Dua E Kamil Pdf 57

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Accuracy of quasiclassical final state

Consider the scattering process of a light particle by a Coulomb potential $V(r)=1/r$. It is well known that the dominant contribution to the cross section comes from the quasi-classical Rutherford trajectory, with a semi-classical phase of $\exp[i\,\tau(E)]$ where $\tau(E)$ is the classical action. This can be seen from the WKB approximation for the scattering amplitude. (cf. Is there a finite asymptotic limit for the inverse scattering problem on the circle?, Phys. Lett. B 772 (2017) 180722) The semi-classical phase is obtained by asymptotic expansion in the WKB approximation of the (semiclassical) propagator. The amplitude is also evaluated by directly using the quasiclassical method. In the semiclassical regime the exact result is obtained with the Balian-Bloch formula, with a unique pole at $t=0$. However, the exact result has a finite and non-zero residue at that pole. By contrast, the quasiclassical formula vanishes at that pole.
Why does the Balian-Bloch formula vanish at the pole of the exact result, while the exact result remains non-zero?

A:

The quasiclassical approximation is only valid for scattering (
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