SilverSight/formal/CoreFormalism/BraidStateN.lean
allaun 48ee7f7fdb fix(c,octave): C stack overflow test fuel, Octave instance methods
C: stack_overflow test now uses AVM_MAX_STACK+10 fuel
Octave: test creates AVM() instance and calls methods on it
2026-06-30 18:26:10 -05:00

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/-
Copyright (c) 2026 SilverSight Contributors. All rights reserved.
Released under Apache 2.0 license.
Generic n-strand braid state, crossStep, and receipt encoding.
Unlike BraidEigensolid.lean (which fixes n=8), this version is
parameterized by strand count (n : Nat).
The crossing pattern is adjacent pairing: (0,1), (2,3), ..., (n-2, n-1).
If n is odd, the last strand (n-1) does not participate in crossing.
-/
import CoreFormalism.BraidCross
import CoreFormalism.BraidStrand
import CoreFormalism.BraidBracket
namespace SilverSight.BraidStateN
open SilverSight.BraidCross
open SilverSight.BraidStrand
open SilverSight.BraidBracket
open SilverSight.FixedPoint.Q16_16
-- ── n-strand receipt ───────────────────────────────────────────────────
structure BraidReceiptN (n : Nat) where
crossing_matrix : BraidBracket
sidon_slack : UInt32
step_count : Nat
residuals : List Q16_16
write_time : UInt64
scar_absent : Bool
deriving Repr, DecidableEq, BEq
-- ── n-strand braid state ───────────────────────────────────────────────
structure BraidStateN (n : Nat) where
strands : Fin n → BraidStrand
step_count : Nat
deriving Repr
-- ── Cross partner (adjacent pairing) ───────────────────────────────────
def crossPartner {n : Nat} (i : Fin n) : Fin n :=
let iv := i.val
if h : iv % 2 = 0 then
if h' : iv + 1 < n then ⟨iv + 1, h'⟩
else i
else
have hpos : iv > 0 := by
by_contra! hle
have hzero : iv = 0 := Nat.le_antisymm hle (Nat.zero_le iv)
have hmod : iv % 2 = 0 := by
simpa [hzero]
exact h hmod
have h_one : 0 < 1 := by norm_num
have hsub1 : iv - 1 < iv := Nat.sub_lt hpos h_one
have hsub : iv - 1 < n := Nat.lt_trans hsub1 i.2
⟨iv - 1, hsub⟩
lemma crossPartner_involutive {n : Nat} (i : Fin n) (hEven : n % 2 = 0) :
crossPartner (crossPartner i) = i := by
apply Fin.ext
have hpar := Nat.mod_two_eq_zero_or_one i.val
rcases hpar with (h_even | h_odd)
· -- i.val is even
have h_add_lt : i.val + 1 < n := by
by_contra! hge
have h_n_odd : (n - 1) % 2 = 1 := by
-- n is even (hEven), so n-1 is odd
omega
have h_even_val : i.val % 2 = 0 := h_even
-- i.val is even AND i.val ≥ n-1 (since ¬(i.val+1 < n) means i.val+1 ≥ n → i.val ≥ n-1)
-- But i.val < n, so i.val = n-1
-- Then i.val is even but n-1 is odd → contradiction
omega
have h_new_odd : (i.val + 1) % 2 = 1 := by omega
have h_sub_lt : i.val + 1 - 1 < n := by
have : i.val + 1 - 1 = i.val := by omega
rw [this]
exact i.2
simp [crossPartner, h_even, h_add_lt, h_new_odd, h_sub_lt]
· -- i.val is odd
have h_pos : i.val > 0 := by
by_contra! hle
have : i.val = 0 := by omega
omega
have h_sub_lt : i.val - 1 < n :=
Nat.lt_trans (Nat.sub_lt h_pos (by norm_num : 0 < 1)) i.2
have h_sub_even : (i.val - 1) % 2 = 0 := by
-- i.val is odd → (i.val - 1) is even
have h_odd_val : i.val % 2 = 1 := h_odd
omega
have h_add_lt : (i.val - 1) + 1 < n := by
have : (i.val - 1) + 1 = i.val := by omega
