The Triangle: A Shape of the Vacuum

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Authors: A. M. Thorn
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Abstract

This document specifies the structure of the vacuum and defines it as an interface whose resting geometry is a right triangle with sides \[(s,\varphi,2)\] satisfying \[s^{2}+\varphi^{2}=4.\] $$ \huge {s^2 + \varphi^2 = (3-\varphi) + (\varphi+1) = 4} $$ The constants \(\varphi\) and \(s\) are fixed geometric parameters. They determine the canonical point of the gyron state space. Using these parameters, the vacuum coordinates are defined as \[W := 2^{6}\pi^{3}\varphi^{2}, \qquadg := 2^{5}\varphi^{2}s,\] \[X := \frac{1}{2^{5}\pi^{2}\varphi^{4}}, \qquadZ := \frac{2s}{\pi\varphi^{4}}.\] Here: - \(W\) is the normal weight of the interface, - \(g\) is the tangent rate, - \(X\) is the interface slip, - \(Z\) is the geometric impedance. These coordinates satisfy the invariant \[W X = q = \frac{2\pi}{\varphi^{2}}.\] The interface slip factor is defined by \[S = 1 - X + \frac{3}{5}X^{2}.\] From this structure arise the constants \[\alpha,\qquad \tilde{G},\qquad \theta_{W}.\] The fine‑structure constant is \[\huge\alpha = \frac{5\sqrt{2\pi}\,S}{W\sqrt{Z}}\] The gravitational constant is \[\tilde{G}= \frac{\alpha^{20}}{(33/32)^{2}g}= \frac{5^{20}(2\pi)^{10}S^{20}}{(33/32)^{2}\,g\,W^{20}Z^{10}}.\] The electroweak mixing angle is \[\sin^{2}\theta_{W} = \frac{3}{13} + X.\] This is a specification of the vacuum’s shape. A triangle at rest. A point of order. A place where the constants begin. $$ \huge z = \sqrt{3-\varphi} + i\varphi $$

Publication details

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