Ahermitian operator a is defined as one for which f av,)dx s(aa)dax, where o and , are any two wavefunctions, and ]* stands for a complex conjugate of [.. ] in which i a) show that the position operator e oo b v-1 is replaced by -i. x is hermitian. hint: since x is a real x, and multiplication by x is commutative so v -x = x- v number b) show that the momentum operator pa is hermitian. hint: use the formula for integration by parts udv dv (dv/dar)da, single particle must have a normalizable wavefunction, which requires that (o0)(o0) = 0. and ihv - /vdu, with u = as well as the fact that any wavefunction corresponding to uv а