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 inferre...

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Hauptverfasser: O'Raifeartaigh, Lochlainn (VerfasserIn) , Pawlowski, Jan M. (VerfasserIn) , Sreedhar, Vinnakota (VerfasserIn)
Dokumenttyp: Article (Journal)
Sprache:Englisch
Veröffentlicht: 2 April 2002
In: Annals of physics
Year: 1999, Jahrgang: 277, Heft: 1, Pages: 117-143
DOI:10.1006/aphy.1999.5951
Online-Zugang:Verlag, Volltext: http://dx.doi.org/10.1006/aphy.1999.5951
Verlag, Volltext: http://www.sciencedirect.com/science/article/pii/S0003491699959511
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Verfasserangaben:L. O'Raifeartaigh, J.M. Pawlowski, and V.V. Sreedhar
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Zusammenfassung: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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DOI:10.1006/aphy.1999.5951