arxiv: 2604.22466 · v2 · submitted 2026-04-24 · ✦ hep-th

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On a quantization of deformed reducible gauge theories

A. A. Averianov , A. O. Barvinsky , I. L. Buchbinder , V. A. Krykhtin , D. V. Nesterov

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Pith reviewed 2026-05-12 01:16 UTC · model grok-4.3

classification ✦ hep-th

keywords reducible gauge theoriesStueckelberg proceduregauge invariance restorationAbelian gauge theoriesquantizationone-loop effective actionAdS spacefermionic tensor fields

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The pith

Stueckelberg procedure converts deformed Abelian reducible gauge theories into exactly gauge-invariant ones.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper shows that Abelian gauge theories whose gauge symmetry is broken by mass or interaction terms can have that symmetry restored by a Stueckelberg-type procedure. Once restored, the theories admit quantization in terms of a functional integral that includes the full set of ghost fields required by first- and second-stage reducibility. Suitable gauge fixing reduces the problem to minimal wave operators that can be handled by the covariant Schwinger-DeWitt method. The same construction is applied to massive fermionic totally antisymmetric tensor fields in AdS space, where the one-loop effective action emerges as a product of functional determinants of Dirac-type operators in several dimensions.

Core claim

A general reducible gauge theory deformed by mass or interaction terms that violate gauge invariance is considered. In the Abelian case the Stueckelberg-type procedure converts the theory with broken symmetry into an exactly gauge-invariant theory. Under a suitable choice of gauge conditions this theory is treated within the formalism of minimal wave operators manageable by the covariant Schwinger-DeWitt technique. Quantization is carried out for generators of gauge transformations of the first and second stages of reducibility, and the partition function is derived as a functional integral containing all corresponding ghost fields. The method is applied to massive fermionic totally antisym

What carries the argument

Stueckelberg-type procedure that restores exact gauge invariance to deformed Abelian reducible theories, allowing reduction to minimal wave operators.

If this is right

The partition function is obtained as a functional integral that includes the complete set of ghost fields for first- and second-stage reducibility.
One-loop effective actions for the tensor-field models are expressed as functional determinants of special Dirac-type operators.
The construction works for the models in AdS space and in various spacetime dimensions.
The restored gauge-invariant theory can be handled by the covariant Schwinger-DeWitt technique.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

The same restoration and quantization steps could be tested on bosonic versions of the tensor fields to compare the resulting determinants.
Explicit evaluation of the determinants in four and six dimensions would give concrete one-loop corrections that can be checked against known flat-space limits.
If the Abelian restriction can be relaxed, the procedure might supply a template for quantizing mildly non-Abelian deformations.

Load-bearing premise

The Stueckelberg-type procedure exactly restores gauge invariance for general first- and second-stage reducible Abelian theories deformed by mass or interaction terms, and suitable gauge conditions exist that reduce the problem to minimal wave operators without new inconsistencies.

What would settle it

A direct check that, after Stueckelberg restoration, the gauge-fixed action for a known test case such as the massive vector field still requires non-minimal operators or yields a partition function whose degrees of freedom do not match the physical count.

Figures

Figures reproduced from arXiv: 2604.22466 by A. A. Averianov, A. O. Barvinsky, D. V. Nesterov, I. L. Buchbinder, V. A. Krykhtin.

**Figure 1.** Figure 1: Diagram of reducibility 4.3 Faddeev-Popov determinant and the functional integral In order to compute the Faddeev-Popov determinant we substitute expressions (4.18), (4.28) and (4.29) into the integral (4.3) and perform the transformation analogous to (3.11): ∆−1 Det(𝑍¯(2)𝑎2 𝑎1 𝜔¯ 𝑎1 𝑏2 ) Det(𝐹′′) Det(𝐹′) Det(𝑍˜(2)𝑎2 𝑎1 𝜎 ′𝑎1 𝑏2 ) = = ∫︁ D𝑓D𝑔D𝑐¯1D𝑐D𝑐˜1 𝛿[𝜔 𝑎1 𝛼 𝑓 𝛼 + 𝜎 ′𝑎1 𝑎2 𝑐¯1 𝑎2 ] 𝛿[𝜔 ′𝑎2 𝑎1 𝑔 𝑎1 ] 𝛿[𝜒… view at source ↗

read the original abstract

We consider a general reducible gauge theory deformed by mass or/and interaction terms violating gauge invariance. It is shown that in the Abelian case, by using the Stueckelberg-type procedure, this theory with broken gauge symmetry can be converted into exactly gauge-invariant theory which under a suitable choice of gauge conditions can be treated within the formalism of minimal wave operators manageable by the covariant Schwinger-DeWitt technique. We carry out quantization of such a theory in general terms when the initial generators of gauge transformations are of the first and second stages of reducibility and derive its partition function in terms of the functional integral with all corresponding ghost fields. This method is applied to quantization of massive fermionic totally antisymmetric tensor field models in $AdS$ space. One-loop quantum effective action for these models is derived in the form of the functional determinants of special Dirac-type differential operators in various dimensions.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Desk Editor's Note private letter to a colleague

