I'm currently reading the following set of lecture notes on quantum chemistry, which includes the so-called "expansion postulate" as a fundamental postulate of quantum mechanics: "The eigenfunctions of a linear and hermitian operator form a complete basis set."
How is this a postulate of quantum mechanics, rather than a provable mathematical property of linear hermitian operators? Isn't the expansion postulate just a consequence of the spectral theorem for an infinite-dimensional Hilbert Space?
If the eigenfunctions of a linear, hermitian operator forming an orthogonal basis is not a mathematically provable fact about wavefunctions, wouldn't that necessarily imply that there exist hermitian, linear operators on wavefunctions whose eigenfunctions do not form an orthogonal basis?