Expand the unknown in Fourier modes:
By Termwise differentiation of a Fourier series,
Also,
Therefore the coefficient of on the left-hand side is
The right-hand side has coefficients
because the coefficient of each of is and the constant coefficient is one. Hence the Fourier spectral system for a cosine-modulated second derivative is
Its coefficient array is an infinite tridiagonal matrix.
For a spectral truncation, retain the modes , set
and impose the displayed coefficient equation for every . This gives an explicit -dimensional tridiagonal system. The resulting finite Fourier series automatically satisfies the periodic boundary conditions.
Insert the Fourier series
into the rectangle rule. The finite geometric sum obeys
Consequently the quadrature value is
whereas
Thus the exact Periodic N-point rectangle-rule error is
By the Fourier coefficient decay of an analytic periodic function, there are constants and such that
It follows that
Therefore
which is exponential, and hence spectral, convergence.

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