In this contribution, we give an integral representation of the wave
functions of the quantum N-particle Toda chain with boundary interaction. In
the case of the Toda chain with one-boundary interaction, we obtain the wave
function by an integral transformation from the wave functions of the open Toda
chain. The kernel of this transformation is given explicitly in terms of
\Gamma-functions. The wave function of the Toda chain with two-boundary
interaction is obtained from the previous wave functions by an integral
transformation. In this case, the difference equation for the kernel of the
integral transformation admits separation of variables. The separated
difference equations coincide with the Baxter equation.Comment: 14 pages, based on the talk given at the Workshop ``Classical and
quantum integrable systems'' (Dubna, January 2004