rw [this]
exact i.2
simp [crossPartner, h_odd, h_pos, h_sub_lt, h_sub_even, h_add_lt,
show (i.val - 1) + 1 - 1 = i.val - 1 by omega]
omega
-- ── Cross step ─────────────────────────────────────────────────────────
def crossStep {n : Nat} (s : BraidStateN n) : BraidStateN n :=
let cross2 (i j : Fin n) : BraidStrand :=
(braidCross (s.strands i) (s.strands j)).1
let newStrands : Fin n → BraidStrand := fun k =>
let kv := k.val
if hpar : kv % 2 = 0 then
if h : kv + 1 < n then
cross2 ⟨kv, k.2⟩ ⟨kv + 1, h⟩
else
s.strands k
else
have hpos : kv > 0 := by
by_contra! hle
have hzero : kv = 0 := by
apply Nat.le_antisymm hle
exact Nat.zero_le kv
have hmod : kv % 2 = 0 := by
simpa [hzero]
exact hpar hmod
have hsub : kv - 1 < n :=
have h_one : 0 < 1 := by norm_num
have hsub1 : kv - 1 < kv := Nat.sub_lt hpos h_one
Nat.lt_trans hsub1 k.2
cross2 k ⟨kv - 1, hsub⟩
{ strands := newStrands
, step_count := s.step_count + 1 }
-- ── Receipt encoding ───────────────────────────────────────────────────
def encodeReceipt {n : Nat} (hn : 0 < n) (s : BraidStateN n) : BraidReceiptN n :=
let rs : List Q16_16 :=
(List.range n).map (fun i =>
if h : i < n then (s.strands ⟨i, h⟩).residue
else Q16_16.zero)
let allAdmissible : Bool :=
(List.range n).all (fun i =>
if h : i < n then (s.strands ⟨i, h⟩).bracket.admissible
else true)
{ crossing_matrix := (s.strands ⟨0, hn⟩).bracket
, sidon_slack :=
let lastSlot := (s.strands ⟨n - 1, Nat.sub_lt hn (by norm_num : 0 < 1)⟩).slot
128 - lastSlot
, step_count := s.step_count
, residuals := rs
, write_time := 0
, scar_absent := allAdmissible }
lemma encodeReceipt_residuals_length {n : Nat} (hn : 0 < n) (s : BraidStateN n) :
(encodeReceipt hn s).residuals.length = n := by
simp [encodeReceipt]
lemma encodeReceipt_step_count {n : Nat} (hn : 0 < n) (s : BraidStateN n) :
(encodeReceipt hn s).step_count = s.step_count := by
rfl
-- ── Eigensolid ─────────────────────────────────────────────────────────
def IsEigensolid {n : Nat} (s : BraidStateN n) : Prop :=
∀ i : Fin n, (crossStep s).strands i = s.strands i
theorem eigensolid_convergence {n : Nat} (s : BraidStateN n)
(h_eig : IsEigensolid (crossStep s)) :
∀ i : Fin n, (crossStep (crossStep s)).strands i = (crossStep s).strands i := by
intro i
exact h_eig i
-- ── Rotational Wave — Braid Correspondence (boundary formalization) ───
--
-- Rossby wave: chiral bias → asymmetric drift (handedness asymmetry
-- in strand crossing creates Rossby-like dispersion)
-- Kelvin wave: achiral (symmetric) → eigensolid fixed point
-- (no handedness, non-dispersive, boundary-trapped)
--
-- The outer strands (i=0, n-1) are "coastal boundaries" where the
-- eigensolid converges first, mimicking Kelvin wave trapping.
--
-- BOUNDARY STATUS: `rossby_convergence_bound` is proven (step-count part).
-- `rossby_energy_dissipation_rate` is the open boundary — it is proven
-- as `True` but needs a substantive Q16_16 energy lemma to complete.
-- `kelvin_wave_eigensolid` is definitionally true.
section RotationalWaveCorrespondence
/--
A chiral label for each strand, encoding handedness bias.
Analogous to the planetary vorticity gradient β in Rossby wave theory.
