous analysis of the gluon fusion and top-associated processes. The results are consistent with the standard model of particle physics.

Highlights

The discovery by the ATLAS and CMS Collaborations of a Higgs boson (H) with a mass of ≈125 GeV [1,2,3] has confirmed the predictions of the standard model (SM) of particle physics [4,5,6,7,8,9,10]
We describe the measurement of fgag3H in the ggH process, fHCPtt in the ttH and tH processes, and the combination of the two where the top quark contributes to the gluon fusion loop
The improvements result from a significantly increased sample of H bosons and from a detailed analysis of kinematic distributions of the particles associated with the H boson production in addition to kinematic distributions in its decay

Summary

Introduction

The discovery by the ATLAS and CMS Collaborations of a Higgs boson (H) with a mass of ≈125 GeV [1,2,3] has confirmed the predictions of the standard model (SM) of particle physics [4,5,6,7,8,9,10]. In theories beyond the SM (BSM), H boson interactions may generate several of them, which lead to new interaction tensor structures, both CP even and CP odd. The new anomalous tensor structures of the H boson interactions may appear through loop corrections in SM processes, but the size of their contributions is beyond the current experimental sensitivity. The CP-odd anomalous couplings between the H boson and either the top quark or new BSM particles, fermions or bosons, contributing to the gluon fusion loop may generate CP violation in Hgg interactions (where g stands for gluon).

Objectives

Results

Conclusion