spaghetti3451
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I know that <Aψ|Aψ> = <A2>. Can anyone tell please tell me how you get one line to the another?
The discussion clarifies the relationship between the Hermitian property of an operator A and the expression \langle A^2 \rangle in quantum mechanics. It establishes that for a self-adjoint (Hermitian) operator A, the equality \langle Aψ|Aψ\rangle = \langle ψ|A^{\dagger}A|ψ\rangle holds true, leading to \langle ψ|A^{2}|ψ\rangle. This derivation is crucial for understanding quantum expectation values and the implications of Hermitian operators in quantum mechanics.
PREREQUISITESQuantum physicists, students of quantum mechanics, and anyone interested in the mathematical foundations of quantum theory will benefit from this discussion.
failexam said:Ok so, <Aψ|Aψ> = <AAψ|ψ> because A is self adjoint (hermitian). What next?