{"title":"Doubly-charged scalar in four-body decays of neutral flavored mesons","authors":"T. Wang 王, Geng 史 Li 李, Y. Jiang 姜, G. Wang 王","doi":"10.1088/1674-1137/43/1/013103","DOIUrl":null,"url":null,"abstract":"We study the four-body decays of neutral flavored mesons, including K ¯ 0 , D0, B ¯ 0 , and B ¯ s 0 . These processes, which could be induced by a hypothetical doubly-charged scalar particle, do not conserve the lepton number. Assuming, as an example, that the mass of the doubly-charged particle is 1000 GeV, and using the upper bounds of the couplings, we calculate the branching ratios of different channels. For K ¯ 0 → h 1 + h 2 + e − e − , D 0 → h 1 − h 2 − e + e + , and B ¯ d , s 0 → h 1 + h 2 + e − e − , it is of the order of 10−30, 10−32–10−29, and 10−33–10−28, respectively. Based on the experimental results for the D 0 → h 1 − h 2 − l 1 + l 2 + channels, we also find the upper limit for the quantity s Δ h i j M Δ 2 .","PeriodicalId":345560,"journal":{"name":"Chinese Physical Society","volume":"135 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Chinese Physical Society","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/1674-1137/43/1/013103","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 four-body decays of neutral flavored mesons, including K ¯ 0 , D0, B ¯ 0 , and B ¯ s 0 . These processes, which could be induced by a hypothetical doubly-charged scalar particle, do not conserve the lepton number. Assuming, as an example, that the mass of the doubly-charged particle is 1000 GeV, and using the upper bounds of the couplings, we calculate the branching ratios of different channels. For K ¯ 0 → h 1 + h 2 + e − e − , D 0 → h 1 − h 2 − e + e + , and B ¯ d , s 0 → h 1 + h 2 + e − e − , it is of the order of 10−30, 10−32–10−29, and 10−33–10−28, respectively. Based on the experimental results for the D 0 → h 1 − h 2 − l 1 + l 2 + channels, we also find the upper limit for the quantity s Δ h i j M Δ 2 .