Step 1: Intensity in interference.
In Young's experiment $I = I_{0}\cos^{2}\!\left(\dfrac{\phi}{2}\right)$, where $\phi$ is the phase difference and $I_{0}$ is the brightest value.
Step 2: Link path and phase.
The phase difference comes from the path difference: $\phi = \dfrac{2\pi}{\lambda}\,\Delta x$.
Step 3: Put in the path difference.
Given $\Delta x = \dfrac{\lambda}{6}$, \[ \phi = \frac{2\pi}{\lambda}\times\frac{\lambda}{6} = \frac{\pi}{3} \]
Step 4: Halve the phase.
\[ \frac{\phi}{2} = \frac{\pi}{6} = 30^{\circ} \]
Step 5: Square the cosine.
\[ \frac{I}{I_{0}} = \cos^{2}(30^{\circ}) = \left(\frac{\sqrt{3}}{2}\right)^{2} = \frac{3}{4} \]
Step 6: State the answer.
So $\dfrac{I}{I_{0}} = \dfrac{3}{4}$, which is option 4.
\[ \boxed{\frac{I}{I_{0}} = \frac{3}{4}} \]