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This paper describes the reduced phase space of $N=1$, $D=4$ supergravity in the fully off-shell Palatini--Cartan formalism. This is achieved through the KT construction, allowing an explicit description of first-class constraints on the…

Mathematical Physics · Physics 2026-01-21 Alberto S. Cattaneo , Filippo Fila-Robattino

For free-field theories associated with BRST first-quantized gauge systems, we identify generalized auxiliary fields and pure gauge variables already at the first-quantized level as the fields associated with algebraically contractible…

High Energy Physics - Theory · Physics 2009-11-10 Glenn Barnich , Maxim Grigoriev , Alexei Semikhatov , Ilya Tipunin

Gauge-invariant systems of a general form with higher order derivatives of gauge parameters are investigated within the framework of the BFV formalism. Higher order terms of the BRST charge and BRST-invariant Hamiltonian are obtained. It is…

High Energy Physics - Theory · Physics 2009-10-30 Khazret S. Nirov

We study the relation between the lagrangian field-antifield formalism and the BRST invariant phase space formulation of gauge theories. Starting from the Batalin-Fradkin-Vilkovisky unitarized action, we demonstrate in a deductive way the…

High Energy Physics - Theory · Physics 2009-11-18 Heinz J. Rothe , Klaus D. Rothe

By using the field-antifield formalism, we show that the method of Batalin, Fradkin, Fradkina and Tyutin to convert Hamiltonian systems submitted to second class constraints introduces compensating fields which do not belong to the BRST…

High Energy Physics - Theory · Physics 2015-06-26 Ricardo Amorim , Ronaldo Thibes

We present a superfield formulation of the quantization program for theories with first class constraints. An exact operator formulation is given, and we show how to set up a phase-space path integral entirely in terms of superfields. BRST…

High Energy Physics - Theory · Physics 2009-10-30 I. A. Batalin , K. Bering , P. H. Damgaard

The off-shell nilpotent BRST charge and the BRST invariant effective action for non-abelian BF topological theories over D-dimensional manifolds are explicitly constructed. These theories have the feature of being reducible with exactly D-3…

High Energy Physics - Theory · Physics 2016-09-06 M. I. Caicedo , R. Gianvittorio , A. Restuccia , J. Stephany

Recent results of BRST quantization on inner product spaces are reviewed. It is shown how relativistic particle models may be quantized with finite norms and that the relation between the operator method and the conventional path integral…

High Energy Physics - Theory · Physics 2007-05-23 Robert Marnelius

We perform the constraint analysis of a three (2 + 1)-dimensional (3D) field-theoretic example for Hodge theory $(i)$ at the classical level within the ambit of Lagrangian formulation, and $(ii)$ at the quantum level within the framework of…

High Energy Physics - Theory · Physics 2024-11-13 Bhagya. R , Harsha Sreekumar , E. Harikumar , R. P. Malik

Covariant quantization of the Nambu-Goto spinning particle in 2+1-dimensions is studied. The model is relevant in the context of recent activities in non-commutative space-time. From a technical point of view also covariant quantization of…

High Energy Physics - Theory · Physics 2009-11-07 Subir Ghosh

Any regular quantum mechanical system may be cast into an abelian gauge theory by simply reformulating it as a reparametrization invariant theory. We present a detailed study of the BRST quantization of such reparametrization invariant…

High Energy Physics - Theory · Physics 2007-05-23 Robert Marnelius , Niclas Sandstrom

The Batalin-Fradkin-Tyutin (BFT) scheme, which is an improved version of Dirac quantization, is applied to the $CP^1$ model, and the compact form of a nontrivial first-class Hamiltonian is directly obtained by introducing the BFT physical…

High Energy Physics - Theory · Physics 2009-10-31 Soon-Tae Hong , Young-Jai Park , Kuniharu Kubodera , Fred Myhrer

The BRST generator is realized as a Hermitian nilpotent operator for a finite-dimensional gauge system featuring a quadratic super-Hamiltonian and linear supermomentum constraints. As a result, the emerging ordering for the Hamiltonian…

High Energy Physics - Theory · Physics 2009-10-30 Rafael Ferraro , Daniel M. Sforza

Gauge theories that have been first quantized using the Hamiltonian BRST operator formalism are described as classical Hamiltonian BRST systems with a BRST charge of the form <\Psi,\Omega\Psi>_{even} and with natural ghost and parity…

High Energy Physics - Theory · Physics 2009-11-10 Glenn Barnich , Maxim Grigoriev

The $CP^{N-1}$ model is quantised in the generalised canonical formalism of Batalin and Tyutin by converting the original second class system into first class. Operator ordering ambiguities present in the conventional quantisation scheme of…

High Energy Physics - Theory · Physics 2009-10-22 N. Banerjee , Subir Ghosh , R. Banerjee

We show that the harmonic Becchi-Rouet-Stora-Tyutin method of quantizing bosonic systems with second-class constraints or first-class holomorphic constraints extends to systems having both bosonic and fermionic second-class or first-class…

High Energy Physics - Theory · Physics 2013-11-13 Theodore J. Allen , Dennis B. Crossley

BRST-methods provide elegant and powerful tools for the construction and analysis of constrained systems, including models of particles, strings and fields. These lectures provide an elementary introduction to the ideas, illustrated with…

High Energy Physics - Theory · Physics 2015-06-26 J. W. van Holten

Canonical transformations relating the variables of the ADM-, Ashtekar's and Witten's formulations of gravity are computed in 2+1~dimensions. Three different forms of the BRST-charge are given in the 2+1 dimensional Ashtekar formalism, two…

General Relativity and Quantum Cosmology · Physics 2010-11-01 Géza Fülöp

We give a solution to the classical master equation of the Hamiltonian BRST-anti-BRST quantization scheme in the case of reducible gauge theories. Our approach does not require redefining constraints or reducibility functions. Classical…

Mathematical Physics · Physics 2014-09-26 A. V. Bratchikov

The conversion of second-class constraints into first-class constraints is used to extend the coordinate-free path integral quantization, achieved by a flat-space Brownian motion regularization of the coherent-state path integral measure,…

High Energy Physics - Theory · Physics 2009-10-30 John R. Klauder , Sergei V. Shabanov