Step 1: Condition for diffraction minima.
For single slit:
\[
a \sin \theta = m \lambda_1, \quad m = 1, 2, 3, ...
\]
For first minima:
\[
a \sin \theta = \lambda_1.
\]
Step 2: Condition for diffraction maxima.
For interference maxima of another wavelength $\lambda_2$:
\[
a \sin \theta = n \lambda_2, \quad n = 1, 2, 3, ...
\]
For first maxima: $n=2$:
\[
a \sin \theta = 2 \lambda_2.
\]
Step 3: Equating conditions.
Since first minima of $\lambda_1$ coincides with first secondary maximum of $\lambda_2$:
\[
\lambda_1 = 2 \lambda_2.
\]
\[
\lambda_2 = \frac{\lambda_1}{2}.
\]
Step 4: Substitution.
\[
\lambda_2 = \frac{660}{2} = 330 \, \text{nm}.
\]
Step 5: Conclusion.
Hence, the required wavelength is $\lambda_2 = 330 \, \text{nm}$.