Sergey Fedoruk
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Research Interests
Sergey Fedoruk has a total of 34 co-authors. Here are the top co-authors by number of shared publications:
- Evgeny Ivanov
Bogoliubov Laboratory of Theoretical Physics, JINR
32 shared publications - Ioseph Lvovich Buchbinder
Joint Institute for Nuclear Research
25 shared publications - Jerzy Lukierski
Institute of Theoretical Physics Wroc law University Plac Maxa Borna 9 Wroc law Poland
24 shared publications - Alexey P. Isaev
Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, Dubna, Russia
21 shared publications - Olaf Lechtenfeld
Leibniz Universität Hannover
12 shared publications - Andrei. V. Smilga
SUBATECH
8 shared publications
Latest Publications
- Open Access
- 2 September 2026
- Published by Elsevier in Nuclear Physics B
- Vol. 1031
N=4 supersymmetric multiparticle systems based on indecomposable multiplets
- 2 September 2026
- Published by Elsevier in Nuclear Physics B
- Vol. 1031
Open AccessN=4 supersymmetric multiparticle systems based on indecomposable multiplets
- Open Access
- 19 May 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (5) , 544
On BRST Lagrangian description of partially massless bosonic fields
We present an exhaustive BRST lagrangian description of partially massless bosonic fields in four-dimensional space. The basic fields are formulated in terms of two-component spin-tensors in (A)dS space where the tracelessness conditions are automatically fulfilled. The mass shell of partially massless fields is reformulated in terms of constraints on Fock space vectors including the second-class constraints. A conversion procedure for transforming second-class constraints into first-class ones is developed, allowing one to construct a Hermitian and nilpotent BRST charge in the Fock space under consideration. It is proven that the hermiticity and nilpotency restrict the conditions on the theory parameters, which are fulfilled only in dS space. The hermiticity of the BRST charge is incompatible with AdS space. The gauge invariant Lagrangian is constructed on the basis of the BRST charge, and for spin s and depth t the allowed states in the Lagrangian include only $$(s-t-1)$$ Stückelberg fields. Their exclusion leads to gauge transformations of degree $$(s-t)$$ for the physical fields. The Lagrangian equations of motion exactly reproduce the mass shell conditions. The Lagrangian in terms of conventional spin-tensor fields is also presented.- 19 May 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (5) , 544
Open AccessOn BRST Lagrangian description of partially massless bosonic fields
We present an exhaustive BRST lagrangian description of partially massless bosonic fields in four-dimensional space. The basic fields are formulated in terms of two-component spin-tensors in (A)dS space where the tracelessness conditions are automatically fulfilled. The mass shell of partially massless fields is reformulated in terms of constraints on Fock space vectors including the second-class constraints. A conversion procedure for transforming second-class constraints into first-class ones is developed, allowing one to construct a Hermitian and nilpotent BRST charge in the Fock space under consideration. It is proven that the hermiticity and nilpotency restrict the conditions on the theory parameters, which are fulfilled only in dS space. The hermiticity of the BRST charge is incompatible with AdS space. The gauge invariant Lagrangian is constructed on the basis of the BRST charge, and for spin s and depth t the allowed states in the Lagrangian include only $$(s-t-1)$$ Stückelberg fields. Their exclusion leads to gauge transformations of degree $$(s-t)$$ for the physical fields. The Lagrangian equations of motion exactly reproduce the mass shell conditions. The Lagrangian in terms of conventional spin-tensor fields is also presented. - Open Access
- 23 September 2025
- Published by Elsevier in Nuclear Physics B
- Vol. 1019
Continuous spin superparticle in 4 D , N = 1 curved superspace
- 23 September 2025
- Published by Elsevier in Nuclear Physics B
- Vol. 1019
Open AccessContinuous spin superparticle in 4 D , N = 1 curved superspace
- Open Access
- 8 August 2025
- Published by Elsevier in Physics Letters B
- Vol. 868
Continuous spin superparticle model
- 8 August 2025
- Published by Elsevier in Physics Letters B
- Vol. 868
Open AccessContinuous spin superparticle model
- Open Access
- 5 May 2025
- Published by Joint Institute for Nuclear Research in Natural Science Review
- Vol. 2 (3) , 100301
On BRST Lagrangian formulation for massive higher-spin fields in 4 D Minkowski space
We give a brief overview of the BRST approach to the gauge-invariant Lagrangian formulation for free massive higher-spin bosonic fields, focusing on two specific aspects. First, the theory is considered in four-dimensional flat space in terms of spin-tensor fields with two-component undotted and dotted indices. This leads to a significant simplification of the whole approach in comparison with the one where the fields with vector indices were used, since now there is no need to introduce a constraint responsible for the traces of the fields into the BRST charge. Second, we develop an extremely simple and clear procedure to eliminate all the auxiliary fields and prove that the BRST equations of motion identically reproduce the basic conditions for irreducible representations of the Poincáre group with a given mass and spin. Similar to the massless theory, the final Lagrangian for massive higher-spin fields is formulated in triplet form. The BRST formulation leads to a system of fields that are clearly subdivided into the basic spin s field, Zinoviev-like auxiliary fields, Singh–Hagen-like auxiliary fields, and special BRST auxiliary fields. The auxiliary fields can be partially eliminated by gauge fixing and/or using the equations of motion. This allows one to obtain formally different (with different numbers of auxiliary fields) but equivalent Lagrangian formulations.
