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Related papers: Critical and non-critical W_{2,4} strings

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BRST operators for two-dimensional theories with spin-2 and spin-$s$ currents, generalising the $W_3$ BRST operator of Thierry-Mieg, have previously been obtained. The construction was based on demanding nilpotence of the BRST operators,…

High Energy Physics - Theory · Physics 2009-10-07 H. Lu , C. N. Pope , X. J. Wang , S. C. Zhao

In this paper, we construct the nilpotent Becchi-Rouet-Stora-Tyutin($BRST$) charges of spinor non-critical $W_{2,s}$ strings. The cases of $s=3,4$ are discussed in detail, and spinor realization for $s=4$ is given explicitly. The $BRST$…

High Energy Physics - Theory · Physics 2010-01-18 Yi-Shi Duan , Yu-Xiao Liu , Li-Jie Zhang

We discuss the conditions under which the BRST operator of a $W$-string can be written as the sum of two operators that are separately nilpotent and anticommute with each other. We illustrate our results with the example of the non-critical…

High Energy Physics - Theory · Physics 2009-10-22 E. Bergshoeff , H. J. Boonstra , M. de Roo , S. Panda , A. Sevrin

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 present a general argument for the construction of BRST charges of the `non-critical' $\W_{2,4}$, $\W_{2,5}$, $\W_{2,6}$, and $\W_{2,8}$ strings. This evidences the existence of BRST charges for a kind of soft-type algebras which can be…

High Energy Physics - Theory · Physics 2009-10-28 L. Palacios

In this paper, we construct non-critical BRST operators for matter and Liouville systems whose currents generate two different $W$ algebras. At the classical level, we construct the BRST operators for $W^{\rm M}_{2,s}\otimes W^{\rm…

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

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

We construct the BRST operator for non-critical $W_3$-strings and discuss the tachyon-like spectrum. For $N$-punctured spheres with $N \leq 5$ we briefly describe a formal definition of the integral over $W_3$-moduli space.

High Energy Physics - Theory · Physics 2009-10-22 M. Bershadsky , W. Lerche , D. Nemeschansky , N. P. Warner

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

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 review the detailed structure of the large $N=4$ superconformal algebra, and construct its BRST operator which constitutes the main object for analyzing $N=4$ strings. We then derive the general condition for the nilpotency of the BRST…

High Energy Physics - Theory · Physics 2009-10-28 Fiorenzo Bastianelli , Nobuyoshi Ohta

In this paper, we investigate the spinor field realizations of the $W_{2,4}$ algebra, making use of the fact that the $W_{2,4}$ algebra can be linearized through the addition of a spin-1 current. And then the nilpotent BRST charges of the…

High Energy Physics - Theory · Physics 2008-11-26 Li-Jie Zhang , Yu-Xiao Liu

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 derive the recently proposed BRST charge for non-critical W strings from a Lagragian approach. The basic observation is that, despite appearances, the combination of two classical ``matter'' and ``Toda'' w_3 systems leads to a closed…

High Energy Physics - Theory · Physics 2009-10-22 E. Bergshoeff , A. Sevrin , X. Shen

We construct BRST operators for certain higher-spin extensions of the Virasoro algebra, in which there is a spin-$s$ gauge field on the world sheet, as well as the spin-2 gauge field corrresponding to the two-dimensional metric. We use…

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

We perform a classical BRST analysis of the symmetries corresponding to a generic $w_N$-algebra. An essential feature of our method is that we write the $w_N$-algebra in a special basis such that the algebra manifestly has a ``nested'' set…

High Energy Physics - Theory · Physics 2009-10-22 E. Bergshoeff , H. J. Boonstra , S. Panda , M. de Roo

The noncritical $D=4$ $W_3$ string is a model of $W_3$ gravity coupled to two free scalar fields. In this paper we discuss its BRST quantization in direct analogy with that of the $D=2$ (Virasoro) string. In particular, we calculate the…

High Energy Physics - Theory · Physics 2015-06-26 Peter Bouwknegt , Jim McCarthy , Krzysztof Pilch

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

The grading Becchi-Rouet-Stora-Tyutin (BRST) method gives a way to construct the integer $W_{2,s}$ strings, where the BRST charge is written as $Q_B=Q_0+Q_1$. Using this method, we reconstruct the nilpotent BRST charges $Q_{0}$ for the…

High Energy Physics - Theory · Physics 2009-01-26 Shao-Wen Wei , Yu-Xiao Liu , Li-Jie Zhang , Ji-Rong Ren

We investigate new realisations of the $W_3$ algebra with arbitrary central charge, making use of the fact that this algebra can be linearised by the inclusion of a spin-1 current. We use the new realisations with $c=102$ and $c=100$ to…

High Energy Physics - Theory · Physics 2016-09-06 H. Lu , C. N. Pope , K. S. Stelle , K. W. Xu
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