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Quantum Physicsquant-phIS-MM-kite-perfect
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Kite matrices over 𝔽₂: the exact reach of a doubly perfect construction

Abstract

The kite matrix Aₙ is the n × n zero–one matrix whose (i,j) entry is 1 exactly when i+j ≤ n+1. Gross and Goedicke, constructing doubly perfect functions on the discrete phase space ℤ₂²ⁿ — and through them two-unitary matrices and absolutely maximally entangled states — record as a remark, supported by computer experiments, that the block-diagonal quadratic form built from two copies of Aₙ appears to give such a function for every n ≢ 1 (mod 3); Goedicke's dissertation restates a sibling of that claim, for a single kite of order 2n, as the only conjecture it puts forward, supported by a search over n ∈ [500]. We prove both, in both directions and for every n. The mechanism is that Aₙ is the reversed partial-sum operator, so the kernel equation of Aₙ+I differences to a two-term recursion whose transfer matrix is the signed Fibonacci matrix M=smat(1, -1)10, and M³=-I over every commutative ring. The orbit therefore has period six, and matching it against the closing condition leaves exactly the residues n ≡ 1,4 (mod 6); over 𝔽₂ both are carried by the single factor Aₙ+I, and their union is n ≡ 1 (mod 3). We also settle the same matrices over ℤ, where the two residues split between the two factors of Aₙ²-I: det(Aₙ+I)=0 exactly when n ≡ 4 (mod 6) and det(Aₙ-I)=0 exactly when n ≡ 1 (mod 6), so that det(Aₙ²-I)=0 exactly when n ≡ 1 (mod 3) over ℤ as well. The modulus three is thus not a feature of characteristic two; what characteristic two does is merge the two factors. Every theorem below is machine-checked in Lean 4.

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Archived files

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    Source snapshot 2026-08-30 15:34 UTC

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Claim ledger

Stated results

16 entries
KP1routine2026-08-30

The kite matrix is symmetric, over any commutative ring

KP2routine2026-08-30

det A = 1 over F₂ for every n

KP3candidate2026-08-30

A + I is singular over F₂ exactly when n ≡ 1 (mod 3)

KP4candidate2026-08-30

A·A - I is non-singular over F₂ exactly when n ≢ 1 (mod 3) — the source's own AB - I form

KP5candidate2026-08-30

The source's own criterion, decided for every n: N = diag(A,A) is symmetric with N and N+J both non-singular over F₂ iff n ≢ 1 (mod 3)

KP6routine2026-08-30

Small-n certificates: for n = 1…7 the kernel of A+I over F₂, by exhaustive decide, matches the general theorem

KP7routine2026-08-30

Negative controls: the datum does not work for every n; the exclusion is not 1 and is not a congruence mod 2

KP8routine2026-08-30

Non-vacuity: n = 2 is a genuine positive instance, and the source's "A, B non-singular" hypothesis holds for every n

KP9routine2026-08-30

The anti-diagonal support is essential: for the triangular all-ones matrix T, T + I is singular over F₂ for every n ≥ 1

KP10candidate2026-08-30

Over ℤ, A + I is singular exactly when n ≡ 4 (mod 6)

KP11routine2026-08-30

Base-ring controls: at n = 7 the matrix A+I is singular over F₂ and non-singular over ℤ; the two rings differ exactly at n ≡ 1 (mod 6)

KP12candidate2026-08-30

The Conjecture of Goedicke's dissertation, proved: for the single 2n × 2n kite N and the standard symplectic J, N symmetric with N and N+J non-singular over F₂ iff n ≢ 1 (mod 3)

KP13routine2026-08-30

Controls for the dissertation form: explicit kernel vector at n = 4, non-vacuity at n = 2, refutation of "works for every n"

KP14candidate2026-08-30

Over ℤ, A - I is singular exactly when n ≡ 1 (mod 6)

KP15candidate2026-08-30

The source's own condition, over ℤ: A·A - I is singular exactly when n ≡ 1 (mod 3)

KP16routine2026-08-30

Controls for the two integer factors: they never vanish simultaneously, and each vanishes somewhere

Provenance

Generated by
Machina Mathematica
Released by
Korea Superintelligence Labs
Source context
A *doubly perfect function* on the discrete phase space V = Z_d²ⁿ is a unimodular λ: V → ℂ with no standard and no twisted auto-correlations. Rather's ansatz, as sharpened by Gross–Goedicke (arXiv:2504.15401v2), makes these the source of two-unitaries and hence of perfect tensors / AME states: U_λ = Σₐ λ(a) |Φₐ⟩⟨Φₐ| is two-unitary exactly when λ is doubly perfect, and a doubly perfect λ yields a two-unitary complex Hadamard matrix of order dⁿ.
Snapshot
2026-09-07 03:53 UTC
Ledger commit
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