The paper works out a Stueckelberg restoration and ghost structure for first- and second-stage reducible Abelian theories, then applies it to massive fermionic tensors in AdS to produce explicit one-loop determinants.

read the letter

The main thing to know is that the authors restore exact gauge invariance in mass-deformed reducible Abelian theories via Stueckelberg auxiliaries, quantize them with the full ghost tower, and obtain one-loop effective actions for totally antisymmetric fermionic tensors in AdS as determinants of Dirac-type operators in several dimensions. This is presented in general terms for both first- and second-stage reducibility before the concrete application.

Referee Report

1 major / 2 minor

Summary. The paper claims that Abelian reducible gauge theories deformed by mass or interaction terms breaking gauge invariance can be restored to exact gauge invariance via a Stueckelberg-type procedure. For generators of first and second stages of reducibility, the restored theory is quantized using functional integrals over fields and ghosts, yielding an explicit partition function. The method is applied to massive fermionic totally antisymmetric tensor fields in AdS space, producing one-loop effective actions as functional determinants of Dirac-type operators in various dimensions.

Significance. If the central derivations hold, the work supplies a covariant quantization framework for deformed reducible Abelian theories that extends standard techniques like the Schwinger-DeWitt method to models of interest in AdS backgrounds. The general expression for the partition function and the concrete determinant forms for the fermionic tensor models constitute a useful technical contribution.

major comments (1)

[General quantization procedure for first- and second-stage reducibility] The core assertion that the Stueckelberg procedure restores exact gauge invariance for second-stage reducible Abelian theories (while preserving the full reducibility structure) is load-bearing for the subsequent reduction to minimal wave operators. No explicit verification is provided that the restored gauge transformations close off-shell or that the quadratic action remains free of non-minimal terms after gauge fixing; without this, the applicability of the covariant Schwinger-DeWitt technique to genuine second-stage examples is not secured.

minor comments (2)

The abstract would benefit from a brief statement of the spacetime dimension(s) in which the AdS models are treated.
[Derivation of the partition function] Notation for the ghost fields and reducibility parameters could be introduced more explicitly when first presenting the partition function.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and for the constructive major comment. We address the point below and will revise the text to incorporate an explicit verification as requested.

read point-by-point responses

Referee: The core assertion that the Stueckelberg procedure restores exact gauge invariance for second-stage reducible Abelian theories (while preserving the full reducibility structure) is load-bearing for the subsequent reduction to minimal wave operators. No explicit verification is provided that the restored gauge transformations close off-shell or that the quadratic action remains free of non-minimal terms after gauge fixing; without this, the applicability of the covariant Schwinger-DeWitt technique to genuine second-stage examples is not secured.

Authors: We agree that an explicit verification strengthens the presentation. In the general construction of Sections 2–3 the Stueckelberg fields are introduced so that the deformed action is rendered exactly invariant while the original reducibility relations are preserved by construction. Because the underlying gauge algebra is Abelian, the commutator of any two restored gauge transformations vanishes identically, which guarantees off-shell closure. The subsequent gauge fixing is chosen precisely so that the quadratic operator becomes minimal; this is already visible in the explicit fermionic-tensor examples. Nevertheless, to meet the referee’s request we will add, in the revised version, a short dedicated paragraph that writes out the restored transformations for the second-stage case, verifies their off-shell closure, and confirms that the gauge-fixed quadratic form contains no non-minimal terms, thereby securing the applicability of the Schwinger–DeWitt technique. revision: yes

Circularity Check

0 steps flagged

Standard Stueckelberg restoration and BRST quantization with independent derivation of determinants; no load-bearing self-references or fitted predictions.

