Using the Born approximation, the scattering amplitude $f(\theta)$ for a particle incident with momentum $\hbar k$ and scattered with momentum $\hbar k'$ by a potential energy $V(r)$ is given by:
$$f(\theta) = -\frac{m}{2\pi \hbar^2} \int e^{i(\vec{k}-\vec{k'})\cdot\vec{r}} V(r) d^3r$$
where $\theta$ is the scattering angle between the incident and scattered momenta.
For the Yukawa potential:
$$V(r) = \alpha \frac{e^{-\mu r}}{r}$$
($\alpha$, $\mu$ are constants)
find the differential scattering cross-section $\frac{d\sigma}{d\Omega}$ and express the result in terms of the scattering angle $\theta$ and the energy $E = \frac{\hbar^2 k^2}{2m}$ of the particle.