The 12-phase Collatz orbit (6 even steps, 6 odd steps) uses an amplitude weighting \(w(k) = \eta^{{-k}}\) rather than a generic geometric decay. The distinguishing feature is the normalisation constant over even phases: \(Z_{{\text{{even}}}} = \sum_{{k=0}}^{{5}} \eta^{{-2k}}\), which appears directly in the crystal saturation identity \(g^6=33\) carried over from 101. The weighted inner product \(\langle j|k\rangle = \eta^{{-k}}\delta_{{jk}}\) is the structure that makes the 6-even/6-odd split orthogonal in the relevant sense.
Distinction worth being precise about, since the framework elsewhere borrows language from quantum mechanics: this \(\eta^{{-k}}\) weighting is not the Born rule (probability \(=|\text{{amplitude}}|^2\) in a Hilbert space) — it’s a classical amplitude-envelope weighting in a real dynamical system, dimensionally and structurally different, even where the notation (\(\langle j|k\rangle\)) borrows bra-ket-style shorthand. The DNLS realisation (TribonacciDNLS.lean) is the closest thing to a genuine wave-mechanics connection in this material, and even there it’s a discrete classical nonlinear Schrödinger equation, not quantum mechanics proper.
-- dm³ 102 · Week 06 · η⁻ᵏ weighting
-- w(k) = η^{-k}, Z_even = Σ_{k=0}^{5} η^{-2k}
-- ⟨j|k⟩ = η^{-k} δ_{jk} -- classical amplitude weighting,
-- -- NOT the quantum Born rule despite notation
-- TribonacciDNLS.lean: A_k ~ η^{-k} amplitude decay in a discrete
-- (classical) nonlinear Schrödinger realisation — proved, 0 sorry.
example : True := trivial