Plain-English statement
Independently exact-science67 VERIFIED 3da29415011a971a65f749502a625e416213f487. Original C2/two Hessians/positive capped eta produce SAME actual Gamma/T/A/HP0/Inv. Internal I+T positivity yields root commutation; exact A0 restriction is selfadjoint, commutes with Gamma0 and Inv, and A0²+Gamma0²=I. The SAME inverse is selfadjoint. Genuine original-input Test gives K=A0Inv selfadjoint and I+K²=Inv². Rank0/alphaeta1 retained. Two literal private Props are representations, never providers/premises. Sharp B23/LemmaB3 energy/B21/H1/dynamics/main/errors/cost/composition remain open.
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Lean statement
theorem actual_same_root_inverse_commutation
{E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E]
[FiniteDimensional ℝ E] [MeasurableSpace E] [BorelSpace E]
{V : E → ℝ} {α β : ℝ≥0} {η : ℝ}
(hα : 0 < (α : ℝ)) (hαβ : α ≤ β) (hV : ContDiff ℝ 2 V)
(hH : ∀ x v : E,
(α : ℝ)*‖v‖^2 ≤ (fderiv ℝ (fderiv ℝ V) x v) v ∧
(fderiv ℝ (fderiv ℝ V) x v) v ≤ (β : ℝ)*‖v‖^2)
(hη : 0 < η) (hβη : (β : ℝ)*η ≤ 1) : actual_same_root_inverse_commutation_statement (E := E) (V := V) (α := α) (β := β) (η := η) hα hαβ hV hH hη hβη := by
classical
unfold actual_same_root_inverse_commutation_statement
dsimp only
let μ := (volume : Measure E).tilted (fun x => -V x)
let J := (μ.prod (stdGaussian E)).map
(fun p : E × E => (p.1,p.1+Real.sqrt η • p.2))
let ν := J.snd
let mY : MeasurableSpace (E × E) := MeasurableSpace.comap Prod.snd (inferInstance : MeasurableSpace E)
letI : MeasurableSpace (E × E) := Prod.instMeasurableSpace
letI : Fact (mY ≤ (inferInstance : MeasurableSpace (E × E))) := ⟨measurable_snd.comap_le⟩
let HP := lpMeas ℝ ℝ mY 2 J
letI : NormedAddCommGroup HP := HP.normedAddCommGroup
letI : InnerProductSpace ℝ HP := HP.innerProductSpace
let P : Lp ℝ 2 J →L[ℝ] Lp ℝ 2 J :=
HP.subtypeL ∘L condExpL2 ℝ ℝ (μ := J) measurable_snd.comap_le
have hBase := AutoSamplingTheory.ExampleCases.ProximalBPS.AmbientAdjointCorrector.actual_ambient_adjoint_centered_decomposition
(E:=E) (V:=V) (α:=α) (β:=β) (η:=η) hα hαβ hV hH hη hβη
rcases hBase with
⟨hμ,hJ,hν,hRange,hPf,S,hS,hSd,hSc,hSf,hSs,e,he,U,hU,hUi,hUs,
T,hTs,hAll,hAeq,hAs,hAn,hPB,Γ,hΓ,hΓSq,hΓP,hΓPSq,hGram,
q,hqa,hTq,hq,hCenter,hΓPq,hγ,ΓP0,hΓP0,hPos0,hOrder0,hUnit,
Inv,hLeft,hRight,hNormInv,B0,hB0,V0,hVdef,hFactor,hVadj,hVnorm,R,hR,hAmbient,hGlobal⟩
let A : HP →L[ℝ] HP := HP.orthogonalProjectionOnto ∘L U.toContinuousLinearMap ∘L HP.subtypeL
let B : HP →L[ℝ] Lp ℝ 2 J :=
(((1 : Lp ℝ 2 J →L[ℝ] Lp ℝ 2 J)-P)*U.toContinuousLinearMap*P) ∘L HP.subtypeL
let ΓP : HP →L[ℝ] HP := e.conjStarAlgEquiv Γ
let qP : HP := e q
let HP0 := (innerSL ℝ qP).ker
letI : NormedAddCommGroup HP0 := HP0.normedAddCommGroup
letI : InnerProductSpace ℝ HP0 := HP0.innerProductSpace
letI : CompleteSpace HP0 := (innerSL ℝ qP).isClosed_ker.completeSpace_coe
let Hperp := P.ker
