Hund's cases for diatomic molecules

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SUMMARY

This discussion focuses on Hund's cases for diatomic molecules, specifically how to determine which case (a), (b), or (c) applies based on the strength of spin-orbit coupling relative to other interactions. The term symbol for molecular electronic states, represented as (2s+1)ΛΩ, is derived from the electronic configuration, with Hund's case C affecting the notation used. The evaluation of spin-orbit interaction terms A and B is discussed, emphasizing the importance of the coupling constant A in determining multiplet splitting. References to Landau and Lifshitz's work provide additional context for understanding these concepts.

PREREQUISITES
  • Understanding of Hund's coupling cases in quantum mechanics
  • Familiarity with molecular electronic states and term symbols
  • Knowledge of spin-orbit coupling and its effects
  • Basic principles of quantum mechanics, particularly in relation to diatomic molecules
NEXT STEPS
  • Study the differences between Hund's cases A, B, and C in detail
  • Learn how to derive molecular term symbols from electronic configurations
  • Research the implications of spin-orbit coupling on molecular spectra
  • Examine Landau and Lifshitz's discussions on Hund's coupling cases for deeper insights
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Physicists, chemists, and students specializing in quantum mechanics, particularly those focusing on molecular spectroscopy and diatomic molecules.

samst
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Dear All,

May anyone please advise me to the following questions in case of diatomic molecules:

1. How do we choose which Hund's case ((a), (b), or (c)...) that best describes a particular diatomic molecule?

2. How can we deduce from Hund's cases molecular electronic states (2s+1)ΛΩ (e,g. Σ+/-, Π, Δ, Φ, Γ...)?

3. When Λ-type doubling for non-sigma states should be taken into consideration?

4. How do we obtain the spin-orbit interaction terms A and B (where Y=A/B)?

Any help would be greatly appreciated...
Best wishes
 
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samst said:
1. How do we choose which Hund's case ((a), (b), or (c)...) that best describes a particular diatomic molecule?
It depends on the strength of the spin-orbit coupling in comparison to other couplings, such as the residual electron-electron interaction. As far as I know, it can be difficult to predict in advance which coupling case is the right one, and it is the actual spectrum that will give the answer (like LS vs jj coupling in atoms).

samst said:
2. How can we deduce from Hund's cases molecular electronic states (2s+1)ΛΩ (e,g. Σ+/-, Π, Δ, Φ, Γ...)?
The term symbol is obtained from the electronic configuration. The Hund cases will affect how the term symbol can be written. For instance, in Hund's case C, Λ is not defined, so one uses Ω instead.

samst said:
3. When Λ-type doubling for non-sigma states should be taken into consideration?
I don't know. Someone more knowledgeable may chime in.

samst said:
4. How do we obtain the spin-orbit interaction terms A and B (where Y=A/B)?
I don't know what this means. Can you explain the notation?
 
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DrClaude said:
It depends on the strength of the spin-orbit coupling in comparison to other couplings, such as the residual electron-electron interaction. As far as I know, it can be difficult to predict in advance which coupling case is the right one, and it is the actual spectrum that will give the answer (like LS vs jj coupling in atoms).

Is there a way we can predict whether L and S are good quantum numbers to choose case (a), for example?

DrClaude said:
The term symbol is obtained from the electronic configuration. The Hund cases will affect how the term symbol can be written. For instance, in Hund's case C, Λ is not defined, so one uses Ω instead.

DrClaude said:
I don't know. Someone more knowledgeable may chime in.

DrClaude said:
I don't know what this means. Can you explain the notation?

The electronic energy of a multiplet term is given to a first approximation by: Te = To + AΛΣ.
where To is the term value when the spin is neglected (spin-free) and A is a constant for a given multiplet term (for spin-orbit). The coupling constant A determines the magnitude of the multiplet splitting. If A>0 , the spin-orbit terms are considered as regular states (2Π1/2, 2Π3/2). For A<0, we have an inverted terms (2Π3/2, 2Π1/2).
How do we evaluate or find A and B terms? I am searching for a relation for A and B, but I am not finding any!
 
Landau, Lifshitz, vol 3, Quantum Mechanics, contains a nice discussion of the Hund's coupling cases.
 
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DrDu said:
Landau, Lifshitz, vol 3, Quantum Mechanics, contains a nice discussion of the Hund's coupling cases.

Thank you so much DrDu!
 
Thank you DrClaude for your help and continuous support...
 

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