How to Find Energy Corrections for a Perturbed Hydrogen Atom?

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SUMMARY

The discussion focuses on finding first-order perturbation corrections to the energy levels of a perturbed hydrogen atom, specifically under the potential V(r) = α/r². The unperturbed hydrogen atom's radial equation is provided, and the challenge lies in determining the exact energy levels of the perturbed system. The participant suggests introducing a new parameter k to replace l in the energy levels, but notes the complication that k may not be an integer due to its dependence on α. References to Griffiths' Quantum Mechanics textbook and time-independent perturbation theory are made for further guidance.

PREREQUISITES
  • Understanding of quantum mechanics, particularly perturbation theory.
  • Familiarity with the radial equation of the hydrogen atom.
  • Knowledge of Griffiths' Quantum Mechanics textbook, specifically Chapter 6.
  • Basic concepts of spherical harmonics and their role in quantum systems.
NEXT STEPS
  • Study Griffiths' Quantum Mechanics Chapter 6 on first-order perturbation corrections.
  • Research time-independent perturbation theory for a deeper understanding.
  • Explore the implications of non-integer quantum numbers in quantum mechanics.
  • Review the mathematical derivation of energy levels in perturbed systems.
USEFUL FOR

Students and researchers in quantum mechanics, particularly those studying perturbation theory and its applications to atomic systems like the hydrogen atom.

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Homework Statement



A hydrogen atom is perturbed with the potential [tex]V(r) = \frac{\alpha}{r^{2}}[/tex] ([tex]\alpha[/tex] is small). Find first-order perturbation corrections to the energy levels and then exact levels of the perturbed system.


Homework Equations



The unperturbed hydrogen atom radial equation is:

[tex]-\frac{\hbar^{2}}{2m} \frac{d^{2}u}{dr^{2}} + [-\frac{e^{2}}{4\pi \epsilon_{0}} \frac{1}{r} + \frac{\hbar^{2}}{2m} \frac{l(l+1)}{r^{2}}]u = Eu[/tex]

where [tex]l[/tex] is an integer.


The Attempt at a Solution



I don't know how to find the exact energy levels of the perturbed system. Because the perturbation is proportional to [tex]\frac{1}{r^{2}}[/tex], in the radial equation for the perturbed atom I can introduce a new parameter [tex]k[/tex] such that:

[tex]\frac{\hbar^{2}}{2m} \frac{k(k+1)}{r^{2}} = \frac{\hbar^{2}}{2m} \frac{l(l+1)}{r^{2}} + \frac{\alpha}{r^{2}}[/tex].

Then new energy levels will be just energy levels of an unperturbed hydrogen atoms with [tex]k[/tex] in place of [tex]l[/tex]. But then, [tex]k[/tex] has to be an integer for the hydrogen solutions to make sense, and it is at the same time a function of the parameter [tex]\alpha[/tex], so it need not be an integer. What's wrong here? How to find the exact energy levels?
 
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It looks like your attempt at a solution is trying to find the exact levels. Take a look at Chapter 6 in Griffiths' QM book for finding the first-order perturbation corrections. You could probably also look up time-independent perturbation theory on the web and find a wikipedia page or something.

I'm not completely sure about finding the exact levels, but I think you have a good idea there. This perturbation won't affect the spherical harmonics at all since it is r-dependent. It seems like it might work to just replace [tex]n=j_{max}+l+1[/tex] with [tex]n=j_{max}+k+1[/tex] and plug the n into the energy formula, but I'm not so sure there because of the issue of k not having to be an integer.
 

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