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

Niles
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Homework Statement


Hi

In QM we define the force operator F as (in the Heisenberg picture)
<br /> F = \frac{1}{i\hbar}[p, H] + (d_t F)(t)<br />
What I can't understand is that usually (actually, always) we write
<br /> F = \frac{1}{i\hbar}[p, H]<br />
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)
<br /> F = \frac{1}{i\hbar}[p, H] + (d_t F)(t)<br />
Shouldn't the second term be the derivative of p, not F?
What I can't understand is that usually (actually, always) we write
<br /> F = \frac{1}{i\hbar}[p, H]<br />
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're looking about the derivative of the operator itself, not the derivative of the momentum of the particle. Second, ∂p/∂t ≠ 0 only if the operator has an explicit time dependence.
 
You are right, thanks for that. In that case it is obvious that the last term is zero.Niles.
 
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