teaJ
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I know that (A\mp )\mp =A . Where A is an Hermitian operator How does one go about proving this through the standard integral to find Hermitian adjoint operators?
I should mention, I don't want anyone to just flat out show me step by step how to do it. I'd just like a solid starting place.
\int (A\mp \psi*) \varphi dx = \int (\psi*)A\varphi dx
I should mention, I don't want anyone to just flat out show me step by step how to do it. I'd just like a solid starting place.
\int (A\mp \psi*) \varphi dx = \int (\psi*)A\varphi dx
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