Nikolay Kozyrev
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Nikolay Kozyrev has a total of 7 co-authors. Here are the top co-authors by number of shared publications:
- Sergey Krivonos
Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, Dubna, Russia
23 shared publications - Anton Sutulin
Bogoliubov Laboratory of Theoretical Physics JINR 141980 Dubna Russia
9 shared publications - Olaf Lechtenfeld
Leibniz Universität Hannover
9 shared publications - Armen Nersessian
Bogoliubov Laboratory of Theoretical Physics JINR 141980 Dubna Russia
5 shared publications - Stefano Bellucci
National Institute of Materials Physics, Atomistilor Str. 405 A, 077125 Magurele, Romania
3 shared publications - Armen Yeranyan
INFN -Laboratori Nazionali di Frascati Via Enrico Fermi 40 I-00044 Frascati ITALY
1 shared publication
Latest Publications
- Open Access
- 27 October 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (10) , 1239
On interacting non-Abelian antisymmetric tensor field models
We study the gauge structure of interacting antisymmetric tensor field models obtained by the dimensional reduction on a group manifold. In such models a dimensionful parameter related to the size of the compact manifold plays the role of a coupling constant. We focus on open issues of reducibility of the gauge transformations in these theories and show that stages of reducibility of the interacting models coincide with ones of corresponding free counterparts.
- 27 October 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (10) , 1239
Open AccessOn interacting non-Abelian antisymmetric tensor field models
We study the gauge structure of interacting antisymmetric tensor field models obtained by the dimensional reduction on a group manifold. In such models a dimensionful parameter related to the size of the compact manifold plays the role of a coupling constant. We focus on open issues of reducibility of the gauge transformations in these theories and show that stages of reducibility of the interacting models coincide with ones of corresponding free counterparts.
- Open AccessA note on $SU(1,1|n)$ and $OSp(6|2)$ superconformal mechanicsIn this article we consider the construction of the superconformal mechanics that realize $SU(1,1|n)$ and $OSp(6|2)$ symmetries and involve interactions with non-Abelian bosonic currents. If is shown that for $N>4$ supersymmetries the currents involved have to satisfy the algebraic equations. General considerations on methods of solving these equations are given. In the obtained particular solutions currents are expressed in terms of semi-dynamical variables (harmonics), and, on one instance, coordinates and momenta.Open AccessA note on $SU(1,1|n)$ and $OSp(6|2)$ superconformal mechanicsIn this article we consider the construction of the superconformal mechanics that realize $SU(1,1|n)$ and $OSp(6|2)$ symmetries and involve interactions with non-Abelian bosonic currents. If is shown that for $N>4$ supersymmetries the currents involved have to satisfy the algebraic equations. General considerations on methods of solving these equations are given. In the obtained particular solutions currents are expressed in terms of semi-dynamical variables (harmonics), and, on one instance, coordinates and momenta.
- Open Access
- 1 October 2025
- Published by Joint Institute for Nuclear Research in Natural Science Review
- Vol. 2 (5) , 100505
New variants of N = 3, 4 superconformal mechanics
We construct superconformal mechanics with N = 3 and N = 4 supersymmetries that were inspired by analogy with the supersymmetric Schwarzian mechanics. The Schwarzian, being another system with superconformal symmetry, provides insight into the field content of supersymmetric mechanics, most notably, on the number and properties of the fermionic fields involved. Adding more fermionic fields (four in the N = 3 case and eight in the N = 4 case) made it possible to construct systems possessing maximal superconformal symmetries in N = 3 and N = 4, namely osp(3|2) and D(1, 2; α). In the case of N = 4 supersymmetry, we explicitly construct a new variant of N = 4 superconformal mechanics in which all bosonic subalgebras of the D(1, 2; α) superalgebra have a bosonic realization. In addition, the constructed systems involve the so(3) currents whose parameterization is not fixed, which allows one to consider different underlying geometries.
- 1 October 2025
- Published by Joint Institute for Nuclear Research in Natural Science Review
- Vol. 2 (5) , 100505
Open AccessNew variants of N = 3, 4 superconformal mechanics
We construct superconformal mechanics with N = 3 and N = 4 supersymmetries that were inspired by analogy with the supersymmetric Schwarzian mechanics. The Schwarzian, being another system with superconformal symmetry, provides insight into the field content of supersymmetric mechanics, most notably, on the number and properties of the fermionic fields involved. Adding more fermionic fields (four in the N = 3 case and eight in the N = 4 case) made it possible to construct systems possessing maximal superconformal symmetries in N = 3 and N = 4, namely osp(3|2) and D(1, 2; α). In the case of N = 4 supersymmetry, we explicitly construct a new variant of N = 4 superconformal mechanics in which all bosonic subalgebras of the D(1, 2; α) superalgebra have a bosonic realization. In addition, the constructed systems involve the so(3) currents whose parameterization is not fixed, which allows one to consider different underlying geometries.
