youngurlee
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The general evolution of a ket |\psi\rangle is according to
-i\hbar\frac{d}{dt}|\psi\rangle=H|\psi\rangle
without specifying a representation.
From this equation, how can you simply get a equation in a certain representation F as below:
-i\hbar\frac{\partial}{\partial t}\langle f|\psi\rangle=\langle f|H|\psi\rangle ?
doesn't it need the validity of
\langle f|\frac{d}{dt}|\psi\rangle=\frac{∂}{∂t}\langle f|\psi\rangle
?
does this always hold for any ket and bra in a Hilbert space and its dual space?
-i\hbar\frac{d}{dt}|\psi\rangle=H|\psi\rangle
without specifying a representation.
From this equation, how can you simply get a equation in a certain representation F as below:
-i\hbar\frac{\partial}{\partial t}\langle f|\psi\rangle=\langle f|H|\psi\rangle ?
doesn't it need the validity of
\langle f|\frac{d}{dt}|\psi\rangle=\frac{∂}{∂t}\langle f|\psi\rangle
?
does this always hold for any ket and bra in a Hilbert space and its dual space?