- #36
fanieh
- 274
- 12
PeterDonis said:I don't think so, because the Hermitian operator itself just picks the basis; it doesn't pick which of the basis elements determines the result of the measurement. The result of the measurement is a random choice among the possible values, with the probability of each value being equal to the squared modulus of the complex amplitude associated with the corresponding basis element.
I would also observe that your suggested language here has nothing whatever to do with wave functions, which I thought was what you were trying to use as your "newbie" version of QM.
I don't know. I'm not sure this is even doable, or worth doing. To me, trying to teach QM without using basis or vectors is like trying to teach arithmetic without using addition.
A key advantage of the state vector formalism in QM is that it avoids having to commit to any specific choice of basis or representation of states; you're just using the underlying Hilbert space structure that is there no matter what basis or representation you choose. That makes it much more general and much more useful than the wave function formalism, which commits you to a specific choice of basis (in wave function language, this would be the variable or variables that the wave function is a function of, like ##x## in the position representation) and a specific representation.
Why, wave function language without committing to any choice of basis and without any specific representation doesn't make sense? but the schroedinger equation can still be written without any basis.. is it not.