The fringe width (\( \beta \)) in a double-slit experiment is given by: \[ \beta = \frac{\lambda D}{d}, \] where: - \( \lambda \) is the wavelength of the light, - \( D \) is the distance between the slits and the screen, - \( d \) is the separation between the slits.
Step 1: Relation between fringe widths. Since \( D \) and \( d \) are constant, the fringe width \( \beta \) is directly proportional to \( \lambda \): \[ \beta \propto \lambda. \]
Step 2: Calculate the new fringe width. Let the initial fringe width (\( \beta_1 \)) correspond to \( \lambda_1 = 400 \, \text{nm} \) and the new fringe width (\( \beta_2 \)) correspond to \( \lambda_2 = 600 \, \text{nm} \). Then: \[ \frac{\beta_2}{\beta_1} = \frac{\lambda_2}{\lambda_1}. \] Substituting \( \beta_1 = 2 \, \text{mm} \), \( \lambda_1 = 400 \, \text{nm} \), and \( \lambda_2 = 600 \, \text{nm} \): \[ \frac{\beta_2}{2} = \frac{600}{400} \implies \beta_2 = 2 \cdot 1.5 = 3 \, \text{mm}. \]
Final Answer: The fringe width for \( \lambda = 600 \, \text{nm} \) is: \[ \boxed{3 \, \text{mm}}. \]
Two plane polarized light waves combine at a certain point, whose "E" components are: \[ E_1 = E_0 \sin \omega t, \quad E_2 = E_0 \sin \left( \omega t + \frac{\pi}{3} \right) \] Find the amplitude of the resultant wave.

Let \( a \in \mathbb{R} \) and \( A \) be a matrix of order \( 3 \times 3 \) such that \( \det(A) = -4 \) and \[ A + I = \begin{bmatrix} 1 & a & 1 \\ 2 & 1 & 0 \\ a & 1 & 2 \end{bmatrix} \] where \( I \) is the identity matrix of order \( 3 \times 3 \).
If \( \det\left( (a + 1) \cdot \text{adj}\left( (a - 1) A \right) \right) \) is \( 2^m 3^n \), \( m, n \in \{ 0, 1, 2, \dots, 20 \} \), then \( m + n \) is equal to: