Can anyone help me understand how the following formula was derived:
If we are in the case of the far field resolution limit. This means that the evanescent waves are not present, as they would have damped out.
Now the condition for the propagation is : All spatial frequencies that can propagate need to be smaller than $k=\frac{2\pi}{\lambda}n$
We have a bandwidth of spatial frequencies $\DeltaK_T<\frac{2\pi}{\lambda}n$
We have a bandwidth in position space $\Delta r_T$.
From the condition $\DeltaK_T\Delta r_T>1$ one gets that: