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After reviewing the Green-Schwarz superstring using the approach of Siegel, the superstring is covariantly quantized by constructing a BRST operator from the fermionic constraints and a bosonic pure spinor ghost variable. Physical massless…

High Energy Physics - Theory · Physics 2015-06-25 Nathan Berkovits

We investigate the gauging of conformal algebras with relations between the generators. We treat the $W_{5/2}$--algebra as a specific example. We show that the gauge-algebra is in general reducible with an infinite number of stages. We show…

High Energy Physics - Theory · Physics 2007-05-23 Kris Thielemans , Stefan Vandoren

Extended BRST invariance (BRST plus anti-BRST invariances) provides in principle a natural way of introducing the complete gauge fixing structure associated to a gauge field theory in the minimum representation of the algebra. However, as…

High Energy Physics - Theory · Physics 2008-11-26 Nelson R. F. Braga , Cresus F. L. Godinho

Using the quantum construction of the BV-BFV method for perturbative gauge theories, we show that the obstruction for quantizing a codimension 1 theory is given by the second cohomology group with respect to the boundary BRST charge.…

Mathematical Physics · Physics 2021-02-26 Nima Moshayedi

We present the BRST cohomologies of a class of constraint (super) Lie algebras as detour complexes. By giving physical interpretations to the components of detour complexes as gauge invariances, Bianchi identities and equations of motion we…

High Energy Physics - Theory · Physics 2014-11-20 D. Cherney , E. Latini , A. Waldron

We characterize the dependence on doublets of the cohomology of an arbitrary nilpotent differential s (including BRST differentials and classical linearized Slavnov-Taylor (ST) operators) in terms of the cohomology of the…

High Energy Physics - Theory · Physics 2009-11-07 Andrea Quadri

We construct the BRST operator for the nonlinear $WB_2$ and $W_4$ algebras. Contrary to the general belief, the nilpotent condition of the BRST operator doesn't determine all the coefficients. We find a three and seven parameter family of…

High Energy Physics - Theory · Physics 2009-10-22 Chuan-Jie Zhu

A superspace formulation is proposed for the osp(1,2)-covariant Lagrangian quantization of general massive gauge theories. The superalgebra os0(1,2) is considered as subalgebra of sl(1,2); the latter may be considered as the algebra of…

High Energy Physics - Theory · Physics 2015-06-26 Bodo Geyer , Dietmar Mülsch

The BRST approach is applied to the description of irreducible massless higher spins representations of the Poincare group in arbitrary dimensions. The total system of constraints in such theory includes both the first and the second class…

High Energy Physics - Theory · Physics 2009-10-31 A. Pashnev , M. Tsulaia

Motivated by construction of isospin generators in particle physics (built form the SU(2) algebra), we find an equivalence between the algebra of these generators and those of the Virasoro algebra. The form of the starting generators is…

High Energy Physics - Theory · Physics 2008-09-26 J. Alfaro , M. Cambiaso

The BRST quantization of a gauge theory in noncommutative geometry is carried out in the ``matrix derivative" approach. BRST/anti-BRST transformation rules are obtained by applying the horizontality condition, in the superconnection…

High Energy Physics - Theory · Physics 2009-10-28 Chang-Yeong Lee , Dae Sung Hwang , Yuval Ne'eman

In a previous paper \cite{Simple} it was shown that the BRST charge $Q$ for any gauge model with a Lie algebra symmetry may be decomposed as $Q=\del+\del^{\dag},\;\;\;\del^2=\del^{\dag 2}=0,\;\;\;[\del, \del^{\dag}]_+=0$ provided dynamical…

High Energy Physics - Theory · Physics 2009-10-22 Robert Marnelius

We write the BRST operator of the N=1 superstring as $Q= e^{-R} (\oint dz \gamma^2 b)e^R$ where $\gamma$ and $b$ are super-reparameterization ghosts. This provides a trivial proof that $Q$ is nilpotent.

High Energy Physics - Theory · Physics 2009-10-31 J. N. Acosta , N. Berkovits , O. Chandia

In this paper we analyse the structure of the BRST charge of nonlinear superalgebras. We consider quadratic non-linear superalgebras where a commutator (in terms of (super) Poisson brackets) of the generators is a quadratic polynomial of…

High Energy Physics - Theory · Physics 2009-11-05 M. Asorey , P. M. Lavrov , O. V. Radchenko , A. Sugamoto

The quantization of the complex linear superfield requires an infinite tower of ghosts. Using the Batalin-Vilkovisky technique, Grisaru, Van Proeyen, and Zanon have been able to define a correct procedure to construct a gauge-fixed action.…

High Energy Physics - Theory · Physics 2009-10-31 P. A. Grassi , G. Policastro , M. Porrati

The method of construction of auxiliary representations for a given Lie algebra is discussed in the framework of the BRST approach. The corresponding BRST charge turns out to be non -- hermitian. This problem is solved by the introduction…

High Energy Physics - Theory · Physics 2009-10-31 C. Burdik , A. Pashnev , M. Tsulaia

Reducible gauge theories with constraints linear in the momenta are quantized. The equivalence of the reduced phase space quantization, Dirac quantization and BRST quantization is established. The ghosts of ghosts are found to play a…

High Energy Physics - Theory · Physics 2014-11-18 R. Ferraro , M. Henneaux , M. Puchin

The study of quantum Lie algebras motivates a use of non-canonical ghosts and anti-ghosts for non-linear algebras, like W-algebras. This leads, for the W_3 and W_3^(2) algebras, to the BRST operator having the conventional cubic form.

Mathematical Physics · Physics 2008-11-26 A. P. Isaev , S. O. Krivonos , O. V. Ogievetsky

The ghost sector of SU(3) gauge field theory is studied, and new BRST-invariant states are presented that do not have any analog in other SU(N) field theories. The new states come in either ghost doublets or triplets, and they appear…

High Energy Physics - Theory · Physics 2007-05-23 Scott Chapman

Motivated by the recent work of Vilar et al. arXiv:0902.2956 we enhance our non-commutative translation invariant gauge model arXiv:0901.1681 by introducing auxiliary fields and ghosts forming a BRST doublet structure. In this way…

High Energy Physics - Theory · Physics 2009-08-03 Daniel N. Blaschke , Arnold Rofner , Manfred Schweda , Rene I. P. Sedmik