Duality in Quantum Liouville Theory
L. O'Raifeartaigh, J. M. Pawlowski, and V. V. Sreedhar

TL;DR
This paper investigates the quantisation of 2D Liouville field theory using path integrals, revealing a duality that explains the two-dimensional lattice of poles in the three-point function, and introduces a dual exponential potential without breaking conformal invariance.
Contribution
It introduces a duality-based approach to Liouville theory, incorporating a two-exponential potential to naturally produce a two-dimensional lattice of poles in the three-point function.
Findings
Derived the general form of N-point functions on the sphere.
Explicitly computed the three-point function.
Showed that duality explains the two-dimensional lattice of poles.
Abstract
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 -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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