The fringe width in Young’s double slit experiment is given by:
\[
\Delta y = \dfrac{\lambda L}{d},
\]
where $\lambda$ is the wavelength, $L$ is the distance to the screen, and $d$ is the slit separation.
The wavelength for a transition $n \to 2$ in the Balmer series is given by:
\[
\lambda = \dfrac{R}{\left(\dfrac{1}{2^2} - \dfrac{1}{n^2}\right)},
\]
where $R$ is the Rydberg constant. For the fringe width to be constant, the slit separation $d$ must be scaled by a factor that compensates for the change in $\lambda$ as $n$ changes.
Thus, the required factor for scaling $d$ is $\dfrac{4n^2}{n^2 - 4}$, which corresponds to option (C).