The angular position of the first minima in single slit diffraction is given by the equation:
\[ a \sin \theta = m\lambda, \quad \text{where } m = \pm 1 \]
For small angles, \( \sin \theta \) can be approximated as \( \tan \theta = \frac{y}{D} \). Thus, the equation simplifies to:
\[ y = \frac{\lambda D}{a} \]
Substitute the given values into the formula:
\[ y = \frac{650 \times 10^{-9} \, \text{m} \times 0.6 \, \text{m}}{0.6 \times 10^{-3} \, \text{m}} = \frac{390 \times 10^{-9}}{0.6 \times 10^{-3}} \, \text{m} = 0.00065 \, \text{m} = 0.65 \, \text{mm} \]
The total distance between the first minima on either side of the central maximum is double the distance \( y \):
\[ 2y = 2 \times 0.65 \, \text{mm} = 1.3 \, \text{mm} \]