A Hermitian operator satisfies on its operator domain. Here
Two integration by parts operations, together with the boundary conditions in the Hamiltonian domain, show that the kinetic term is Hermitian; multiplication by the real function is Hermitian as well. Thus is Hermitian.
For a time-independent operator , the Schrodinger equation and its adjoint give the Ehrenfest theorem
Using the canonical commutation relation ,
Consequently

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