First excited state of Helium. Triplets and Singlet

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SUMMARY

The discussion focuses on the first excited state of helium and the classification of electron spin states into singlet and triplet configurations. The user presents various antisymmetric states generated using Slater's determinant, specifically states |u2> and |u4>, and inquires about their classification. The response clarifies that the correct classification requires forming linear combinations of these states to identify the triplet state |1,0⟩ and the singlet state |0,0⟩. Additionally, it explains that the energy differences between singlet and triplet states arise from electron-electron repulsion, which is not accounted for in the initial Hamiltonian.

PREREQUISITES
  • Understanding of Slater's determinant for generating antisymmetric states
  • Familiarity with quantum mechanics concepts such as spin states and coupling
  • Knowledge of helium's electronic structure and excited states
  • Basic principles of perturbation theory in quantum mechanics
NEXT STEPS
  • Study the formation of linear combinations of quantum states in quantum mechanics
  • Learn about the implications of electron-electron repulsion in multi-electron systems
  • Explore the concept of spin states in quantum mechanics, focusing on singlet and triplet states
  • Investigate perturbation theory and its application to quantum systems, particularly in helium
USEFUL FOR

Quantum physicists, students studying quantum mechanics, and researchers focusing on atomic structure and electron interactions will benefit from this discussion.

JamesHG
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My question is the following one:

If i have the first excited state of helium, the possibilities for the two electrons are : 1s+,2s+ , 1s+2s-, 1s-,2s- and 1s-,2s+ , where + and - denotes spin up and down. If I use the slater's determinant to generate antisymmetric states, I get :

$$|u1> = \frac{1}{\sqrt{2}}[|1s,2s> - |2s,1s>]\otimes|1,1>$$
$$|u2> = \frac{1}{\sqrt{2}}[|1s+,2s-> - |2s-,1s+>]$$
$$|u3> = \frac{1}{\sqrt{2}}[|1s,2s> - |2s,1s>]\otimes|1,-1>$$
$$|u4> = \frac{1}{\sqrt{2}}[|1s-,2s+> - |2s+,1s->]$$

how i should i know which state (|u2> or |u4>) belows to singlet or triplet state if they can't be separed as tensorial product?

And why the energy from singlet and triplets are different?

Note : The |1,1> ... etc kets are referred to the coupled basis.

Thanks.
 
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The eigenstates of He have a (approximately) definite spin, therefore its eigenstates must be a product between the spatial function and the spin function. Your first and third states already satisfy this requirement, but the rest do not. If you write those improper states correctly you should get one with spin function ##|1,0\rangle## which is a triplet and the other one with spin function ##|0,0\rangle## which is the only singlet. Hint: try forming linear combinations of ##u_2## and ##u_4##.
JamesHG said:
And why the energy from singlet and triplets are different?
The states you write there result from a Hamiltonian ignoring electron-electron repulsion. You can see how the incorporation of this Coulomb term affect the energies by treating it as a perturbation. You should see that the excited singlet states lie higher than the corresponding triplet state.
 
Thank you so much for answering my question!
 

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