{"title":"通过介子的轻子味道违反衰变来约束主动-轻子中微子混合","authors":"Shiyong Hu, Sam Ming-Yin Wong, Fanrong Xu","doi":"10.1007/s43673-022-00051-6","DOIUrl":null,"url":null,"abstract":"<div><p>As a hypothetic particle, a sterile neutrino can exist in types of new physics models. In this work by investigating flavor violating semileptonic and leptonic decays of <i>K</i>,<i>D</i>, and <i>B</i> mesons induced by the GeV scale sterile neutrino, we explore its allowed regions in parameter space. Analytically, we derive branching fractions of semileptonic decay <span>\\(M^{+}_{h}\\to M_{l}^{+}\\ell _{1}^{+}\\ell _{2}^{-}\\)</span> and leptonic decay <span>\\(M^{0}\\to \\ell _{1}^{-}\\ell _{2}^{+}\\)</span>, including the contribution from a new box diagram contribution due to the massive sterile neutrino. Imposing its mass ranges, we numerically analyze the active-sterile neutrino mixings in corresponding regions. We find that when the sterile neutrino mass is located in between pion and kaon mass, <i>K</i><sup>+</sup>→<i>π</i><sup>+</sup><i>e</i><sup>±</sup><i>μ</i><sup>∓</sup> gives the strongest constraint while <i>B</i><sup>+</sup>→<i>π</i><sup>+</sup><i>e</i><sup>±</sup><i>μ</i><sup>∓</sup> provides the dominated constraint when its mass in between of kaon and <i>B</i> meson. If the sterile neutrino is even heavier than <i>B</i>mesons, the LHCb <span>\\(B^{0}_{s}\\to \\mu ^{\\pm } e^{\\mp }\\)</span> results gives the strongest constraint.</p></div>","PeriodicalId":100007,"journal":{"name":"AAPPS Bulletin","volume":"32 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2022-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s43673-022-00051-6.pdf","citationCount":"0","resultStr":"{\"title\":\"Constraining active-sterile neutrino mixing via lepton flavor violating decays of mesons\",\"authors\":\"Shiyong Hu, Sam Ming-Yin Wong, Fanrong Xu\",\"doi\":\"10.1007/s43673-022-00051-6\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>As a hypothetic particle, a sterile neutrino can exist in types of new physics models. In this work by investigating flavor violating semileptonic and leptonic decays of <i>K</i>,<i>D</i>, and <i>B</i> mesons induced by the GeV scale sterile neutrino, we explore its allowed regions in parameter space. Analytically, we derive branching fractions of semileptonic decay <span>\\\\(M^{+}_{h}\\\\to M_{l}^{+}\\\\ell _{1}^{+}\\\\ell _{2}^{-}\\\\)</span> and leptonic decay <span>\\\\(M^{0}\\\\to \\\\ell _{1}^{-}\\\\ell _{2}^{+}\\\\)</span>, including the contribution from a new box diagram contribution due to the massive sterile neutrino. Imposing its mass ranges, we numerically analyze the active-sterile neutrino mixings in corresponding regions. We find that when the sterile neutrino mass is located in between pion and kaon mass, <i>K</i><sup>+</sup>→<i>π</i><sup>+</sup><i>e</i><sup>±</sup><i>μ</i><sup>∓</sup> gives the strongest constraint while <i>B</i><sup>+</sup>→<i>π</i><sup>+</sup><i>e</i><sup>±</sup><i>μ</i><sup>∓</sup> provides the dominated constraint when its mass in between of kaon and <i>B</i> meson. If the sterile neutrino is even heavier than <i>B</i>mesons, the LHCb <span>\\\\(B^{0}_{s}\\\\to \\\\mu ^{\\\\pm } e^{\\\\mp }\\\\)</span> results gives the strongest constraint.</p></div>\",\"PeriodicalId\":100007,\"journal\":{\"name\":\"AAPPS Bulletin\",\"volume\":\"32 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2022-08-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1007/s43673-022-00051-6.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"AAPPS Bulletin\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s43673-022-00051-6\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"AAPPS Bulletin","FirstCategoryId":"1085","ListUrlMain":"https://link.springer.com/article/10.1007/s43673-022-00051-6","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Constraining active-sterile neutrino mixing via lepton flavor violating decays of mesons
As a hypothetic particle, a sterile neutrino can exist in types of new physics models. In this work by investigating flavor violating semileptonic and leptonic decays of K,D, and B mesons induced by the GeV scale sterile neutrino, we explore its allowed regions in parameter space. Analytically, we derive branching fractions of semileptonic decay \(M^{+}_{h}\to M_{l}^{+}\ell _{1}^{+}\ell _{2}^{-}\) and leptonic decay \(M^{0}\to \ell _{1}^{-}\ell _{2}^{+}\), including the contribution from a new box diagram contribution due to the massive sterile neutrino. Imposing its mass ranges, we numerically analyze the active-sterile neutrino mixings in corresponding regions. We find that when the sterile neutrino mass is located in between pion and kaon mass, K+→π+e±μ∓ gives the strongest constraint while B+→π+e±μ∓ provides the dominated constraint when its mass in between of kaon and B meson. If the sterile neutrino is even heavier than Bmesons, the LHCb \(B^{0}_{s}\to \mu ^{\pm } e^{\mp }\) results gives the strongest constraint.