Simple question concerning Hermitian operators

[Nikitin]

Hi. This might sound like a stupid question, but is it, in general, true that $(\hat{H} \psi)^* \psi'= \psi^* \hat{H}^*\psi'$? Here $\hat{H}$ is a hermitian operator and $\psi$ a wave function.

I.e. do they switch places even when not inside an inner product? I am aware of the fact that you can move hermitian operators around inside an inner product, i.e. <H X| Y> = <X | H Y>, but I am unsure as to why you can do that. Can somebody link me to some proofs that explain all this?

thanks.

edit: fixed mistake in my question..

 

[Orodruin]

<H X| Y> = <X | H Y>

This is the definition of a self-adjoint operator so naturally a self-adjoint operator is going to fulfil it.

With regards to your original question, if you see the wave function simply as a function here you may be in trouble. Consider instead $\langle \psi| H$ as a linear map from the state space to complex numbers.

Writing down the inner product in position representation, you will get that the linear maps defined by multiplication with $(H\psi)^*$ and acting with $\psi^* H^*$ on any wave function before integration will give the same result (by definition of the adjoint, that H is self-adjoint gives $H^* = H$.

 

[Nikitin]

arghh I forgot to put a function to the right of the expression I was asking about, sorry about that. It's fixed now. Anyway:

what is position representation? I'm not sure if I follow your explanation..