full rationale

The derivation begins with the standard Stueckelberg auxiliary-field procedure to restore exact Abelian gauge invariance for first- and second-stage reducible theories, then applies the conventional minimal-wave-operator formalism and Schwinger-DeWitt technique to obtain the partition function and one-loop effective action. These steps rely on established QFT tools rather than re-deriving them from the deformation parameters. The final determinants for the AdS fermionic tensor models are obtained by direct operator construction and are not forced by any prior fit or self-citation chain. A low score of 2 accounts for possible routine self-citations to the authors' earlier gauge-theory work, but these are not load-bearing for the central claims.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claims rest on the applicability of the Stueckelberg procedure to restore invariance exactly and the existence of gauge conditions compatible with minimal operators; these are domain assumptions in gauge QFT rather than new postulates.

axioms (2)

domain assumption Stueckelberg-type procedure converts broken gauge symmetry to exact invariance for Abelian reducible theories
Invoked to enable the subsequent quantization step.
domain assumption Suitable gauge fixing reduces the theory to minimal wave operators treatable by Schwinger-DeWitt technique
Required for deriving the functional determinants.

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Works this paper leans on

66 extracted references · 66 canonical work pages

[1]

Superstring Theory

M. B. Green, J. H.Schwarz, E. Witten, “Superstring Theory", vols. 1 and 2, Cambridge Univ. Press, 1987

work page 1987
[2]

String Theory

J. Polchinnski, “String Theory", vols. 1 and 2, Cambridge Univ. Press, 1998

work page 1998
[3]

D-Branes

C. V. Johnson, “D-Branes”, Cambridge Univ. Press, 2003, 548 p

work page 2003
[4]

Gravity and Strings

T. Ortin, “Gravity and Strings”, Cambridge Univ. Press, 2004

work page 2004
[5]

String Theory and M-Theory: A Modern Introduction

K. Becker, M. Becker, J. Y. Schwarz, “String Theory and M-Theory: A Modern Introduction", Cambridge Univ. Press, 2007

work page 2007
[6]

Supergravity

D. Z. Freedman, A. Van Proeyen, “Supergravity”, Cambridge Univ. Press, 2012

work page 2012
[7]

Basic Concepts of String Theory

R. Blumenhagen, D. Luest, S. Theisen, “Basic Concepts of String Theory", Springer, 2013

work page 2013
[8]

Introduction to Supergravity

Y. Tanii, “Introduction to Supergravity", Springer, 2014

work page 2014
[9]

Duality for non-specialist

S. E. Hjielmeland, U. Lindstrom, “Duality for non-specialist",arXiv:hep-th/9705122

work page arXiv
[10]

Effective actions for dual massive (super)𝑝-forms

S. M. Kuzenko, K. Turner, “Effective actions for dual massive (super)𝑝-forms", JHEP01(2021) 040, arXiv:2009.08262 [hep-th],

work page arXiv 2021
[11]

On the duality of massive Kalb-Ramond and Proca fields,

A. Hell, “On the duality of massive Kalb-Ramond and Proca fields," JCAP01(2022) 056, arXiv:2109.050302 [hep-th]

work page arXiv 2022
[12]

On the Kalb-Ramond field with non-minimal coupling to gravity,

A. Hell, I. Obata, “On the Kalb-Ramond field with non-minimal coupling to gravity,"arXiv:2602.21675 [hep-th]

work page arXiv
[13]

Schwinger-DeWitt expansion for the heat kernel of nonminimal operators in causal theories

A. O. Barvinsky, A. E. Kalugin, W. Wachowski, “Schwinger-DeWitt expansion for the heat kernel of nonminimal operators in causal theories", Phys. Rev. D112(2025) 076032,arXiv:2508.06439 [hep-th]. 21

work page arXiv 2025
[14]

The Stueckelberg Field

H. Ruegg, M. Ruiz-Altaba, “The Stueckelberg field", Int. J. Mod. Phys. A19(2004) 3265, arXiv:hep-th/0304245

work page Pith review arXiv 2004
[15]

Quantum effects in softly broken gauge theories in curved spacetimes

I. L. Buchbinder, G. de Berredo-Peixoto, I. L. Shapiro, “Quantum effects in softly broken gauge theories in curved spacetimes". Phys. Lett. B649(2007) 454,arXiv:hep-th/0703189

work page arXiv 2007
[16]

Quantum equivalence of massive antisymmetric tensor field models in curved space

I. L. Buchbinder, E. N. Kirillova, N. G. Pletnev, “Quantum equivalence of massive antisymmetric tensor field models in curved space", Phys. Rev. D78(2008) 084024,arXiv:0806.3505 [hepth]

work page arXiv 2008
[17]

