import CompleteOS import AFSourceBridge import CommonScaleAudit import TwoPointPhysicalObservable import CompletenessAudit import WardFormulationAudit import LGTWilsonBridge import Construction /-! # Combined acceptance target for the verified scope This statement binds ONE Wilson family C, ONE extracted table S and ONE Final F. The selected scalar OS family, UV trace and translation tensor are fixed by F. The Wilson limit is the unselected table; the phase-average clause relates it to the selected theory without identifying the selected state with the mixture. This is a proposed acceptance specification, not a record of human signoff. IR uniqueness, intrinsic scale setting, two-loop/all-orders matching, SD1--SD4, contact/dilation Ward identities and improvement uniqueness are not clauses. Builds, Comparator and Palomar are external checks, not mathematical fields. -/ set_option autoImplicit false noncomputable section namespace YMReview.Acceptance open YM YM.Table Filter Set MeasureTheory open scoped Topology BigOperators variable {g : YangMills.GaugeGroup} {C : Family g.core} variable {o : Extraction.Order} {S : Table C.book} /-- The actual finite law and common calibration, with full UV then extracted IR. The coupling conversion is beta_lgt = beta_submission / representation dimension. -/ structure LatticeAndScale (C : Family g.core) (o : Extraction.Order) (S : Table C.book) : Prop where makes : C.Makes regular : YangMills.WilsonRegularity (YangMills.wilsonFamily C) finite_law (N p : ℕ) : MeasurePreserving (YMLGTBridge.configEquiv g (C.side N p)) (ymMeasure g.image (g.n+1) 4 (C.side N p).val (C.beta N p / (g.n+1 : ℕ)) Finset.univ) (YangMills.wilsonLaw g (C.side N p) (C.beta N p) g.core.probHaar) finite_moments (N p : ℕ) {n : ℕ} (v : Fin n → C.book.Token) (x : Fin n → Lattice.Site (C.side N p)) : (YangMills.wilsonFamily C).finiteMoment N p v x = C.numeric N p v x ordered : (Extraction.Order.mk Extraction.Sequence.full o.per).Ordered C S public_limit : (YangMills.wilsonFamily C).Converges o.per (fun v x => S.read x v) positions_uv : FullVolume.PositionsUV C Extraction.Sequence.full reference_spacing : C.S.a 0 = 1 physical_side (N p : ℕ) : C.S.a N * (C.side N p).val = (C.S.period p).val common_coupling : ∃ betaRef : ℝ, 0 < betaRef ∧ ∀ N p, C.path.β N p 0 = betaRef shared_kinetic_paths (N p q m : ℕ) (hm : m ≤ N) : (C.path.rep N p m).path = (C.path.rep N q m).path insertion_readout (d N p : ℕ) (hN : C.ref d ≤ N) (v : C.label d) : ((C.factory d N p).entries (C.ref d) ((C.factory d N p).terminal.symm v)).x = v calibrated_reset : ∃ alpha : ℕ → ℕ → ℝ, ∀ N m p, m < N → |C.path.β N p m - C.path.β N p (m+1) - alpha N m| ≤ 1 /-- Exact group OS interface on the selected centered trace, plus the actual integral and the phase-average identification with the lattice-limit table. -/ structure PhaseAndOS (F : Spec.Final C o S) : Prop where phase_probability : IsProbabilityMeasure F.α.space.μ phase_full_support : F.α.space.μ.IsOpenPosMeasure phase_average (w : C.book.Word) (hw : Word.distinct w) : (∫ i, (F.α.ensemble i).expect w ∂F.α.space.μ) = S.expect w os_and_growth : ∃ axioms : OsterwalderSchraderAxioms 3, axioms.S = YMOSBridge.schwinger F ∧ Nonempty (OSArityLinearGrowthCondition 3 axioms) normalized (f : ZeroDiagonalSchwartz 3 0) : YMOSBridge.schwinger F 0 f = f.1 0 centered (f : ZeroDiagonalSchwartz 3 1) : YMOSBridge.schwinger F 1 f = 0 integrable (n : ℕ) (f : ZeroDiagonalSchwartz 3 n) : Integrable (fun x : NPointDomain 3 n => (YMOSBridge.targetKernel F n x : ℂ) * f.1 x) pairing (n : ℕ) (f : ZeroDiagonalSchwartz 3 n) : YMOSBridge.schwinger F n f = ∫ x : NPointDomain 3 n, YMOSBridge.scalarKernel F n (YMOSBridge.configEquiv n x) * f.1 x same_trace : TraceExtension.center F = Trace.traceField F /-- The coefficient and sign are fixed here, not existentially fitted. Every central field and every phase is covered; shell integrability is explicit. -/ structure TranslationWard (F : Spec.Final C o S) : Prop where windows {n : ℕ} (x : Points (n+1)) (hx : x ∈ conf (n+1)) : ∃ χ : E4 → ℝ, Window x χ translation (i : F.α.space.X) {n d : ℕ} {x : Points (n+1)} (hx : x ∈ conf (n+1)) (q : Fin n → S.Tag) {χ : E4 → ℝ} (hχ : Window x χ) (b : Axis) (B : S.Field d) : - ∑ a : Axis, ∫ y : E4, ((Analysis.D (basis a) χ y : ℝ) : ℂ) * S.useAt (F.