Plain-English statement
- One actual global PBPS process preserves the Gibbs phase law at each fixed time and satisfies bounded signed momentum-flipped duality.
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Lean statement
theorem actual_bounded_gibbs_duality
{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_bounded_gibbs_duality_statement hα hαβ hV hH hη hβη := by
classical
unfold actual_bounded_gibbs_duality_statement
intro c Φ S rate Λ τ next record P ε history Rec Hist readTime Δ Prefix m zAt K qReal q A eventTime I N liveTime d survival weight C Path Ψ Γ ρ R Vy nu
obtain ⟨Z, hZm, hZa, hZf, hZ0, h105⟩ :=
AutoSamplingTheory.ExampleCases.ProximalBPS.ActualCountableEndpointLaw.actual_countable_endpoint_law
hα hαβ hV hH hη hβη
refine ⟨Z, hZm, hZa, hZf, hZ0, ?_⟩
intro y r T op endpoint
have h103 := AutoSamplingTheory.ExampleCases.ProximalBPS.ActualPhaseNormalization.actual_phase_gibbs_normalization
hα hαβ hV hH hη hβη y
letI : IsProbabilityMeasure (nu y) := by
have hp := h103.2.2.2.2.2.1
rw [h103.2.2.2.2.2.2] at hp
exact hp
letI : IsProbabilityMeasure P :=
AutoSamplingTheory.TechnicalLemmas.Probability.UnitExponentialProduct.unit_exponential_product_laws.1
have hemb : Measurable (fun a : (E × E) × (ℕ → ℝ) => (((y, r), a.1), T, a.2)) :=
(measurable_const.prodMk measurable_fst).prodMk (measurable_const.prodMk measurable_snd)
have he : Measurable endpoint := hZm.comp hemb
let M : (E × E) × (ℕ → ℝ) → (E × E) × (E × E) := fun a => (a.1, endpoint a)
let Q : Measure ((E × E) × (E × E)) := Measure.map M ((nu y).prod P)
let J : (E × E) × (E × E) → (E × E) × (E × E) := fun a => (R a.2, R a.1)
have hM : Measurable M := measurable_fst.prodMk he
have hJ : MeasurePreserving J Q Q := (h105 y r T).2.2
letI : IsProbabilityMeasure Q := (h105 y r T).2.1
have hRm : Measurable R := by dsimp [R]; fun_prop
have hneg : Measure.map (fun p : E => -p) (stdGaussian E) = stdGaussian E := by
simpa using (stdGaussian_map (LinearIsometryEquiv.neg ℝ (E := E)))
have hR : MeasurePreserving R (nu y) (nu y) := by
refine ⟨hRm, ?_⟩
change Measure.map (Prod.map id (fun p : E => -p))
(((volume : Measure E).tilted (fun x => -Vy y x)).prod (stdGaussian E)) = _
rw [← Measure.map_prod_map _ _ measurable_id (by fun_prop), hneg, Measure.map_id]
have hMP : MeasurePreserving M ((nu y).prod P) Q := ⟨hM, rfl⟩
have hfst : MeasurePreserving Prod.fst Q (nu y) := by
refine ⟨measurable_fst, ?_⟩
change Measure.map Prod.fst (Measure.map M ((nu y).prod P)) = nu y
rw [Measure.map_map measurable_fst hM]
change Measure.map Prod.fst ((nu y).prod P) = nu y
simp only [Measure.map_fst_prod, measure_univ, one_smul]
have hinvariant : MeasurePreserving endpoint ((nu y).prod P) (nu y) := by
have h := hR.comp ((hfst.comp hJ).comp hMP)
simpa only [Function.comp_def, M, J, R, neg_neg] using h
refine ⟨hinvariant, ?_⟩
have htest (F G : (E × E) → ℝ) (CF CG : ℝ)
(hF : Measurable F) (hG : Measurable G) (hCF : 0 ≤ CF) (hCG : 0 ≤ CG)
(hFb : ∀ z, |F z| ≤ CF) (hGb : ∀ z, |G z| ≤ CG) :
Integrable (fun z => F z * op G z) (nu y) ∧
(∫ z, F z * op G z ∂nu y) = ∫ a, F a.1 * G a.2 ∂Q := by
