QUANTUM MECHANICS 3155.64 3D Delta Function (Princeton)
For a particle of wave vector Schrödinger’s equation for the radial part
of the wave function isOnly scattering is important at very low energies, so solve for
Also define and getAt is well behaved, so Thus we choose our wave
functions to beThe quantity is the phase shift. We match the wave functions at
The formula for matching the slopes is derived from (S.5.64.2):Matching the function and slope produces the equationswhich are solved to eliminate A and B and getIn the limit of low energy, we want We assume there are no bound
states so that where is a constant. We find in thislimit:We also give the formula for the cross section in terms of the scattering
length The assumption of no bound state is that