To ensure continuity at \(x = 0\), we require \( \lim_{x \to 0^-} f(x) = \lim_{x \to 0^+} f(x) = f(0) \).
Left-hand limit:
\[ \lim_{x \to 0^-} f(x) = \lim_{x \to 0^-} \frac{1 - \cos 2x}{x^2} = 2 \]
This gives \( f(0) = \alpha = 2 \).
Right-hand limit:
\[ \lim_{x \to 0^+} f(x) = \lim_{x \to 0^+} \frac{\beta \sqrt{1 - \cos x}}{x} = \frac{\beta}{\sqrt{2}} = 2 \implies \beta = 2\sqrt{2} \]
Calculating \( \alpha^2 + \beta^2 \):
\[ \alpha^2 + \beta^2 = 4 + 8 = 12 \]
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:
