Step 1: Given:
\[
\text{Angle of incidence } i = 60^\circ,
\text{Prism angle } A = 30^\circ
\]
Step 2: Since the ray retraces its path, the emergent angle inside the prism is equal to the angle of incidence on the second face:
\[
\text{Total deviation } = 0^\circ \Rightarrow \text{ray is normal to second face}
\]
Step 3: Use Snell’s law at the first surface:
\[
\mu = \frac{\sin i}{\sin r}
\]
Use geometry in prism: if angle of prism \( A = 30^\circ \), and the ray goes normally to the second face (internal angle of refraction = 90° to face), then internal angle at first face:
\[
r = \frac{A}{2} = 15^\circ
\]
Step 4:
\[
\mu = \frac{\sin 60^\circ}{\sin 15^\circ} = \frac{\sqrt{3}/2}{\sin 15^\circ}
\]
But for retracing, \( r = 30^\circ \) leads to:
\[
\mu = \frac{\sin 60^\circ}{\sin 30^\circ} = \frac{\sqrt{3}/2}{1/2} = \boxed{\sqrt{3}}
\]