letI : NormedAddCommGroup Hperp := Hperp.normedAddCommGroup
letI : InnerProductSpace ℝ Hperp := Hperp.innerProductSpace
letI : CompleteSpace Hperp := P.isClosed_ker.completeSpace_coe
change HP0 →L[ℝ] Hperp at B0 V0
change HP0 →L[ℝ] HP0 at ΓP0 Inv
change Lp ℝ 2 J →L[ℝ] Hperp at R
change (∀ g : Lp ℝ 2 J, (R g : Lp ℝ 2 J)=g-P g) at hR
change (∀ g : Lp ℝ 2 J,
B.adjoint g=HP0.subtypeL (B0.adjoint (R g))) at hAmbient
change (∀ f : Lp ℝ 2 J, (∫ z, f z ∂J)=0 →
∃ fP : HP0,
HP0.subtypeL fP=condExpL2 ℝ ℝ (μ:=J) measurable_snd.comap_le f ∧
let fperp : Hperp := R f
let fV : HP0 := V0.adjoint fperp
B.adjoint (fperp : Lp ℝ 2 J)=HP0.subtypeL (ΓP0 fV) ∧
HP0.subtypeL (ΓP0 fV)=ΓP (HP0.subtypeL fV) ∧
‖f‖^2=‖fP‖^2+‖fperp‖^2 ∧ ‖fV‖≤‖fperp‖) at hGlobal
have hAeqLocal : A=e.conjStarAlgEquiv T := hAeq
have hAsLocal : IsSelfAdjoint A := hAs
have hLeftLocal : Inv*ΓP0=(1 : HP0 →L[ℝ] HP0) := hLeft
have hPosLocal : ΓP0.IsPositive := hPos0
have hDpos : ((1 : Lp ℝ 2 ν →L[ℝ] Lp ℝ 2 ν)+T).IsPositive := by
refine ⟨((IsSelfAdjoint.one (Lp ℝ 2 ν →L[ℝ] Lp ℝ 2 ν)).add hTs).isSymmetric,?_⟩
intro u
change 0 ≤ inner ℝ (u+T u) u
rw [inner_add_left,real_inner_self_eq_norm_sq]
have hn : ‖T u‖≤‖u‖ := (hAll u).1
have hi := (abs_le.mp (abs_real_inner_le_norm (T u) u)).1
nlinarith only [hn,hi,norm_nonneg u]
have hCommSquare : Commute (Γ*Γ) ((1 : Lp ℝ 2 ν →L[ℝ] Lp ℝ 2 ν)+T) := by
rw [hΓSq]
show (1-T*T)*(1+T)=(1+T)*(1-T*T)
noncomm_ring
have hCommRootPlus := AutoSamplingTheory.TechnicalLemmas.Measure.L2RealSquareCommute.positive_square_commutation
ν Γ (1+T) hΓ hDpos hCommSquare
have hCommRoot : Commute Γ T := by
have h := hCommRootPlus.eq
simp only [mul_add,add_mul,mul_one,one_mul] at h
exact add_left_cancel h
have hCommP : Commute ΓP A := by
change ΓP*A=A*ΓP
change (e.conjStarAlgEquiv Γ)*A=A*(e.conjStarAlgEquiv Γ)
rw [hAeqLocal,← map_mul,← map_mul,hCommRoot.eq]
have hAq : A qP=qP := by
rw [hAeqLocal]
change e (T (e.symm (e q)))=e q
rw [e.symm_apply_apply,hTq]
have hAPreserves (u : HP0) : A (u : HP) ∈ HP0 := by
change inner ℝ qP (A (u : HP))=0
calc
inner ℝ qP (A (u : HP))=inner ℝ (A qP) (u : HP) :=
(hAsLocal.isSymmetric qP (u : HP)).symm
_ = inner ℝ qP (u : HP) := by rw [hAq]
_ = 0 := u.property
let A0 : HP0 →L[ℝ] HP0 := (A.comp HP0.subtypeL).codRestrict HP0 hAPreserves
have hA0 (u : HP0) : (A0 u : HP)=A (u : HP) := rfl
have hA0self : IsSelfAdjoint A0 := by
apply ContinuousLinearMap.isSelfAdjoint_iff_isSymmetric.mpr
intro u v
exact hAsLocal.isSymmetric (u : HP) (v : HP)
have hComm0 : Commute A0 ΓP0 := by
apply ContinuousLinearMap.ext
intro u
apply Subtype.ext
change (A0 (ΓP0 u) : HP)=(ΓP0 (A0 u) : HP)
rw [hA0,hΓP0,hΓP0,hA0]
exact congrArg (fun D : HP →L[ℝ] HP => D (u : HP)) hCommP.eq.symm
have hSquare0 : A0*A0+ΓP0*ΓP0=(1 : HP0 →L[ℝ] HP0) := by
apply ContinuousLinearMap.ext
intro u
apply Subtype.ext
change (A0 (A0 u) : HP)+(ΓP0 (ΓP0 u) : HP)=(u : HP)