α.ensemble i) (Points.cons y x) (Fin.cons ⟨4, F.sector.energy a b⟩ (Fin.cons ⟨d, B⟩ q)) = Points.gradient 0 b (fun z => S.useAt (F.α.ensemble i) z (Fin.cons ⟨d, B⟩ q)) x integrable (i : F.α.space.X) {n d : ℕ} {x : Points (n+1)} (hx : x ∈ conf (n+1)) (q : Fin n → S.Tag) {χ : E4 → ℝ} (hχ : Window x χ) (a b : Axis) (B : S.Field d) : Integrable (fun y : E4 => ((Analysis.D (basis a) χ y : ℝ) : ℂ) * S.useAt (F.α.ensemble i) (Points.cons y x) (Fin.cons ⟨4, F.sector.energy a b⟩ (Fin.cons ⟨d, B⟩ q))) window_independent (i : F.α.space.X) {n d : ℕ} {x : Points (n+1)} (hx : x ∈ conf (n+1)) (q : Fin n → S.Tag) {χ ψ : E4 → ℝ} (hχ : Window x χ) (hψ : Window x ψ) (b : Axis) (B : S.Field d) : shellGrad (F.α.ensemble i) F.sector.energy χ b x q B = shellGrad (F.α.ensemble i) F.sector.energy ψ b x q B /-- The accepted registered local content, no additional null fields and dense word domain. This is not an isomorphism to a separately specified canonical QFT. -/ structure OperatorContent (F : Spec.Final C o S) : Prop where raw_exhaustive (p : Labels.Pol g.core) (hp : p ∈ Labels.invariantSpace g.core) : ∃ d : ℕ, ∃ v : Labels.Label g.core d, v.val = p free_no_extra_nulls (d : ℕ) : Maxwell.residual g.core d = ⊥ free_sector (d : ℕ) (p : Maxwell.WickPol g.core) : p ∈ Maxwell.shellSector g.core d ↔ p ∈ Maxwell.Free.lowerCap g.core d ∧ ∀ u : g.core.El, Maxwell.Free.pigment u p = p local_content (d : ℕ) : Nonempty (S.Field d ≃ₗ[ℂ] ↥(Maxwell.shellSector g.core d)) phase_content (i : F.α.space.X) (d : ℕ) : Nonempty ((F.α.ensemble i).Field d ≃ₗ[ℂ] ↥(Maxwell.shellSector g.core d)) dense_words : Dense ((Submodule.span ℂ (Set.range F.action.operators.vector) : Submodule ℂ F.action.operators.H) : Set F.action.operators.H) faithful (p : S.Union) (hp : p ≠ 0) : ∃ f : Boundary.Test4, F.action.operators.field p f ≠ 0 /-- The fixed leading coefficient on the same selected field, in all directions. No two-loop rate, intrinsic Lambda or positive-order matching is asserted. -/ structure LeadingTrace (F : Spec.Final C o S) : Prop where positive : 0 < 3 * (g.core.lieDim : ℝ) / Real.pi ^ 4 leading : Tendsto (fun x : SpaceTime => YMAFBridge.K₂ F x * ‖x‖ ^ 8 * uvLog 1 x ^ 2) (𝓝[≠] 0) (𝓝 (3 * (g.core.lieDim : ℝ) / Real.pi ^ 4)) group_predicate : KernelUVPowerLaw (YMAFBridge.K₂ F) /-- Retain the already proved public and stronger source conclusions on F. These retain their SOURCE status: bundling them is not an independent semantic verification of every reconstruction, OPE, contact or perturbative definition. -/ def SourceConclusions (hg : g.IsSimple) (F : Spec.Final C o S) : Prop := ∃ (L : EveryPhase.Almanac F) (Q : OPE.Orbits.Reader F.sector.derivatives F.sector.turns F.room.kernel.spin) (M : Contacts.Devices F.sector.derivatives) (X : Climb.Scaling S), (YangMills.hierarchy F Q).Properties o.per ∧ (YangMills.hierarchy F Q).Contacts ∧ Independent.Core.{0,0} (YangMills.GaugeGroup.coreSimple hg) F L Q ∧ Nonperturbative.Headline.Reconstruction F L ∧ (∀ i, (YangMills.view (L.actors i)).Axioms) ∧ Nonperturbative.Headline.SeparatedOPE F Q ∧ Nonperturbative.Headline.NestedOPE F Q ∧ Nonperturbative.Headline.TraceExclusions.{0,0} F ∧ M.basis = Q.port ∧ Contacts.Solstice.MultipleLight F M ∧ Nonempty (Contacts.Transport.SystemBasis M) ∧ Nonempty (Contacts.Solstice.Thresholds M) ∧ Pert.FirstExtension F X ∧ Pert.Position.FourMeters F X /-- Proposed combined acceptance at the currently verified scope. There are no fresh per-clause choices of family, phase or trace. -/ structure Accepted (hg : g.IsSimple) (F : Spec.Final C o S) : Prop where lattice : LatticeAndScale C o S phase_os : PhaseAndOS F translation : TranslationWard F operators : OperatorContent F trace_uv : LeadingTrace F positive_lattice_probe : TwoPointScale.MassLimit F source : SourceConclusions hg F /-- Family precedes the requested order; one refinement and one F serve all clauses. The input order's UV subsequence is replaced by the full UV order in the lattice clause, while its IR order is refined as in the submitted result. -/ def CombinedAcceptance (g : YangMills.GaugeGroup) (hg : g.IsSimple) (b : ℝ) : Prop := ∃ C : Family g.core, C.path.levels.clock.kernel.penalty = b ∧ ∀ p : Extraction.Order, ∃ (q : Extraction.Order) (S : Table C.book) (F : Spec.Final C (p.refine q) S), Accepted hg F end YMReview.Acceptance