Commutation Relation: Hi Parity Operator?

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The discussion focuses on the commutation relation between the translation operator and the parity operator. It is established that these two operators do not commute, as demonstrated through specific examples involving their actions on position eigenvectors. The translation operator shifts the position, while the parity operator reflects it, leading to different outcomes when applied in succession. The mathematical expressions provided illustrate the non-commutativity clearly. Overall, the relationship between the translation and parity operators highlights fundamental aspects of quantum mechanics.
fatema
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hi, do the translation operator commute with parity operator?
 
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Parity operator ##\hat\pi## is defined such that when acting on a position eigenvector ##|x\rangle## to be ##\hat\pi|x\rangle = |-x\rangle##. Start from
$$\hat x \hat\pi = \int dx' \ \hat x \hat\pi |x'\rangle \langle x'|$$
and with the help of the eigenvalue relation ##\hat x|x'\rangle = x'|x'\rangle##.
 
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It's enough to find a single example of a translation ##T\psi (x) = \psi (x+\Delta x)## and a function ##\psi (x)## for which ##TP\psi (x)## and ##PT\psi (x)## don't have the same value at some point ##x##.
 
hilbert2 said:
It's enough to find a single example of a translation ##T\psi (x) = \psi (x+\Delta x)## and a function ##\psi (x)## for which ##TP\psi (x)## and ##PT\psi (x)## don't have the same value at some point ##x##.
I was thinking since it's easy to show that the two operators do not commute, why not push it a little further to know the exact relation between ##TP## and ##PT##.
 
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fatema said:
hi, do the translation operator commute with parity operator?
On coordinate basis |x \rangle, the action of translation operator T_{a} = e^{- i a p} is given by T_{a} | x \rangle = | x + a \rangle \ . And in the same basis, the parity operator is given by \pi = \int dy \ |-y \rangle \langle y | \ . Now it is an easy exercise to show that T_{a} \ \pi = \int dy \ |y \rangle \langle - y + a | \ , \pi \ T_{a} = \int dy \ |y \rangle \langle - y - a |\ . So, in general they do not commute. This becomes clear if you use the above two equations to evaluate the action on the wave function \left( T_{a} \ \pi \Psi \right) ( - x) = \Psi (x + a) \ , \left( \pi \ T_{a} \Psi \right) ( - x) = \Psi ( x - a) \ .
 
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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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