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| DOI | 10.1007/JHEP02(2024)215 | ||||
| Año | 2024 | ||||
| Tipo | artículo de investigación |
Citas Totales
Autores Afiliación Chile
Instituciones Chile
% Participación
Internacional
Autores
Afiliación Extranjera
Instituciones
Extranjeras
We investigate rare decays of tau leptons that occur via exchange of heavy on -shell neutrinos N-j (j =1,2). These neutrinos can be either Dirac or Majorana, and are considered to be almost degenerate in mass. The decays can thus be either lepton number conserving (LNC), tau(-/+) -> pi N--/+(j) -> pi(-/+)mu(-/+)pi(+/-), or lepton number violating (LNV), tau(-/+) -> pi N--/+(j) -> pi(-/+)mu(+/-)pi(-/+). If neutrinos are Dirac, only LNC decays are possible. If they are Majorana, both LNC and LNV are possible. We derive the corresponding expressions for the effective decay widths Gamma((X)) (eff,-/+) (X=LNC, LNV) of these rare decays, where we account for N-1 -N-2 overlap and oscillation effects and for the finite detector length effects. We then numerically evaluate these decay widths as well as the related CP violation asymmetry width triangle Gamma((X))(CP) = (Gamma((X))(eff) ,- - Gamma((X))(eff,+)). We conclude that for certain, presently allowed, ranges of the heavy -light neutrino mixing parameters, such decays and asymmetries could be observed in Belle II experiment.
| Ord. | Autor | Género | Institución - País |
|---|---|---|---|
| 1 | Cvetic, Gorazd | Hombre |
Universidad Técnica Federico Santa María - Chile
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| 2 | Kim, Choong Sun | - |
Yonsei Univ - Corea del Sur
Yonsei University - Corea del Sur |
| Fuente |
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| National Research Foundation of Korea |
| Fondo Nacional de Desarrollo Científico y Tecnológico |
| FONDECYT (Chile) |
| NRF of Korea |
| Agradecimiento |
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| This work of G.C.was supported in part by FONDECYT (Chile) Grant No. 1220095, The work of C.S.K. was supported by NRF of Korea (NRF-2022R1A5A1030700 and NRF-2022R1I1A1A01055643). |
| This work of G.C.was supported in part by FONDECYT (Chile) Grant No. 1220095, The work of C.S.K. was supported by NRF of Korea (NRF-2022R1A5A1030700 and NRF-2022R1I1A1A01055643). |