Quantum Chaos

Why quantum systems inherit chaos from phase transport non-closure, not randomness

Claim: Quantum chaos arises when phase transport fails to close under classically chaotic frame evolution.

The Apparent Paradox

Yet quantum systems exhibit spectral statistics indistinguishable from chaos.

Standard Responses (Symptoms, Not Cause)

These describe outcomes, not mechanism.

Transport Reinterpretation

Quantum mechanics is phase transport.

Classical chaos moves the transport frame beneath the phase.

When frames fail to close, phase coherence fragments.

Path A — Semiclassical Transport Geometry

Primitive: Phase accumulated along transported paths

Semiclassically, quantum amplitudes sum over paths:

$$ \psi \sim \sum_{\gamma} A_\gamma e^{i S_\gamma/\hbar} $$

In chaotic systems:

Phase cancellation becomes unavoidable.

Path B — Phase Space Mixing

Primitive: Phase distribution under unitary transport

The Wigner function evolves under transport:

$$ \partial_t W = \{H, W\} + O(\hbar^2) $$

Classical chaos stretches and folds phase space.

Quantum resolution limits prevent closure.

Fine-scale phase information is lost.

Agreement Condition

$$ \text{Geometric non-closure of paths} \iff \text{Phase-space decoherence} $$

Why Random Matrix Statistics Appear

Once phase correlations are destroyed, only symmetry constraints remain.

Spectral statistics follow transport-invariant ensembles.

Ehrenfest Time Reinterpreted

The Ehrenfest time marks when transport non-closure exceeds phase resolution:

$$ t_E \sim \frac{1}{\lambda} \log \frac{1}{\hbar} $$

Not a breakdown of quantum mechanics, but of closure.

Connection to Earlier Problems

Transport-First Summary