Commutation Relation: Hi Parity Operator?

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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 [itex]|x \rangle[/itex], the action of translation operator [itex]T_{a} = e^{- i a p}[/itex] is given by [tex]T_{a} | x \rangle = | x + a \rangle \ .[/tex] And in the same basis, the parity operator is given by [tex]\pi = \int dy \ |-y \rangle \langle y | \ .[/tex] Now it is an easy exercise to show that [tex]T_{a} \ \pi = \int dy \ |y \rangle \langle - y + a | \ ,[/tex] [tex]\pi \ T_{a} = \int dy \ |y \rangle \langle - y - a |\ .[/tex] 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 [tex]\left( T_{a} \ \pi \Psi \right) ( - x) = \Psi (x + a) \ ,[/tex] [tex]\left( \pi \ T_{a} \Psi \right) ( - x) = \Psi ( x - a) \ .[/tex]
 
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