/- BraidBracket.lean - Bracket Shell for Braid Strand Admissibility Brackets bound the flow. Each braid strand carries a bracket shell that encodes local admissibility geometry. Key rule: merge in linear space first, derive bracket afterward. -/ import CoreFormalism.DynamicCanal open SilverSight.FixedPoint.Q16_16 set_option linter.dupNamespace false namespace SilverSight.BraidBracket open DynamicCanal /-- PhaseVec: ℝ² accumulator for AMMR (Q16.16 fixed-point) -/ structure PhaseVec where x : Q16_16 y : Q16_16 deriving Repr, DecidableEq, BEq namespace PhaseVec def zero : PhaseVec := { x := Q16_16.zero, y := Q16_16.zero } def add (p q : PhaseVec) : PhaseVec := if p.x.val == 0 && p.y.val == 0 then q else if q.x.val == 0 && q.y.val == 0 then p else { x := Q16_16.add p.x q.x, y := Q16_16.add p.y q.y } def neg (p : PhaseVec) : PhaseVec := { x := Q16_16.neg p.x, y := Q16_16.neg p.y } def scale (s : Q16_16) (p : PhaseVec) : PhaseVec := { x := Q16_16.mul s p.x, y := Q16_16.mul s p.y } def isZero (p : PhaseVec) : Bool := p.x.val == 0 && p.y.val == 0 /-- Octagonal norm approximation: κ ≈ max(|x|,|y|) + (3/8)·min(|x|,|y|) -/ def normApprox (p : PhaseVec) : Q16_16 := let ax := if p.x.val < 0 then p.x else Q16_16.neg p.x let ay := if p.y.val < 0 then p.y else Q16_16.neg p.y let hi := if ax.val > ay.val then ax else ay let lo := if ax.val > ay.val then ay else ax -- 3/8 = 0x00006000 in Q16.16 let lo38 : Q16_16 := Q16_16.ofRawInt ((lo.val.toNat * 0x6000 / 0x10000) : Int) Q16_16.add hi lo38 end PhaseVec /-- BraidBracket: local admissibility geometry shell C(z, μ) where z is phase accumulation and μ is the slot/transport parameter. The bracket bounds the strand's accumulated state. -/ structure BraidBracket where lower : Q16_16 upper : Q16_16 gap : Q16_16 kappa : Q16_16 phi : Q16_16 admissible : Bool deriving Repr, DecidableEq, BEq namespace BraidBracket /-- Zero bracket (initial state) -/ def zero : BraidBracket := { lower := Q16_16.zero , upper := Q16_16.zero , gap := Q16_16.zero , kappa := Q16_16.zero , phi := Q16_16.zero , admissible := true } /-- Compute bracket from PhaseVec accumulator and slot parameter μ C(z, μ): derive lower, upper, gap from accumulated phase state. This is the core bracket calculus operator. -/ def fromPhaseVec (z : PhaseVec) (μ : Q16_16) : BraidBracket := let κ := z.normApprox -- φ = 0 when z = (0,0) let ϕ := if z.isZero then Q16_16.zero else -- atan2 approximation placeholder (actual would use Cordic or table) Q16_16.ofRawInt 0x00008000 -- π/4 placeholder let lo := Q16_16.sub κ μ let up := Q16_16.add κ μ let g := Q16_16.sub up lo { lower := lo , upper := up , gap := g , kappa := κ , phi := ϕ , admissible := lo.val <= up.val } /-- Check gap conservation (bracketed DIAT property) -/ def gapConserved (b : BraidBracket) : Bool := let expectedGap := Q16_16.sub b.upper b.lower b.gap.val == expectedGap.val /-- Componentwise addition of bracket bounds (for residual calculation) -/ def addComponentwise (x y : BraidBracket) : BraidBracket := { lower := Q16_16.add x.lower y.lower , upper := Q16_16.add x.upper y.upper , gap := Q16_16.add x.gap y.gap , kappa := Q16_16.add x.kappa y.kappa , phi := Q16_16.add x.phi y.phi , admissible := x.admissible && y.admissible } /-- Crossing residual: Rᵢⱼ = Bᵢⱼ - (Bᵢ + Bⱼ) Measures the interaction energy between two merged strands. -/ def crossingResidual (bij bi bj : BraidBracket) : BraidBracket := let sum := addComponentwise bi bj { lower := Q16_16.sub bij.lower sum.lower , upper := Q16_16.sub bij.upper sum.upper , gap := Q16_16.sub bij.gap sum.gap , kappa := Q16_16.sub bij.kappa sum.kappa , phi := Q16_16.sub bij.phi sum.phi , admissible := bij.admissible && bi.admissible && bj.admissible } end BraidBracket /-- AVMR (Append-Only Vector Magnitude Registry) hierarchy entry Stores the immutable history of braid operations for audit/attestation. -/ structure AVMREntry where slot : UInt32 phaseAcc : PhaseVec bracket : BraidBracket residual : Option BraidBracket -- Some if from crossing, None if leaf timestamp : UInt64 deriving Repr, DecidableEq, BEq namespace AVMREntry def leafEntry (slot : UInt32) (z : PhaseVec) (μ : Q16_16) (ts : UInt64) : AVMREntry := { slot := slot , phaseAcc := z , bracket := BraidBracket.fromPhaseVec z μ , residual := none , timestamp := ts } def crossingEntry (slot : UInt32) (z : PhaseVec) (μ : Q16_16) (res : BraidBracket) (ts : UInt64) : AVMREntry := { slot := slot , phaseAcc := z , bracket := BraidBracket.fromPhaseVec z μ , residual := some res , timestamp := ts } end AVMREntry #eval (PhaseVec.zero).normApprox.val #eval (BraidBracket.zero).admissible /-- Row 80: Cosine Similarity between two PhaseVec accumulators cos(θ) = (a·b) / (|a| · |b|) — using octagonal norm approximation -/ def cosineSimilarity (a b : PhaseVec) : Q16_16 := let dot := Q16_16.add (Q16_16.mul a.x b.x) (Q16_16.mul a.y b.y) let normA := a.normApprox let normB := b.normApprox let denom := Q16_16.mul normA normB if denom.val == 0 then Q16_16.zero else Q16_16.div dot denom /-- Row 81: Gradient Alignment — cosine of angle between gradient vectors alignment = ∇gᵢ · ∇gⱼ / (‖∇gᵢ‖ · ‖∇gⱼ‖) Reuses cosineSimilarity on gradient PhaseVecs. -/ def gradientAlignment (gradI gradJ : PhaseVec) : Q16_16 := cosineSimilarity gradI gradJ /-- Row 82: Phase Accumulation — discrete line integral Σ y · dx phase += Σ y · dx along trajectory Inputs: parallel arrays of (y, dx) samples. -/ def phaseAccumulation (ys dxs : Array Q16_16) : Q16_16 := let n := Nat.min ys.size dxs.size (Array.range n).foldl (fun (acc : Q16_16) (i : Nat) => Q16_16.add acc (Q16_16.mul ys[i]! dxs[i]!) ) Q16_16.zero #eval cosineSimilarity { x := Q16_16.ofRawInt 65536, y := Q16_16.zero } { x := Q16_16.ofRawInt 65536, y := Q16_16.zero } -- expect 1.0 end SilverSight.BraidBracket