Duality in quantum Liouville theory

The quantisation of the two-dimensional Liouville field theory is investigated using the path integral, on the sphere, in the large radius limit. The general form of the $N$-point functions of vertex operators is found and the three-point function is derived explicitly. In previous work it was infer...

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Bibliographic Details
Main Authors: O'Raifeartaigh, Lochlainn (Author) , Pawlowski, Jan M. (Author) , Sreedhar, Vinnakota (Author)
Format: Article (Journal) Chapter/Article
Language:English
Published: 1999
In: Arxiv

Online Access:Verlag, kostenfrei, Volltext: http://arxiv.org/abs/hep-th/9811090
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Author Notes:L. O'Raifeartaigh, J.M. Pawlowski, and V.V. Sreedhar
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Summary:The quantisation of the two-dimensional Liouville field theory is investigated using the path integral, on the sphere, in the large radius limit. The general form of the $N$-point functions of vertex operators is found and the three-point function is derived explicitly. In previous work it was inferred that the three-point function should possess a two-dimensional lattice of poles in the parameter space (as opposed to a one-dimensional lattice one would expect from the standard Liouville potential). Here we argue that the two-dimensionality of the lattice has its origin in the duality of the quantum mechanical Liouville states and we incorporate this duality into the path integral by using a two-exponential potential. Contrary to what one might expect, this does not violate conformal invariance; and has the great advantage of producing the two-dimensional lattice in a natural way.
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