The Right of &lt;i&gt;Actio Popularis&lt;/i&gt; before International Courts and Tribunals

Ahmadov, Farid

doi:10.1163/9789004380981

Cited by 8 publications

(1 citation statement)

References 96 publications

(20 reference statements)

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“…At the same time, due to the energy restrictions caused by the τ -lepton mass, intermediate mesons in these states play the main role in the τ -lepton decays. That is why, the use of the extended NJL model allowed a successful description of a series of τ -decays, specifically τ → (π, π(1300))ν τ [24], τ → (η, η )πν τ [25], τ → πων τ [26], τ → (η, η )2π [27], τ → (ρ(770), ρ(1450))ν τ , τ → (K * (892), K * (1410))ν τ [28], τ → K − π 0 ν τ [29].…”

Section: Introductionmentioning

confidence: 99%

Decays τ → (η, η')K–ντ in the extended Nambu–Jona-Lasinio model

Волков

Пивоваров

2016

Jetp Lett.

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The decays τ → (η, η )K − ντ are described in the framework of the extended Nambu-Jona-Lasinio model. Both full and differential widths of these decays are calculated. The vector and scalar channels are considered. In the vector channels, the subprocesses with intermediate K * (892) and K * (1410) mesons play the main role. In the scalar channels, the subprocesses with intermediate K * 0 (800) and K * 0 (1430) mesons are taken into account. Scalar channels play a less important role in calculation of the full width of the decay τ → (η, η )K − ντ . The obtained results are in satisfactory agreement with the experimental data.

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Section: Introductionmentioning

confidence: 99%