Abstract:
The Faddeev equations in a model with the two-particle boundary conditions are
reformulated in order to remove the characteristic singularities of the model. The
equations are reduced to a set of one-dimensional integral equations the kernel of
which is defined by another independent set of one-dimensional integral equations.
The equations obtained for three-particle system with the pair interaction in a finite
number of partial states determines the three-particle wave function uniquely.