The mean free path (\( \lambda \)) of a gas molecule is given by the following relation:
\[
\lambda = \frac{1}{\sqrt{2} \, n \sigma}
\]
where:
- \( n \) is the number of molecules per unit volume,
- \( \sigma \) is the effective collision cross-section, which depends on the molecular diameter (\( d \)).
The effective cross-section is proportional to the square of the molecular diameter:
\[
\sigma \propto d^2
\]
Since both gases have the same number of molecules per unit volume, the ratio of their mean free paths will be inversely proportional to the ratio of their molecular diameters squared:
\[
\frac{\lambda_1}{\lambda_2} = \left( \frac{d_2}{d_1} \right)^2
\]
Given that the molecular diameters are in the ratio 1 : 3, we have:
\[
\frac{\lambda_1}{\lambda_2} = \left( \frac{3}{1} \right)^2 = 9
\]
Thus, the ratio of their mean free paths is:
\[
\boxed{9 : 1}
\]