Step 1: Retardation condition.
For conversion between opposite circular polarizations, phase difference = \(\pi\) radians.
\[
\Delta \phi = \frac{2\pi (n_e - n_o) t}{\lambda} = \pi
\]
Step 2: Solve for thickness \(t\).
\[
t = \frac{\lambda}{2(n_e - n_o)} = \frac{600 \times 10^{-9}}{2(1.551 - 1.542)} = \frac{600 \times 10^{-9}}{0.018} = 33.33 \times 10^{-6} \, \text{m}
\]
\[
t = 33.33 \, \mu\text{m}
\]
Step 3: Conclusion.
Hence, the thickness of the retarder = 33.33 µm.
A beam of light traveling horizontally consists of an unpolarized component with intensity \( I_0 \) and a polarized component with intensity \( I_p \). The plane of polarization is oriented at an angle \( \theta \) with respect to the vertical. The figure shows the total intensity \( I_{\text{total}} \) after the light passes through a polarizer as a function of the angle \( \alpha \), that the axis of the polarizer makes with respect to the vertical. Identify the correct statement(s). 