How Can Higher Order Relativistic Corrections Improve Hydrogen Atom Models?

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Discussion Overview

The discussion focuses on higher order relativistic corrections to hydrogen atom models, specifically exploring the implications of including corrections beyond the first order, such as the second order correction involving the p^6 term. Participants examine the perturbative techniques used to derive these corrections and the mathematical expressions involved.

Discussion Character

  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant notes that standard treatments of hydrogen atoms typically include corrections up to 1/c^2, represented by the perturbation term -P^4/8*m^3*c^2, and discusses the method of evaluating p^4.
  • Another participant suggests that the same technique can be applied to evaluate the new term \langle n,\ell|\frac{1}{r^3}|n,\ell\rangle for the second order correction.
  • A further inquiry is made about the treatment of the p^6 term in the perturbative expansion.
  • One participant provides a detailed expression for the p^6 term, rewriting it in terms of the Hamiltonian H_0 and expanding it to show how it relates to the eigenvalue for H_0.
  • A participant expresses gratitude for the clarification provided regarding the calculations.

Areas of Agreement / Disagreement

Participants appear to agree on the applicability of perturbative techniques to higher order corrections, but the discussion does not resolve any potential disagreements regarding the specific mathematical steps or interpretations involved.

Contextual Notes

The discussion does not clarify any assumptions regarding the validity of the perturbative approach at higher orders or the specific conditions under which these corrections are applicable.

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For hydrogen atoms, all book take correction up to 1/c^2 where the perturbation is -P^4/8*m^3*c^2. And they go solving it by sandwiching p^4 term where they consider p^2 = 2m*(1+e^2/r). and they square it to solve for p^4.

To get a better view of perturbation to first order please see attachment.


What if I want it to the second order correction, that is to p^6? The additional perturbative term would be p^6/16*m^5*c^4. What should be done in this case?
 

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I think you can use the same technique. The only new term you need to evaluate is [itex]\langle n,\ell|\frac{1}{r^3}|n,\ell\rangle[/itex].
 
And what to do with P^6?
 
It's the same technique, you can write:
$$
\frac{p^6}{16m^5c^4}=\frac{1}{2m^2c^4}\left(\frac{p^2}{2m}\right)^3= \frac{1}{2m^2c^4}\left(\frac{p^2}{2m}-\frac{e^2}{r}+\frac{e^2}{r}\right)^3.
$$
You now realize that [itex]\frac{p^2}{2m}-\frac{e^2}{r}=H_0[/itex] and so:
$$
\frac{p^6}{16m^5c^4}=\frac{1}{2m^2c^4}\left(H_0^3+\frac{e^6}{r^3}+3H_0^2\frac{e^2}{r}+3H_0\frac{e^4}{r^2}\right),
$$
and the you exactly what is the eigenvalue for [itex]H_0[/itex].
 
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Ohhhh thank you very much!
 

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