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Related papers: A BRST charge for non-critical $\W_{2,s}$ strings

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The detailed description of the method of the construction of the nilpotent BRST charges for nonlinear algebras of constraints appearing in the description of the massless higher spin fields on the $AdS_D$ background is presented. It is…

High Energy Physics - Theory · Physics 2007-05-23 I. L. Buchbinder , A. Pashnev , M. Tsulaia

In this paper, we mainly investigate the $W_{2,s}^{M}\otimes W_{2,s}^{L}$ system, in which the matter and the Liouville subsystems generate $W_{2,s}^{M}$ and $W_{2,s}^L$ algebras respectively. We first give a brief discussion of the…

High Energy Physics - Theory · Physics 2009-04-24 Yu-Xiao Liu , Shao-Wen Wei , Li-Jie Zhang , Ji-Rong Ren

We give an explicit formula for the Becchi-Rouet-Stora-Tyutin (BRST) charge associated with Poisson superalgebras. To this end, we split the master equation for the BRST charge into a pair of equations such that one of them is equivalent to…

High Energy Physics - Theory · Physics 2012-03-09 A. V. Bratchikov

In this paper the spinor field BRST charges of the W2,6 string and W6 string are constructed, where the BRST charges are graded.

High Energy Physics - Theory · Physics 2007-05-23 Shu-Cheng Zhao , Li-Jie Zhang , Yu-Xiao Liu

The noncritical $4D$ $\cW_3$ string is a model of $\cW_3$ gravity coupled to two free scalar fields. In this paper we discuss its BRST quantization in direct analogy with that of the $2D$ (Virasoro) string. The physical operators form a…

High Energy Physics - Theory · Physics 2016-09-06 Peter Bouwknegt , Jim McCarthy , Krzysztof Pilch

We investigate the new spinor field realizations of the $W_{3}$ algebra, making use of the fact that the $W_{3}$ algebra can be linearized by the addition of a spin-1 current. We then use these new realizations to build the nilpotent…

High Energy Physics - Theory · Physics 2009-11-11 Li-Jie Zhang , Yu-Xiao Liu , Ji-Rong Ren

The method of the BRST quantization is considered for the system of constraints, which form a Lie algebra. When some of the Cartan generators do not imply any conditions on the physical states, the system contains the first and the second…

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

In this paper, we examine the conditions under which a higher-spin string theory can be quantised. The quantisability is crucially dependent on the way in which the matter currents are realised at the classical level. In particular, we…

High Energy Physics - Theory · Physics 2009-10-07 H. Lu , C. N. Pope , K. Thielemans , X. J. Wang , K. -W. Xu

Possible ways of constructing extended fermionic strings with $N=4$ world-sheet supersymmetry are reviewed. String theory constraints form, in general, a non-linear quasi(super)conformal algebra, and can have conformal dimensions $\geq 1$.…

High Energy Physics - Theory · Physics 2010-04-06 Sergei V. Ketov

It is shown that for a large class of non-holonomic quantum mechanical systems one can make the computation of BRST charge fully algorithmic. Two computer algebra programs written in the language of {\tt REDUCE} are described. They are able…

High Energy Physics - Theory · Physics 2015-06-26 A. Burnel , H. Caprasse , A. Dresse

We construct a sequence of nilpotent BRST charges in RNS superstring theory, based on new gauge symmetries on the worldsheet, found in this paper. These new local gauge symmetries originate from the global nonlinear space-time…

High Energy Physics - Theory · Physics 2010-01-07 Dimitri Polyakov

In a recent work it has been shown that the bosonic strings could be embedded into a special class of $N=1$ fermionic strings. We argue that the superpartners of any physical state in the spectrum of this fermionic string is non-physical.…

High Energy Physics - Theory · Physics 2009-10-28 Pablo M. Llatas , Shibaji Roy

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

A general method of the BRST--anti-BRST symmetric conversion of second-class constraints is presented. It yields a pair of commuting and nilpotent BRST-type charges that can be naturally regarded as BRST and anti-BRST ones. Interchanging…

High Energy Physics - Theory · Physics 2009-11-10 I. A. Batalin , M. A. Grigoriev

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

It has been shown that certain $W$ algebras can be linearised by the inclusion of a spin--1 current. This provides a way of obtaining new realisations of the $W$ algebras. Recently such new realisations of $W_3$ were used in order to embed…

High Energy Physics - Theory · Physics 2009-10-07 H. Lu , C. N. Pope , K. W. Xu

We investigate the cohomology structure of a general noncritical $W_N$-string. We do this by introducing a new basis in the Hilbert space in which the BRST operator splits into a ``nested'' sum of nilpotent BRST operators. We give explicit…

High Energy Physics - Theory · Physics 2009-10-22 E. Bergshoeff , J. de Boer , M. de Roo , T. Tjin

We study the cohomology of the critical $W_4$ string using the $W_4$ BRST charge in a special basis in which it contains three separately nilpotent BRST charges. This allows us to obtain the physical operators in three steps. In the first…

High Energy Physics - Theory · Physics 2010-04-06 H. J. Boonstra

We extend our formulation of the covariant quantum superstring as a WZNW model with N=2 superconformal symmetry to N=4. The two anticommuting BRST charges in the N=4 multiplet of charges are the usual BRST charge Q_S and a charge Q_V…

High Energy Physics - Theory · Physics 2009-11-10 P. A. Grassi , P. van Nieuwenhuizen

It is 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 Lagrange multipliers are used but without…

High Energy Physics - Theory · Physics 2016-08-14 Robert Marnelius