Dixanadu
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Hey guys,
So this question is sort of a fundamental one but I'm a bit confused for some reason. Basically, say I have a Hermitian operator \hat{A}. If I have a system that is prepared in an eigenstate of \hat{A}, that basically means that \hat{A}\psi = \lambda \psi, where \lambda is real, right? So can I say the following, because the system is prepared in an eigenstate of \hat{A}
∫\psi^{*}\psi=1?
The reason I'm asking is because \psi is just a function of x - in literature the normalization is always written in terms of the big psi (\Psi), which is a function of x,t.
Also, while I am at it - by saying that it is prepared in an eigenstate of \hat{A} does that also mean that the probability of measuring this state is equal to 1? so that the wavefunction is collapsed to this eigenstate?
So this question is sort of a fundamental one but I'm a bit confused for some reason. Basically, say I have a Hermitian operator \hat{A}. If I have a system that is prepared in an eigenstate of \hat{A}, that basically means that \hat{A}\psi = \lambda \psi, where \lambda is real, right? So can I say the following, because the system is prepared in an eigenstate of \hat{A}
∫\psi^{*}\psi=1?
The reason I'm asking is because \psi is just a function of x - in literature the normalization is always written in terms of the big psi (\Psi), which is a function of x,t.
Also, while I am at it - by saying that it is prepared in an eigenstate of \hat{A} does that also mean that the probability of measuring this state is equal to 1? so that the wavefunction is collapsed to this eigenstate?