- Open AccessNew variants of $N=3,4$ superconformal mechanicsWe construct superconformal mechanics with $N=3$ and $N=4$ supersymmetries that were inspired by analogies with the supersymmetric Schwarzian mechanics. The Schwarzian, being another system with superconformal symmetry, provides insight into the field content of supersymmetric mechanics, most notably, on the number and properties of the fermionic fields involved. Adding more fermionic fields (four in the $N=3$ case and eight in the $N=4$ case) made it possible to construct systems possessing maximal superconformal symmetries in $N=3$ and $N=4$, namely $OSp(3|2)$ and $D(1,2;α)$. In the case of $N=4$ supersymmetry, we explicitly construct a new variant of $N=4$ superconformal mechanics in which all bosonic subalgebras of $D(1,2;α)$ superalgebra have bosonic realization. In addition, the constructed systems involve $so(3)$ currents whose parametrization is not fixed, which allows to consider different underlying geometries.Open AccessNew variants of $N=3,4$ superconformal mechanicsWe construct superconformal mechanics with $N=3$ and $N=4$ supersymmetries that were inspired by analogies with the supersymmetric Schwarzian mechanics. The Schwarzian, being another system with superconformal symmetry, provides insight into the field content of supersymmetric mechanics, most notably, on the number and properties of the fermionic fields involved. Adding more fermionic fields (four in the $N=3$ case and eight in the $N=4$ case) made it possible to construct systems possessing maximal superconformal symmetries in $N=3$ and $N=4$, namely $OSp(3|2)$ and $D(1,2;α)$. In the case of $N=4$ supersymmetry, we explicitly construct a new variant of $N=4$ superconformal mechanics in which all bosonic subalgebras of $D(1,2;α)$ superalgebra have bosonic realization. In addition, the constructed systems involve $so(3)$ currents whose parametrization is not fixed, which allows to consider different underlying geometries.
- Open Access
- 11 February 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (2) , 1-23
Improved non-Abelian tensor multiplet action
Construction of the superfield action of the N = (1, 0), d = 6 non-Abelian tensor multiplet based on the non-Abelian tensor hierarchies is considered. It is shown that while straightforward non-Abelian generalization of the Pasti-Sorokin-Tonin action is not a workable solution, a suitable truncation of the PST action still can be modified to include non-Abelian tensor field. In the modified action, the self-dual equation of motion of the tensor field is induced by a composite Lagrange multiplier, which is not a component of a standard dynamical tensor multiplet. As a result, the constraint that enforces the gauge group to be non-compact, as in the usual tensor hierarchies, can be avoided.
- 11 February 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (2) , 1-23
Open AccessImproved non-Abelian tensor multiplet action
Construction of the superfield action of the N = (1, 0), d = 6 non-Abelian tensor multiplet based on the non-Abelian tensor hierarchies is considered. It is shown that while straightforward non-Abelian generalization of the Pasti-Sorokin-Tonin action is not a workable solution, a suitable truncation of the PST action still can be modified to include non-Abelian tensor field. In the modified action, the self-dual equation of motion of the tensor field is induced by a composite Lagrange multiplier, which is not a component of a standard dynamical tensor multiplet. As a result, the constraint that enforces the gauge group to be non-compact, as in the usual tensor hierarchies, can be avoided.
- Open Access
- 28 March 2023
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2023 (3) , 1-25
Supersymmetrizing the Pasti-Sorokin-Tonin action
In this paper the harmonic superspace action of the tensor multiplet of N = (1, 0), d = 6 supersymmetry is constructed which in the bosonic limit reduces to the known Pasti-Sorokin-Tonin action for the self-dual tensor field. The action involves, besides the potential containing the dynamical fields, also an auxiliary tensor multiplet and a set of analytic superfields with gauge PST scalar among them. For each of gauge symmetries of the PST action, a superfield analog is found. The equations of motion are calculated and it is shown that no extra degrees of freedom appear.
