Angular width of the first minimum on either side of the central maximum due to a single slit of width \(a\), illuminated by a light of wavelength \(\lambda\) is
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Single-slit central maximum extends from first minimum on one side to first minimum on the other side, so its angular width is doubled.
For the first minimum in single slit diffraction:
\[
a\sin\theta=\lambda
\]
For small angles:
\[
\theta\approx \frac{\lambda}{a}
\]
The first minimum occurs on both sides of the central maximum, so angular width is:
\[
2\theta = 2\frac{\lambda}{a}
\]
Hence,
\[
\boxed{(C)\ \frac{2\lambda}{a}}
\]