The mean free path \( \lambda \) is inversely proportional to the number of particles and the volume. The mean free path for the initial state is \( \lambda_1 \), and after the change, it becomes \( 4\lambda_1 \). Thus, we have:
\[
\lambda_1 \propto \frac{V_1}{N_i}.
\]
After halving the number of particles,
\[
\lambda_2 \propto \frac{V_2}{\frac{N_i}{2}} = \frac{2V_2}{N_i}.
\]
Using the given condition that \( \lambda_2 = 4 \lambda_1 \), we get:
\[
\frac{2V_2}{N_i} = 4 \times \frac{V_1}{N_i} \Rightarrow 2V_2 = 4V_1 \Rightarrow V_2 = 2V_1.
\]
Final Answer: The ratio \( \frac{V_1}{V_2} \) is \( 0.5 \).