T T Hong, V K Le, L T T Phuong, N C Hoi, N T K Ngan, N H T Nha
{"title":"Decays of standard model like higgs boson h → γγ, Zγ in a minimal left-right symmetric model","authors":"T T Hong, V K Le, L T T Phuong, N C Hoi, N T K Ngan, N H T Nha","doi":"10.1093/ptep/ptae029","DOIUrl":null,"url":null,"abstract":"Two decay channels h → γγ, Zγ of the Standard Model-like Higgs in a left-right symmetry model are investigated under recent experimental data. We will show there exist one-loop contributions that affect the h → Zγ amplitude, but not the h → γγ amplitude. From numerical investigations, we show that the signal strength μZγ of the decay h → Zγ is still constrained strictly by that of h → γγ, namely $|\\Delta \\mu _{\\gamma \\gamma }|<38\\%$ results in max $|\\Delta \\mu _{Z \\gamma }|<46\\%$. On the other hand, the future experimental sensitivity $|\\Delta \\mu _{\\gamma \\gamma }|=4\\%$ still allows |ΔμZγ| reaches to values larger than the expected sensitivity $|\\Delta \\mu _{Z \\gamma }|=23\\%$.","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":null,"pages":null},"PeriodicalIF":4.3000,"publicationDate":"2024-03-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Electronic Materials","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1093/ptep/ptae029","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
Abstract
Two decay channels h → γγ, Zγ of the Standard Model-like Higgs in a left-right symmetry model are investigated under recent experimental data. We will show there exist one-loop contributions that affect the h → Zγ amplitude, but not the h → γγ amplitude. From numerical investigations, we show that the signal strength μZγ of the decay h → Zγ is still constrained strictly by that of h → γγ, namely $|\Delta \mu _{\gamma \gamma }|<38\%$ results in max $|\Delta \mu _{Z \gamma }|<46\%$. On the other hand, the future experimental sensitivity $|\Delta \mu _{\gamma \gamma }|=4\%$ still allows |ΔμZγ| reaches to values larger than the expected sensitivity $|\Delta \mu _{Z \gamma }|=23\%$.