Top-KPQ Collision Geometry
Complete Fibers and the 576-Level Dense Local Ring

Muhammad Arshad · September 2026 · MPRC Z₂₅₆ collision classification, canonical terminal forms, and dense-local ramification

Abstract

What Is Closed

This chapter records two results reached after the five-paper dyadic-cubic series. First, the frozen MPRC fingerprint (K,P,Q) is a complete invariant of the congruence generated by the primitive same-sign Top-3 repartitions together with temporal permutation. Equality of (K,P,Q) is therefore not merely necessary: it is sufficient for two selections to lie in the same rewrite component. Second, the dense diagonal localization of the collision algebra over Z₂₅₆ has one relative rotor parameter and exact maximal-ideal nilpotence length 576.

Scope boundary. These theorems classify the frozen MPRC collision model. They do not prove the still-open unoriented sheet quotient, the full Q-space symmetry audit, the higher Betti claims, or a structural identification of the numbers 252 and 576 with the CXR 3×3 and 4×4 grids.


01 · Frozen Fingerprint

The (K,P,Q) Object

Let c=(x₀,…,x_{K−1}) be a temporally ordered MPRC selection of K selected positions on Z₂H. For the MPRC ring H=128 and 2H=256. Its movement multiset has cardinality m=K−1. Define

P = (x_last − x_first) mod 2H
D = min(P, 2H − P)
L = Σ d_circle(x_i,x_{i+1})
Q = (L − D)/2.

K is the observed number of selected positions, not a tuned Top-K hyperparameter; m=K−1 is the number of movements. U, the sliding observer, changes the candidate domain; it is not part of the fingerprint of a fixed selection.


02 · Primitive Collision Law

The Native Repartition

For ordinary positive magnitudes 1≤i≤j≤H−1, and separately for the negative orientation, the primitive collision move is

{+i,+j} ↔ {+(i−1),+(j+1)}
{−i,−j} ↔ {−(i−1),−(j+1)}.

Zero and the half-turn H are sign-free boundary states. Each primitive move preserves K, P and L, hence also Q.


03 · Theorem

Top-KPQ Completeness Theorem

Theorem 26.1. Two MPRC selections are congruent under primitive same-sign repartitions and temporal permutation if and only if they have the same frozen fingerprint (K,P,Q).

F(c₁)=F(c₂) ⇔ c₁ ~ c₂,    F(c)=(K,P,Q).

The forward implication is invariance. For the converse, orient each primitive rewrite toward increasing

Ψ = Σ D(e)².

A move (i,j)→(i−1,j+1) changes the potential by

(i−1)²+(j+1)²−i²−j² = 2(j−i+1) ≥ 2.

Ψ is integer and bounded above by mH², so every oriented rewrite sequence terminates. A terminal multiset contains at most one ordinary positive magnitude and at most one ordinary negative magnitude; all remaining entries are 0 or H. The invariants force that terminal uniquely.


04 · Canonical Terminal

Closed Form in (a,b,h,z)

For a reachable fiber, write the unique terminal as one positive residue a when a>0, one negative residue b when b>0, h half-turns and z zero moves. With P represented in Z₂H,

a = ((L+P)/2) mod H
b = ((L−P)/2) mod H
h = (L−a−b)/H
z = m−h−[a>0]−[b>0] = (K−1)−h−[a>0]−[b>0].

Hence every (K,P,Q) fiber has one irreducible normal form. Two selections with the same fingerprint reduce to the same terminal and are therefore in the same undirected rewrite component.


05 · Verification

Falsification Record

The theorem is analytical; finite computation is retained as regression evidence rather than substituted for the proof. Exhaustive enumeration checked H=2…7 and K=2…4, including P=0, P=H, mixed-sign selections, zero moves, half-turns and repeated values. For H=128, the K=2 case exhausts all 32,896 multisets with zero mismatches against the closed form.


06 · Collision Presentation

The Dense Quadrics

Introduce variables x_i for the positive orientation and y_i for the negative orientation, with shared sign-free endpoints x₀=y₀ and x_H=y_H. The primitive repartitions are represented by

x_i x_j = x_{i−1} x_{j+1}
y_i y_j = y_{i−1} y_{j+1},    1≤i≤j≤H−1.

There are H(H−1)/2 quadrics per orientation and therefore H(H−1) in total. At H=128 this is 16,256.


07 · One Relative Rotor

Dense Localization Collapses

Localize at the dense diagonal prime

𝔭 = (2, y_i−x_i).

The x_i and y_i are units there. Put z=x₀=y₀. From the i=1 positive quadrics, if t=x₁/x₀ then x_j=z t^j. Similarly, with s=y₁/y₀, y_j=z s^j. The shared half-turn gives t^H=s^H. Defining u=s/t yields

u^H=1
y_i=x_i u^i
y_i−x_i=x_i(u^i−1).

Because y₁−x₁=x₁(u−1) and x₁ is a unit, all 127 interior difference directions generate the same ideal:

(y_i−x_i : 1≤i≤H−1) = (u−1).

Thus 𝔭=(2,u−1). The dense collision algebra has one relative rotor direction, not 127 independent nilpotent directions.


08 · Theorem

Dense MPRC Collision Ramification

For H=128 set u=1+ε. Then u¹²⁸=1 gives

(1+ε)¹²⁸ = 1.

