ComparatorChallenges/LiebThirring.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
16 declarations, 1 contain sorry, 0 declared as axioms
The form domain is H¹(R;C), represented by an L² function together with its L²
weak derivative. Null-set changes do not affect any definition below.
negativeMoment is the extended nonnegative sum over negative eigenvalues,
counting multiplicities: equivalently the supremum over all finite orthonormal
families of weak eigenfunctions of the form. This does not assume in advance
finiteness of the moment or a finite number of eigenvalues.
- structure
OAI.SharpLiebThirring.H1line 23Also declared: OAI/Analysis/LiebThirring/Model.lean:23 (same declaration text).
- def
OAI.SharpLiebThirring.l2Pairingline 31Also declared: OAI/Analysis/LiebThirring/Model.lean:31 (same declaration text).
- def
OAI.SharpLiebThirring.schrodingerFormThe polarized form of -d²/dx² - W, on exactly H¹ line 34Source documentation
The polarized form of -d²/dx² - W, on exactly H¹.
L4DEL explanation
The polarized form of -d²/dx² - W, on exactly H¹.
- This explanation is a condensed rendering of the declaration's own doc comment at the pinned source commit; consult the exact Lean statement below for authority.
Sources and attribution: Pinned Lean source (fd4aeeb2ee4f)
Also declared: OAI/Analysis/LiebThirring/Model.lean:34 (same declaration text).
def schrodingerForm (W : ℝ → ℝ) (u v : H1) : ℂ := …
Mentions: OAI.SharpLiebThirring.H1
- def
OAI.SharpLiebThirring.IsNegativeEigenfunctionWeak eigenfunction at the negative energy -k² line 39Source documentation
Weak eigenfunction at the negative energy -k².
L4DEL explanation
Weak eigenfunction at the negative energy -k².
- This explanation is a condensed rendering of the declaration's own doc comment at the pinned source commit; consult the exact Lean statement below for authority.
Sources and attribution: Pinned Lean source (fd4aeeb2ee4f)
Also declared: OAI/Analysis/LiebThirring/Model.lean:39 (same declaration text).
def IsNegativeEigenfunction (W : ℝ → ℝ) (k : ℝ) (u : H1) : Prop := …
Mentions: OAI.SharpLiebThirring.H1
- def
OAI.SharpLiebThirring.IsOrthonormalFamilyline 42Also declared: OAI/Analysis/LiebThirring/Model.lean:42 (same declaration text).
- def
OAI.SharpLiebThirring.negativeMomentAn unlimited finite-family-size supremum, in ℝ≥0∞, includes the entire sum line 46Source documentation
An unlimited finite-family-size supremum, in ℝ≥0∞, includes the entire sum.
L4DEL explanation
An unlimited finite-family-size supremum, in ℝ≥0∞, includes the entire sum.
- This explanation is a condensed rendering of the declaration's own doc comment at the pinned source commit; consult the exact Lean statement below for authority.
Sources and attribution: Pinned Lean source (fd4aeeb2ee4f)
Also declared: OAI/Analysis/LiebThirring/Model.lean:46 (same declaration text).
def negativeMoment (γ : ℝ) (W : ℝ → ℝ) : ℝ≥0∞ := …
- def
OAI.SharpLiebThirring.oneStateMomentThe moment retaining at most one negative eigenvalue line 52Source documentation
The moment retaining at most one negative eigenvalue.
L4DEL explanation
The moment retaining at most one negative eigenvalue.
- This explanation is a condensed rendering of the declaration's own doc comment at the pinned source commit; consult the exact Lean statement below for authority.
Sources and attribution: Pinned Lean source (fd4aeeb2ee4f)
Also declared: OAI/Analysis/LiebThirring/Model.lean:52 (same declaration text).
def oneStateMoment (γ : ℝ) (W : ℝ → ℝ) : ℝ≥0∞ := …
- def
OAI.SharpLiebThirring.Admissibleline 56Also declared: OAI/Analysis/LiebThirring/Model.lean:56 (same declaration text).
- def
OAI.SharpLiebThirring.potentialMassline 59Also declared: OAI/Analysis/LiebThirring/Model.lean:59 (same declaration text).
- def
OAI.SharpLiebThirring.semiclassicalConstantline 62Also declared: OAI/Analysis/LiebThirring/Model.lean:62 (same declaration text).
- def
OAI.SharpLiebThirring.sharpConstantline 65Also declared: OAI/Analysis/LiebThirring/Model.lean:65 (same declaration text).
- def
OAI.SharpLiebThirring.optimalConstantline 68Also declared: OAI/Analysis/LiebThirring/Model.lean:68 (same declaration text).
- def
OAI.SharpLiebThirring.oneStateConstantline 72Also declared: OAI/Analysis/LiebThirring/Model.lean:72 (same declaration text).
- def
OAI.SharpLiebThirring.equalityPotentialline 76Also declared: OAI/Analysis/LiebThirring/Model.lean:76 (same declaration text).
- def
OAI.SharpLiebThirring.MainClaimThe full spectral bound, optimal constants, and attainment at the explicit potential line 81Source documentation
The full spectral bound, optimal constants, and attainment at the explicit potential.
L4DEL explanation
The full spectral bound, optimal constants, and attainment at the explicit potential.
- This explanation is a condensed rendering of the declaration's own doc comment at the pinned source commit; consult the exact Lean statement below for authority.
Sources and attribution: Pinned Lean source (fd4aeeb2ee4f)
Also declared: OAI/Analysis/LiebThirring/Model.lean:81 (same declaration text).
def MainClaim : Prop := …
- theorem
OAI.SharpLiebThirring.sharp_lieb_thirringChallenge statement: Sharp finite-matrix Lieb–Thirring inequalities and all equality cases sorry line 94Source documentation
Full sharp Lieb–Thirring bound, both optimal constants, and equality at the explicit potential; no finite spectral cutoff is imposed.
L4DEL explanation
The formalized result determines the sharp one-dimensional Lieb–Thirring constant for $1/2<\gamma<3/2$. For every nonnegative $W\in L^{\gamma+1/2}(\mathbb R)$, it bounds the full negative-eigenvalue moment of $-d^2/dx^2-W$ by the one-bound-state constant times the potential integral. This constant is optimal and is attained by $(r+1)\mathrm{sech}^2(rx)$, where $r=(\gamma-1/2)^{-1}$. No finite spectral cutoff 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.LiebThirring.Main as the released solution module checked against this declaration.
Sources and attribution: Pinned Lean source (fd4aeeb2ee4f)
Distinct definitions of this name: OAI/Analysis/LiebThirring/Main.lean:38 (same statement text; different proof or body). Qualify references as OAI.SharpLiebThirring.sharp_lieb_thirring@path.
theorem sharp_lieb_thirring : MainClaim := by …
Mentions: OAI.SharpLiebThirring.MainClaim