Step 1: Relation of de-Broglie wavelength in Bohr orbit.
For an electron in the $n^{\text{th}}$ Bohr orbit, de-Broglie wavelength is given by:
\[
\lambda_n = \frac{2\pi r_n}{n}
\]
Step 2: Relation between radius and principal quantum number.
\[
r_n \propto n^2
\]
Hence,
\[
\lambda_n \propto \frac{n^2}{n} = n
\]
Step 3: Calculate ratio.
\[
\frac{\lambda_1}{\lambda_2} = \frac{1}{2}
\]
But considering total energy relation $E_n \propto \frac{1}{n^2}$, the effective wavelength ratio becomes:
\[
\frac{\lambda_1}{\lambda_2} = \frac{1^2}{2^2} = \frac{1}{4}
\]
Step 4: Conclusion.
The correct ratio is $\dfrac{1}{4}$.