Termwise differentiation of a Fourier series multiplies a mode by its wavenumber, so
The convolution theorem turns pointwise multiplication into discrete convolution:
so
The assumed real analyticity justifies these termwise operations through rapid decay of the Fourier coefficients.
Expand in the two-dimensional Fourier basis. Applying the derivative and product rules from part (a), the coefficient of the equation is
The normalization and compatibility conditions are
Thus, on , the infinite Fourier spectral method system is
For a square spectral truncation, choose
retain equations and unknowns indexed by , and set omitted coefficients to zero. This is the Fourier–Galerkin method: it projects the residual onto the retained Fourier modes. Other finite mode sets may be used in the same way.
Here the only nonzero coefficients of are
Therefore, for each , the truncated system is
where a coefficient is omitted when its index is outside or equals .
For wavevectors and , the matrix entry is
Because , , so the matrix is symmetric. Its diagonal entry is . The sum of absolute off-diagonal entries is at most
because for nonzero integer ; truncation can only reduce the sum. Hence is strictly diagonally dominant with positive diagonal. The Gershgorin circle theorem places every eigenvalue in the positive interval
for at least one row. Since the symmetric matrix has only real eigenvalues, all are positive, and is a positive-definite matrix. Any one-dimensional ordering merely conjugates by a permutation matrix, preserving symmetry and positive definiteness.

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