Expectation formula in Dirac notation.

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[tex]\langle \hat{A} \rangle = \langle x|\hat{A}|x \rangle = \int \psi_{x}^{"*"} \hat{A} \psi_{x} \,d \tau[/tex]

This is the expectation value postulate of quantum mechanics.

If the wavefunction [tex]\psi_{x}[/tex] is not an eigenfunction of the operator [tex]\hat{A}[/tex] then the measured value of the observable [tex]A[/tex] is variable. When [tex]\psi_{x}[/tex] is normalized such that
[tex]\int \psi_{x}^{"*"}\psi_{x} \,d \tau=1[/tex]
the expectation value above yeilds the average measurement of all possible measurements of [tex]A[/tex]. (Note that [tex]d \tau[/tex] indicates an integration over all space.) This works because, since [tex]\hat{A}[/tex] is an Hermitian operator, its eigenvectors form an orthonormal basis. It follows that any function can be written as an infinite linear combination of eigenfunctions of [tex]\hat{A}[/tex].
 
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