Step 1: Link wavelength to the orbit number.
The de Broglie wavelength is $\lambda = \tfrac{h}{p}$. In Bohr orbits the speed falls as $\tfrac1n$, so the momentum also falls as $\tfrac1n$, which makes $\lambda \propto n$.
Step 2: Identify the two levels.
The ground state is $n=1$. The third excited state is $n=4$ (ground, then first, second, third excited give $1,2,3,4$).
Step 3: Take the ratio.
Since $\lambda \propto n$, going from $n=4$ to $n=1$ scales the wavelength by $\tfrac{1}{4}$.
Step 4: State the change.
\[ \boxed{\lambda \to \tfrac14\ \text{of its value}} \]