English

Representations of affine Lie algebras, parabolic differential equations, and Lame functions

High Energy Physics - Theory 2016-09-06 v2 Classical Analysis and ODEs Quantum Algebra

Abstract

We consider correlation functions for the Wess-Zumino-Witten model on the torus with the insertion of a Cartan element; mathematically this means that we consider the function of the form F=\Tr(Φ1(z1)Φn(zn)q\deh)F=\Tr (\Phi_1 (z_1)\ldots \Phi_n (z_n)q^{-\d}e^{h}) where Φi\Phi_i are intertwiners between Verma modules and evaluation modules over an affine Lie algebra \ghat\ghat, \d\d is the grading operator in a Verma module and hh is in the Cartan subalgebra of \g\g. We derive a system of differential equations satisfied by such a function. In particular, the calculation of q\d\dqFq\frac{\d} {\d q} F yields a parabolic second order PDE closely related to the heat equation on the compact Lie group corresponding to \g\g. We consider in detail the case n=1n=1, \g=\sltwo\g = \sltwo. In this case we get the following differential equation (q=eπ\iτq=e^{\pi \i \tau}): (2π\i(K+2)\d\dτ+\d2\dx2)F=(m(m+1)(x+τ2)+c)F \left( -2\pi\i (K+2)\frac{\d}{\d\tau} +\frac{\d^2}{\d x^2}\right) F = (m(m+1)\wp(x+\frac{\tau}{2}) +c)F, which for K=2K=-2 (critical level) becomes Lam\'e equation. For the case mZm\in\Z we derive integral formulas for FF and find their asymptotics as K2K\to -2, thus recovering classical Lam\'e functions.

Keywords

Cite

@article{arxiv.hep-th/9310083,
  title  = {Representations of affine Lie algebras, parabolic differential equations, and Lame functions},
  author = {Pavel Etingof and Alexander Kirillov},
  journal= {arXiv preprint arXiv:hep-th/9310083},
  year   = {2016}
}

Comments

30 pages, no figures