Riley hobson bence · Problem 4.36

Series and limits

Mathematics — Methods · lhopitals-rule-scattering-amplitude

Problem

In quantum theory, a certain method (the Born approximation) gives the (so-called) amplitude f(θ)f(\theta) for the scattering of a particle of mass mm through an angle θ\theta by a uniform potential well of depth V0V_0 and radius bb (i.e. the potential energy of the particle is −V0-V_0 within a sphere of radius bb and zero elsewhere) as f(θ)=2mV0ℏ2K3(sin⁡Kb−Kbcos⁡Kb).f(\theta) = \frac{2mV_0}{\hbar^2 K^3}(\sin Kb - Kb\cos Kb). Here ℏ\hbar is the Planck constant divided by 2π2\pi, the energy of the particle is ℏ2k2/(2m)\hbar^2 k^2/(2m) and KK is 2ksin⁡(θ/2)2k\sin(\theta/2). Use l'H\^{o}pital's rule to evaluate the amplitude at low energies, i.e. when kk and hence KK tend to zero, and so determine the low-energy total cross-section. [Note: the differential cross-section is given by ∣f(θ)∣2|f(\theta)|^2 and the total cross-section by the integral of this over all solid angles, i.e. 2π∫0π∣f(θ)∣2sin⁡θ dθ2\pi \int_0^\pi |f(\theta)|^2 \sin\theta\, d\theta.]

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