The Gyron: A State Equation of the Vacuum

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Authors: A. M. Thorn
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Abstract

e²πi⁄5 → φ → s → (W,g,X) → W·X = 𝒬 → Σ Natura This is not a proof but a definition. It fixes a canonical vacuum point GYRON from fifth-root geometry. Admissible states are constrained by the invariant W \cdot X = \mathcal{Q}. PRIMITIVES\[\varphi := \frac{1+\sqrt{5}}{2}, \qquads := \sqrt{3-\varphi} = 2\sin\frac{\pi}{5}, \qquads^2 + \varphi^2 = 4.\] GYRON PARAMETERS\[\begin{aligned}W &:= 2^6 \pi^3 \varphi^2 &&\text{(vacuum weight)}\\g &:= 2^5 \varphi^2 s &&\text{(geometric stiffness)}\\X &:= \frac{1}{2^5 \pi^2 \varphi^4} &&\text{(slip)}\end{aligned}\] DERIVED QUANTITIES\[\mathcal{Q} := \frac{2\pi}{\varphi^2}, \qquadZ := \frac{2s}{\pi\varphi^4} = W \cdot g \cdot X^2, \qquad\Omega := \frac{5}{X} = 5 \cdot 2^5 \pi^2 \varphi^4.\] CONSTRAINTS\[W \cdot X = \mathcal{Q}, \qquad\frac{g}{W} = \frac{s}{2\pi^3}.\] SLIP FACTOR (five-gate survival)\[S := \left(\frac{\Omega}{\Omega+1}\right)^{\!5} = \left(1 + \frac{X}{5}\right)^{\!-5} = 1 - X + \frac{3}{5}X^2 + O(X^3).\] THE QUEEN (fine structure)\[\alpha = \frac{5\sqrt{2\pi}\,S}{W\sqrt{Z}} = \frac{5S}{(8\pi)^2\sqrt{s}}, \qquad\alpha^{-1} = \frac{(8\pi)^2}{5} \cdot \frac{\sqrt{s}}{S}.\] PROJECTION MAP\[\begin{array}{rcl}e^{2\pi i/5} &\to& \varphi\\\varphi &\to& s\\(W,g,X) &\to& W \cdot X = \mathcal{Q}\\A_5 &\to& \mathrm{SU}(3)\times\mathrm{SU}(2)\times\mathrm{U}(1)\\\mathcal{Q} = 2\pi/\varphi^2 &\to& \alpha^{-1} = 6|A_5|/\varphi^2\end{array}\] The vacuum is not empty.It is a counting machine with three gears (W, g, X),one lock ($$W \cdot X = \mathcal{Q}$$), and 240 causal channels.

Publication details

Journal / source
Zenodo (CERN European Organization for Nuclear Research)
Publication date
5 January 2026