Decays <i>τ</i> → <i>ππην<sub>τ</sub></i> and <i>τ</i> → <i>πηην<sub>τ</sub> </i>in the extended Nambu–Jona-Lasinio model
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Decays τ → ππηντ and τ → πηηντ in the extended Nambu–Jona-Lasinio model

Распады τ → ππηντ и τ → πηηντ в расширенной модели Намбу–Иона–Лазинио

Abstract

In the framework of the extended Nambu–Jona-Lasinio model, the processes τ → ππη(η′)ντ and τ → πηη(η′)ντ are considered taking into account mesons in the ground and first radially excited intermediate states. It is shown that in the processes τ → ππη(η′)ντ the vector channel is dominant, and in the processes τ → πηη(η′)ντ the main contribution is given by the axial-vector channel. The scalar meson a0 plays a dominant role in processes with two η mesons in the final state. The significance of the relative phase between the ground and first radially excited states for these processes is shown. The obtained results for the τ → ππηντ process are in satisfactory agreement with the recent experimental data from BaBar and CMD-3, which differ from the averaged values given in the PDG tables.

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