Encyclopedia Quantum Quantum Recognition First Eight Tick Weyl
ARTICLE 3 claims 2 theorems 1 open
Quantum Recognition First Eight Tick Weyl
In quantum mechanics, position and momentum do not commute; Recognition Science derives that fact from an eight-step cycle of recognition events.
The eight-tick Weyl relation
Quantum mechanics traditionally begins with a postulate: the position operator x and the momentum operator p do not commute, and their commutator is [x, p] = iħ, where ħ is the reduced Planck constant. This non-commutativity is the mathematical root of the uncertainty principle. Recognition Science (RS) asks whether this postulate can be derived rather than assumed. The module EightTickWeyl.lean provides a finite, exact derivation on a cycle of eight discrete recognition events, which it calls ticks.
The framework models a recognition event as a discrete record in a ledger. On an eight-tick cycle, two operations are defined. The first, shift, advances the occupation state by one tick. The second, clock, multiplies the state by a phase factor ω, a primitive 8th root of unity, which is exp(2πi/8). The core theorem, eightTick_weyl, proves that these two operations satisfy the Weyl relation: clock ∘ shift = ω · (shift ∘ clock). This means the order of operations matters, and the failure to commute is exactly the phase ω, not a larger structure. The proof is machine-checked in the framework's library of formal theorems, with no additional axioms beyond the standard three.
The significance is that canonical non-commutativity, the heart of quantum mechanics, is not an axiom here. It emerges from the cyclic structure of recognition itself. The theorem canonical_noncommutativity states that there exists a state for which clock and shift do not commute, which is a direct consequence of ω ≠ 1. The continuum limit, where the discrete cycle becomes continuous and the commutator becomes [x, p] = iħ, remains an open target, as does the specific magnitude ħ = φ⁻⁵. What is established is the finite, exact root of non-commutativity.
This result reframes a foundational question. Instead of asking why position and momentum do not commute, RS asks what structure forces that behavior. The answer, within the framework, is that an eight-step cycle of recognition events carries a built-in phase, and that phase is the source of the commutation failure. The module does not claim to have derived the full continuum quantum theory, but it provides a concrete, checkable starting point for that larger project.
THEOREM eightTick_weyl · IndisputableMonolith/Quantum/RecognitionFirst/EightTickWeyl.lean
/-- **The eight-tick Weyl relation.** `clock (shift ψ) = ω • (shift (clock ψ))`,
pointwise. This is the recognition root of the canonical commutator: occupation and
cost-rate do not commute, their failure to commute is exactly the 8-tick phase `ω`. -/
theorem eightTick_weyl (ψ : ZMod 8 → ℂ) (k : ZMod 8) :
clock (shift ψ) k = omega * shift (clock ψ) k := by
have hval : ∀ j : ZMod 8,
j.val = (j - 1).val + 1 ∨ (j.val = 0 ∧ (j - 1).val = 7) := by decide
have e : omega ^ (k.val) = omega ^ ((k - 1).val + 1) := by
rcases hval k with h | ⟨h0, h7⟩
· rw [h]
· rw [h0, h7, pow_zero]; exact omega_pow_eight.symm
simp only [clock, shift]
rw [e]
simp [pow_succ, mul_comm, mul_assoc, mul_left_comm]
THEOREM canonical_noncommutativity · IndisputableMonolith/Quantum/RecognitionFirst/EightTickWeyl.lean
/-- **Canonical non-commutativity emerges.** The clock and shift operators do not
commute. This is the finite, exact RS root of `[x,p] ≠ 0`; the continuum limit (node D3)
turns it into `[x,p] = iℏ`. -/
theorem canonical_noncommutativity :
∃ ψ : ZMod 8 → ℂ, clock (shift ψ) ≠ shift (clock ψ) := by
refine ⟨fun _ => 1, fun h => omega_ne_one ?_⟩
have h1 := congrFun h 1
simp only [clock, shift, mul_one] at h1
rw [show ZMod.val (1 : ZMod 8) = 1 by decide, pow_one,
show ((1 : ZMod 8) - 1).val = 0 by decide, pow_zero] at h1
exact h1
What this page does not claim
The continuum limit [x, p] = iħ is not derived in this module and remains an open problem. The specific value ħ = φ⁻⁵ is not established by this module. The module does not claim that the eight-tick cycle is the only possible source of non-commutativity.
Verify this page
Every tagged claim above names its theorem. To check one yourself rather than trust this page, elaborate the source module with Lean 4 and audit its axiom basis:
$ lake env lean IndisputableMonolith/Quantum/RecognitionFirst/EightTickWeyl.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
A page whose claims cannot be reproduced this way does not ship. In production, every anchor links to the exact declaration in the public source release, and this block carries the build receipt for the page itself.
Derived articles
This page is generated by a question-recursion engine: the questions its answers raise become the next pages. The current agenda, with open targets marked red:
- How does the discrete eight-tick cycle scale up to the continuous commutator [x, p] = iħ?
- What physical interpretation does the phase ω carry in the continuum limit?
- Does the derivation extend to other non-commuting observables beyond position and momentum?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM eightTick_weyl · IndisputableMonolith/Quantum/RecognitionFirst/EightTickWeyl.lean
/-- **The eight-tick Weyl relation.** `clock (shift ψ) = ω • (shift (clock ψ))`, pointwise. This is the recognition root of the canonical commutator: occupation and cost-rate do not commute, their failure to commute is exactly the 8-tick phase `ω`. -/ theorem eightTick_weyl (ψ : ZMod 8 → ℂ) (k : ZMod 8) : clock (shift ψ) k = omega * shift (clock ψ) k := by have hval : ∀ j : ZMod 8, j.val = (j - 1).val + 1 ∨ (j.val = 0 ∧ (j - 1).val = 7) := by decide have e : omega ^ (k.val) = omega ^ ((k - 1).val + 1) := by rcases hval k with h | ⟨h0, h7⟩ · rw [h] · rw [h0, h7, pow_zero]; exact omega_pow_eight.symm simp only [clock, shift] rw [e] simp [pow_succ, mul_comm, mul_assoc, mul_left_comm]The core theorem, eightTick_weyl, proves that these two operations satisfy the Weyl relation: clock ∘ shift = ω · (shift ∘ clock). eightTick_weyl · IndisputableMonolith/Quantum/RecognitionFirst/EightTickWeyl.leanTHEOREM canonical_noncommutativity · IndisputableMonolith/Quantum/RecognitionFirst/EightTickWeyl.lean
/-- **Canonical non-commutativity emerges.** The clock and shift operators do not commute. This is the finite, exact RS root of `[x,p] ≠ 0`; the continuum limit (node D3) turns it into `[x,p] = iℏ`. -/ theorem canonical_noncommutativity : ∃ ψ : ZMod 8 → ℂ, clock (shift ψ) ≠ shift (clock ψ) := by refine ⟨fun _ => 1, fun h => omega_ne_one ?_⟩ have h1 := congrFun h 1 simp only [clock, shift, mul_one] at h1 rw [show ZMod.val (1 : ZMod 8) = 1 by decide, pow_one, show ((1 : ZMod 8) - 1).val = 0 by decide, pow_zero] at h1 exact h1The theorem canonical_noncommutativity states that there exists a state for which clock and shift do not commute, which is a direct consequence of ω ≠ 1. canonical_noncommutativity · IndisputableMonolith/Quantum/RecognitionFirst/EightTickWeyl.lean- OPENThe continuum limit, where the discrete cycle becomes continuous and the commutator becomes [x, p] = iħ, remains an open target.