Graduate What are the quantum numbers used to label helium atom eigenfunctions?

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The discussion focuses on the quantum numbers used to label the eigenfunctions of the helium atom, particularly in the context of its non-perturbative structure. The base Hamiltonian yields quantum numbers that form the term symbol: L, S, J, and MJ. Due to the complexity of the three-body problem, analytical solutions are not available, but variational methods can provide accurate results. References to significant works, such as those by Drake and Yan, highlight high-precision calculations related to helium's eigenfunctions. Overall, understanding these quantum numbers is crucial for characterizing helium atom eigenfunctions effectively.
HomogenousCow
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Are there any results on the structure of the helium atom eigenfunctions? By this I'm referring to the non-perturbative structure of the eigenfunctions, AKA what are the quantum numbers that one would use to label the eigenfunctions?
 
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I am nit sure what you mean by "non-perturbative," as it is a 3-body problem, hence no analytical solutions.

Using the base Hamiltonian, the quantum numbers you get are those that make up the term symbol, L, S, J, and MJ.
 
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There are also variational methods. With suitably chosen basis functions you can get quite accurate results -- see for example chapter 3 in "Intermediate Quantum Mechanics" by Bethe and Jackiw.
 
HomogenousCow said:
Are there any results on the structure of the helium atom eigenfunctions? By this I'm referring to the non-perturbative structure of the eigenfunctions, AKA what are the quantum numbers that one would use to label the eigenfunctions?
  • Drake, G. W. F., & Van, Z. C., Variational eigenvalues for the S states of helium. Chemical Physics Letters 229 (1994), 486-490.
  • Yan, Z. C., & Drake, G. W. F., High precision calculation of fine structure splittings in helium and He-like ions. Physical review letters, 74 (1995), 4791.
 
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HomogenousCow said:
Are there any results on the structure of the helium atom eigenfunctions? By this I'm referring to the non-perturbative structure of the eigenfunctions, AKA what are the quantum numbers that one would use to label the eigenfunctions?
The following may be relevant: http://www.scholarpedia.org/article/Semiclassical_theory_of_helium_atom
 
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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