Looking at some examples in the "handbook of MRI Pulse Sequences" by Bernstein, I see the following:
So if I can generate an RF pulse with a bandwidth of 2 kHz and I want a 3 mm slice thickness, the gradient amplitude can be chosen with:
$$ G_z = \frac{2\pi \Delta f}{\gamma \Delta_z} $$
Plugging the values, this gives a gradient strength of 15.6 mT/m.
Now, my question is that will this gradient select a 3 mm thick slice at the magnet isocenter?
Now say in my MR experiment I am acquiring 128 such slices. Now, if I want to excite the "bottom most slice" than I need to adjust the RF bandwidth and the change in RF BW is given by:
$$ \delta f = \frac{\gamma G_z \delta_z}{2 \pi} $$
Here now, my $\delta_z = -64 * 0.003 m$. Hence, the new RF BW will need to be
$$ f = \Delta f - 64 \Delta f = -126 khz $$
I am not sure if this calculation is correct. The RF value seems quite high to be although I am not sure what is the range of modern MR scanner RF generators.