LS coupling for identical electrons

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SUMMARY

The discussion focuses on the LS coupling for identical electrons, specifically analyzing the 3p2 electron configuration. It highlights the implications of the Pauli Exclusion Principle, which prohibits certain combinations of magnetic quantum numbers (ml and ms) for identical electrons. The allowed terms derived from this analysis are 1S, 1D, and 3P, with the discussion questioning the exclusion of the 1P term despite having valid quantum numbers. The reasoning behind the selection of terms is rooted in the requirements for total angular momentum (L) and spin multiplicity (S).

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly the Pauli Exclusion Principle.
  • Familiarity with angular momentum quantum numbers (ml and ms).
  • Knowledge of term symbols and their significance in atomic physics.
  • Basic grasp of LS coupling and its application in electron configurations.
NEXT STEPS
  • Study the derivation of term symbols in atomic physics.
  • Explore the implications of the Pauli Exclusion Principle in multi-electron systems.
  • Research the differences between LS coupling and jj coupling in quantum mechanics.
  • Examine specific examples of electron configurations and their corresponding term symbols.
USEFUL FOR

Students and professionals in physics, particularly those specializing in quantum mechanics, atomic physics, and spectroscopy. This discussion is beneficial for anyone looking to deepen their understanding of electron configurations and term symbols in multi-electron atoms.

mk_gm1
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Let's say I'm considering the 3p^2 electrons. From the Pauli Exclusion Principle, we know that two electrons cannot have the same state, which in this case means ml and ms cannot both be the same for each electron.

What this means is that the following 6 terms must not be allowed:

m_{l1} \hspace{0.1 in} m_{l2} \hspace{0.1 in} m_{s1} \hspace{0.1 in} m_{s2}

-1 \hspace{0.1 in} -1 \hspace{0.1 in} \downarrow \hspace{0.3 in} \downarrow
-1 \hspace{0.1 in} -1 \hspace{0.1 in} \uparrow \hspace{0.3 in} \uparrow
0 \hspace{0.4 in} 0 \hspace{0.3 in} \downarrow \hspace{0.3 in} \downarrow
0 \hspace{0.4 in} 0 \hspace{0.3 in} \uparrow \hspace{0.3 in} \uparrow
+1 \hspace{0.1 in} +1 \hspace{0.1 in} \downarrow \hspace{0.3 in} \downarrow
+1 \hspace{0.1 in} +1 \hspace{0.1 in} \uparrow \hspace{0.3 in} \uparrow

These correspond to M_L=\sum m_{li}<br /> = -2, -2, 0, 0, 2, 2 and M_S = \sum m_{si} = -1, 1, -1, 1, -1, 1 respectively.

My question is this - how does this lead to the conclusion that the allowed terms are 1S, 1D and 3P ? For example, there's a ML = 0, MS= -1 term in both 3S and 3P - why do we disallow one and not the other?

Also, what leads us to disallow 1P (for which ML=-1, 0, 1 and MS=0)? Surely the only way to have MS = 0 is to have \downarrow_1 \hspace{0.1 in} \uparrow_2 or vice versa, and hence m_{s1} \neq m_{s2} and we have no violation of the Pauli Exclusion Principle?
 
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What do you mean by ''why do we disallow one and not the other?''
 
Ok let me try and clarify what I'm confused by. Have a look at the following table which I have taken from my notes:

UZYKl.png


In this table we are looking at part of the identical (np)2 configuration. There are 15 possible configurations, all of which I haven't posted.

Take a look at the 2nd row. I can see why this state corresponds to the 3P term. For it to be a P term, it must have L = 1 where L \geq |M_L|. It clearly has this. For it to be a 3P term, the multiplicity 2S+1=3 i.e. S=1 where S \geq | M_S |. This is obvious.

Now if you look at the 4th row, I am not sure why it also has to be a 3P state . I understand that it can be (i.e. that the 3P term includes this state), but this could equally well be a 1P state, no? This is because here S=0. Therefore why do we choose one and not the other?
 

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