Partition Function, Grand Potential

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The discussion centers on a potential error in the final expression for the grand potential, specifically regarding the factor of (2S+1). Participants suggest that this factor should be squared, indicating it appears twice in the equation. The argument is made that while (2S+1) states exist for each k value, it should either be included in front of the integral or within g(E), but not both. This clarification aims to resolve confusion about the correct application of the factor in the context of the partition function. The conversation emphasizes the importance of accurate representation in equations to avoid misinterpretation.
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It seems like they have missed out a factor of ##(2S+1)## in the final expression for grand potential? I'm thinking it should be ##(2S+1)^2## instead.

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I don't know, didn't they write the (2S+1) factor twice? There are 2S+1 states for each value of k, so in Eq.(30.3) you can put this factor in front of the integral, or include it in g(E), but you should not do both!
 
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Bill_K said:
I don't know, didn't they write the (2S+1) factor twice? There are 2S+1 states for each value of k, so in Eq.(30.3) you can put this factor in front of the integral, or include it in g(E), but you should not do both!

Good point. Thanks alot
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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