The minimum resolvable distance \( d \) in a microscope can be related to the refractive index \( n \) and the wavelength \( \lambda \) using the formula:
\[
d = \frac{\lambda}{n}
\]
Assuming the wavelength in air is the same as the minimum resolvable distance when \( n = 1 \), that is, \( \lambda = 6 \, \mu m \):
When the medium changes to a refractive index of \( n = 1.5 \), the new resolvable distance is:
\[
d' = \frac{6 \, \mu m}{1.5} = 4 \, \mu m
\]