Finite Fourier generator identities used in the classical Galerkin estimates.
Use normalized Haar measure on the unit circle for periodic integrals.
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- classicalGeneratorMeasureSpaceUnitAddCircle = { toMeasurableSpace := QuotientAddGroup.measurableSpace (AddSubgroup.zmultiples 1), volume := AddCircle.haarAddCircle }
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Closed spatial unit cell used for compactness and periodic integration.
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Real Fourier mode with the finite-dimensional Galerkin indexing.
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Spatial gradient of a real Fourier mode with Galerkin indexing.
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The finite ambient real Fourier expansion is smooth and retains integer periodicity.
Coordinate derivatives of a finite real Fourier synthesis are the corresponding sums of mode derivatives.
The positive real Fourier coefficient derivative formula iterates to every ordered spatial derivative: finite projection commutes with each such derivative.
Finite real Fourier synthesis agrees with the ambient smooth periodic synthesis on the quotient torus.
On a finite real Fourier span, the weak matrix is precisely the orthogonal projection of
κ Δu - b · ∇u. The diffusion part is identified by periodic integration by parts, while the
drift part is expanded directly in the finite Fourier synthesis.
Multiplication by a bounded smooth periodic function followed by Fourier projection is
bounded by the multiplier's uniform norm. The finite Fourier synthesis has exactly the
coefficient-space L² norm.
The real Fourier projection as a continuous linear map from torus L² to coefficients.
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Integral-defined projection coefficients agree with the continuous L² projection map.
Real Fourier projection is additive on square-integrable inputs.
Real Fourier projection is homogeneous on square-integrable inputs.
Real Fourier projection is subtractive on square-integrable inputs.
A continuous integer-periodic scalar function is bounded on the whole space.
The torus representative of a continuous periodic scalar is square-integrable.
Fourier projection of a smooth periodic scalar is bounded in coefficient norm by any global uniform bound for the scalar.
Fourier projection commutes with finite sums of continuous periodic ambient functions.
The norm of a projected finite list sum is bounded by the sum of the projected term norms.
Ordered spatial derivatives distribute over a finite sum of smooth scalar functions.
Ordered spatial derivatives commute with subtraction.
Ordered spatial derivatives commute with multiplication by a real constant.
Spatial derivatives commute with the Laplacian on smooth functions.