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Related papers: Embedding of the Bosonic String into the $W_3$ Str…

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The string theory defined by gauging $\W_{\infty/2}$, the sub-algebra of $\W_{\infty}$ generated by the currents of even spin, is discussed. The critical value of the central charge is calculated using zeta-function techniques and shown to…

High Energy Physics - Theory · Physics 2015-06-26 C. M. Hull , Z. Khatun

The central theme of this thesis is noncommutativity in string theory. We explore in detail how noncommutative structures can emerge in case of the interacting bosonic string and even in the fermionic sector of superstring theory. We have…

High Energy Physics - Theory · Physics 2010-06-01 Arindam Ghosh Hazra

We study the $N=2$ string with a real structure on the $(2,2)$ spacetime, using BRST methods. Several new features emerge. In the diagonal basis, the operator $\exp(\lambda \int^z J^{\rm tot})$, which is associated with the moduli for the…

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

We generalise BMS algebras in three dimensions by the introduction of an arbitrary real parameter $\lambda$, recovering the standard algebras (BMS, extended BMS and Weyl-BMS) for $\lambda=-1$. We exhibit a realisation of the (centreless)…

High Energy Physics - Theory · Physics 2024-12-17 Carlos Batlle , José Figueroa-O'Farrill , Joaquim Gomis , Girish Vishwa

We study the spectrum of $W_3$ strings. In particular, we show that for appropriately chosen space-time signature, one of the scalar fields is singled out by the spin-3 constraint and is ``frozen'': no creation operators from it can appear…

High Energy Physics - Theory · Physics 2009-10-07 C. N. Pope , L. J. Romans , E. Sezgin , K. S. Stelle

It was previously shown that at critical central charge, $N$-extended superstrings can be embedded in $(N+1)$-extended superstrings. In other words, $(N=0,c=26)\to (N=1,c=15)\to (N=2,c=6)\to (N=3,c=0) \to (N=4,c=0) $. In this paper, we show…

High Energy Physics - Theory · Physics 2009-10-28 Nathan Berkovits , Nobuyoshi Ohta

We consider the nonlinear algebras $W(sl(4),sl(3))$ and $W(sl(3|1),sl(3))$ and find their realizations in terms of currents spanning conformal linearizing algebras. The specific structure of these algebras, allows us to construct…

High Energy Physics - Theory · Physics 2009-10-28 S. Bellucci , S. Krivonos , A. Sorin

We present the complete structure of the nonlinear $N=2$ super extension of Polyakov-Bershadsky, $W_3^{(2)}$, algebra with the generic central charge, $c$, at the {\it quantum} level. It contains extra two pairs of fermionic currents with…

High Energy Physics - Theory · Physics 2016-09-06 C. Ahn , S. Krivonos , A. Sorin

The W_3 algebra of central charge 6/5 is realized as a subalgebra of the vertex operator algebra V_{\sqrt{2}A_2} associated with a lattice of type \sqrt{2}A_2 by using both coset construction and orbifold theory. It is proved that W_3 is…

Quantum Algebra · Mathematics 2007-05-23 C. Dong , C. H. Lam , K. Tanabe , H. Yamada , K. Yokoyama

We observed that the null strings, tensionless strings with Carrollian worldsheets, exhibit an extra gauge symmetry, \textit{Carroll-Weyl} gauge symmetry, which cannot be obtained from ultra-relativistic Carrollian limit of tensile strings.…

High Energy Physics - Theory · Physics 2026-05-29 M. M. Sheikh-Jabbari , H. Yavartanoo

The BMS$_3$ Lie algebra belongs to a one-parameter family of Lie algebras obtained by centrally extending abelian extensions of the Witt algebra by a tensor density representation. In this paper we call such Lie algebras…

High Energy Physics - Theory · Physics 2025-04-15 José Figueroa-O'Farrill , Girish S Vishwa

The conformal extension of the BMS$_{3}$ algebra is constructed. Apart from an infinite number of 'superdilatations,' in order to incorporate 'superspecial conformal transformations,' the commutator of the latter with supertranslations…

High Energy Physics - Theory · Physics 2021-03-10 Oscar Fuentealba , Hernan A. Gonzalez , Alfredo Perez , David Tempo , Ricardo Troncoso

We give the explicite form of the BRST charge Q for the algebra W_4=WA_3 in the basis where the spin-3 and the spin-4 field are primary as well as for a basis where the algebra closes quadratically.

High Energy Physics - Theory · Physics 2009-10-22 K. Hornfeck

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

Berkovits and Vafa recently showed that critical string theories can be considered as critical superstring theories with a special choice of background. The embedding of the Virasoro algebra into the super-Virasoro algebra involved in this…

High Energy Physics - Theory · Physics 2009-10-28 I. N. McArthur

We present a procedure for computing gauge-invariant scattering amplitudes in the $W_3$ string, and use it to calculate three-point and four-point functions. We show that non-vanishing scattering amplitudes necessarily involve external…

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

In this paper, a continuation of \cite{MPS}, we investigate the $S_3$-orbifold subalgebra of $(\mathcal{V}_c)^{\otimes 3}$, that is, we consider the $S_3$-fixed point vertex subalgebra of the tensor product of three copies of the universal…

Quantum Algebra · Mathematics 2022-09-28 Antun Milas , Michael Penn , Christopher Sadowski

We perform a systematic investigation of free-scalar realisations of the Za\-mo\-lod\-chi\-kov $W_3$ algebra in which the operator product of two spin-three generators contains a non-zero operator of spin four which has vanishing norm. This…

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

Motivated by recent progress on the correspondence between string theory on anti-de Sitter space and conformal field theory, we address the question of constructing space-time N extended superconformal algebras on the boundary of AdS_3.…

High Energy Physics - Theory · Physics 2014-11-18 Jorgen Rasmussen

We consider the sl(2) current algebra at level k=-4 when the sl(2) BRST operator is nilpotent. We formulate a spectral sequence converging to the cohomology of this BRST operator. At the second term of the spectral sequence, we observe an…

High Energy Physics - Theory · Physics 2011-07-19 A M Semikhatov , I Yu Tipunin