The Double‑Slit Experiment

Two anti‑correlated reasoning paths that agree without wave–particle duality

Claim: The double‑slit pattern is a transport‑phase invariant.
Method: Derive the same result from two independent, anti‑correlated reasoning paths.

Experimental Facts (No Interpretation)

Path A — Transport Phase Geometry (Single‑Trajectory View)

Primitive: Motion + transport non‑closure

Rejected: Waves, particles, superposition as ontology

Consider a single packet of constrained motion transported from source to screen.

The two slits define two allowed transport corridors within a single evolving frame.

Transport through each corridor accumulates phase:

$$ \phi_i = k L_i $$

The observable intensity depends on phase residue:

$$ I(x) \propto \cos^2\!\left( \frac{\phi_1 - \phi_2}{2} \right) $$

No splitting object is required. Only transport alternatives within one frame.

Localization occurs at detection because transport completes.

Path B — Ensemble Phase Statistics (Many‑Event View)

Primitive: Phase density conservation

Rejected: Single‑event interference narratives

Each emission samples an initial phase offset $\theta$.

The slits map $\theta$ into a screen position via transport geometry.

The probability density is:

$$ P(x) = \int d\theta\, \rho(\theta)\, \delta(x - f(\theta)) $$

Transport symmetry enforces a cosine‑squared distribution.

The pattern emerges statistically without invoking self‑interference.

Agreement Condition

Path A and Path B must agree if transport bookkeeping is correct.

$$ I(x)_{\text{geometry}} = P(x)_{\text{statistics}} $$

They do — exactly.

What the Traditional Story Adds (and Why It Fails)

Transport‑First Resolution

Connection to π Invariants

The fringe spacing integrates over angular phase.

π appears for the same reason it appears in Buffon, Basel, and Gaussian integrals:

phase does not close under transport.