Muonic hydrogen, change in potential of the muon.

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SUMMARY

The discussion focuses on calculating the change in potential experienced by a muon in muonic hydrogen when considering a proton as a uniformly charged sphere rather than a point charge. The key conclusion is that while the potential outside the proton remains unchanged, the potential inside differs, necessitating the use of first-order perturbation theory to account for this difference. The muon's wave function has a non-zero probability at the origin, allowing for a finite probability of being found inside the proton, which influences the ground-state energy shift.

PREREQUISITES
  • Understanding of first-order perturbation theory in quantum mechanics
  • Familiarity with the concept of electric potential and electric fields
  • Knowledge of Gaussian law and its application to charged spheres
  • Basic principles of quantum mechanics, particularly wave functions
NEXT STEPS
  • Study the application of first-order perturbation theory in quantum mechanics
  • Learn about the differences in electric potential between point charges and uniformly charged spheres
  • Explore the implications of wave functions in quantum systems, particularly in relation to particle localization
  • Investigate the properties of muonic hydrogen and its significance in particle physics
USEFUL FOR

This discussion is beneficial for physics students, particularly those studying quantum mechanics and particle physics, as well as researchers interested in the properties of muonic hydrogen and perturbation theory applications.

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Homework Statement



Taking the proton to be a uniformly charged sphere of radius 1 fm, find an
expression for the change in potential experienced by the muon as compared with that
in the case of a point-like proton. Use first order perturbation theory to calculate the
ground-state energy shift in muonic hydrogen



Homework Equations



E=-grad(V)

The Attempt at a Solution



The electric field due to a uniformly charged sphere is exactly the same as the field due to a point charge of the region outside the sphere (by a simple application of gauss's law). For this reason I see no need for the potential to change. What am I missing?
 
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What you say is true - the potential outside of the proton is unchanged. However, the potential inside the proton is different in the two cases. Since the wave function at the origin is non-zero, there is some finite probability for the muon to be found inside the proton. So you can take the standard 1S solution as the unperturbed state, and apply a perturbation which is a difference between the potential of a point charge and the potential of a sphere. The perturbation is only non-zero inside the proton.
 
Thanks. That makes sense.
 

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