OAI.ElasticityDistribution.weak_physical_leading: intermediate lemma from OpenAI, Global Uniqueness for the Smooth Isotropic Elasticity Inverse Problem
ProvedOAI.ElasticityDistribution.weak_physical_leadingAn intermediate lemma of the split of OpenAI's proof of OAI.Elasticity.global_uniqueness, carved from OpenAI's openai/math development for this platform. The statement and its proof are OpenAI's (OpenAI, Global Uniqueness for the Smooth Isotropic Elasticity Inverse Problem, OpenAI Math Release, September 24, 2026, result family 372, github.com/openai/math, Apache License 2.0); in Lean it is the declaration OAI.ElasticityDistribution.weak_physical_leading of lean/OAI/MathematicalPhysics/Elasticity/WeakLimits.lean at commit adc7f12, ported to Lean 4.33.1 and Mathlib 0df444a.
The statement, as published (namespace OAI.ElasticityDistribution, with open MeasureTheory TemperedDistribution Filter Topology, open scoped SchwartzMap InnerProductSpace, open ElasticityAugmented):
theorem weak_physical_leading {U : ℕ → AugHilbert} {W : AugHilbert}
(hU : ∀ v, Tendsto (fun n => inner ℂ (U n) v) atTop (𝓝 (inner ℂ W v)))
(Ω : Set X) (eps : ℕ → ℂ) (heps : Tendsto eps atTop (𝓝 0))
(hne : ∀ n, eps n ≠ 0) (θ : Fin 3 → ℂ) (hθ : ∑ i, θ i*θ i=0)
(lam m : Coeff)
(hR : ∀ n i, LocalEq Ω (rd ((eps n)⁻¹ • θ) lam m
(fun j => (U n j.succ : Dist)) (U n 0 : Dist) i) 0)
(hS : ∀ n, LocalEq Ω (scd ((eps n)⁻¹ • θ) lam m
(fun j => (U n j.succ : Dist)) (U n 0 : Dist)) 0)
(hdiv : ∀ n, LocalEq Ω (divd ((eps n)⁻¹ • θ) (fun j => (U n j.succ : Dist)))
(U n 0 : Dist)) :
(∀ i, LocalEq Ω (leadingRd θ lam m (fun j => (W j.succ : Dist)) (W 0 : Dist) i) 0) ∧
LocalEq Ω (leadingSd θ lam m (fun j => (W j.succ : Dist)) (W 0 : Dist)) 0 ∧
LocalEq Ω (normald θ (fun j => (W j.succ : Dist))) 0
Definitions. The statement is written with OAI.ElasticityAugmented.Smooth, OAI.ElasticityAugmented.X, OAI.ElasticityDistribution.Coeff, OAI.ElasticityDistribution.Dist and OAI.ElasticityDistribution.X (definitions bundle OAIQ6El000 of this split); OAI.ElasticityDistribution.AugHilbert, OAI.ElasticityDistribution.LocalEq, OAI.ElasticityDistribution.divd, OAI.ElasticityDistribution.rd and OAI.ElasticityDistribution.scd (definitions bundle OAIQ6El004 of this split); OAI.ElasticityDistribution.normald (definitions bundle OAIQ6El005 of this split); OAI.ElasticityDistribution.leadingRd and OAI.ElasticityDistribution.leadingSd (definitions bundle OAIQ6El006 of this split).
Used by. The proofs of OAI.ElasticityDistribution.actual_transferred_limit and OAI_ElasticityDistribution_bounded_physical_limit of this split import it.
import Mathlib import Definitions.Def_OAIQ6El006
section
set_option linter.all false
set_option linter.unusedVariables false
set_option linter.unusedTactic false
set_option linter.unreachableTactic false
namespace OAI
noncomputable section
namespace ElasticityDistribution
open MeasureTheory TemperedDistribution Filter Topology
open scoped SchwartzMap InnerProductSpace
open ElasticityAugmented
theorem weak_physical_leading {U : ℕ → AugHilbert} {W : AugHilbert}
(hU : ∀ v, Tendsto (fun n => inner ℂ (U n) v) atTop (𝓝 (inner ℂ W v)))
(Ω : Set X) (eps : ℕ → ℂ) (heps : Tendsto eps atTop (𝓝 0))
(hne : ∀ n, eps n ≠ 0) (θ : Fin 3 → ℂ) (hθ : ∑ i, θ i*θ i=0)
(lam m : Coeff)
(hR : ∀ n i, LocalEq Ω (rd ((eps n)⁻¹ • θ) lam m
(fun j => (U n j.succ : Dist)) (U n 0 : Dist) i) 0)
(hS : ∀ n, LocalEq Ω (scd ((eps n)⁻¹ • θ) lam m
(fun j => (U n j.succ : Dist)) (U n 0 : Dist)) 0)
(hdiv : ∀ n, LocalEq Ω (divd ((eps n)⁻¹ • θ) (fun j => (U n j.succ : Dist)))
(U n 0 : Dist)) :
(∀ i, LocalEq Ω (leadingRd θ lam m (fun j => (W j.succ : Dist)) (W 0 : Dist) i) 0) ∧
LocalEq Ω (leadingSd θ lam m (fun j => (W j.succ : Dist)) (W 0 : Dist)) 0 ∧
LocalEq Ω (normald θ (fun j => (W j.succ : Dist))) 0 := by
sorry
end ElasticityDistribution
end
end OAI
end