The intensity at a point in Young's double-slit experiment is given by:
\[
I = I_0 \cos^2\left(\frac{\delta}{2}\right)
\]
where \( \delta \) represents the phase difference between the two waves.
Given a path difference of \( \frac{\lambda}{6} \), the corresponding phase difference is:
\[
\delta = \frac{2\pi}{\lambda} \cdot \frac{\lambda}{6} = \frac{2\pi}{6} = \frac{\pi}{3}
\]
The intensity can now be calculated as:
\[
I = I_0 \cos^2\left(\frac{\pi}{6}\right) = I_0 \left(\cos\frac{\pi}{6}\right)^2 = I_0 \left(\frac{\sqrt{3}}{2}\right)^2 = I_0 \cdot \frac{3}{4}
\]
Therefore, the required intensity is:
\[
\boxed{I = \frac{3}{4} I_0}
\]