The Dillon--Kashyap phase formula, as a hypothesis #
The one statement this development takes from the literature is fixed here as
a Prop-valued definition, never as an axiom. Nothing is assumed
globally: every theorem that uses it carries it as an explicit hypothesis, and
MCM/PhaseFormula.lean then discharges it internally, so #print axioms on the final
theorem lists only propext, Classical.choice and Quot.sound.
Provenance: Theorems 1--2 of J. F. Dillon and N. Kashyap, Jacobi-like sums and
difference sets with Singer parameters, Australas. J. Combin. 55 (2013),
49--63. Their Theorem 1 gives the Fourier coefficient
G(χ) G(χ^(2^k+1)) / G(χ³) and their Theorem 2 identifies the corresponding
difference set as the complement of this same Δ; the sign convention here is
therefore opposite to theirs.
For every multiplicative character χ,
F̂(χ) = G(χ) G(χ^(2^k+1)) / G(χ³), where F = +1 on Δ* and -1 off it.
The substantive imported theorem: it supplies the phases, not merely the magnitudes, of the Kasami Fourier spectrum. Dillon--Kashyap Theorems 1--2, in the sign convention used here.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Non-degeneracy of the phase formula. In Lean x / 0 = 0, so if the
denominator G(χ³) could vanish the right-hand side of
DillonKashyapPhaseFormula would silently become the junk value 0 and the
whole property could be satisfiable only by accident. For a primitive additive
character no Gauss sum vanishes, so the quotient is a genuine division.