Nurlan K 1
1. Research of pedagogical conditions for the development of students’ educational independence
2. τ Lepton Decays with Production of Strange Scalar Mesons K*0(700) and K*0(1430) in the Extended Nambu–Jona-Lasinio Model
3. 1 /Nc approximation and universality of vector mesons
4. Decays τ→ 3 Kντ in the U(3) × U(3) quark NJL model
5. Decays f 1 → a0π; πππ(η) and f 1 → KKπ in the chiral U(3) × U(3) quark NJL model
6. Decays τ→f0(π,K)ντ and τ→3πντ accounting for the contribution of f0(500)
7. Decays of radially excited vector mesons ρ′ and ω′ in the extended NJL model
8. Description of the decay τ →Kππντ in the NJL-type chiral quark model
9. Description of the Processes and within the Extended NJL Model
10. Description of the processes e+e− → π+π− and τ− → π−π0ντ in the NJL model with value of the vector coupling constant gρ = 6
11. e + e – → a 1π, e + e – → K 1(1270)K, and e + e – → K 1(1400)K Processes within the Chiral Quark Nambu–Jona-Lasinio Model
12. Low-Energy Interactions of Mesons with Participation of the First Radially Excited States in U(3) × U(3) NJL Model
13. On the decay widths of radially excited scalar meson K0∗(1430) in view of new experimental data
14. Processes τ → (a 1π, K 1π, K 1 K)ντ and e + e – → (a 1π, K 1 K) in the NJL Model
15. Semileptonic Decays of ρ , ω , ϕ , η and η′ Mesons in Ground and First Radially Excited States in the U(3) × U(3) NJL Model
16. Semileptonic Decays of Vector Mesons [ρ,ω,φ]→π[e+e−,μ+μ−] in a Chiral NJL Model
17. The decay τ → 3πντ and axial-vector meson a1 in the NJL model
18. The decays τ → a 1 π ν τ, τ → K 1 π ν τ and τ → K 1 K ν τ in the extended U (3) × U (3) chiral NJL model
19. The Decays in the NJL Quark Model
20. The second-class current decays τ → π η (η) ν τ in the NJL model including the interaction of mesons in the final state
21. Three-meson τ decays involving kaons and η mesons in the NJL model
22. Three-Meson Tau Decays with Strange Particles in the NJL Model
23. Weak Semileptonic Decays of Vector Mesons in the NJL Model
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