Solution (source code)

= Solution

The <five-point Laplacian> applied to $f$ has expansion
$$
\Gamma_5f=h^2\Delta f+\frac{h^4}{12}(f_{xxxx}+f_{yyyy})+O(h^6).
$$
The corrected right side $h^2f+(h^2/12)\Gamma_5f$ cancels the $h^4\Delta f/12$ term in $\Gamma_9u$. Consequently
$$
\boxed{h^{-2}\left(\Gamma_9u-h^2f-\frac{h^2}{12}\Gamma_5f\right)=O(h^4).}
$$
More precisely, the unscaled residual's $h^6$ coefficient is $-(u_{xxxxxx}+u_{yyyyyy})/240+(u_{xxxxyy}+u_{xxyyyy})/144$. This <fourth-order correction of the nine-point Poisson stencil> does not require $f$ to be harmonic.