the interaction potential acts only between the electrons, it is natural to
write the orbital part in center-of-mass coordinates, where
and
The problem stated that the totalmomentum was zero, so set We
must now determine the form for the relative eigenfunction It obeys
the Schrödinger equation with the reduced mass where is the
electron mass:
We have reduced the problem to solving the bound state of a “particle” in
a box. Here the “particle” is the relative motion of two electrons. However,
since the orbital part of the wave function must have odd parity, we need
to find the lowest energy state which is antisymmetric,
Bound states have where the bindingenergy Define
two wave vectors: for outside the box, and
when the particle is in the box, The lowest
antisymmetric wave function is
We match the wave function and its derivative at one edge, say
which gives two equations:
We divide these two equations, which eliminates the constants A and B.
The remaining equation is the eigenvalue equation for
Since and are both positive, the cotangent of must be negative,
which requires that This imposes a constraint for the existence
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