- 5 May 2025
- Published by Joint Institute for Nuclear Research in Natural Science Review
- Vol. 2 (3) , 100301
Open AccessOn BRST Lagrangian formulation for massive higher-spin fields in 4 D Minkowski space
We give a brief overview of the BRST approach to the gauge-invariant Lagrangian formulation for free massive higher-spin bosonic fields, focusing on two specific aspects. First, the theory is considered in four-dimensional flat space in terms of spin-tensor fields with two-component undotted and dotted indices. This leads to a significant simplification of the whole approach in comparison with the one where the fields with vector indices were used, since now there is no need to introduce a constraint responsible for the traces of the fields into the BRST charge. Second, we develop an extremely simple and clear procedure to eliminate all the auxiliary fields and prove that the BRST equations of motion identically reproduce the basic conditions for irreducible representations of the Poincáre group with a given mass and spin. Similar to the massless theory, the final Lagrangian for massive higher-spin fields is formulated in triplet form. The BRST formulation leads to a system of fields that are clearly subdivided into the basic spin s field, Zinoviev-like auxiliary fields, Singh–Hagen-like auxiliary fields, and special BRST auxiliary fields. The auxiliary fields can be partially eliminated by gauge fixing and/or using the equations of motion. This allows one to obtain formally different (with different numbers of auxiliary fields) but equivalent Lagrangian formulations.
- Open Access
On BRST Lagrangian formulation of massless higher spin fields
The paper is dedicated to the blessed memory of Professor Vladislav Gavrilovich Bagrov, an outstanding Russian scientist in the area of theoretical and mathematical physics. He had a great influence on the formation of the scientific interests dozens of scientists in Tomsk and Russia as a whole. Two of the authors of this paper (I.L.B and V.A.K) are to one degree or another grateful to Professor V.G. Bagrov for comprehensive support in the initial period of their scientific career. Two other authors (S.A.F. and A.P.I.) are familiar with and use the work of scientists from the Tomsk School of Theoretical Physics, founded by Professor V.G. Bagrov. The paper is devoted to certain aspects of the higher-spin field theory, which were mainly initiated and continued during of I.L.B and V.A.K work in Tomsk. We demonstrate in details the simplicity and clearity of the Lagrangian formulation for free four-dimensional massless higher-spin fields within the universal BRST approach, while describing these fields in terms of two-component spin-tensors.
Open AccessOn BRST Lagrangian formulation of massless higher spin fields
The paper is dedicated to the blessed memory of Professor Vladislav Gavrilovich Bagrov, an outstanding Russian scientist in the area of theoretical and mathematical physics. He had a great influence on the formation of the scientific interests dozens of scientists in Tomsk and Russia as a whole. Two of the authors of this paper (I.L.B and V.A.K) are to one degree or another grateful to Professor V.G. Bagrov for comprehensive support in the initial period of their scientific career. Two other authors (S.A.F. and A.P.I.) are familiar with and use the work of scientists from the Tomsk School of Theoretical Physics, founded by Professor V.G. Bagrov. The paper is devoted to certain aspects of the higher-spin field theory, which were mainly initiated and continued during of I.L.B and V.A.K work in Tomsk. We demonstrate in details the simplicity and clearity of the Lagrangian formulation for free four-dimensional massless higher-spin fields within the universal BRST approach, while describing these fields in terms of two-component spin-tensors.
- 1 November 2024
- Published by Springer Nature in Russian Physics Journal
- Vol. 67 (11) , 1806-1818
ON BRST Lagrangian Formulation of Massless Higher Spin Fields
- 1 November 2024
- Published by Springer Nature in Russian Physics Journal
- Vol. 67 (11) , 1806-1818
ON BRST Lagrangian Formulation of Massless Higher Spin Fields
- 16 July 2024
- Published by Springer Nature in The European Physical Journal Plus
- Vol. 139 (7) , 1-11
BRST construction for infinite spin field on $AdS_4$- 16 July 2024
- Published by Springer Nature in The European Physical Journal Plus
- Vol. 139 (7) , 1-11
BRST construction for infinite spin field on $AdS_4$- Open Access
- 6 May 2024
- Published by Elsevier in Physics Letters B
- Vol. 853
Infinite (continuous) spin particle in constant curvature space
- 6 May 2024
- Published by Elsevier in Physics Letters B
- Vol. 853
Open AccessInfinite (continuous) spin particle in constant curvature space
- Open Access
- 11 April 2024
- Published by Sissa Medialab Srl
- Vol. 455, 039
Generalization of the Bargmann-Wigner approach to constructing relativistic fields
We review the method for constructing local relativistic fields corresponding to the Bargmann-Wigner wave functions that describe the unitary irreducible representations of the $4D$ Poincar\'{e} group. The method is based on the use of the generalized Wigner operator connecting the wave functions of induced representations and local relativistic fields. Applications of this operator for constructing massive local relativistic fields as well as massless helicity local fields and massless local infinite spin fields are considered.- 11 April 2024
- Published by Sissa Medialab Srl
- Vol. 455, 039
Open AccessGeneralization of the Bargmann-Wigner approach to constructing relativistic fields
We review the method for constructing local relativistic fields corresponding to the Bargmann-Wigner wave functions that describe the unitary irreducible representations of the $4D$ Poincar\'{e} group. The method is based on the use of the generalized Wigner operator connecting the wave functions of induced representations and local relativistic fields. Applications of this operator for constructing massive local relativistic fields as well as massless helicity local fields and massless local infinite spin fields are considered.