In single slit diffraction, the angular width \( \theta \) of the central maxima is given by:
\[
\sin \theta = \frac{\lambda}{\alpha}
\]
Where:
- \( \lambda \) is the wavelength of light,
- \( \alpha \) is the slit width.
The width of the central maxima \( \beta \) is given by:
\[
\beta = 2L \tan \theta
\]
Where \( L \) is the distance to the screen.
Now, if we double the slit width, i.e., \( \alpha \) becomes \( 2\alpha \), the angular width \( \theta \) changes as follows:
\[
\sin \theta = \frac{\lambda}{2\alpha}
\]
Since \( \theta \) decreases when \( \alpha \) increases, the corresponding width of the central maxima will also decrease. Hence, the new width will be:
\[
\beta_{\text{new}} = \frac{\beta}{2}
\]
Thus, the width of the central maxima is halved when the slit width is doubled.