Theorem 26.2. In the dense diagonal localization over Z₂₅₆,

𝔭⁵⁷⁵ ≠ 0,    𝔭⁵⁷⁶ = 0,
𝔭⁵⁷⁵ = ⟨128 ε¹²⁷⟩.

For 1≤j<128, ν₂(C(128,j))=7−ν₂(j). Give the monomial 2^a ε^b the MPRC weight

W(2^a ε^b)=64a+b.

The unique lowest-weight collision in the binomial relation is between ε¹²⁸ and the j=64 term 2·(odd)·ε⁶⁴; both have weight 128. Every reduction is therefore weight-nondecreasing. A nonzero normal form has a≤7 and b≤127, so its weight is at most

7·64+127 = 575.

Every generator 2^a ε^(576−a) of 𝔭⁵⁷⁶ has weight 576+63a≥576 and must vanish. Repeatedly taking the unique weight-128 branch gives

ε⁵⁷⁵ = 128 ε¹²⁷ ≠ 0.

Hence the exact nilpotence length is 576.


09 · Numerical Corollary, Not Yet Geometry

The 252 → 576 Observation

The proven ramification length has the exact arithmetic forms

576 = 9·64 = 9·4·16 = 24².

The established active-address count has

252 = 7·36 = 7·4·9.

Therefore the pair may be written (4,7,9)→(4,9,16). This is especially suggestive because the CXR work used 3×3 and 4×4 grids. The arithmetic identity is exact; a theorem identifying these factors with the CXR grid construction has not yet been proved and is intentionally left open.



10 · Theorem

Unoriented Sheet Quotient

Theorem 26.3. On the self-conjugate displacement sheets P=0 and P=H, charge conjugation acts on the static simplex exactly by (η⁺,η⁻,η_H)↦(η⁻,η⁺,η_H). The unoriented sheet is therefore Δ_T/ℤ₂.

Circular magnitude is invariant under e↦−e, so L and Q are unchanged while P↦−P. The only fixed displacement sheets are 0 and H. On those sheets the base residues coincide, a=b, so conjugation swaps only the two oriented excess coordinates and leaves the half-turn coordinate fixed. The K-admissibility condition is symmetric in the two oriented sums, hence the quotient is exact.

|Δ_T/ℤ₂| = ½[ C(T+2,2) + ⌊T/2⌋ + 1 ]

for the unrestricted simplex; K-admissible subsets inherit the same involution orbit construction.


11 · Theorem

Exact Metric-Affine Symmetry

Theorem 26.4. The uniform metric-affine ring symmetries are exactly V₄={I,C,A,AC}; with m=K−1 movement-coordinate permutations the full stated group is S_m×V₄.

For f(e)=ae+b with gcd(a,2H)=1, requiring either D(f(e))=D(e) for all e or D(f(e))=H−D(e) for all e forces, from e=0 and e=1 alone, b∈{0,H} and a∈{+1,−1}. Thus no other affine ring map survives.

C: P↦−P, L↦L, Λ↦Λ
A: P↦P+mH, L↦mH−L, Λ↦−Λ
Λ = 2L−mH.

Coordinate permutations commute with the uniform V₄ action, yielding the direct product.


12 · Theorem

Collision Presentation Closure

Theorem 26.5. The H(H−1) primitive collision quadrics form a Gröbner basis. Their initial ideal is X²+Y², the quotient has Hilbert series ((1+(H−1)t)²)/(1−t)², is Cohen–Macaulay and Koszul of Krull dimension 2 and projective dimension 2H−2, and its Betti polynomial is the square of the one-sign Eagon–Northcott polynomial.

Each sign family is exactly the 2×2-minor ideal of a 2×H Hankel matrix with shared endpoints z and h. The Top-KPQ unique-terminal theorem supplies the normal-form interpretation: an irreducible monomial contains at most one positive interior variable and at most one negative interior variable. Thus the standard monomials are z^a h^b times 1, x_i, y_j, or x_i y_j.

in(I_H)= (x₁,…,x_{H−1})² + (y₁,…,y_{H−1})²
Hilb(t)=((1+(H−1)t)²)/(1−t)²
N_m=H[H(m−1)+2]

For one sign, the Eagon–Northcott quotient Betti numbers are β_i=i·C(H,i+1) with shift i+1. The positive and negative resolutions tensor over the shared free base k[z,h], so the full Betti polynomial factors as B_H(u,t)².

13 · Open Register

What Remains Open

ItemStatus
Top-KPQ completenessPROVEN — closed
Dense Z₂₅₆ collision ramification length 576PROVEN — closed at the dense diagonal localization
Unoriented P∈{0,H} sheet swap / Δ_T quotientPROVEN — Theorem 26.3
Metric-affine S_m × V₄ Q-space symmetryPROVEN — Theorem 26.4
Gröbner basis, Hilbert series and Betti factorizationPROVEN — Theorem 26.5
Associated graded layer structure gr_𝔭Open
CXR structural law behind 252=4·7·9 and 576=4·9·16Observation; not yet a theorem

14 · Provenance

Frozen Research Record

Preprint drafts derived from this chapter:

The collision theorem and audits were first frozen in the SILIQ/MPRC math ledger and verifier code before this booklet chapter was created. This chapter preserves the mathematical statement and its scope; it does not turn unaudited adjacent claims into consequences.