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Related papers: Extra States in C<1 String Theory

200 papers

We describe the (chiral) BRST-cohomology of matter with central charge $1<c_M<25$ coupled to a ``Liouville" theory, realized as a free field with a background charge $Q_L$ such that $c_M+c_L=26$. We consider two cases: a) matter is realized…

High Energy Physics - Theory · Physics 2009-10-22 Adel Bilal

States in the absolute (semi-relative) cohomology but not in the relative cohomology are examined through the component decomposition of the string field theory action for the 2-D string. It is found that they are auxiliary fields without…

High Energy Physics - Theory · Physics 2010-11-01 Norisuke Sakai , Yoshiaki Tanii

States obtained by projecting boundary states, associated with D-branes, to fixed mass-level and momentum generically define non-trivial cohomology classes. For on-shell states the cohomology is the standard one, but when the states are…

High Energy Physics - Theory · Physics 2009-10-30 S. Ramgoolam , L. Thorlacius

We generalize the ground ring structure to all special BRST invariant operators in the right branch in the c=1 Liouville theory. We also discuss correlation functions of special states on the sphere.

High Energy Physics - Theory · Physics 2009-10-22 Miao Li

In the framework of the Sen conjectures a construction of vacuum superstring field theory on a non-BPS brane is discussed. A distinguished feature of this theory is a presence of a ghost kinetic operator mixing GSO+/- sectors. A candidate…

High Energy Physics - Theory · Physics 2009-11-07 I. Ya. Aref'eva , D. M. Belov , A. A. Giryavets

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

We study the $\NN=2$ string theory or the $\NN=4$ topological string on the deformed CHS background. That is, we consider the $\NN=2$ minimal model coupled to the $\NN=2$ Liouville theory. This model describes holographically the…

High Energy Physics - Theory · Physics 2010-04-05 Anatoly Konechny , Andrei Parnachev , David A. Sahakyan

Closed string physical states are BRST cohomology classes computed on the space of states annihilated by $b_0^-$. Since $b_0^-$ does not commute with the operations of picture changing, BRST cohomologies at different pictures need not…

High Energy Physics - Theory · Physics 2014-11-18 Nathan Berkovits , Barton Zwiebach

We provide a simple lagrangian interpretation of the meaning of the $b_0^-$ semi-relative condition in closed string theory. Namely, we show how the semi-relative condition is equivalent to the requirement that physical operators be…

High Energy Physics - Theory · Physics 2010-11-01 C. M. Becchi , R. Collina , C. Imbimbo

An analysis of the BRST cohomology of the G/G topological models is performed for the case of $A_1^{(1)}$. Invoking a special free field parametrization of the various currents, the cohomology on the corresponding Fock space is extracted.…

High Energy Physics - Theory · Physics 2019-08-15 O. Aharony , O. Ganor , N. Sochen J. Sonnenschein , S. Yankielowicz

The wedge states form an important subalgebra in the string field theory. We review and further investigate their various properties. We find in particular a novel expression for the wedge states, which allows to understand their star…

High Energy Physics - Theory · Physics 2009-11-07 Martin Schnabl

We discuss the BSRT quantization of 2D $N=1$ supergravity coupled to superconformal matter with $\hat{c} \leq 1$ in the conformal gauge. The physical states are computed as BRST cohomology. In particular, we consider the ring structure and…

High Energy Physics - Theory · Physics 2009-09-11 P. Bouwknegt , J. McCarthy , K. Pilch

We review the BRST analysis of the system of a (super)conformal matter coupled to 2D (super)gravity. The spectrum and its operator realization are reported. In particular, the operators associated with the states of nonzero ghost number are…

High Energy Physics - Theory · Physics 2008-11-26 Katsumi Itoh , Nobuyoshi Ohta

We complete the construction of vacuum string field theory by proposing a canonical choice of ghost kinetic term -- a local insertion of the ghost field at the string midpoint with an infinite normalization. This choice, supported by level…

High Energy Physics - Theory · Physics 2009-09-15 Davide Gaiotto , Leonardo Rastelli , Ashoke Sen , Barton Zwiebach

Recent results about topological coset models are summarized. The action of a topological ${G\over H}$ coset model ($rank\ H = rank\ G$) is written down as a sum of ``decoupled" matter, gauge and ghost sectors. The physical states are in…

High Energy Physics - Theory · Physics 2007-05-23 J. Sonnenschein

The discrete states in the $c=1$ string are shown to be the physical states of a certain topological sigma model. We define a set of new fields directly from $c=1$ variables, in terms of which the BRST charge and energy-momentum tensor are…

High Energy Physics - Theory · Physics 2009-10-22 H. Ishikawa , M. Kato

We show that a special superconformal coset (with $\hat c =3$) is equivalent to $c=1$ matter coupled to two dimensional gravity. This identification allows a direct computation of the correlation functions of the $c=1$ non-critical string…

High Energy Physics - Theory · Physics 2009-10-22 S. Mukhi , C. Vafa , E. Frenkel

In the study of the Type II superstring, it is useful to consider the BRST complex associated to the sum of two pure spinors. The cohomology of this complex is an infinite-dimensional vector space. It is also a finite-dimensional algebra…

High Energy Physics - Theory · Physics 2013-07-22 Andrei Mikhailov , Albert Schwarz , Renjun Xu

In this work, a particular BRST-exact class of deformations of the b ghost in the non-minimal pure spinor formalism is investigated and the impact of this construction in the $\mathcal{N}=2$ $\hat{c}=3$ topological string algebra is…

High Energy Physics - Theory · Physics 2013-07-24 Renann Lipinski Jusinskas

I present a toy model for the Berkovits pure spinor superparticle. It is a D=1, N=2 superparticle with no physical degrees of freedom. We study the cohomology in various ways, in particular finding an explicit expression for the `b'-field.…

High Energy Physics - Theory · Physics 2009-06-10 Michael Chesterman