Pointless in talking about atomic term for a certain micro-state?

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SUMMARY

This discussion centers on the understanding of atomic term symbols in multi-electron configurations, specifically addressing the relationship between micro-states and term symbols characterized by quantum numbers L and S. It is established that micro-states can belong to multiple term symbols, such as 3d2 containing both 1D and 3P terms. The Pauli exclusion principle guides the assignment of micro-states to term symbols, emphasizing that the focus should be on the term symbols for a given electron configuration rather than individual micro-states. The RS coupling scheme is utilized to derive the total angular momentum J from L and S.

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  • Understanding of quantum mechanics, specifically angular momentum and quantum numbers.
  • Familiarity with multi-electron configurations and their associated micro-states.
  • Knowledge of the Pauli exclusion principle and its implications in electron configurations.
  • Experience with the RS coupling scheme for calculating total angular momentum.
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  • Research the derivation of term symbols for various electron configurations in quantum chemistry.
  • Study the implications of the Pauli exclusion principle on electron arrangements in atoms.
  • Explore the RS coupling scheme in detail and its application in determining total angular momentum.
  • Examine case studies of multi-electron systems to understand the assignment of micro-states to term symbols.
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Chemists, physicists, and students studying quantum mechanics and atomic structure, particularly those focused on electron configurations and term symbols in multi-electron systems.

bearcharge
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I'm a chemist trying to understand atomic term symbol.

If we list all the micro-states of certain multi-electron configuration, these micro-states can be grouped into several certain terms characterized by L and S. In other words, when we compute the ML and MS for each of the micro-state, they should belong to certain (L, S) configuration, much analogous to the single electron case where l sets boundary for ml, s for ms. It is legitimate to do so because the operator L and S commute with H, so L and S are good quantum numbers describing the states. After deriving L and S, we use RS coupling scheme to calculate J.

If my understanding is correct, then this point should follow: certain micro-state can arbitrarily belong to several terms. For example, 3d2 contains terms 1D and 3P. A micro-state with ML=1, MS=0 can be either 1D or 3P, right? In that sense, it seems pointless talking about specific term of a micro-state, right?
 
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Usually, the point of listing microstates for equivalent electrons is to determine which term symbols are possible, such that the Pauli exclusion principle is obeyed. For that purpose, microstates are assigned to term symbols without regard to which term symbol they actually belong to. In your example, once you have identified that you have a 1D term and therefore need an ##M_L = 1, M_S=0## microstate, you "remove" one such microstate from the list only to see what other terms you can have.

I would venture to say that in many cases, if you have more than one microstate with a given pair of ##M_L, M_S## values, then these microstates will appear in linear combinations in the actual terms
 
Thanks for the answer! So can we say what is important is what are the term symbols for a given electron configuration, rather than what is the term symbol for a specific microstate?
 
bearcharge said:
Thanks for the answer! So can we say what is important is what are the term symbols for a given electron configuration, rather than what is the term symbol for a specific microstate?
Yes. As I said, except for the extreme cases (e.g., maximum ##M_L=L##), you can't say specifically which microstate will belong to which term symbol.
 
Thanks!
 

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