let H : (E × E) × (ℕ → ℝ) → ℝ := fun a => F a.1 * G (endpoint a)
have hHm : Measurable H := (hF.comp measurable_fst).mul (hG.comp he)
have hHi : Integrable H ((nu y).prod P) :=
Integrable.of_bound hHm.aestronglyMeasurable (CF * CG)
(Filter.Eventually.of_forall fun a => by
change |F a.1 * G (endpoint a)| ≤ CF * CG
rw [abs_mul]
exact mul_le_mul (hFb a.1) (hGb (endpoint a)) (abs_nonneg _) hCF)
have houter : Integrable (fun z => F z * op G z) (nu y) := by
simpa only [H, endpoint, integral_const_mul] using hHi.integral_prod_left
refine ⟨houter, ?_⟩
have hpair : Measurable (fun a : (E × E) × (E × E) => F a.1 * G a.2) :=
(hF.comp measurable_fst).mul (hG.comp measurable_snd)
calc
(∫ z, F z * op G z ∂nu y) = ∫ a, H a ∂((nu y).prod P) := by
rw [integral_prod H hHi]
simp only [H, endpoint, op, integral_const_mul]
_ = ∫ a, F a.1 * G a.2 ∂Q :=
(integral_map hM.aemeasurable hpair.aestronglyMeasurable).symm
intro F G CF CG hF hG hCF hCG hFb hGb
have hleft := htest F G CF CG hF hG hCF hCG hFb hGb
have hright := htest (fun z => G (R z)) (fun z => F (R z)) CG CF
(hG.comp hRm) (hF.comp hRm) hCG hCF (fun z => hGb (R z)) (fun z => hFb (R z))
refine ⟨hleft.1, hright.1, ?_⟩
rw [hleft.2, hright.2]
have hpair : Measurable (fun a : (E × E) × (E × E) => F a.1 * G a.2) :=
(hF.comp measurable_fst).mul (hG.comp measurable_snd)
calc
(∫ a, F a.1 * G a.2 ∂Q) = ∫ a, F (J a).1 * G (J a).2 ∂Q := by
conv_lhs => rw [← hJ.map_eq]
exact integral_map hJ.measurable.aemeasurable hpair.aestronglyMeasurable
_ = ∫ a, G (R a.1) * F (R a.2) ∂Q := by
apply integral_congr_ae
exact Filter.Eventually.of_forall fun a => mul_comm _ _
#print axioms actual_bounded_gibbs_duality
end
end AutoSamplingTheory.ExampleCases.ProximalBPS.ActualBoundedGibbsDuality
Open AutoSamplingTheory/ExampleCases/ProximalBPS/ActualBoundedGibbsDuality.lean:152published source at ed709a7f320d
Proof architecture
Actual bounded duality and fixed-time invariance; no SALD claim
Lean proof walkthrough
- Read the quantified variables and typeclass brackets as part of the mathematical statement; inferred arguments are not missing assumptions.
- `intro` introduces quantified hypotheses into the local proof context.
- `have` creates a named intermediate mathematical fact.
- `calc` records an equality or inequality chain matching a paper calculation.
- `rw` rewrites by an established identity.
- `simp` normalizes through registered definitional and theorem rewrites.
- `apply` reduces the goal to the hypotheses of a reusable theorem.
- `refine` instantiates a reusable theorem while leaving explicit subgoals.
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
- Measurability is represented explicitly or must be supplied by a dependency.
- Integrability is an input or proved output; a displayed integral alone does not supply it.
- Totalized `fderiv` values must not be read as a differentiability theorem.
- Almost-everywhere hypotheses depend on the stated measure and representative.
- A Gibbs expression is not automatically a probability law or an invariant law.