Volkov Mikhail Konstantinovich

Publications in Math-Net.Ru

1. $\tau$ lepton decays with production of strange scalar mesons $K^*_0(700)$ and $K^*_0(1430)$ in the extended Nambu–Jona–Lasinio model
   
   Pis'ma v Zh. Èksper. Teoret. Fiz., 117:5 (2023),  325–331
2. $e^+e^- \to a_1\pi$, $e^+e^- \to K_1(1270)K$ and $e^+e^- \to K_1(1400)K$ processes within the chiral quark Nambu-Jona-Lasinio model
   
   Pis'ma v Zh. Èksper. Teoret. Fiz., 116:4 (2022),  191–196
3. Calculation of the width of the $\tau \to K^{-} K^{0} \nu_{\tau}$ decay in the extended Nambu–Jona-Lasinio model with estimation of the contribution from the final-state interaction
   
   Pis'ma v Zh. Èksper. Teoret. Fiz., 114:6 (2021),  353–357
4. $\tau \to K^{-} \eta \nu_{\tau}$ decay in the extended Nambu–Jona-Lasinio model including the final-state interaction
   
   Pis'ma v Zh. Èksper. Teoret. Fiz., 114:4 (2021),  199–203
5. $\tau \to K^{-} \pi^{0} \nu_{\tau}$ decay in the Nambu–Jona-Lasinio model including the final-state interaction of mesons
   
   Pis'ma v Zh. Èksper. Teoret. Fiz., 113:12 (2021),  777–783
6. $\tau^- \to \pi^- \pi^0 \nu_{\tau}$ and $e^{+}e^{-} \to \pi^{+} \pi^{-}$ processes in the chiral Nambu–Jona-Lasinio model including the interaction of pions in the final state
   
   Pis'ma v Zh. Èksper. Teoret. Fiz., 112:8 (2020),  493–498
7. Contribution of intermediate axial vector states to the $[\rho(770), \omega(782)] \to \gamma [\pi, \eta]$ electromagnetic decays in the Nambu–Jona-Lasinio model
   
   Pis'ma v Zh. Èksper. Teoret. Fiz., 110:6 (2019),  376–378
8. The $\tau \to \bar{K}^{0*}(892) \pi^{-}\nu_{\tau}$ decay taking into account the splitting of an intermediate ground-state axial-vector meson $K_{1A}$ into two physical states $K_1(1270)$ and $K_1(1400)$
   
   Pis'ma v Zh. Èksper. Teoret. Fiz., 110:4 (2019),  217–221
9. On the dependence of the widths of the $\tau \rightarrow [\rho^{0}(770), \rho^{0}(1450)] \pi^{-} \nu_{\tau}$ decays on the parameters of the intermediate $a_1$ meson
   
   Pis'ma v Zh. Èksper. Teoret. Fiz., 109:4 (2019),  219–222
10. The $\tau \rightarrow \bar{K}^{*0}(892) \pi^{-}\nu_{\tau}$ decay in the Nambu–Jona–Lasinio model
    
    Pis'ma v Zh. Èksper. Teoret. Fiz., 108:6 (2018),  369–373
11. Production $\rho(770)$ of meson pairs in the decays $\rho(1450)\rightarrow \rho(770)\eta$ and $\tau\rightarrow \rho(770)\eta\nu_{\tau}$ and in the process $e^{+}e^{-} \rightarrow \rho(770)\eta$ in the Extended Nambu–Jona–Lasinio model
    
    Pis'ma v Zh. Èksper. Teoret. Fiz., 106:12 (2017),  737–740
12. Axial-vector mesons and the problem of $\pi a_1$ mixing
    
    Pis'ma v Zh. Èksper. Teoret. Fiz., 105:4 (2017),  205–208
13. Meson production processes in electron–positron collisions and tau-lepton decays within the extended Nambu – Jona-Lasinio model
    
    UFN, 187:7 (2017),  689–714
14. The decays $\tau \rightarrow (\eta,\eta')K^{-}\nu_{\tau}$ in the extended Nambu–Jona-Lasinio model
    
    Pis'ma v Zh. Èksper. Teoret. Fiz., 103:10 (2016),  697–701
15. Meson correlation functions for a model with nonlocal four-fermion interaction
    
    TMF, 161:3 (2009),  406–419
16. About the role of vector mesons on the $\eta\to\pi^0\gamma\gamma$ decay width in meson – baryon chiral model
    
    Pis'ma v Zh. Èksper. Teoret. Fiz., 86:3 (2007),  190–192
17. The Nambu–Jona-Lasinio model and its development
    
    UFN, 176:6 (2006),  569–580
18. The strong and radiative decays of $D^*$-mesons
    
    TMF, 102:2 (1995),  217–222
19. Quark and gluon condensates in the Nambu–Jona–Lasinio model at finite temperature
    
    TMF, 101:3 (1994),  442–449
20. Vector and axial-vector dominance of the weak interactions
    
    TMF, 87:1 (1991),  57–61
21. $\pi a_1$ Transitions and low-energy limit in the linear sigma model
    
    TMF, 86:3 (1991),  385–390
22. Quark model of superconducting type and nondiagonal $P$–$A$ transitions
    
    TMF, 81:3 (1989),  354–368
23. Dimesic atoms in a quark model of superconducting type
    
    TMF, 71:3 (1987),  381–387
24. Masses of vector and pseudoscalar mesons in the quark loop model
    
    TMF, 69:1 (1986),  156–160
25. Meson Lagrangians of the group $U(3)$ in a model with four-quark interactions
    
    TMF, 57:1 (1983),  21–34
26. The present status of quantum field theory
    
    UFN, 136:3 (1982),  542–546
27. Renormalizations in nonlinear chiral theory
    
    TMF, 28:1 (1976),  46–55
28. Quantum field theory with a chiral Lagrangian and low-energy meson physics
    
    UFN, 120:3 (1976),  363–391
29. Exponential interaction of scalar massless fields (third order)
    
    Trudy Mat. Inst. Steklov., 135 (1975),  87–94
30. Nonpolynomial Lagrangians (higher perturbation orders)
    
    TMF, 11:3 (1972),  273–287
31. Analytic structure of superpropagators in the coupling constant
    
    TMF, 6:1 (1971),  21–27
32. Second International Conference on Nonlocal Quantum Field Theory
    
    UFN, 103:3 (1971),  559–564
33. A method of describing nonrenormalizable interactions, taking account of unitarity
    
    TMF, 2:2 (1970),  197–209
34. Consideration of superfluid effects in $\alpha$-decay to the vibration levels of the daughter nuclei
    
    Dokl. Akad. Nauk SSSR, 148:4 (1963),  799–802


35. Erratum to: On the dependence of the widths of the $\tau \rightarrow [\rho^{0}(770), \rho^{0}(1450)] \pi^{-} \nu_{\tau}$ decays on the parameters of the intermediate $a_1$ meson
    
    Pis'ma v Zh. Èksper. Teoret. Fiz., 109:12 (2019),  858
36. The present status of quantum field theory (From materials of the Fifth International Meeting on Nonlocal Quantum Field Theory, Alushta, the Crimea, April 19–25,1979)
    
    UFN, 130:1 (1980),  177–183
37. Fundamental problems of quantum field theory (From materials of the Fourth International Meeting on Non-Local Quantum Field Theory, Alushta, April 21–27, 1976)
    
    UFN, 121:1 (1977),  171–174
38. Международное совещание по нелокальной квантовой теории поля (Дубна, 4–7 июля 1967 г.)
    
    UFN, 94:4 (1968),  745–748