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

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Discussion Overview

The discussion revolves around the concept of atomic term symbols in the context of multi-electron configurations and their associated micro-states. Participants explore the relationship between micro-states characterized by quantum numbers L and S, and the implications for identifying term symbols in atomic systems.

Discussion Character

  • Conceptual clarification
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant suggests that micro-states can belong to multiple term symbols, exemplifying this with the 3d2 configuration, which can correspond to both 1D and 3P terms.
  • Another participant emphasizes the importance of identifying possible term symbols for equivalent electrons while adhering to the Pauli exclusion principle, indicating that micro-states are assigned to term symbols without strict adherence to specific associations.
  • A later reply confirms that the focus should be on the term symbols for a given electron configuration rather than for individual micro-states, noting that in most cases, specific micro-states cannot be definitively assigned to term symbols.

Areas of Agreement / Disagreement

Participants generally agree that the term symbols for a given electron configuration are more significant than those for specific micro-states. However, there remains some uncertainty regarding the assignment of micro-states to term symbols, particularly in non-extreme cases.

Contextual Notes

Participants acknowledge that the assignment of micro-states to term symbols is influenced by the Pauli exclusion principle and the nature of linear combinations of micro-states within terms, but do not resolve the implications of these factors fully.

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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