PATH ROTATION: QM AS GEOMETRY

Roof — Speculative Extension

Version 11.2  |  Originally March 5, 2026; nav updated April 6, 2026  |  John Pepin

⚠️ Ongoing research project — SPECULATIVE. Internal consistency is high and numerical results are exact to machine precision, but not destruction-tested. The sigmoid tanh form was predicted by TSO from first principles; whether it holds in a tunable Rydberg experiment is the decisive test (see predictions page).

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The Path Identity Assignment

PathPhysical identityForces actingMetric g
X1Non-locality (entanglement)Suppressed by EM/QCD; accessible at low ΓC+1
X2SuperpositionSuppressed by EM/QCD; accessible at low ΓC+1
x, y, zThree spatial dimensionsBoth EM and gravity; contested+1 each
TTimeGravity only−1
Vacuum / originGravity only0

T and ∅ are gravity-only paths. Wfloor = 2/7 because no EM process can close T or ∅.

The Rotatable Group: SO(5)

{X1, X2, x, y, z} share metric signature g = +1. They can rotate into each other. T (g = −1) and ∅ (g = 0) cannot. The rotation angle θ is set by environmental coupling:

θ = arccos(tanh(Γeff / Γc))

where Γeff is the effective driving and Γc is the aggregate closing tension threshold.

Notation note (April 6, 2026):c" in this equation means the aggregate closing tension Σγc,i — the running sum of all individual closing contributions. This is the same quantity written elsewhere on the site as "ΓC" (uppercase C); the subscript case is cosmetic. This equation is not affected by the April 4 retirement, which only retired a specific numerical frequency value (1.5 × 1015 Hz) and its spurious derivation, not the concept of aggregate Γc. See house page notation section.

High Γc: θ → 0, classical basis locked. Low Γc: θ → π/2, X1 enters the x-slot.

The Double-Slit as Projection

The interference pattern is the shadow of X1 projected onto the x-axis of the detector. When Γc is low, X1 slides into the x-slot. The electron isn't "in two places" — x isn't the active dimension. X1 spans both slit positions simultaneously because non-locality has no preferred location.

The detector (high Γc) forces X1 to project onto x. Result: cos²(πdx/λL) — standard Young's fringes. Which-path measurement is a Γc spike that evicts X1 from the x-slot.

Four QM Postulates Become Geometry

QM postulateTSO originExact?
Born rule P = |α|²cos²(θ) — projection of rotating framesExact (machine-precision)
Complementarity V² + D² ≤ 1sin²θ + cos²θ = 1 — Pythagorean theoremExact
Wave-particle dualityWhether X1 or x is in the windowGeometric
Wavefunction collapseΓc spike forces θ → 0; basis snaps backMechanistic

Important caveat: TSO does not derive the Born rule from scratch. The Born rule follows from Gleason's theorem (1957) and CPn geometry — mathematics that predates TSO. What TSO adds is a geometric mechanism (path rotation + collapse trigger). The probability assignment itself is inherited.

Kincaid 2016 Reanalysis

Modeln=1 R²free n R²best n
TSO sech²0.98240.99991.80
Gaussian0.98860.99971.61
Power-law0.96150.99962.32
Exponential0.91320.99953.22

TSO sech² reaches R² = 0.9999 with a free mapping exponent. Separating from Gaussian requires high-Γc tail data that is not in the Kincaid dataset.

What's Strong, What's Open

Strong

Born rule = cos²(θ) inherited structure is exact to machine precision

Complementarity = Pythagorean identity

T and ∅ as gravity-only paths derived from metric

Resolution C (W ⊥ window) derived from geometry

Open

Path identities are motivated, not proved

SO(5) asserted from metric — group theory needs development

Path-space metric itself is conjectured

Not destruction-tested

Notebooks

Mathematical Consistency Check (14/14)

Interference as Shadow (7/7)

Kincaid 2016 Reanalysis