Partial wave scattering cross section in spherical well

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SUMMARY

The discussion focuses on calculating the l = 0 partial wave scattering cross section for a spherical well potential defined by V(r PREREQUISITES

  • Understanding of quantum mechanics, specifically wave functions and scattering theory.
  • Familiarity with spherical potentials and their mathematical representations.
  • Knowledge of phase shifts in quantum scattering processes.
  • Ability to solve differential equations, particularly the radial wave equation.
NEXT STEPS
  • Study the derivation of phase shifts in quantum scattering, focusing on low-energy limits.
  • Learn about the radial wave equation solutions in spherical coordinates.
  • Explore the implications of continuity and differentiability in quantum mechanics.
  • Investigate the role of partial wave analysis in scattering theory.
USEFUL FOR

Students and researchers in quantum mechanics, particularly those focusing on scattering theory and potential wells, will benefit from this discussion.

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Homework Statement



Consider the spherical well such that V(r<a) = -V0 and V(r≥a) = 0. Calculate the l = 0 partial wave scattering cross section in the low energy limit for this potential.

Homework Equations



σ = \frac{4 \pi}{k^2} * \Sigma (2l+1)*sin^2(\delta_l)

The Attempt at a Solution



For l=0, the above equation just becomes

σ = \frac{4 \pi}{k^2} *sin^2(\delta_0).

But how do I get the phase shift \delta_0?
 
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you have to solve the radial part of the wave eqn with l=0.One solution with -V0 potential will be ASinkr type,while outside r=a it will contain the phase shift δ0 type term added.use continuity and differentiability to find δ0 from the wave function determined, at r=a.
 

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