On the spectral theory of one functional-difference operator from conformal field theory

preprint2014arXivOpen access

Abstract

In the paper we consider a functional-difference operator H=U+U−1+VH=U+U^{-1}+V, where UU and VV are self-adjoint Weyl operators satisfying UV=q2VUUV=q^{2}VU with q=eπiτq=e^{πiτ} and τ>0τ>0. The operator HH has applications in the conformal field theory and in the representation theory of quantum groups. Using modular quantum dilogarithm - a qq-deformation of the Euler's dilogarithm - we define the scattering solution and the Jost solutions, derive an explicit formula for the resolvent of the self-adjoint operator HH in the Hilbert space L2(R)L^{2}(\mathbb{R}), and prove the eigenfunction expansion theorem. The latter is a qq-deformation of the well-known Kontorovich-Lebedev transform in the theory of special functions. We also present a formulation of the scattering theory for the operator HH.

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