ComparatorChallenges/VlasovMaxwell.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
29 declarations, 1 contain sorry, 0 declared as axioms
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OAI.RVM.Vecline 10Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:13 (same declaration text).
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OAI.RVM.Phaseline 11Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:14 (same declaration text).
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OAI.RVM.Particleline 12Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:15 (same declaration text).
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OAI.RVM.Fieldline 13Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:16 (same declaration text).
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OAI.RVM.qline 15Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:18 (same declaration text).
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OAI.RVM.velocityline 16Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:19 (same declaration text).
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OAI.RVM.basisline 18Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:21 (same declaration text).
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OAI.RVM.dotline 19Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:22 (same declaration text).
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OAI.RVM.crossline 20Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:23 (same declaration text).
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OAI.RVM.spatialPartialline 24Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:27 (same declaration text).
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OAI.RVM.divergenceline 26Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:29 (same declaration text).
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OAI.RVM.curlline 29Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:32 (same declaration text).
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OAI.RVM.rholine 34Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:37 (same declaration text).
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OAI.RVM.currentline 35Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:38 (same declaration text).
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OAI.RVM.Datumline 38Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:41 (same declaration text).
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OAI.RVM.BoundedSmoothline 43Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:46 (same declaration text).
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OAI.RVM.Admissibleline 47Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:50 (same declaration text).
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OAI.RVM.Solutionline 54Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:57 (same declaration text).
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OAI.RVM.particleHalfSpaceline 59Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:62 (same declaration text).
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OAI.RVM.fieldHalfSpaceline 60Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:63 (same declaration text).
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OAI.RVM.particleSlabline 61Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:64 (same declaration text).
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OAI.RVM.fieldSlabline 62Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:65 (same declaration text).
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OAI.RVM.TimeContinuousL2line 64Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:67 (same declaration text).
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OAI.RVM.Equationsline 69Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:72 (same declaration text).
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OAI.RVM.CompactOnFiniteHorizonsline 82Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:85 (same declaration text).
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OAI.RVM.Classicalline 86Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:89 (same declaration text).
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OAI.RVM.SmoothOnFiniteHorizonsline 95Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:98 (same declaration text).
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OAI.RVM.SameNonnegativeTimeline 99Also declared: OAI/Analysis/VlasovMaxwell/Model.lean:102 (same declaration text).
- theorem
OAI.RVM.global_classical_solutionChallenge statement: Global smoothness for relativistic Vlasov–Maxwell sorry line 103L4DEL explanation
The formalized result gives global existence and uniqueness for the three-dimensional one-species relativistic Vlasov–Maxwell system. The initial particle density is nonnegative, smooth, and compactly supported; the initial fields have bounded derivatives of all orders, finite energy, and satisfy both Gauss constraints. The solution is smooth on every finite time interval, has compact particle phase support there, and is unique among classical solutions. No smallness, symmetry, or neutrality assumption is imposed.
- 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.VlasovMaxwell.Main as the released solution module checked against this declaration.
Sources and attribution: Pinned Lean source (fd4aeeb2ee4f)
Distinct definitions of this name: OAI/Analysis/VlasovMaxwell/Main.lean:44 (same statement text; different proof or body). Qualify references as OAI.RVM.global_classical_solution@path.
theorem global_classical_solution (d : Datum) (hd : Admissible d) : ∃ s : Solution, Classical d s ∧ SmoothOnFiniteHorizons s ∧ ∀ s' : Solution, Classical d s' → SameNonnegativeTime s s' := by …Mentions: OAI.RVM.Datum, OAI.RVM.Admissible, OAI.RVM.Solution, OAI.RVM.Classical, OAI.RVM.SmoothOnFiniteHorizons, OAI.RVM.SameNonnegativeTime