Step 1: Understanding the Concept:
The ray returns along the same path when it strikes the silvered second surface at normal incidence, so that it is reflected back on itself.
Step 2: Angle conditions:
For a prism, \(r_1 + r_2 = A\). If the ray falls normally on the second surface, \(r_2 = 0\), so \(r_1 = A\).
Step 3: Apply Snell's law at the first surface:
\[ \mu = \frac{\sin i}{\sin r_1} = \frac{\sin 2A}{\sin A} = \frac{2\sin A\cos A}{\sin A} = 2\cos A \]
Step 4: Why the other options are wrong.
\(2\sin A\) would result from \(\sin 2A\) divided by \(\cos A\). Options with a factor \(\frac12\) cannot be greater than 1 for typical prism angles, whereas the refractive index must exceed 1.
Final Answer:
The refractive index is \(2\cos A\), option (B).
\[ \boxed{2\cos A} \]