Abstract

AbstractVector boson scattering (VBS) can be idealized as an interaction of gauge bosons radiated from initial state quarks, yielding a final state with two bosons and two jets (VVjj) where V can be W or Z bosons. These VBS processes are widely recognized as being the most sensitive to the effects of new physics, which can be described using the effective field theory (EFT) approach. In this paper, we discuss the implementation of the EFT dimension-eight operators in the study of VBS in the \(pp \rightarrow WZjj\) channel. As a final state, two jets and three leptons in proton-proton collisions at \(\sqrt{s} = 13\) TeV (\(pp \rightarrow 2 jets + WZ\) \(\rightarrow \) j j l \(\nu \) \(l^{'}\) \(l^{'}\) where \(l = e\), \(\mu \)) are observed at the Large Hadron Collider (LHC). The data used are collected by the Compact Muon Solenoid (CMS) detector during Run II from the years 2016–2018 with an integrated luminosity of 137 \(fb^{-1}\). Results for the searches of the anomalous quartic gauge couplings (aQGC) in the electroweak WZ data sample for the full Run II are presented.KeywordsVector Boson Scattering (VBS)Beyond Standard Model(BSM)Effective Field Theory (EFT)

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.