An approximate symmetry of the three-body Coulomb problem revealed via appr
oximate separability of the hyperspherical adiabatics Hamiltonian in hypers
pherical elliptic coordinates is discussed. In the zeroth order this symmet
ry leads to a completely separable representation of the three-body wave fu
nction. Taking into account the non-adiabatic couplings, as well as the Iro
n-separable part of the Coulomb potential by mixing a few zeroth-order stat
es, permits one to obtain accurate results for systems with arbitrary masse
s and charges of particles, and for a wide spectrum below the three-body br
eakup threshold.