Лаборатория физики высоких энергий и элементарных частиц

Decays f₁→a₀π,πππ(η) and f₁→KKπ in the chiral U(3)×U(3) quark NJL model

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

Phys. Rev. D 2025

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Decays τ→f₀(π,K)ντ and τ→3πντ accounting for the contribution of f₀(500)

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

Eur. Phys. J. A 2025

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Article Description of the processes e⁺e⁻→π⁺π⁻ and τ⁻→π⁻π⁰ντ in the NJL model

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

Nuclear Physics A 2025

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Weak Semileptonic Decays of Vector Mesons in the NJL Model

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

Int. J. Theor. Phys. 2025

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Three-Meson Tau Decays with Strange Particles in the NJL Model

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

Phys. Part. Nucl. 2025

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Amplitude analysis of the light mesons leptonic decays

K. Nurlan

J. Phys. Conf. Ser. 2025

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Description of the processes e⁺e⁻→K⁺K⁻π⁰ and e⁺e⁻→K⁺K⁻η within the extended NJL model

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

Phys. Part. Nucl. Lett. 2025

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Three-meson τ decays involving kaons and η mesons in the NJL model

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

Physical Review D 2024

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Decays of radially excited vector mesons ρ' and ω' in the extended NJL model

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

Int. J. Mod. Phys. A 2024

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The Decays τ→[K⁻K⁰π⁰,K⁻K⁺π⁻,K⁰K⁰π⁻]ντ in the NJL Quark Model

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

Phys. Part. Nucl. Lett. 2024

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Description of the decay τ→Kππντ in the NJL-type chiral quark model

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

Physical Review D 2023

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Decays τ→3Kντ in the U(3)×U(3) quark NJL model

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

European Physical Journal A 2023

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