{"title":"衰减\\(\\tau \\rightarrow f_0(\\pi ,K) \\nu _\\tau \\)和\\(\\tau \\rightarrow 3 \\pi \\nu _\\tau \\)占贡献 \\(f_0(500)\\)","authors":"M. K. Volkov, A. A. Pivovarov, K. Nurlan","doi":"10.1140/epja/s10050-025-01531-7","DOIUrl":null,"url":null,"abstract":"<div><p>In the <span>\\(U(3) \\times U(3)\\)</span> quark NJL model, <span>\\(\\tau \\)</span> lepton decays with the production of scalar mesons <span>\\(f_0(\\pi ,K)\\)</span> and neutrinos are studied, where <span>\\(f_0=f_0(500), f_0(980)\\)</span>. It is shown that these decays mainly occur via contact channels and channels with axial-vector mesons <span>\\(a_1(1260)\\)</span>, <span>\\(K_1(1270)\\)</span> and <span>\\(K_1(1400)\\)</span>. All mesons are considered as quark-antiquark states in this case. The obtained results can be considered as predictions for future experiments. The obtained estimates for the branching fractions of the <span>\\(\\tau \\rightarrow \\pi ^-2\\pi ^0 \\nu _\\tau \\)</span> decay taking into account the contributions of the <span>\\(\\rho \\pi \\)</span> and <span>\\(f_0(500)\\pi \\)</span> states are in satisfactory agreement with experimental data.</p></div>","PeriodicalId":786,"journal":{"name":"The European Physical Journal A","volume":"61 3","pages":""},"PeriodicalIF":2.6000,"publicationDate":"2025-03-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Decays \\\\(\\\\tau \\\\rightarrow f_0(\\\\pi ,K) \\\\nu _\\\\tau \\\\) and \\\\(\\\\tau \\\\rightarrow 3 \\\\pi \\\\nu _\\\\tau \\\\) accounting for the contribution of \\\\(f_0(500)\\\\)\",\"authors\":\"M. K. Volkov, A. A. Pivovarov, K. Nurlan\",\"doi\":\"10.1140/epja/s10050-025-01531-7\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>In the <span>\\\\(U(3) \\\\times U(3)\\\\)</span> quark NJL model, <span>\\\\(\\\\tau \\\\)</span> lepton decays with the production of scalar mesons <span>\\\\(f_0(\\\\pi ,K)\\\\)</span> and neutrinos are studied, where <span>\\\\(f_0=f_0(500), f_0(980)\\\\)</span>. It is shown that these decays mainly occur via contact channels and channels with axial-vector mesons <span>\\\\(a_1(1260)\\\\)</span>, <span>\\\\(K_1(1270)\\\\)</span> and <span>\\\\(K_1(1400)\\\\)</span>. All mesons are considered as quark-antiquark states in this case. The obtained results can be considered as predictions for future experiments. The obtained estimates for the branching fractions of the <span>\\\\(\\\\tau \\\\rightarrow \\\\pi ^-2\\\\pi ^0 \\\\nu _\\\\tau \\\\)</span> decay taking into account the contributions of the <span>\\\\(\\\\rho \\\\pi \\\\)</span> and <span>\\\\(f_0(500)\\\\pi \\\\)</span> states are in satisfactory agreement with experimental data.</p></div>\",\"PeriodicalId\":786,\"journal\":{\"name\":\"The European Physical Journal A\",\"volume\":\"61 3\",\"pages\":\"\"},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2025-03-28\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The European Physical Journal A\",\"FirstCategoryId\":\"4\",\"ListUrlMain\":\"https://link.springer.com/article/10.1140/epja/s10050-025-01531-7\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The European Physical Journal A","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1140/epja/s10050-025-01531-7","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
Decays \(\tau \rightarrow f_0(\pi ,K) \nu _\tau \) and \(\tau \rightarrow 3 \pi \nu _\tau \) accounting for the contribution of \(f_0(500)\)
In the \(U(3) \times U(3)\) quark NJL model, \(\tau \) lepton decays with the production of scalar mesons \(f_0(\pi ,K)\) and neutrinos are studied, where \(f_0=f_0(500), f_0(980)\). It is shown that these decays mainly occur via contact channels and channels with axial-vector mesons \(a_1(1260)\), \(K_1(1270)\) and \(K_1(1400)\). All mesons are considered as quark-antiquark states in this case. The obtained results can be considered as predictions for future experiments. The obtained estimates for the branching fractions of the \(\tau \rightarrow \pi ^-2\pi ^0 \nu _\tau \) decay taking into account the contributions of the \(\rho \pi \) and \(f_0(500)\pi \) states are in satisfactory agreement with experimental data.
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