OAI.StrictHotSpots.Conformal.ClosedDiskChart.scalarSolution_closed_ae: intermediate lemma from OpenAI, The hot spots conjecture for simply connected planar domains
ProvedOAI.StrictHotSpots.Conformal.ClosedDiskChart.scalarSolution_closed_aeAn intermediate lemma of the split of OpenAI's proof of OAI.StrictHotSpots.main_theorem, carved from OpenAI's openai/math development for this platform. The statement and its proof are OpenAI's (OpenAI, The hot spots conjecture for simply connected planar domains, OpenAI Math Release, September 24, 2026, result family 369, github.com/openai/math, Apache License 2.0); in Lean it is the declaration OAI.StrictHotSpots.Conformal.ClosedDiskChart.scalarSolution_closed_ae of lean/OAI/Analysis/HotSpots/HotSpots/ClosedSolution.lean at commit adc7f12, ported to Lean 4.33.1 and Mathlib 0df444a.
The statement, as published (namespace OAI.StrictHotSpots.Conformal.ClosedDiskChart, with open Set MeasureTheory Filter, open scoped ContDiff InnerProductSpace ENNReal NNReal Topology, open DiskH10 PlaneGreen Hodge):
lemma scalarSolution_closed_ae {w : Plane → ℝ} (hw : ContDiffOn ℝ ∞ w (closure Ω))
{M : ℝ} (hM : ∀ s : Boundary, ‖w (c.F s)‖ ≤ M) :
let _ : IsFiniteMeasure c.potential := c.potential_finite hΩ.2.2.1
(H1.value (c.scalarSolution hΩ.2.2.1 hΩ.2.2.2.2 hμ hw) : Plane → ℝ)
=ᵐ[volume.restrict Ω]
(boundaryClosedSolution c.densityBound_ne_top (c.density_bound hμ.le)
(c.datumTrace w hw.continuousOn) hM) ∘ c.G
Definitions. The statement is written with OAI.StrictHotSpots.H1, OAI.StrictHotSpots.H1Ambient, OAI.StrictHotSpots.Conformal.ClosedDiskChart, OAI.StrictHotSpots.H1.value, OAI.StrictHotSpots.PlaneGreen.Boundary, OAI.StrictHotSpots.Conformal.ClosedDiskChart.datumTrace, OAI.StrictHotSpots.Conformal.ClosedDiskChart.densityBound, OAI.StrictHotSpots.Conformal.ClosedDiskChart.densityBound_ne_top, OAI.StrictHotSpots.Conformal.ClosedDiskChart.density_bound and OAI.StrictHotSpots.Conformal.ClosedDiskChart.potential (definitions bundle OAIQ3Ho000 of this split); OAI.StrictHotSpots.PlaneGreen.boundaryClosedSolution (definitions bundle OAIQ3Ho003 of this split); OAI.StrictHotSpots.Conformal.ClosedDiskChart.potential_finite and OAI.StrictHotSpots.Conformal.ClosedDiskChart.scalarSolution (definitions bundle OAIQ3Ho004 of this split); OAI.StrictHotSpots.AdmissibleDomain, OAI.StrictHotSpots.Plane, OAI.StrictHotSpots.SmoothBoundary and OAI.StrictHotSpots.firstPositiveNeumannValue (the published bundle Def_HotSpots).
Used by. The proof of OAI.StrictHotSpots.Conformal.ClosedDiskChart.lipschitzMultipliedGradient_closed of this split imports it.
import Mathlib import Definitions.Def_HotSpots import Definitions.Def_OAIQ3Ho004
section
set_option linter.all false
set_option linter.unusedVariables false
set_option linter.unusedTactic false
set_option linter.unreachableTactic false
namespace OAI
section PhysicalMultiplierClosed
noncomputable section
open Set MeasureTheory Filter
open scoped ContDiff InnerProductSpace ENNReal NNReal Topology
namespace StrictHotSpots.Conformal.ClosedDiskChart
open DiskH10 PlaneGreen Hodge
variable {Ω : Set Plane} (c : ClosedDiskChart Ω) (hΩ : AdmissibleDomain Ω)
variable (hμ : 0 < firstPositiveNeumannValue Ω)
variable {L : ℝ} (hl : firstPositiveNeumannValue Ω < L)
(hD : ∀ j : H10 hΩ.2.1, L*‖H10.value hΩ.2.1 j‖^2 ≤ ‖H10.grad hΩ.2.1 j‖^2)
lemma scalarSolution_closed_ae {w : Plane → ℝ} (hw : ContDiffOn ℝ ∞ w (closure Ω))
{M : ℝ} (hM : ∀ s : Boundary, ‖w (c.F s)‖ ≤ M) :
let _ : IsFiniteMeasure c.potential := c.potential_finite hΩ.2.2.1
(H1.value (c.scalarSolution hΩ.2.2.1 hΩ.2.2.2.2 hμ hw) : Plane → ℝ)
=ᵐ[volume.restrict Ω]
(boundaryClosedSolution c.densityBound_ne_top (c.density_bound hμ.le)
(c.datumTrace w hw.continuousOn) hM) ∘ c.G := by
sorry
end StrictHotSpots.Conformal.ClosedDiskChart
end
end PhysicalMultiplierClosed
end OAI
end