In quantum theory, a certain method (the Born approximation) gives the (so-called) amplitude f(θ) for the scattering of a particle of mass m through an angle θ by a uniform potential well of depth V0 and radius b (i.e. the potential energy of the particle is −V0 within a sphere of radius b and zero elsewhere) as
f(θ)=ℏ2K32mV0(sinKb−KbcosKb).
Here ℏ is the Planck constant divided by 2π, the energy of the particle is ℏ2k2/(2m) and K is 2ksin(θ/2).
Use l'H\^{o}pital's rule to evaluate the amplitude at low energies, i.e. when k and hence K tend to zero, and so determine the low-energy total cross-section.
[Note: the differential cross-section is given by ∣f(θ)∣2 and the total cross-section by the integral of this over all solid angles, i.e. 2π∫0π∣f(θ)∣2sinθdθ.]