Ontherenormalizationofmassivevec- torfieldtheorycoupledtoscalarincurvedspace-time,

I.L.Buchbinder, PRB.R.doVale, G.Y.Oyadomari, I.L.Shapiro, “Ontherenormalizationofmassivevec- torfieldtheorycoupledtoscalarincurvedspace-time,"Phys.Rev., D110(2024)12505,arXiv:2410.00991 [hep-th]

work page arXiv 2024
[18]

Lagrangian formulation of massive fermionic totally antisymmetric tensor field theory in AdS(d) space,

I. L. Buchbinder, V. A. Krykhtin, L. L. Ryskina, “Lagrangian formulation of massive fermionic totally antisymmetric tensor field theory in AdS(d) space,” Nucl. Phys. B819(2009), 453-477,arXiv:0902.1471 [hep-th]

work page arXiv 2009
[19]

Note on antisymmetric spin-tensors,

Yu. M Zinoviev, “Note on antisymmetric spin-tensors,” JHEP04(2009), 035,arXiv:0903.0262 [hep-th]

work page arXiv 2009
[20]

Unconstrained higher spins of mixed symmetry. II.Fermi0fields

A. Campoleoni, D. Francia, J. Mourad, A. Sagnotti, “Unconstrained higher spins of mixed symmetry. II.Fermi0fields”, Nucl. Phys. B828(2010) 405,arXiv:0904.4447 [hep-th]

work page arXiv 2010
[21]

Stronly coupled gravity and dualities

C. M. Hull, “Stronly coupled gravity and dualities”, Nucl. Phys. B583(2000) 237,arXiv:heo-th/0004195

work page arXiv 2000
[22]

Symmetries and compactifications of (4,0) conformal gravity

C. M. Hull, “Symmetries and compactifications of (4,0) conformal gravity”, JHEP12(2000) 007, arXiv:hep-th/0011215

work page arXiv 2000
[23]

Duality in gravity and higher spin gauge fields

C. M. Hull, “Duality in gravity and higher spin gauge fields”, JHEP09(2001) 027,arXiv:/hep-th0107149

work page 2001
[24]

𝐸(11)and M theory

P. West, “𝐸(11)and M theory”, Class. Quant. Grav.18(2001) 443,arXiv:hep-th-0104081

work page 2001
[25]

𝐷= 6,𝒩= (2,0)and𝒩= (4,0)theories

L. Borsten, “𝐷= 6,𝒩= (2,0)and𝒩= (4,0)theories”, Phys. Rev. D97(2018) 066014, arXiv:1708.02573 [hep-th]

work page arXiv 2018
[26]

The action of the (free) (4,0)-theory

M. Henneaux, V. Lekeu, A. Leonard, “The action of the (free) (4,0)-theory”, JHEP01(2018) 114, arXiv:01711.07448 [hep-th], [Erratum: JHEP05(2018) 105]

work page arXiv 2018
[27]

The action the (free)𝒩= (3,1)theory in six spacetime dimensions

M. Henneaux, V. Lekeu, J. Matulich, S. Prohazka, “The action the (free)𝒩= (3,1)theory in six spacetime dimensions”, JHEP06(2018) 057,arXiv:1804.10125 [hep-th]

work page arXiv 2018
[28]

On symmetries and dynamics of exotic supermultiplets,

R. Minasian, C. Strickland-Constable, Y.‘Zhang, “On symmetries and dynamics of exotic supermultiplets,” JHEP01(2021) 174,arXiv:2007.08888 [hepth]

work page arXiv 2021
[29]

Towards exotic6𝐷supergravities,

Y. Bertrand, S. Hohenegger, O. Holm, H. Samtleben, “Towards exotic6𝐷supergravities,” Phys. Rev. D 103(2021) 046002,arXiv:2007.11644 [hep-th]

work page arXiv 2021
[30]

Unified non-metric (1,0) tensor-Einstein supergravity theories and (4,0) supergravity in six dimensions

M. Gunaydin, “Unified non-metric (1,0) tensor-Einstein supergravity theories and (4,0) supergravity in six dimensions”, JHEP06(2021) 081,arXiv:2009.01274 [hep-th]

work page arXiv 2021
[31]

The notoph and its possible interactions

V. I. Ogievetsky, I. V. Polubarinov, “The notoph and its possible interactions”, Yadernaya Fizika (Soviet Journal Nuclear Physics),4(1967) 156; reprinted inSupersymmetries and Quantum Symmetries, J. Wess and E. A. Ivanov (Eds.), Springer, 1999, pp. 391-396

work page 1967
[32]

