Abstract
By expressing the two-electron wave functions in hyperspherical coordinates (R,Ω) in an adiabatic approximation Fμ(R)Φμ(R;Ω), I describe a simple procedure for obtaining the channel functions Φμ(R;Ω) analytically. These analytical functions, Φμ(R;Ω) in the finite-R region, are obtained by generalizing the known hydrogenic solutions in the asymptotic (R) limit for each channel μ and are required to satisfy proper boundary conditions in the hyperangles Ω rigorously. It is shown that these analytical functions compare well with the channel functions obtained previously from numerical calculations and, in a straightforward manner, describe the + and - channels of doubly excited states. The implication of this result as a method of generalizing hyperspherical coordinates to many-electron problems is discussed.