Step 1:
For the reflected light to be completely polarized, the angle of incidence must be equal to the Brewster angle, \( \theta_B \), which is given by:
\[
\tan \theta_B = n
\]
where \( n \) is the refractive index of the medium.
Step 2:
Given that the angle of incidence is \( 60^\circ \), we can equate this to the Brewster angle:
\[
\tan 60^\circ = n
\]
\[
n = \sqrt{3}
\]