Classical direct interstring action

M. Kalb, P. Ramond, “Classical direct interstring action”, Phys. Rev. D9(1974) 2273

work page 1974
[33]

Spontneous dynamical breaking of gauge symmetry in dual models

E. Kremmer, J. Scherk, “Spontneous dynamical breaking of gauge symmetry in dual models", Nucl. Phys., B72(1974) 117

work page 1974
[34]

Supersymmetry, supergravity theories and the dual spinor model

F. Glozzi, J. Scherk, D. I. Olive, “Supersymmetry, supergravity theories and the dual spinor model", Nucl. Phys. B122(1977) 253

work page 1977
[35]

Gauge Fields, Nonlinear Realizations, Supersymmetry

E. A. Ivanov, “Gauge Fields, Nonlinear Realizations, Supersymmetry”, Phys. Part. Nucl.,47(2016) 508, arXiv:1604.01379 [hep-th]. 22

work page arXiv 2016
[36]

Covariant quantization of tensor multiplet models

S. M.Kuzenko, E. S. N. Raptakis, “Covariant quantization of tensor multiplet models", JHEP09(2024) 182,arXiv:2406.0176

work page arXiv 2024
[37]

The partition function of degenerate quadratic functionals and Ray-Singer invariants

A. S. Schwarz, “The partition function of degenerate quadratic functionals and Ray-Singer invariants”, Lett. Math. Phys.2(1978) 247

work page 1978
[38]

The partition function of a degenerate functional

A. S. Schwarz, “The partition function of a degenerate functional”, Commun. Math. Phys.67(1979) 1

work page 1979
[39]

Hidden ghosts

W. Siegel, “Hidden ghosts", Phys. Lett. B93(1980) 170

work page 1980
[40]

Renormalizability properties of antisymmetric tensor field coupled to gravity

E. Sezgin, P. van Nieuwenhuizen, “Renormalizability properties of antisymmetric tensor field coupled to gravity", Phys. Rev. D22(1980) 179

work page 1980
[41]

Skew-symmetric tensor gauge field theory dynamically realized in the QCD U(1) channel

H. Hata, T. Kugo, N. Ohta, “Skew-symmetric tensor gauge field theory dynamically realized in the QCD U(1) channel", Nucl. Phys. B178(1981) 527

work page 1981
[42]

The geometrical approach to antisymmetric tensor field theory

Y. N.Obukhov, “The geometrical approach to antisymmetric tensor field theory", Phys. Lett, B109(1982) 195

work page 1982
[43]

Antisymmetric tensor gauge theories and nonlinear sigma models

D. Z.Freedman, P. K. Townsend, “Antisymmetric tensor gauge theories and nonlinear sigma models", Nucl. Phys. B177(1981) 282

work page 1981
[44]

Covariant quantization of nonabelian antisymmetric tensor gauge theories

J. Thierry-Mieg, L. Baulieu, “Covariant quantization of nonabelian antisymmetric tensor gauge theories", Nucl. Phys. B228(1983) 259

work page 1983
[45]

Quantum equivalence of dual field theories

E. S. Fradkin, A. A Tseytlin, “Quantum equivalence of dual field theories", Ann. Phys.162(1985) 31

work page 1985
[46]

B190(1987) 122

S.P.deAlwis, M.T.Grisaru, L.Mazincescu, “Unitariryinantisymmetrictensorgaugetheories:, Phys.Lett. B190(1987) 122

work page 1987
[47]

Quantization of non-abelian antisymmetric tensor field

A. A. Slavnov, S. A. Frolov, “Quantization of non-abelian antisymmetric tensor field", Theor. Math. Phys. 75(1988) 470

work page 1988
[48]

Quantum equivalence of the Freedman-Townsend model and the principal chiral𝜎-model

I. L. Buchbinder, S. M. Kuzenko, “Quantum equivalence of the Freedman-Townsend model and the principal chiral𝜎-model", unpublished (1987),arXiv:2405.16782 [hep-th]

work page arXiv 1987
[49]

Quantization and unitary in antisymmetric tensor gauge theories

S. P. de Alwis, M. T. Grisaru, L. Mazincescu, “Quantization and unitary in antisymmetric tensor gauge theories", Nucl. Phys. B303(1988) 57

work page 1988
[50]

Lagrangian and Hamiltonian BRST structures of the antisymmetric tensor gauge theory

