{"title":"Full angular spectrum analysis of tensor current contribution to $A_{cp}(\\tau \\rightarrow K_{s} \\pi \\nu_{\\tau})$.","authors":"L. Dhargyal","doi":"10.31526/LHEP.3.2018.03","DOIUrl":null,"url":null,"abstract":"Babar collaboration has reported an intriguing opposite sign in the integrated decay rate asymmetry $A_{cp}(\\tau \\rightarrow K_{s} \\pi \\nu_{\\tau})$ than that of SM prediction from the known $K^{0}$ - $\\bar{K^{0}}$ mixing. Babar's result deviate from the SM prediction by about 2.7$\\sigma$. If the result stands with higher precision in the future experiments, the observed sign anomaly in the $A_{cp}(\\tau \\rightarrow K_{s} \\pi \\nu_{\\tau})$ can most likely come only from a NP. In this work we present a full angular spectrum analysis on the contribution to $A_{cp}(\\tau \\rightarrow K_{s} \\pi \\nu_{\\tau})$ coming from the tensorial term. Assuming the real part of the NP tensorial coupling is negligible compare to its imaginary part and with $A_{cp}(\\tau \\rightarrow K_{s} \\pi \\nu_{\\tau})$ and $Br(\\tau \\rightarrow K_{s} \\pi \\nu_{\\tau})$ as data points to fit the imaginary part of the NP coupling, we have been able to fit the result within 1$\\sigma$ of the experimental values.","PeriodicalId":36085,"journal":{"name":"Letters in High Energy Physics","volume":"16 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2016-05-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Letters in High Energy Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.31526/LHEP.3.2018.03","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"Physics and Astronomy","Score":null,"Total":0}
引用次数: 5
Abstract
Babar collaboration has reported an intriguing opposite sign in the integrated decay rate asymmetry $A_{cp}(\tau \rightarrow K_{s} \pi \nu_{\tau})$ than that of SM prediction from the known $K^{0}$ - $\bar{K^{0}}$ mixing. Babar's result deviate from the SM prediction by about 2.7$\sigma$. If the result stands with higher precision in the future experiments, the observed sign anomaly in the $A_{cp}(\tau \rightarrow K_{s} \pi \nu_{\tau})$ can most likely come only from a NP. In this work we present a full angular spectrum analysis on the contribution to $A_{cp}(\tau \rightarrow K_{s} \pi \nu_{\tau})$ coming from the tensorial term. Assuming the real part of the NP tensorial coupling is negligible compare to its imaginary part and with $A_{cp}(\tau \rightarrow K_{s} \pi \nu_{\tau})$ and $Br(\tau \rightarrow K_{s} \pi \nu_{\tau})$ as data points to fit the imaginary part of the NP coupling, we have been able to fit the result within 1$\sigma$ of the experimental values.