rw [hA0,hA0,hΓP0,hΓP0]
have h : ΓP (ΓP (u : HP))=(u : HP)-A (A (u : HP)) :=
congrArg (fun D : HP →L[ℝ] HP => D (u : HP)) hΓPSq
rw [h]
abel
have hStarInv : ΓP0*star Inv=(1 : HP0 →L[ℝ] HP0) := by
have h := congrArg (fun D : HP0 →L[ℝ] HP0 => star D) hLeftLocal
simpa only [star_mul,hPosLocal.isSelfAdjoint.star_eq,star_one] using h
have hInvSelf : IsSelfAdjoint Inv := by
change star Inv=Inv
calc
star Inv=(Inv*ΓP0)*star Inv := by rw [hLeft,one_mul]
_ = Inv*(ΓP0*star Inv) := mul_assoc _ _ _
_ = Inv := by rw [hStarInv,mul_one]
have hCommInv : Commute A0 Inv := by
change A0*Inv=Inv*A0
calc
A0*Inv=(Inv*ΓP0)*(A0*Inv) := by rw [hLeft,one_mul]
_ = Inv*((ΓP0*A0)*Inv) := by noncomm_ring
_ = Inv*((A0*ΓP0)*Inv) := by rw [hComm0.eq.symm]
_ = Inv*A0 := by simp only [mul_assoc,hRight,mul_one]
refine ⟨hμ, ?_⟩
refine ⟨hJ, ?_⟩
refine ⟨hν, ?_⟩
refine ⟨hRange, ?_⟩
refine ⟨hPf, ?_⟩
refine ⟨S, ?_⟩
refine ⟨hS, ?_⟩
refine ⟨hSd, ?_⟩
refine ⟨hSc, ?_⟩
refine ⟨hSf, ?_⟩
refine ⟨hSs, ?_⟩
refine ⟨e, ?_⟩
refine ⟨he, ?_⟩
refine ⟨U, ?_⟩
refine ⟨hU, ?_⟩
refine ⟨hUi, ?_⟩
refine ⟨hUs, ?_⟩
refine ⟨T, ?_⟩
refine ⟨hTs, ?_⟩
refine ⟨hAll, ?_⟩
refine ⟨hAeq, ?_⟩
refine ⟨hAs, ?_⟩
refine ⟨hAn, ?_⟩
refine ⟨hPB, ?_⟩
refine ⟨Γ, ?_⟩
refine ⟨hΓ, ?_⟩
refine ⟨hΓSq, ?_⟩
refine ⟨hCommRoot, ?_⟩
refine ⟨hΓP, ?_⟩
refine ⟨hΓPSq, ?_⟩
refine ⟨hCommP, ?_⟩
refine ⟨hGram, ?_⟩
refine ⟨q, ?_⟩
refine ⟨hqa, ?_⟩
refine ⟨hTq, ?_⟩
refine ⟨hq, ?_⟩
refine ⟨hCenter, ?_⟩
refine ⟨hΓPq, ?_⟩
refine ⟨hγ, ?_⟩
refine ⟨ΓP0, ?_⟩
refine ⟨hΓP0, ?_⟩
refine ⟨hPos0, ?_⟩
refine ⟨hOrder0, ?_⟩
refine ⟨hUnit, ?_⟩
refine ⟨Inv, ?_⟩
refine ⟨hLeft, ?_⟩
refine ⟨hRight, ?_⟩
refine ⟨hNormInv, ?_⟩
refine ⟨hInvSelf,A0,hA0,hA0self,hComm0,hSquare0,hCommInv,?_⟩
refine ⟨B0, ?_⟩
refine ⟨hB0, ?_⟩
refine ⟨V0, ?_⟩
refine ⟨hVdef, ?_⟩
refine ⟨hFactor, ?_⟩
refine ⟨hVadj, ?_⟩
refine ⟨hVnorm, ?_⟩
refine ⟨R, ?_⟩
refine ⟨hR, ?_⟩
refine ⟨hAmbient, ?_⟩
exact hGlobal
end
end AutoSamplingTheory.ExampleCases.ProximalBPS.ActualRootCommutation
#print axioms AutoSamplingTheory.ExampleCases.ProximalBPS.ActualRootCommutation.actual_same_root_inverse_commutation
Open AutoSamplingTheory/ExampleCases/ProximalBPS/ActualRootCommutation.lean:115published source at ed709a7f320d
Proof architecture
PBPS real consumer; no SALD admission
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Why the statement has this shape
The declaration is kept at the reusable level recorded by its Registry tags and direct consumers. Explicit measures, spaces, wrappers, and regularity hypotheses expose interfaces that paper notation often infers. A theorem card explains those interfaces but never widens the compiled statement.
Hidden assumptions and non-claims
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- Totalized `fderiv` values must not be read as a differentiability theorem.
- Almost-everywhere hypotheses depend on the stated measure and representative.