Dynamics in the heizenberg picture

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The discussion centers on the time-derivative of an operator A(t) in the Heisenberg picture, specifically the equation \(\frac{dA(t)}{dt} = \frac{i}{\hbar} [H,A(t)] + U^\dagger(\frac{da(t)}{dt})U\). The user seeks clarification on the conditions under which this equation holds, particularly when the Hamiltonian is time-dependent, as illustrated by the example \(H = a^\dagger e^{-i\omega t} + a e^{i\omega t}\). It is established that even with a time-dependent Hamiltonian, the equation can still be valid under certain circumstances.

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dudy
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Hello,
The time-derivative of an operator A(t) = U^\dagger a(t)U in the heizenberg picture is given by:

\frac{dA(t)}{dt} = \frac{i}{\hbar} [H,A(t)] + U^\dagger(\frac{da(t)}{dt})U

Now, I know that under some conditions, we can write:

\frac{dA(t)}{dt} = \frac{i}{\hbar} U^\dagger[H,a(t)]U + U^\dagger(\frac{da(t)}{dt})U

My question is- what are those conditions?

thanks
 
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Under the condition that the Hamiltonian is not dependent on time.
 
is there a more specific rule?
take for example:

H = a^\dagger e^{-i\omega t} + a e^{i\omega t}

(here a is the annihilation operator).

This Hamiltonian is of course time-dependent,
but, non-the-less, it is also true that:

\frac{dA(t)}{dt} = \frac{i}{\hbar} U^\dagger[H,a]U

(where A(t) is the annihilation operator in heizenberg's picture)
 

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