- 28 March 2023
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2023 (3) , 1-25
Open AccessSupersymmetrizing the Pasti-Sorokin-Tonin action
In this paper the harmonic superspace action of the tensor multiplet of N = (1, 0), d = 6 supersymmetry is constructed which in the bosonic limit reduces to the known Pasti-Sorokin-Tonin action for the self-dual tensor field. The action involves, besides the potential containing the dynamical fields, also an auxiliary tensor multiplet and a set of analytic superfields with gauge PST scalar among them. For each of gauge symmetries of the PST action, a superfield analog is found. The equations of motion are calculated and it is shown that no extra degrees of freedom appear.
- Open Access
- 23 January 2023
- Published by American Physical Society (APS) in Physical Review D
- Vol. 107 (2) , 026018
Generalized Schwarzians
In this paper we demonstrate that the different generalizations of the Schwarzians, supersymmetric or purely bosonic, can be easily constructed by using the nonlinear realizations technique.
- 23 January 2023
- Published by American Physical Society (APS) in Physical Review D
- Vol. 107 (2) , 026018
Open AccessGeneralized Schwarzians
In this paper we demonstrate that the different generalizations of the Schwarzians, supersymmetric or purely bosonic, can be easily constructed by using the nonlinear realizations technique.
- Open Access
- 19 April 2022
- Published by American Physical Society (APS) in Physical Review D
- Vol. 105 (8) , 085010
supersymmetric Schwarzian with symmetryIt was recently demonstrated that super-Schwarzian derivatives can be constructed from the Cartan forms of the superconformal supergroups , , , . Roughly speaking, the super-Schwarzian is just the component of the corresponding Cartan forms with the lowest dimension. In this paper, we apply the same approach to superalgebra . The minimal set of constraints we used includes: (a) introducing new superspace coordinates the Cartan forms depend on, which are completely invariant with respect to the corresponding group; (b) nullifying the form for dilatation. In contrast to the case, the new super-Schwarzian appears to be a component of the form for automorphism.- 19 April 2022
- Published by American Physical Society (APS) in Physical Review D
- Vol. 105 (8) , 085010
Open Accesssupersymmetric Schwarzian with symmetryIt was recently demonstrated that super-Schwarzian derivatives can be constructed from the Cartan forms of the superconformal supergroups , , , . Roughly speaking, the super-Schwarzian is just the component of the corresponding Cartan forms with the lowest dimension. In this paper, we apply the same approach to superalgebra . The minimal set of constraints we used includes: (a) introducing new superspace coordinates the Cartan forms depend on, which are completely invariant with respect to the corresponding group; (b) nullifying the form for dilatation. In contrast to the case, the new super-Schwarzian appears to be a component of the form for automorphism. - Open Access
- 21 March 2022
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2022 (3) , 1-27
(Super)Schwarzian mechanics
- 21 March 2022
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2022 (3) , 1-27
Open Access(Super)Schwarzian mechanics
- Open Access${\cal N}{=}4$ supersymmetric Schwarzian with $D(1,2;α)$ symmetryIt was recently demonstrated that super-Schwarzian derivatives can be constructed from the Cartan forms of the super-conformal supergroups $OSp(1|2),SU(1,1|1), OSp(3|2), SU(1,1|2)$. Roughly speaking, the super-Schwarzian is just the component of the corresponding Cartan forms with the lowest dimension. In this paper, we apply the same approach for superalgebra $D(1,2;\alpha)$. The minimal set of constraints we used includes: a) introducing new superspace coordinates the Cartan forms depend on, which are completely invariant with respect to the corresponding group; b) nullifying the form for dilatation. In contrast to the $SU(1,1|2)$ case, the new super-Schwarzian appears to be a $d\theta^{ia}$ component of the form for $su(2)$ automorphism.Open Access${\cal N}{=}4$ supersymmetric Schwarzian with $D(1,2;α)$ symmetryIt was recently demonstrated that super-Schwarzian derivatives can be constructed from the Cartan forms of the super-conformal supergroups $OSp(1|2),SU(1,1|1), OSp(3|2), SU(1,1|2)$. Roughly speaking, the super-Schwarzian is just the component of the corresponding Cartan forms with the lowest dimension. In this paper, we apply the same approach for superalgebra $D(1,2;\alpha)$. The minimal set of constraints we used includes: a) introducing new superspace coordinates the Cartan forms depend on, which are completely invariant with respect to the corresponding group; b) nullifying the form for dilatation. In contrast to the $SU(1,1|2)$ case, the new super-Schwarzian appears to be a $d\theta^{ia}$ component of the form for $su(2)$ automorphism.