Assume a central potential of finite range, i.e.
.
Then stationary state solutions of the eigenvalue equation
with the asymptotic form
exist. Here
is the scattering amplitude, dl is called the phase shift of the lth partial wave.
The differential scattering cross section is
![]()
and the total scattering cross section is
![]()
![]()
Let R be the range of the potential. If
, then dl=0.
![]()
Assume
for all l except l=0.
Then
,
and
. This is called s-wave
scattering.
For a finite range potential U(r) of range R the phase shift d0 is negative if
and
it is positive if
. If
then
if kR<<1.
For
we can have
.
If
. This is called the Ramsauer-Townsend
effect.
![]()
The elastic scattering cross section in the Born Approximation is
, and m
is the reduced mass.