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Related papers: Extra Observables in Gauged WZW Models

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We introduce a consistent gauge extension of the SL(2,R) WZNW system, defined by a difference of two simple WZNW actions. By integrating out some dynamical variables in the functional integral, we show that the resulting effective theory…

High Energy Physics - Theory · Physics 2007-05-23 M. Blagojevic , B. Sazdovic

We modify the $SL(2,{\bf R})/U(1)$ WZW theory, which was shown to describe strings in a 2D black hole, to be invariant under chiral $U(1)$ gauge symmetry by introducing a Steukelberg field. We impose several interesting gauge conditions for…

High Energy Physics - Theory · Physics 2015-06-26 Haruhiko Terao , Kiyonori Yamada

A closed formula for the structure constants in the SL(2,C)/SU(2) WZNW model is derived by a method previously used in Liouville theory. With the help of a reflection amplitude that follows from the structure constants one obtains a…

High Energy Physics - Theory · Physics 2009-10-30 J. Teschner

Liouville, SL(2,R)/U(1) and SL(2,R)/R_+ coset structures are completely described by gauge invariant Hamiltonian reduction of the SL(2,R) WZNW theory.

High Energy Physics - Theory · Physics 2007-05-23 George Jorjadze , Gerhard Weigt

It is proved that Liouville theory and the two dimensional SO(2,1) gauged Wess-Zumino-Witten term are on-shell equivalent. This shed light on a possible higher dimensional generalization of the former theory.

High Energy Physics - Theory · Physics 2011-07-26 Andres Anabalon

We consider the gauging of $ SL(2,R) $ WZNW model by its nilpotent subgroup E(1). The resulting space-time of the corresponding sigma model is seen to collapse to a one dimensional field theory of Liouville. Gauging the diagonal subgroup $…

High Energy Physics - Theory · Physics 2009-10-22 M. Alimohammadi , F. Ardalan , H. Arfaei

We derive a relation between correlation functions of supergroup WZNW models and conformal field theories with extended superconformal symmetry. The supergroups considered have a bosonic subgroup of the form SL(2) x A for some Lie group A.…

High Energy Physics - Theory · Physics 2015-05-27 Thomas Creutzig , Yasuaki Hikida , Peter B. Ronne

Recently, a duality between Liouville theory and four dimensional N=2 gauge theory has been uncovered by some of the authors. We consider the role of extended objects in gauge theory, surface operators and line operators, under this…

High Energy Physics - Theory · Physics 2010-03-02 Luis F. Alday , Davide Gaiotto , Sergei Gukov , Yuji Tachikawa , Herman Verlinde

We propose a definition of irregular vertex operators in the H3+ WZW model. Our definition is compatible with the duality [1] between the H3+ WZW model and Liouville theory, and we provide the explicit map between correlation functions of…

High Energy Physics - Theory · Physics 2013-01-24 Davide Gaiotto , Joel Lamy-Poirier

The $SL(2,\R)$ WZNW $\rightarrow$ Liouville reduction leads to a nontrivial phase space on the classical level both in $0+1$ and $1+1$ dimensions. To study the consequences in the quantum theory, the quantum mechanics of the $0+1$…

High Energy Physics - Theory · Physics 2009-10-28 Tamas Fulop

We consider the standard vector gauging of Lorentz group $ SO(3,1) $ WZW model by its non-semisimple null Euclidean subgroup in two dimensions $ E(2) $. The resultant effective action of the theory is seen to describe a one dimensional…

High Energy Physics - Theory · Physics 2014-11-18 Amir Masoud Ghezelbash

Three explicit and equivalent representations for the monodromy of the conformal blocks in the SL(2,C)/SU(2) WZNW model are proposed in terms of the same quantity computed in Liouville field theory. We show that there are two possible…

High Energy Physics - Theory · Physics 2015-06-26 Benedicte Ponsot

(This talk was presented at the Third International Wigner Symposium on Group Theory, Oxford, September, 1993.) Matrix models provides us with the most powerful framework in which to analyze D=2 string theory, yet some of its miraculous…

High Energy Physics - Theory · Physics 2007-05-23 Michio Kaku

We study the connection between Zamolodchikov operator-valued relations in Liouville field theory and in the SL(2,R)_k WZNW model. In particular, the classical relations in SL(2,R)_k can be formulated as a classical Liouville hierarchy in…

High Energy Physics - Theory · Physics 2009-11-10 Gaetano Bertoldi , Stefano Bolognesi , Gaston Giribet , Marco Matone , Yu Nakayama

After reviewing some aspects of gravity in two dimensions, it is shown that non-trivial embeddings of sl(2) in a semi-simple (super) Lie algebra give rise to a very large class of extensions of 2D gravity. The induced action is constructed…

High Energy Physics - Theory · Physics 2014-11-18 A. Sevrin

We consider a generalization of the two-dimensional Liouville conformal field theory to any number of even dimensions. The theories consist of a log-correlated scalar field with a background $\mathcal{Q}$-curvature charge and an exponential…

High Energy Physics - Theory · Physics 2018-11-07 Tom Levy , Yaron Oz

Alday, Gaiotto, and Tachikawa conjectured relations between certain 4d N=2 supersymmetric field theories and 2d Liouville conformal field theory. We study generalizations of these relations to 4d theories with surface operators. For one…

High Energy Physics - Theory · Physics 2016-03-23 Edward Frenkel , Sergei Gukov , Joerg Teschner

We study the "topological gauged WZW model associated with $SU(2)/U(1)$",which is defined as the twisted version of the corresponding supersymmetric gauged WZW model. It is shown that this model is equivalent to a topological conformal…

High Energy Physics - Theory · Physics 2009-10-22 Toshio Nakatsu , Yuji Sugawara

The two-dimensional manifestly locally supersymmetric actions describing the N=2 and N=4 extended super-Liouville theory coupled to the N=2 and N=4 conformal supergravity, respectively, are constructed in superspace. It is shown that the…

High Energy Physics - Theory · Physics 2011-07-19 Sergei Ketov

We study the three-dimensional SU(2) lattice gauge theory at finite temperature using an observable which is dual to the Wilson line. This observable displays a behaviour which is the reverse of that seen for the Wilson line. It is non-zero…

High Energy Physics - Lattice · Physics 2009-10-30 Srinath Cheluvaraja
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