OAI.StrictHotSpots.PlaneGreen.boundarySolution_energy: intermediate lemma from OpenAI, The hot spots conjecture for simply connected planar domains
ProvedOAI.StrictHotSpots.PlaneGreen.boundarySolution_energyAn 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.PlaneGreen.boundarySolution_energy of lean/OAI/Analysis/HotSpots/HotSpots/GreenSolution.lean at commit adc7f12, ported to Lean 4.33.1 and Mathlib 0df444a.
The statement, as published (namespace OAI.StrictHotSpots.PlaneGreen, with open Set MeasureTheory Filter Metric, open scoped Topology ContDiff InnerProductSpace ENNReal NNReal, open DiskH10):
theorem boundarySolution_energy (hT : ‖weightedIntegralOperator hC hν‖ < 1)
(f g : C(Boundary,ℝ)) {A B : ℝ≥0} (hf : LipschitzWith A f) (hg : LipschitzWith B g) :
inner ℝ (H1.grad (boundarySolution hC hν f hf)) (H1.grad (boundarySolution hC hν g hg)) -
inner ℝ (SubcriticalExtension.observe hC hν (boundarySolution hC hν f hf))
(SubcriticalExtension.observe hC hν (boundarySolution hC hν g hg)) =
(1/2:ℝ)*(∫ z : Boundary × Boundary, boundaryInteraction z.1 z.2 *
inner ℝ (f z.1-f z.2) (g z.1-g z.2) ∂boundaryMeasure.prod boundaryMeasure) -
(∫ z : Boundary × Boundary, fullBoundaryR hC hν z.1 z.2 * f z.1 * g z.2
∂boundaryMeasure.prod boundaryMeasure)
Definitions. The statement is written with OAI.StrictHotSpots.H1, OAI.StrictHotSpots.H1Ambient, OAI.StrictHotSpots.DiskH10.disk, OAI.StrictHotSpots.H1.grad and OAI.StrictHotSpots.PlaneGreen.Boundary (definitions bundle OAIQ3Ho000 of this split); OAI.StrictHotSpots.PlaneGreen.boundarySolution and OAI.StrictHotSpots.SubcriticalExtension.observe (definitions bundle OAIQ3Ho002 of this split); OAI.StrictHotSpots.PlaneGreen.boundaryInteraction, OAI.StrictHotSpots.PlaneGreen.boundaryMeasure, OAI.StrictHotSpots.PlaneGreen.fullBoundaryR and OAI.StrictHotSpots.PlaneGreen.weightedIntegralOperator (definitions bundle OAIQ3Ho003 of this split); OAI.StrictHotSpots.Plane (the published bundle Def_HotSpots).
Used by. The proof of OAI.StrictHotSpots.Conformal.ClosedDiskChart.multipliedGradient_coordinate_difference of this split imports it.
import Mathlib import Definitions.Def_HotSpots import Definitions.Def_OAIQ3Ho002 import Definitions.Def_OAIQ3Ho003
section
attribute [-instance] _root_.OAI.StrictHotSpots.N1.completeSpace _root_.OAI.StrictHotSpots.N1.innerProductSpace _root_.OAI.StrictHotSpots.N1.normedAddCommGroup
set_option linter.all false
set_option linter.unusedVariables false
set_option linter.unusedTactic false
set_option linter.unreachableTactic false
namespace OAI
section BoundaryScalarEnergy
noncomputable section
open Set MeasureTheory Filter Metric
open scoped Topology ContDiff InnerProductSpace ENNReal NNReal
namespace StrictHotSpots.PlaneGreen
open DiskH10
variable {ν : Measure Plane} [IsFiniteMeasure ν] {C : ℝ≥0∞}
(hC : C ≠ (∞ : ℝ≥0∞)) (hν : ν ≤ C • volume.restrict disk)
theorem boundarySolution_energy (hT : ‖weightedIntegralOperator hC hν‖ < 1)
(f g : C(Boundary,ℝ)) {A B : ℝ≥0} (hf : LipschitzWith A f) (hg : LipschitzWith B g) :
inner ℝ (H1.grad (boundarySolution hC hν f hf)) (H1.grad (boundarySolution hC hν g hg)) -
inner ℝ (SubcriticalExtension.observe hC hν (boundarySolution hC hν f hf))
(SubcriticalExtension.observe hC hν (boundarySolution hC hν g hg)) =
(1/2:ℝ)*(∫ z : Boundary × Boundary, boundaryInteraction z.1 z.2 *
inner ℝ (f z.1-f z.2) (g z.1-g z.2) ∂boundaryMeasure.prod boundaryMeasure) -
(∫ z : Boundary × Boundary, fullBoundaryR hC hν z.1 z.2 * f z.1 * g z.2
∂boundaryMeasure.prod boundaryMeasure) := by
sorry
end StrictHotSpots.PlaneGreen
end
end BoundaryScalarEnergy
end OAI
end