A quantum mechanical three-body problem for two identical fermions of mass
m and a distinct particle of mass m1 in the universal limit of zero-range
two-body interaction is studied. For the unambiguous formulation of the problem
in the interval μr<m/m1≤μc (μr≈8.619 and μc≈13.607) an additional parameter b determining the wave function near
the triple-collision point is introduced; thus, a one-parameter family of
self-adjoint Hamiltonians is defined. The dependence of the bound-state
energies on m/m1 and b in the sector of angular momentum and parity LP=1− is calculated and analysed with the aid of a simple model