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Related papers: On structure constants and fusion rules in the $SL…

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We propose exact formulas for the 2- and 3-point functions of the WZNW model on the non-compact supergroup OSP(1|2). Using the path integral approach that was recently developed in arXiv:0706.1030 we show how local correlation functions in…

High Energy Physics - Theory · Physics 2008-11-26 Yasuaki Hikida , Volker Schomerus

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

The fusion products of admissible representations of the su(2) WZW model at the fractional level k=-4/3 are analysed. It is found that some fusion products define representations for which the spectrum of L_0 is not bounded from below.…

High Energy Physics - Theory · Physics 2009-11-07 Matthias R Gaberdiel

Gauged WZNW models are integrable conformal field theories. We integrate the classical \slu{} theory with periodic boundary conditions, which describes closed strings moving in a curved target-space geometry. We calculate its Poisson…

High Energy Physics - Theory · Physics 2009-10-31 Uwe Mueller , Gerhard Weigt

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

It is known that Liouville theory can be represented as an SL(2,R) gauged WZW model. We study a two dimensional field theory which can be obtained by analytically continuing some of the variables in the SL(2,R) gauged WZW model. We can…

High Energy Physics - Theory · Physics 2009-10-22 Nobuyuki Ishibashi

Many qualitatively new features of WZNW models associated to noncompact cosets are due to zero modes with continuous spectrum. Insight may be gained by reducing the theory to its zero-mode sector, the mini-superspace limit. This will be…

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

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

An infinite set of operator-valued relations that hold for reducible representations of the sl(2)_k algebra is derived. These relations are analogous to those recently obtained by Zamolodchikov which involve logarithmic fields associated to…

High Energy Physics - Theory · Physics 2014-11-18 Gaetano Bertoldi , Gaston Giribet

he analytic formulas for structure constants of $su(2S+1)$ algebra in terms of $3jm$ and $6j$ symbols of $su(2)$ have been derived for the decomplexification of the Liouville-von Neumann equation.

Quantum Physics · Physics 2008-07-21 E. A. Ivanchenko

We compute the gauge field functional integral giving the scalar product of the SU(2) Chern-Simons theory states on a Riemann surface of genus > 1. The result allows to express the higher genera partition functions of the SU(2) WZNW…

High Energy Physics - Theory · Physics 2008-02-03 Krzysztof Gawedzki

We provide the analytic expressions of the totally symmetric and anti-symmetric structure constants in the $\mathfrak{su}(N)$ Lie algebra. The derivation is based on a relation linking the index of a generator to the indexes of its non-null…

Mathematical Physics · Physics 2021-08-17 Duncan Bossion , Pengfei Huo

An analytic expression is proposed for the three-point function of the exponential fields in the Liouville field theory on a sphere. In the classical limit it coincides with what the classical Liouville theory predicts. Using this function…

High Energy Physics - Theory · Physics 2011-07-19 A. B. Zamolodchikov , Al. B. Zamolodchikov

The symplectic and Poisson structures of the Liouville theory are derived from the symplectic form of the SL(2,R) WZNW theory by gauge invariant Hamiltonian reduction. Causal non-equal time Poisson brackets for a Liouville field are…

High Energy Physics - Theory · Physics 2009-11-07 George Jorjadze , Gerhard Weigt

Using a gauge invariant reduction we directly integrate the SL(2,R)/U(1) WZNW theory. We prove that the conserved parafermions of this theory are coset currents. Quantum mechanically, the parafermion algebra, the energy-momentum tensor, and…

High Energy Physics - Theory · Physics 2007-05-23 C. Ford , G. Jorjadze , G. Weigt

In the first of this two-part series, we find `fixed point factorisation' formulas, towards an understanding of the fusion ring of WZW models. Fixed-point factorisation refers to the simplifications in the data of a CFT involving primary…

High Energy Physics - Theory · Physics 2015-06-03 Elaine Beltaos

We discuss Liouville field theory in the framework of Schwinger-Dyson approach and derive a functional equation for the three-point structure constant. We argue the existence of a second Schwinger-Dyson equation on the basis of the duality…

High Energy Physics - Theory · Physics 2015-01-20 Parikshit Dutta

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 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

An approach to studying lattice gauge models in the weak coupling region is proposed. Conceptually, it is based on the crucial role of the original Z(N) symmetry and the invariant gauge group measure. As an example, we calculate an…

High Energy Physics - Lattice · Physics 2007-05-23 O. A. Borisenko , V. K. Petrov , G. M. Zinovjev , J. Boháčik
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