{"title":"Constraining anomalous $ZH$ couplings using $Z$ polarization parameters","authors":"P. Sarmah, K. Rao, S. Rindani","doi":"10.22323/1.390.0277","DOIUrl":null,"url":null,"abstract":"We study the anomalous ZZH vertex contributing to the Higgsstrahlung process at the LHC and future e+e− colliders using the polarization of the Z as a probe. We calculate the eight independent polarization parameters of the Z boson by using the spin density matrix formalism. We estimate 1σ limits on the anomalous ZZH couplings using the angular asymmetries of leptons from Z decay which are simply related to the eight polarization parameters. We discuss the results for a) two possible c.m.energies ( √ s =) 250 GeV and 500 GeV for the e+e− colliders, with the possibility of polarized e+e− beams, b) LHC at √ s = 14 TeV.","PeriodicalId":20428,"journal":{"name":"Proceedings of 40th International Conference on High Energy physics — PoS(ICHEP2020)","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2021-02-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of 40th International Conference on High Energy physics — PoS(ICHEP2020)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.22323/1.390.0277","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
We study the anomalous ZZH vertex contributing to the Higgsstrahlung process at the LHC and future e+e− colliders using the polarization of the Z as a probe. We calculate the eight independent polarization parameters of the Z boson by using the spin density matrix formalism. We estimate 1σ limits on the anomalous ZZH couplings using the angular asymmetries of leptons from Z decay which are simply related to the eight polarization parameters. We discuss the results for a) two possible c.m.energies ( √ s =) 250 GeV and 500 GeV for the e+e− colliders, with the possibility of polarized e+e− beams, b) LHC at √ s = 14 TeV.