Fourier-Koide lemma
$Q_{\rm Koide} = 2/3 \iff |a_1|/|a_0| = 1/\sqrt{2} = \sqrt{s}$ — Parseval equivalence on $\mathbb{Z}/3\mathbb{Z}$.
Statement
Let be the triplet of square roots of lepton masses. Decompose it via discrete Fourier on :
Then:
That is: the Koide condition is rigorously equivalent to saying the AC/DC ratio of the lepton mass spectrum (oscillating component / constant component) equals the square root of the fundamental spin.
ThéorèmeWhy it matters
Before this lemma, was a strange numerical regularity. With this lemma, becomes the equation “the sieve sees spin in masses”: lepton masses are not independent data, they encode through their Fourier transform on .
This is why the lemma was promoted from COND to THM in April 2026: it establishes a direct algebraic bridge between an experimental quantity (lepton masses) and an arithmetic theorem (T1, which forces ).
Plain reading. Looking at the three lepton masses as a signal on three sites (one per generation), this signal has a mean part and an oscillating part. The theorem says: the ratio between oscillation and mean is exactly . And is the square root of the sieve’s fundamental spin. So Koide’s formula simply says: “lepton masses measure the spin of the sieve”.
Proof
Step 1 — Fourier decomposition on
The triplet decomposes as:
The coefficient is the mean (DC); is the oscillation amplitude (AC).
Step 2 — Parseval identity
By Parseval on :
The Koide definition then reads:
Step 3 — Inversion
With the canonical PT normalisation (unit vector), one obtains:
This is the proven equality. See monograph ch10 for the exact canonical normalisation.
Consequence: as an information principle
The lemma turns the Koide condition into an information statement:
The AC/DC ratio of the lepton mass spectrum is the square root of the fundamental spin.
This means the lepton spectrum cannot be perturbed arbitrarily: it is constrained by the sieve’s spin. This is what ensures Koide stability under renormalisation-group evolution, and what motivates the Fisher-Koide identity for .