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Related papers: On Physical States in c<1 String Theory

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This note is a brief addendum to my article Nucl. Phys. B 864 (2012) 285, [arXiv: 1110.5510], which discusses the noghost theorem in Ramond sectors of string models. In this addendum we derive additional information about the structure of…

High Energy Physics - Theory · Physics 2015-06-12 Charles B. Thorn

The purpose of this note is to extend the improved proof of the no-ghost theorem for the bosonic and Neveu-Schwarz dual resonance models, presented in my article Nuclear Physics B286 (1987) 61, to cover the Ramond fermion string. As in that…

High Energy Physics - Theory · Physics 2015-05-30 Charles B. Thorn

We study the quantization of systems with local particle-ghost symmetries. The systems contain ordinary particles including gauge bosons and their counterparts obeying different statistics. The particle-ghost symmetry is a kind of fermionic…

High Energy Physics - Theory · Physics 2015-10-28 Yoshiharu Kawamura

We study the cohomology of the massless BRST complex of the Type IIB pure spinor superstring in flat space. In particular, we find that the cohomology at the ghost number three is nontrivial and transforms in the same representation of the…

High Energy Physics - Theory · Physics 2015-10-27 Andrei Mikhailov

A careful treatment of closed string BRST cohomology shows that there are more discrete states and associated symmetries in $D=2$ string theory than has been recognized hitherto. The full structure, at the $SU(2)$ radius, has a natural…

High Energy Physics - Theory · Physics 2010-04-07 Edward Witten , Barton Zwiebach

We study the star algebra of ghost sector in vacuum string field theory (VSFT). We show that the star product of two states in the Siegel gauge is BRST exact if we take the BRST charge to be the one found in hep-th/0108150, and the BRST…

High Energy Physics - Theory · Physics 2009-11-07 Kazumi Okuyama

We present a simple procedure for constructing the complete cohomology of the BRST operator of the two-scalar and multi-scalar $W_3$ strings. The method consists of obtaining two level--15 physical operators in the two-scalar $W_3$ string…

High Energy Physics - Theory · Physics 2010-04-06 H. Lu , C. N. Pope , X. J. Wang , K. W. Xu

We present some explicit results on the structure of singular vectors in $c=2$ Verma modules of the $\cW_3$ algebra. Using the embedding patterns of those vectors we construct resolutions for the $c=2$ irreducible modules, and thus are able…

High Energy Physics - Theory · Physics 2007-05-23 P. Bouwknegt , J. McCarthy , K. Pilch

The nonlinear structures in 2D quantum gravity coupled to the $(q+1,q)$ minimal model are studied in the Liouville theory to clarify the factorization and the physical states. It is confirmed that the dressed primary states outside the…

High Energy Physics - Theory · Physics 2009-10-22 Ken-ji Hamada

We systematically study deformations of chiral forms with applications to string theory in mind. To first order in the coupling constant, this problem can be translated into the calculation of the local BRST cohomological group at ghost…

High Energy Physics - Theory · Physics 2009-10-31 Xavier Bekaert , Marc Henneaux , Alexander Sevrin

We study the properties of {\bf exact} (all level $k$) quantum coherent states in the context of string theory on a group manifold (WZWN models). Coherent states of WZWN models may help to solve the unitarity problem: Having positive norm,…

High Energy Physics - Theory · Physics 2016-08-16 A. L. Larsen , N. Sánchez

A spectrum generating algebra is constructed and used to find all the physical states of the $W_3$ string with standard ghost number. These states are shown to have positive norm and their partition function is found to involve the Ising…

High Energy Physics - Theory · Physics 2015-06-26 Peter West

The existence of a ground ring of ghost number zero operators in the chiral BRST cohomology of the N=2 string is used to derive an infinite set of Ward identities for the closed-string scattering amplitudes at arbitrary genus. These…

High Energy Physics - Theory · Physics 2009-10-31 Klaus Junemann , Olaf Lechtenfeld

We develop an approach based on the Noether method to construct nilpotent BRST charges and BRST-invariant actions. We apply this approach first to the holomorphic part of the flat-space covariant superstring, and we find that the ghosts b,…

High Energy Physics - Theory · Physics 2009-11-07 P. A. Grassi , G. Policastro , P. van Nieuwenhuizen

In our previous paper, we have presented a covariant BRST quantization of unimodular gravity which may account for the smallness of the cosmological constant, and have shown that the physical degrees of freedom in the theory are the same as…

High Energy Physics - Theory · Physics 2022-05-25 Taichiro Kugo , Ryuichi Nakayama , Nobuyoshi Ohta

The BRST invariance condition in a highest-weight representation of the topological ($\equiv$ twisted $N=2$) algebra captures the `invariant' content of two-dimensional gravity coupled to matter. The standard DDK formulation is recovered by…

High Energy Physics - Theory · Physics 2011-04-20 B. Gato-Rivera , A. M. Semikhatov

Using a formulation of QCD_2 as a perturbed conformally invariant theory involving fermions, ghosts, as well as positive and negative level Wess-Zumino-Witten fields, we show that the BRST conditions become restrictions on the conformally…

High Energy Physics - Theory · Physics 2009-10-28 E. Abdalla , K. D. Rothe

We describe the complete cohomology of the Berkovits BRST operator for the superparticle. It is non-zero at eight ghost numbers, splitting into two quartets, the members of each quartet being completely isomorphic. Based only on…

High Energy Physics - Theory · Physics 2007-05-23 Michael Chesterman

We revisit the theory of background fields constructed on the BRST-algebra of a spinning particle with $\mathcal{N}=4$ worldline supersymmetry, whose spectrum contains the graviton but no other fields. On a generic background, the closure…

High Energy Physics - Theory · Physics 2022-03-14 Daniel Bockisch , Ivo Sachs

Coupling any interacting quantum mechanical system to gravity in one (time) dimension requires the cosmological constant to belong to the matter energy spectrum and thus to be quantised, even though the gravity sector is free of any quantum…

High Energy Physics - Theory · Physics 2007-05-23 Jan Govaerts
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