Let the electric field in some region $R$ be given by $\vec{E} = e^{-y^2}\hat{i} + e^{-x^2}\hat{j}$. From this we conclude that
Step 1: Use Gauss's law in differential form.
\[
\nabla \cdot \vec{E} = \frac{\rho}{\varepsilon_0}
\]
Compute divergence:
\[
\nabla \cdot \vec{E} = \frac{\partial}{\partial x}(e^{-y^2}) + \frac{\partial}{\partial y}(e^{-x^2})
\]
Both terms are nonzero because derivatives of exponentials exist.
Thus $\nabla \cdot \vec{E} \neq 0$.
Step 2: Interpretation.
If divergence is nonzero, charge density is nonzero.
Thus region contains a non-uniform charge distribution.
Step 3: Conclusion.
Correct: (A).
