K. Nurlan

activity

20162026

most citedOn the mixing angle of the vector mesons

ω (782)

and

ϕ (1020)

8 citations · 8 across the 18 of their papers we have counts for

collaborators

Showing 2019Show all

5 papers · 1 filter

hep-ph2019

The decay $τ \to K^{* 0} (892) K^{-} ν_{τ}$ in the extended NJL model

M. K. Volkov, A. A. Pivovarov, K. Nurlan

In the extended Nambu -- Jona-Lasinio model, the decay width of $τ \to K^{* 0} (892) K^{-} ν_{τ}$ is calculated. The contributions from the contact diagram and diagrams with intermediate…

hep-ph2019

The decay $τ \to K^{*-} (892) η ν_{τ}$ in the NJL model

M. K. Volkov, A. A. Pivovarov, K. Nurlan

The decay width $τ \to K^{*-} (892) η ν_{τ}$ was calculated in the Nambu--Jona-Lasinio model. Four channels were taken into account: the contact channel (the final states are directly p…

hep-ph2019

The decays $τ \to [ω (782), ϕ (1020)] K^{-} ν_{τ}$ in the extended NJL model

M. K. Volkov, A. A. Pivovarov, K. Nurlan

In the extended Nambu--Jona-Lasinio model, the decay widths of the processes $τ \to [ω (782), ϕ (1020)] K^{-} ν_{τ}$ were calculated. The intermediate channels with axial vector ($K_{1}…

hep-ph2019

The decays $τ \to (K, K (1460)) ν_{τ}$ and the value of the weak decay coefficients $F_{K}$ and $F_{K^{^{'}}}$ in the extended NJL model

M. K. Volkov, K. Nurlan, A . A. Pivovarov

In the extended NJL model, the decay widths of $τ \to (K, K (1460)) ν_{τ}$ , $(K, K (1460)) \to μ ν_{μ}$ are calculated. The contributions from intermediate axial-vector meson…

hep-ph2019

The tetraquark $K_{1} (1400)$ in the decays $τ \to [ω (782), ϕ (1020)] K^{-} ν_{τ}$

M. K. Volkov, Aleksey A. Pivovarov, K. Nurlan

In the extended Nambu--Jona-Lasinio model, the decay widths of the processes $τ \to [ω (782), ϕ (1020)] K^{-} ν_{τ}$ were calculated. The intermediate strange quark-antiquark mesons in…

The decay τ→K∗0(892)K−ντ​ in the extended NJL model

The decay τ→K∗−(892)ηντ​ in the NJL model

The decays τ→[ω(782),ϕ(1020)]K−ντ​ in the extended NJL model

The decays τ→(K,K(1460))ντ​ and the value of the weak decay coefficients FK​ and FK′​ in the extended NJL model

The tetraquark K1​(1400) in the decays τ→[ω(782),ϕ(1020)]K−ντ​

The decay $τ \to K^{* 0} (892) K^{-} ν_{τ}$ in the extended NJL model

The decay $τ \to K^{*-} (892) η ν_{τ}$ in the NJL model

The decays $τ \to [ω (782), ϕ (1020)] K^{-} ν_{τ}$ in the extended NJL model

The decays $τ \to (K, K (1460)) ν_{τ}$ and the value of the weak decay coefficients $F_{K}$ and $F_{K^{^{'}}}$ in the extended NJL model

The tetraquark $K_{1} (1400)$ in the decays $τ \to [ω (782), ϕ (1020)] K^{-} ν_{τ}$