Natural monochromatic light of intensity. \(I_{0}\) falls on a system of two Polaroids between which a crystalline plate is inserted, cut parallel to its optical axis. The plate introduces a phase difference \(\delta\) between the ordinary and extraordinary rays. Demonstrate that the intensity of light transmitted through that system is equal to \[ I=\frac{1}{2} I_{0}\left[\cos ^{2}\left(\varphi-\varphi^{\prime}\right)-\sin 2 \varphi \cdot \sin 2 \varphi^{\prime} \sin ^{2}(\delta / 2)\right] \] where \(\varphi\) and \(\varphi^{\prime}\) are the angles between the optical axis of the crystal and the principal directions of the Polaroids. In particular, consider the cases of crossed and parallel Polaroids.