C. Battle, J. Gomes, “Lagrangian and Hamiltonian BRST structures of the antisymmetric tensor gauge theory", Phys. Rev. D38(1988) 1179

work page 1988
[51]

Quantum equivalence of four-dimensional nonlinear sigma-model and antisymmetric tensor model

N. K. Nielsen, “Quantum equivalence of four-dimensional nonlinear sigma-model and antisymmetric tensor model", Nucl. Phys. B332(1990) 391

work page 1990
[52]

Antibracket, antifields and gauge theory quantization,

J. Gomis, J. Paris and S. Samuel, “Antibracket, antifields and gauge theory quantization,” Phys. Repts. 259(1995), 1,arXiv:hep-th/9412228 [hep-th]

work page arXiv 1995
[53]

Gauge spinor superfield as a scalar multiplet

W. Siegel, “Gauge spinor superfield as a scalar multiplet", Phys. Lett. B85(1979) 333

work page 1979
[54]

Super𝑝-form gauge superfields

S. J.Gates, “Super𝑝-form gauge superfields", Nucl.Phys. B184(1981) 381

work page 1981
[55]

Energy-momentum tensors, supercurrents, (super)traces and quantum equivalence

M. T.Grisaru, N. K. Nielsen, W. Siegel, D. Zanon, “Energy-momentum tensors, supercurrents, (super)traces and quantum equivalence", Nucl. Phys. B247(1984) 157

work page 1984
[56]

Quantization of the classically equivalent theories in the superspace of simple supergravity and quantum equivalence

I. L. Buchbinder, S. M. Kuzenko, “Quantization of the classically equivalent theories in the superspace of simple supergravity and quantum equivalence", Nucl. Phys. B308(1988) 162

work page 1988
[57]

Ideas and Methods of Supersymmetry and Supergravity or a Walk Through Superspace

I. L. Buchbinder, S. M. Kuzenko, “Ideas and Methods of Supersymmetry and Supergravity or a Walk Through Superspace", IOP Publishing, 1998

work page 1998
[58]

Supersymmetric extension of nonAbelian scalar tensor dual- ity

K. Furita, T. Inami, H. Nakajima, M. Nitta, “Supersymmetric extension of nonAbelian scalar tensor dual- ity”, Prog. Theor. Phys.106(2001) 851,arXiv:hep-th/0106138. 23

work page arXiv 2001
[59]

Quantization of relativistic systems with constraints,

E. S. Fradkin and G. Vilkovisky, “Quantization of relativistic systems with constraints," Phys. Lett. B55 (1975) 224

work page 1975
[60]

Relativistic S-matrix of dynamical systems with boson and fermion con- straints,

I. A. Batalin, E. S. Fradkin, “Relativistic S-matrix of dynamical systems with boson and fermion con- straints," Phys. Lett. B69(1977) 309

work page 1977
[61]

Quantization of gauge systems,

M. Henneaux, C. Teitelboim, “Quantization of gauge systems,” Princeton Univ. Press, 1992

work page 1992
[62]

Gauge Algebra and Quantization,

I. A. Batalin, G. A. Vilkovisky, “Gauge Algebra and Quantization,” Phys. Lett. B102(1981) 27

work page 1981
[63]

Quantization of Gauge Theories with Linearly Dependent Generators,

I. Batalin, G. Vilkovisky, “Quantization of Gauge Theories with Linearly Dependent Generators,” Phys. Rev. D28(1983) 2567, [Erratum: Phys. Rev. D30(1984) 508]

work page 1983
[65]

Covariant quantization of totally an- tisymmetric tensor-spinor field in𝐴𝑑𝑆𝑑

A. O. Barvinsky, I. L. Buchbinder, V. A. Krykhtin, D. V. Nesterov, “Covariant quantization of totally an- tisymmetric tensor-spinor field in𝐴𝑑𝑆𝑑", Phys. Rev. D113(2026) 045022,arXiv:2509.01863 [hep-th]

work page arXiv 2026
[66]

On the quantization and anomalies of antisymmetric tensor-spinors,

V. Lekeu, Y. Zhang, “On the quantization and anomalies of antisymmetric tensor-spinors,” JHEP11(2021) 078,arXiv:2109.03963 [hep-th]

work page arXiv 2021
[67]

Feynman Diagramms for the Yang-Mills Field

L. D. Faddeev, V. N. Popov, “Feynman Diagramms for the Yang-Mills Field", Phys. Lett. B25(1967) 29. 24

work page 1967