ComparatorChallenges/Conductivity.lean
Explanation legend Lean4 Domain Explanation Language (L4DEL)
L4DEL explanations are a separate layer. They do not change the Lean source. Intuition is explanatory prose; numbered items are a reading path; sources link the wording back to evidence.
- L4DEL
- Lean4 Domain Explanation Language
Credit: OpenAI's pinned repository says an unreleased internal model produced the manuscripts and supporting proof artifacts. The collection builds on the mathematics community's accumulated problems, results, language, and formal libraries; each manuscript's BibTeX and bibliography are the authority for individual scholarly credit.
Project sources: Pinned openai/math documentation, Pinned formalization catalogue
24 declarations, 1 contain sorry, 0 declared as axioms
- abbrev
OAI.ScalarConductivity.R3line 11Also declared: OAI/Analysis/Conductivity/Model.lean:11 (same declaration text).
- abbrev
OAI.ScalarConductivity.JetFiberline 12Also declared: OAI/Analysis/Conductivity/Model.lean:12 (same declaration text).
- def
OAI.ScalarConductivity.ballline 13Also declared: OAI/Analysis/Conductivity/Model.lean:13 (same declaration text).
- def
OAI.ScalarConductivity.ballMeasureline 14Also declared: OAI/Analysis/Conductivity/Model.lean:14 (same declaration text).
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OAI.ScalarConductivity.JetSpaceline 15Also declared: OAI/Analysis/Conductivity/Model.lean:15 (same declaration text).
- def
OAI.ScalarConductivity.smoothJetline 17Also declared: OAI/Analysis/Conductivity/Model.lean:17 (same declaration text).
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OAI.ScalarConductivity.smoothJetsline 20Also declared: OAI/Analysis/Conductivity/Model.lean:20 (same declaration text).
- def
OAI.ScalarConductivity.compactSmoothJetsline 24Also declared: OAI/Analysis/Conductivity/Model.lean:24 (same declaration text).
- def
OAI.ScalarConductivity.H1Spaceline 29Also declared: OAI/Analysis/Conductivity/Model.lean:29 (same declaration text).
- abbrev
OAI.ScalarConductivity.H1line 31Also declared: OAI/Analysis/Conductivity/Model.lean:31 (same declaration text).
- def
OAI.ScalarConductivity.zeroTraceAmbientline 33Also declared: OAI/Analysis/Conductivity/Model.lean:33 (same declaration text).
- def
OAI.ScalarConductivity.H10line 36Also declared: OAI/Analysis/Conductivity/Model.lean:36 (same declaration text).
- instance
OAI.ScalarConductivity.H10_isClosedline 38Also declared: OAI/Analysis/Conductivity/Model.lean:38 (same declaration text).
- abbrev
OAI.ScalarConductivity.TraceSpaceline 42Also declared: OAI/Analysis/Conductivity/Model.lean:42 (same declaration text).
- abbrev
OAI.ScalarConductivity.TraceDualline 43Also declared: OAI/Analysis/Conductivity/Model.lean:43 (same declaration text).
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OAI.ScalarConductivity.DNOperatorline 44Also declared: OAI/Analysis/Conductivity/Model.lean:44 (same declaration text).
- def
OAI.ScalarConductivity.traceline 46Also declared: OAI/Analysis/Conductivity/Model.lean:46 (same declaration text).
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OAI.ScalarConductivity.weakGradientline 48Also declared: OAI/Analysis/Conductivity/Model.lean:48 (same declaration text).
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OAI.ScalarConductivity.energyline 51Also declared: OAI/Analysis/Conductivity/Model.lean:51 (same declaration text).
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OAI.ScalarConductivity.Harmonicline 54Also declared: OAI/Analysis/Conductivity/Model.lean:54 (same declaration text).
- def
OAI.ScalarConductivity.IsDirichletToNeumannline 57Also declared: OAI/Analysis/Conductivity/Model.lean:57 (same declaration text).
- def
OAI.ScalarConductivity.EqualOneNearBoundaryline 63Also declared: OAI/Analysis/Conductivity/Model.lean:63 (same declaration text).
- def
OAI.ScalarConductivity.MainStatementline 66Also declared: OAI/Analysis/Conductivity/Model.lean:66 (same declaration text).
- theorem
OAI.ScalarConductivity.main_nonuniquenessChallenge statement: Joint metric and connection recovery from one boundary patch sorry line 77L4DEL explanation
The Calderón inverse problem asks whether boundary measurements determine an interior conductivity. The formalized result gives nonuniqueness for bounded measurable scalar conductivities on the ball $B(0,3)\subset\mathbb R^3$: two uniformly positive conductivities differ on a set of positive volume, equal $1$ near the boundary, and have the same full weak Dirichlet-to-Neumann operator. Weak solutions exist uniquely for every boundary trace.
- This is an exact comparator target linked by the pinned repository's formalization note for this result.
- The repository's comparator configuration selects OAI.Analysis.Conductivity.Main as the released solution module checked against this declaration.
Sources and attribution: Pinned Lean source (fd4aeeb2ee4f)
Distinct definitions of this name: OAI/Analysis/Conductivity/Main.lean:73 (same statement text; different proof or body). Qualify references as OAI.ScalarConductivity.main_nonuniqueness@path.
theorem main_nonuniqueness : MainStatement := by …
Mentions: OAI.ScalarConductivity.MainStatement