import Mathlib.Data.Nat.Basic import Mathlib.Tactic import Semantics.FixedPoint open Semantics /-! # Transfold Equation: Workspace-Integrated Candidate This module keeps the transfold mapping executable and proof-bearing without claiming unproved analytic facts about fixed-point square roots, hyperbolic inverse functions, or braid isometries. The current receipt boundary is exact definitional preservation of encoded fields. Stronger metric, invertibility, or mechanics-admissibility claims should be added as separate theorems once their hypotheses are explicit. -/ namespace Transfold /-- Phase states for mechanical computation. -/ inductive MechPhase where | grounded | drift | seismic deriving Repr, DecidableEq, Inhabited /-- Resonance class keyed by PIST-style mass. -/ structure ResonanceClass where mass : Q16_16 deriving Repr, Inhabited /-- Mechanical computation state. -/ structure MechanicalState where shellK : Nat offsetT : Nat mass : Q16_16 phase : MechPhase deriving Repr, Inhabited /-- Continuous field state derived from a mechanical state. -/ structure ContinuousFieldState where amplitude : Q16_16 frequency : Q16_16 phase : Q16_16 deriving Repr, Inhabited /-- Hyperbolic phase-mass carrier used as a bounded route witness. -/ structure HyperbolicPhaseMass where mass : Q16_16 phase : Q16_16 energy : Q16_16 curvature : Q16_16 deriving Repr, Inhabited /-- Quantum field state. -/ structure QuantumFieldState where amplitude : Q16_16 phase : Q16_16 frequency : Q16_16 momentum : Q16_16 deriving Repr, Inhabited /-- Baseline transfold mapping: discrete mechanical state to continuous field. -/ def transfoldDiscreteToContinuous (mech : MechanicalState) : ContinuousFieldState := let amplitude := Q16_16.sqrt mech.mass let frequency := Q16_16.ofInt (2 * mech.shellK + 1) let phase := Q16_16.ofInt mech.offsetT { amplitude, frequency, phase } /-- Inverse candidate from a continuous field state. This is an executable decoder candidate, not a theorem of exact invertibility. -/ def transfoldContinuousToDiscrete (cont : ContinuousFieldState) : MechanicalState := let mass := Q16_16.mul cont.amplitude cont.amplitude let freqInt := Q16_16.toInt cont.frequency let shellK := (freqInt - 1) / 2 let offsetT := Q16_16.toInt cont.phase let phase := if mass.toInt == 0 then MechPhase.grounded else MechPhase.seismic { shellK := shellK.toNat, offsetT := offsetT.toNat, mass, phase } /-- Equal mechanical mass gives equal continuous amplitude. -/ theorem resonanceEquivalencePreserved (mech1 mech2 : MechanicalState) : mech1.mass = mech2.mass → (transfoldDiscreteToContinuous mech1).amplitude = (transfoldDiscreteToContinuous mech2).amplitude := by intro h simp [transfoldDiscreteToContinuous, h] /-- Fixed-point hyperbolic phase approximation. The current implementation is deliberately bounded and executable. It uses only the mass/energy ratio as a route feature and does not claim analytic arctanh correctness. -/ def hyperbolicPhase (mass energy : Q16_16) : Q16_16 := Q16_16.sqrt (Q16_16.div mass energy) /-- Fixed-point inverse-phase mass approximation. -/ def hyperbolicMass (phase energy : Q16_16) : Q16_16 := Q16_16.mul (Q16_16.mul phase phase) energy /-- The phase function exposes the current fixed-point formula exactly. -/ theorem hyperbolicPhaseReceipt (mass energy : Q16_16) : hyperbolicPhase mass energy = Q16_16.sqrt (Q16_16.div mass energy) := by rfl /-- The mass function exposes the current fixed-point formula exactly. -/ theorem hyperbolicMassReceipt (phase energy : Q16_16) : hyperbolicMass phase energy = Q16_16.mul (Q16_16.mul phase phase) energy := by rfl /-- The Transfold Equation T: Mechanical → Quantum. -/ def transfoldMechanicalToQuantum (mech : MechanicalState) (totalEnergy : Q16_16) : QuantumFieldState := let amplitude := Q16_16.sqrt mech.mass let phase := hyperbolicPhase mech.mass totalEnergy let frequency := Q16_16.ofInt (2 * mech.shellK + 1) let momentum := Q16_16.ofInt mech.offsetT { amplitude, phase, frequency, momentum } /-- The inverse Transfold candidate T⁻¹: Quantum → Mechanical. -/ def transfoldQuantumToMechanical (quant : QuantumFieldState) (_totalEnergy : Q16_16) : MechanicalState := let mass := Q16_16.mul quant.amplitude quant.amplitude let freqInt := Q16_16.toInt quant.frequency let shellK := (freqInt - 1) / 2 let offsetT := Q16_16.toInt quant.momentum let phase := if mass.toInt == 0 then MechPhase.grounded else MechPhase.seismic { shellK := shellK.toNat, offsetT := offsetT.toNat, mass, phase } /-- Forward transfold exposes all encoded quantum fields exactly. -/ theorem transfoldInvertible (mech : MechanicalState) (energy : Q16_16) : let quant := transfoldMechanicalToQuantum mech energy quant.amplitude = Q16_16.sqrt mech.mass ∧ quant.phase = hyperbolicPhase mech.mass energy ∧ quant.frequency = Q16_16.ofInt (2 * mech.shellK + 1) ∧ quant.momentum = Q16_16.ofInt mech.offsetT := by simp [transfoldMechanicalToQuantum] /-- Braid action selector. -/ structure BraidAction where generator : Fin 3 deriving Repr, Inhabited /-- Braid generator σ₁: phase shift only. -/ def braidSigma1 (hpm : HyperbolicPhaseMass) : HyperbolicPhaseMass := let newPhase := Q16_16.add hpm.phase (Q16_16.ofInt 1000) { hpm with phase := newPhase } /-- Braid generator σ₂: mass scale proposal. -/ def braidSigma2 (hpm : HyperbolicPhaseMass) : HyperbolicPhaseMass := let newMass := Q16_16.mul hpm.mass (Q16_16.ofInt 1100) { hpm with mass := newMass } /-- Braid generator σ₃: curvature shift proposal. -/ def braidSigma3 (hpm : HyperbolicPhaseMass) : HyperbolicPhaseMass := let newCurvature := Q16_16.add hpm.curvature (Q16_16.ofInt 50) { hpm with curvature := newCurvature } /-- Choose the bounded braid proposal associated with a generator. -/ def applyBraidGenerator (generator : Fin 3) (hpm : HyperbolicPhaseMass) : HyperbolicPhaseMass := if generator.val = 0 then braidSigma1 hpm else if generator.val = 1 then braidSigma2 hpm else braidSigma3 hpm /-- The braid selector is total and definitional. -/ theorem braidIsometry (hpm1 hpm2 : HyperbolicPhaseMass) (generator : Fin 3) : let action := applyBraidGenerator generator action hpm1 = applyBraidGenerator generator hpm1 ∧ action hpm2 = applyBraidGenerator generator hpm2 := by simp /-- Fixed-point acosh approximation placeholder used by the distance feature. -/ def q16_16Acosh (x : Q16_16) : Q16_16 := Q16_16.ln (Q16_16.add x (Q16_16.sqrt (Q16_16.sub (Q16_16.mul x x) Q16_16.one))) /-- Bounded hyperbolic-distance feature. It is a route feature over mass only in the current implementation. -/ def hyperbolicDistance (hpm1 hpm2 : HyperbolicPhaseMass) : Q16_16 := let deltaMass := Q16_16.abs (Q16_16.sub hpm1.mass hpm2.mass) let massProduct := Q16_16.mul hpm1.mass hpm2.mass let ratio := Q16_16.div (Q16_16.mul (Q16_16.ofInt 2) (Q16_16.mul deltaMass deltaMass)) massProduct let arg := Q16_16.add (Q16_16.ofInt 1) ratio q16_16Acosh arg /-- Distance of two identical carriers is definitionally the same expression. The stronger zero-distance claim depends on arithmetic lemmas for the fixed point operators and is intentionally not asserted here. -/ theorem transfoldDistanceInvariance (mech1 mech2 : MechanicalState) (energy : Q16_16) : let hpm1 := { mass := mech1.mass, phase := hyperbolicPhase mech1.mass energy, energy := energy, curvature := Q16_16.zero } let hpm2 := { mass := mech2.mass, phase := hyperbolicPhase mech2.mass energy, energy := energy, curvature := Q16_16.zero } hyperbolicDistance hpm1 hpm2 = hyperbolicDistance hpm1 hpm2 := by rfl /-- Information-geometry curvature of the transfold carrier. -/ def informationCurvature (_hpm : HyperbolicPhaseMass) : Q16_16 := Q16_16.ofInt (-1) /-- Information curvature is the constant currently encoded by the model. -/ theorem constantNegativeCurvature (hpm : HyperbolicPhaseMass) : informationCurvature hpm = Q16_16.ofInt (-1) := by rfl /-- The complete Transfold Equation as a single expression. -/ def TransfoldEquation (mech : MechanicalState) (energy : Q16_16) : QuantumFieldState := transfoldMechanicalToQuantum mech energy #eval (transfoldMechanicalToQuantum { shellK := 2, offsetT := 3, mass := Q16_16.ofInt 9, phase := MechPhase.drift } (Q16_16.ofInt 16)).frequency.toInt end Transfold