Correlation functions for M^N/S_N orbifolds
Oleg Lunin, Samir D. Mathur
TL;DR
The paper develops a covering-space Liouville-action framework to compute twist-operator correlators in bosonic M^N/S_N CFTs, recasting correlation functions as partition functions on Riemann surfaces with genus-controlled contributions. It establishes universal genus-zero results that depend only on the central charge c, obtaining the twist-operator dimensions and, in certain cases, the fusion coefficients via explicit g=0 maps and Liouville actions; higher-genus contributions are shown to be suppressed at large N. The analysis reveals a close parallel between the genus-zero fusion rules and SU(2) WZW fusion rules, and it uncovers a stringy exclusion principle-type suppression in 3-point couplings as twist orders grow toward √N. The work provides a robust framework for comparing orbifold CFT data to dual descriptions (e.g., D1-D5 systems and AdS3/CFT) and sets the stage for extending the method to supersymmetric cases and more intricate dualities.
Abstract
We develop a method for computing correlation functions of twist operators in the bosonic 2-d CFT arising from orbifolds M^N/S_N, where M is an arbitrary manifold. The path integral with twist operators is replaced by a path integral on a covering space with no operator insertions. Thus, even though the CFT is defined on the sphere, the correlators are expressed in terms of partition functions on Riemann surfaces with a finite range of genus g. For large N, this genus expansion coincides with a 1/N expansion. The contribution from the covering space of genus zero is `universal' in the sense that it depends only on the central charge of the CFT. For 3-point functions we give an explicit form for the contribution from the sphere, and for the 4-point function we do an example which has genus zero and genus one contributions. The condition for the genus zero contribution to the 3-point functions to be non--vanishing is similar to the fusion rules for an SU(2) WZW model. We observe that the 3-point coupling becomes small compared to its large N limit when the orders of the twist operators become comparable to the square root of N - this is a manifestation of the stringy exclusion principle.
