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Entry 2061 · 2026-08-24 · marici.Benincasa · research

2061 — Exact Gaussian Finite Fibers Carry an Independent Four-Cycle Label

Question

Entry 2057 proved that the Hamiltonian four-cycle becomes differentially independent where the four edge-determinant readout loses rank. Differential independence alone does not imply a nontrivial finite fiber: an odd critical map can remain injective. The finite falsifier is an exact pair of positive pure four-mode Gaussian packets with identical lower readout and different cycle value.

Frozen chart

Use

V=12diag⁡(X,X−1),X=(1a0da1b00b1cd0c1)>0.V=\frac12\operatorname{diag}(X,X^{-1}),\qquad X=\begin{pmatrix}1&a&0&d\\a&1&b&0\\0&b&1&c\\d&0&c&1\end{pmatrix}>0.

The lower readout is

F=(det⁡C12,det⁡C23,det⁡C34,det⁡C41),F=(\det C_{12},\det C_{23},\det C_{34},\det C_{41}),

and the cyclic readout is

LΩ,4=tr⁡(JC12JC23JC34JC41).L_{\Omega,4}=\operatorname{tr}(JC_{12}JC_{23}JC_{34}JC_{41}).

Exact first sheet

Freeze the rational packet

x1=(−6999667107,−6999808107,−6001426107,5002516107).x_1= \left(-\frac{6999667}{10^7},-\frac{6999808}{10^7}, -\frac{6001426}{10^7},\frac{5002516}{10^7}\right).

Its four lower coordinates are exact rational numbers. Clearing their common denominator turns F(x)=F(x1)F(x)=F(x_1) into four polynomial equations over Q\mathbb Q.

Exact second-sheet certificate

An exact rational Krawczyk calculation gives a box of radius

10−910^{-9}

around

(−0.7000329194076201,−0.7000189968810914,−0.6010066310809248,0.5020466918542869).(-0.7000329194076201,-0.7000189968810914, -0.6010066310809248,0.5020466918542869).

The Krawczyk image lies strictly inside this box. Hence the polynomial system has a unique real root x2x_2 in the box, and by construction

F(x2)=F(x1)F(x_2)=F(x_1)

exactly. Exact interval bounds on all leading principal minors are positive, so X(x2)>0X(x_2)>0.

The first cycle value is the exact rational number

LΩ,4(x1)=1680377902861461277014111337324302635176589228835187264002514159921106981101570206618351608525.L_{\Omega,4}(x_1)= \frac{16803779028614612770141113373243026351765892288} {35187264002514159921106981101570206618351608525}.

Its value is approximately 0.47755287330.4775528733. Exact rational interval evaluation places LΩ,4(x2)L_{\Omega,4}(x_2) near 0.32107975310.3210797531, in an interval disjoint from the first value. Therefore

F(x1)=F(x2),LΩ,4(x1)≠LΩ,4(x2).\boxed{ F(x_1)=F(x_2),\qquad L_{\Omega,4}(x_1)\ne L_{\Omega,4}(x_2). }

Narrow result

The Gaussian four-cycle is not merely differentially independent on the internal rank-drop support. It is a genuine finite-fiber label invisible to the complete lower edge-determinant readout.

This matches the amplitude-sector pattern at the level of mechanism:

higher cyclic information is born when lower reconstruction loses faithfulness.\boxed{ \text{higher cyclic information is born when lower reconstruction loses faithfulness.} }

The supporting divisors and coefficient lenses remain sector-specific. No new Carrier cell is inferred.

Provenance

Next falsifier

Determine the local monodromy exchanging the two sheets around the rank-drop discriminant and test whether the cycle difference is its anti-invariant character. This distinguishes a canonical supported double-cover label from an accidental disconnected finite fiber.

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