Exact finite Fourier projection and square filtering #
The L-term Fourier average (the paper: L = 5 * M) is applied to an arbitrary branch coefficient.
The label bounds eliminate modular wrap. The weights on the three tensor legs
then give a nonnegative square degree on every surviving branch. Taking the
constant coefficient retains exactly the branches with g = h and u = v.
The finite-family statements permit arbitrary coefficients and arbitrary repetitions of labels; they use only linearity of the Fourier projection and coefficient extraction, without assumptions on an ambient tensor.
A normalized finite Fourier average of one branch coefficient.
Equations
- MatrixMultiplicationAllFields.MatrixMultiplication.AuxiliarySeparation.finiteFourierCoefficient ζ L e c = (↑L)⁻¹ * ∑ r ∈ Finset.range L, ζ ^ (↑r * e) * c
Instances For
The Fourier average is a scalar support indicator, for every coefficient.
Averaging a finite family of branches agrees with averaging each branch.
Exactly L phases select the integer support equation, for any period
L > 3 * (M - 1) that is nonzero in K (the paper uses L = 5 * M).
A projected branch, recorded as an ordinary polynomial after Fourier averaging.
Equations
- One or more equations did not get rendered due to their size.
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The surviving polynomial weight is the square (g - h)^2.
A coefficient occurs exactly on the Fourier support at its integer total weight.
Each projected branch has no polynomial coefficient above (M - 1)^2.
Constant coefficient extraction is the exact square filter, with no restriction on the original coefficient.
Apply the finite Fourier projection and square weights branch by branch.
Equations
- One or more equations did not get rendered due to their size.
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Every coefficient of the projected polynomial has the exact integer support.
Exact finite filtering for an arbitrary finite family of branch coefficients.
The finite projected polynomial has support only in degrees at most (M - 1)^2.
The degree bound is independent of the number or values of the coefficients.