Permutation Operator: Understanding & Application

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I can't really imagine how this was approached.

Let P_{\alpha0} fixed

P_{a0}A=\frac{1}{N!}\sum_{\alpha}\epsilon_{\alpha}P_{\alpha0}P_{\alpha}=\frac{1}{N!}\epsilon_{\alpha0}\sum_{\alpha}\epsilon_{\beta}P_{\beta}=\epsilon_{\alpha0}A<br /> <br />


I can understand that P_{\alpha0}P_{\alpha} = P_{\beta} is a new permutation operator.

P_{a0}A=\frac{1}{N!}\sum_{\alpha}\epsilon_{\alpha}P_{\alpha0}P_{\alpha}=\frac{1}{N!}\sum_{\alpha}\epsilon_{\alpha}P_{\beta}
 
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can you tell me where you got this from or what is this about?

what i think happened was that

Ea = EB x Ea0 (sorry i don't know how to put in the greek words and the subscripts here)

so since Ea0 is a constant it was brought out of the equation, then the summation divided by the N! was equal to A... and hence we get the answer
 
Actually, P is the permutation operator that we frequently come across from a chapter of identical particles of any quantum textbook.
 
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