OAI.ElasticityAugmented.forced_equations_at: intermediate lemma from OpenAI, Global Uniqueness for the Smooth Isotropic Elasticity Inverse Problem
ProvedOAI.ElasticityAugmented.forced_equations_atAn 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.ElasticityAugmented.forced_equations_at of lean/OAI/MathematicalPhysics/Elasticity/ForcedTransport.lean at commit adc7f12, ported to Lean 4.33.1 and Mathlib 0df444a.
The statement, as published (namespace OAI.ElasticityAugmented, with open scoped BigOperators):
lemma forced_equations_at (θ : Fin 3 → ℂ) (k r : Smooth)
(hr : ∀ x,(r : X → ℂ) x≠0) (hk : ∀ x,(k : X → ℂ) x≠0)
(hl : ∀ x,((k+r*r : Smooth) : X → ℂ) x≠0)
(H : Fin 3 → Smooth) (K : Smooth) (a : Fin 3 → Smooth) (b : Smooth) (x : X)
(hp : ∀ i,(direction (A := Smooth) coord θ (changeP r a i) : X → ℂ) x=
θ i*(changeS k r hr a b : X → ℂ) x+(topSource r hr H i : X → ℂ) x)
(hs : (direction (A := Smooth) coord θ (changeS k r hr a b) : X → ℂ) x=
((transportT θ k r hk hl*changeS k r hr a b+
∑ i,transportQ θ k r hr hk hl i*changeP r a i : Smooth) : X → ℂ) x+
(scalarSource k r hr hl H K : X → ℂ) x) :
(∀ i,((leadingR coord θ (k-r*r) (r*r) a b i : Smooth) : X → ℂ) x=(H i : X → ℂ) x) ∧
((leadingS coord θ (k-r*r) (r*r) a b : Smooth) : X → ℂ) x=(K : X → ℂ) x
Definitions. The statement is written with OAI.ElasticityAugmented.Smooth, OAI.ElasticityAugmented.X, OAI.ElasticityAugmented.changeP, OAI.ElasticityAugmented.changeS, OAI.ElasticityAugmented.coord, OAI.ElasticityAugmented.direction, OAI.ElasticityAugmented.leadingR and OAI.ElasticityAugmented.leadingS (definitions bundle OAIQ6El000 of this split); OAI.ElasticityAugmented.scalarSource, OAI.ElasticityAugmented.topSource, OAI.ElasticityAugmented.transportQ and OAI.ElasticityAugmented.transportT (definitions bundle OAIQ6El004 of this split).
Used by. The proof of OAI.ElasticityAugmented.exists_physical_forced_transport of this split imports it.
import Mathlib import Definitions.Def_OAIQ6El004
section
attribute [-instance] _root_.OAI.ElasticityGeneralSlicing.cylinder_temperate
set_option linter.all false
set_option linter.unusedVariables false
set_option linter.unusedTactic false
set_option linter.unreachableTactic false
namespace OAI
section
noncomputable section
open scoped BigOperators
namespace ElasticityAugmented
lemma forced_equations_at (θ : Fin 3 → ℂ) (k r : Smooth)
(hr : ∀ x,(r : X → ℂ) x≠0) (hk : ∀ x,(k : X → ℂ) x≠0)
(hl : ∀ x,((k+r*r : Smooth) : X → ℂ) x≠0)
(H : Fin 3 → Smooth) (K : Smooth) (a : Fin 3 → Smooth) (b : Smooth) (x : X)
(hp : ∀ i,(direction (A := Smooth) coord θ (changeP r a i) : X → ℂ) x=
θ i*(changeS k r hr a b : X → ℂ) x+(topSource r hr H i : X → ℂ) x)
(hs : (direction (A := Smooth) coord θ (changeS k r hr a b) : X → ℂ) x=
((transportT θ k r hk hl*changeS k r hr a b+
∑ i,transportQ θ k r hr hk hl i*changeP r a i : Smooth) : X → ℂ) x+
(scalarSource k r hr hl H K : X → ℂ) x) :
(∀ i,((leadingR coord θ (k-r*r) (r*r) a b i : Smooth) : X → ℂ) x=(H i : X → ℂ) x) ∧
((leadingS coord θ (k-r*r) (r*r) a b : Smooth) : X → ℂ) x=(K : X → ℂ) x := by
sorry
end ElasticityAugmented
end
end
end OAI
end