OAI.StrictHotSpots.Conformal.ClosedDiskChart.subcritical: intermediate lemma from OpenAI, The hot spots conjecture for simply connected planar domains
ProvedOAI.StrictHotSpots.Conformal.ClosedDiskChart.subcriticalAn 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.subcritical of lean/OAI/Analysis/HotSpots/HotSpots/Pullback.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 ENNReal InnerProductSpace, open DiskH10):
theorem subcritical (hb : Bornology.IsBounded Ω) (hne : Ω.Nonempty)
(hμ : 0 < firstPositiveNeumannValue Ω) :
∃ δ : ℝ, 0 < δ ∧ δ < 1 ∧ ∀ v : H10 PlaneGreen.diskOpen,
‖H10.weightedValue PlaneGreen.diskOpen c.densityBound_ne_top (c.density_bound hμ.le) v‖^2 ≤
δ*‖H10.grad PlaneGreen.diskOpen v‖^2
Definitions. The statement is written with OAI.StrictHotSpots.H1, OAI.StrictHotSpots.H10, OAI.StrictHotSpots.H1Ambient, OAI.StrictHotSpots.Conformal.ClosedDiskChart, OAI.StrictHotSpots.DiskH10.disk, OAI.StrictHotSpots.H10.grad, OAI.StrictHotSpots.PlaneGreen.diskOpen, 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.H10.weightedValue (definitions bundle OAIQ3Ho002 of this split); OAI.StrictHotSpots.Plane and OAI.StrictHotSpots.firstPositiveNeumannValue (the published bundle Def_HotSpots).
Used by. The proofs of OAI.StrictHotSpots.Conformal.ClosedDiskChart.gradient_K_representation, OAI.StrictHotSpots.Conformal.ClosedDiskChart.noncritical, OAI.StrictHotSpots.Conformal.ClosedDiskChart.operator_norm_lt_one, OAI.StrictHotSpots.Conformal.ClosedDiskChart.scalarSolution_eq_of_helmholtz and OAI_StrictHotSpots_Conformal_ClosedDiskChart_scalarSolution_form of this split import it.
import Mathlib import Definitions.Def_HotSpots import Definitions.Def_OAIQ3Ho002
section
attribute [-instance] _root_.OAI.StrictHotSpots.N1.innerProductSpace
set_option linter.all false
set_option linter.unusedVariables false
set_option linter.unusedTactic false
set_option linter.unreachableTactic false
namespace OAI
section ActualPotential
noncomputable section
open Set MeasureTheory Filter
open scoped ENNReal InnerProductSpace
namespace StrictHotSpots.Conformal
open DiskH10
namespace ClosedDiskChart
variable {Ω : Set Plane} (c : ClosedDiskChart Ω)
theorem subcritical (hb : Bornology.IsBounded Ω) (hne : Ω.Nonempty)
(hμ : 0 < firstPositiveNeumannValue Ω) :
∃ δ : ℝ, 0 < δ ∧ δ < 1 ∧ ∀ v : H10 PlaneGreen.diskOpen,
‖H10.weightedValue PlaneGreen.diskOpen c.densityBound_ne_top (c.density_bound hμ.le) v‖^2 ≤
δ*‖H10.grad PlaneGreen.diskOpen v‖^2 := by
sorry
end ClosedDiskChart
end StrictHotSpots.Conformal
end
end ActualPotential
end OAI
end