Degenerate pertubation theory when the first order fails

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SUMMARY

The discussion focuses on the application of degenerate perturbation theory, specifically addressing scenarios where the first-order perturbation does not break degeneracy. It is established that when perturbation matrix elements are zero in the degenerate subspace, diagonalization of the Hamiltonian provides an exact solution to all orders. To achieve nonzero results, additional states must be included beyond the degenerate subspace, as illustrated by the example of atomic hydrogen's n=2 level interacting with a static electric field.

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  • Understanding of degenerate perturbation theory
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The basic algorithm of degenerate perturbation theory is quite simple:
1.Write the perturbed Hamiltonian as a matrix in the degenerate subspace.
2.Diagonalize it.
3.The eigenstates are the 'correct' states to which the system will go as the perturbation ->0.

But what to do if the first order does not break the degeneracy?
For instance, if the perturbation matrix elements are all 0 in the degenerate subspace.

It seems unlikely to me that there is nothing else to be done in that case...
 
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Actually when you diagonalize you solve the problem EXACTLY to all orders(in the framework of the set of states you use). It's when you have both degenerate and nondegenerate that order makes sense. To your question, if in the degerenate subspace the perturbation is 0, then to get a nonzero result you need more states.
Example: Take a static electric field (z-axis) and the n=2 level of atomic hydrogen.
210 and 200 get mixed, but 211 and 21-1 are not affected. So to affect them, you need to
include more states, e.g. n=3, when they an mix with 321 and 32-1 for example.
This is not degenerate anymore, of course
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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