In the quantum-mechanical study of the scattering of a particle by a potential, a Born-approximation solution can be obtained in terms of a function y(r) that satisfies an equation of the form
(−∇2−K2)y(r)=F(r).
Assuming that yk(r)=(2π)−3/2exp(ik⋅r) is a suitably normalised eigenfunction of −∇2 corresponding to eigenvalue k2, find a suitable Green's function GK(r,r′). By taking the direction of the vector r−r′ as the polar axis for a k-space integration, show that GK(r,r′) can be reduced to
4π2∣r−r′∣1∫−∞∞w2−w02wsinwdw,
where w0=K∣r−r′∣.
[This integral can be evaluated using a contour integration (chapter 24) to give (4π∣r−r′∣)−1exp(iK∣r−r′∣).]