(a) The Born approximation gives
where qh is the magnitude of the momentum transfer and q = 2k sin \(\frac\theta 2\). For q → 0,
replacing V by \(\bar V\), some average value of the potential in the effective force range R. For a small momentum transfer q0, we have
Note that |f(q0)l2 is the measured value of \(\frac{d\sigma}{s\Omega}|_{q_0}\) for some small q0, |f(0)l2 is the value of \(\frac{d\sigma}{s\Omega}\) for a set of small q0 extrapolated to q = 0. From these values the effective range of the potential can be estimated.
(b) In view of the behavior of the scattering cross section for large q, we can say that the Born integral consists mainly of contributions from the region qr ≤ π, outside which, on account of the oscillation between the limits \(\pm1\) of the sine function, the contributions of the integrand are nearly zero. Thus we need only consider the integral from qr = 0 to π. Assuming V(r) \(\sim\) rn for small T, where n is to be determined, we have
A comparison with the given data gives \(\frac N2\) = 3 + n. Hence \(\bar V\) behaves like \(r^{(\frac N2 - 3)}\).