-/
inductive ChiralLabel
| achiral_stable
| chiral_scarred
| left_handed_mass_bias
| right_handed_vector_bias
deriving Repr, DecidableEq
/--
Rossby drift: the net chiral asymmetry across all strands.
Non-zero → Rossby wave regime (dispersive, drift toward eigensolid).
Zero → Kelvin wave regime (non-dispersive, boundary-trapped).
-/
structure RossbyDrift where
asymmetry : Q16_16
isActive : Bool
deriving Repr
/--
Collapse a per-strand chirality distribution into a single Rossby drift value.
Positive asymmetry = left-handed bias; negative = right-handed bias; zero = achiral.
-/
def rossbyDriftFromChirality (chiralLabels : Fin n → ChiralLabel) : RossbyDrift :=
-- Sum across all strand indices: left=+1, right=-1, scarred=±0.5, achiral=0
let contributions : List Q16_16 :=
(List.finRange n).map (λ i =>
match chiralLabels i with
| ChiralLabel.left_handed_mass_bias => Q16_16.one
| ChiralLabel.right_handed_vector_bias => -Q16_16.one
| ChiralLabel.chiral_scarred => Q16_16.ofRawInt 32768 -- 0.5 in Q16_16
| ChiralLabel.achiral_stable => Q16_16.zero)
let sum := contributions.foldl Q16_16.add Q16_16.zero
{ asymmetry := sum
, isActive := sum ≠ Q16_16.zero }
/--
True when the chiral distribution is perfectly balanced (Kelvin regime).
-/
def isAchiral (chiralLabels : Fin n → ChiralLabel) : Prop :=
rossbyDriftFromChirality chiralLabels = { asymmetry := Q16_16.zero, isActive := false }
variable {n : Nat}
/--
Rossby convergence bound: crossStep strictly increases the step count,
bounding convergence from below.
The non-trivial chirality-dependent part (that crossing energy decreases
faster under Rossby drift) requires Q16_16 sum-inequality lemmas and is
deferred to the TODO below. The step-count part is definitional.
-/
theorem rossby_convergence_bound (s : BraidStateN n) (h_pos : 0 < n)
(h_rossby : ¬ isAchiral (λ (i : Fin n) => ChiralLabel.achiral_stable)) :
(crossStep s).step_count > s.step_count := by
-- crossStep always increments step_count by 1 (definitional)
have h_inc : (crossStep s).step_count = s.step_count + 1 := rfl
omega
/--
TODO(RotationalWave): under non-zero chiral asymmetry (Rossby regime),
the weighted crossing-action decreases faster than in the achiral
(Kelvin) regime. Proving this requires:
1. A Q16_16 measure of "crossing energy" that depends on chirality
2. A lemma that this measure strictly decreases under crossStep
3. A comparison bound showing the decrease is faster when
rossbyDriftFromChirality is active
Until then, `rossby_convergence_bound` above provides only the
trivial step-count guarantee.
-/
theorem rossby_energy_dissipation_rate (s : BraidStateN n) (h_pos : 0 < n)
(h_rossby : ¬ isAchiral (λ (i : Fin n) => ChiralLabel.achiral_stable)) :
True := by
trivial
/--
Kelvin wave eigensolid: an achiral braid converges to a symmetric
crossing matrix fixed point — no drift, boundary-trapped eigensolid.
This is definitionally true: `IsEigensolid` already asserts that
crossStep is idempotent on all strands.
-/
theorem kelvin_wave_eigensolid (s : BraidStateN n) (h_pos : 0 < n)
(h_achiral : isAchiral (λ (i : Fin n) => ChiralLabel.achiral_stable))
(h_convergent : IsEigensolid (crossStep s)) :
IsEigensolid (crossStep s) :=
h_convergent
end RotationalWaveCorrespondence
-- ── n=8 specialization ─────────────────────────────────────────────────
abbrev BraidState8 : Type := BraidStateN 8
def crossStep8 : BraidState8 → BraidState8 := crossStep
def encodeReceipt8 (s : BraidState8) : BraidReceiptN 8 := encodeReceipt (by norm_num) s
def IsEigensolid8 (s : BraidState8) : Prop := IsEigensolid s
end SilverSight.BraidStateN