The phase difference \( \Delta \phi \) between the ordinary and extraordinary rays is given by: \[ \Delta \phi = \frac{2\pi}{\lambda_0} (n_e - n_o) \, d. \] For the light to remain linearly polarized, the phase difference must be a multiple of \( 2\pi \): \[ \Delta \phi = 2\pi m \quad \text{(where \( m \) is an integer)}. \]
Substituting \( \Delta \phi = 2\pi \) for the minimum thickness (i.e., \( m = 1 \)): \[ \frac{2\pi}{\lambda_0} (n_e - n_o) \, d = 2\pi. \] Simplify: \[ \frac{(n_e - n_o) \, d}{\lambda_0} = 1. \] Rearrange for \( d \): \[ d = \frac{\lambda_0}{n_e - n_o}. \]
Given: \[ \lambda_0 = 600 \, \text{nm} = 0.6 \, \mu\text{m}, \quad n_e - n_o = 0.05. \] Substitute into the formula: \[ d = \frac{0.6}{0.05} = 12 \, \mu\text{m}. \]
The plateβs thickness must account for half-wavelength retardation for the given wavelength, dividing \( d \) by 2: \[ d_{\text{min}} = \frac{12}{2} = 6 \, \mu\text{m}. \]
The minimum thickness of the plate is 6 Β΅m.
In a Youngβs double slit experiment, a combination of two glass wedges $ A $ and $ B $, having refractive indices 1.7 and 1.5, respectively, are placed in front of the slits, as shown in the figure. The separation between the slits is $ d = 2 \text{ mm} $ and the shortest distance between the slits and the screen is $ D = 2 \text{ m} $. Thickness of the combination of the wedges is $ t = 12 \, \mu\text{m} $. The value of $ l $ as shown in the figure is 1 mm. Neglect any refraction effect at the slanted interface of the wedges. Due to the combination of the wedges, the central maximum shifts (in mm) with respect to 0 by ____
