Is the Force Operator in Quantum Mechanics Always Time-Independent?

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Niles
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Homework Statement


Hi

In QM we define the force operator F as (in the Heisenberg picture)
[tex] F = \frac{1}{i\hbar}[p, H] + (d_t F)(t)[/tex]
What I can't understand is that usually (actually, always) we write
[tex] F = \frac{1}{i\hbar}[p, H][/tex]
and neglegt the last time derivative. How can we be so certain that the force is time-independent?Niles.
 
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Niles said:

Homework Statement


Hi

In QM we define the force operator F as (in the Heisenberg picture)
[tex] F = \frac{1}{i\hbar}[p, H] + (d_t F)(t)[/tex]
Shouldn't the second term be the derivative of p, not F?
What I can't understand is that usually (actually, always) we write
[tex] F = \frac{1}{i\hbar}[p, H][/tex]
and neglegt the last time derivative. How can we be so certain that the force is time-independent?


Niles.
 
You are right, it is the derivative of p. But the velocity is not necessarily time-independent?
 
You are right, thanks for that. In that case it is obvious that the last term is zero.Niles.