Plain-English statement
- The normalized Gibbs measure annihilates the displayed Langevin operator on the compactly supported `C²` core. This is a normalized-measure corollary of the whole-space weighted-IBP theorem. It is a core-level infinitesimal stationarity statement, not semigroup invariance: extending it to a semigroup-stable generator domain requires an additional closure/core theorem or a separate martingale-problem argument.
Read the mathematics first, then descend into Lean
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Proof architecture
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How to read the exact Lean declaration
Read a Lean theorem left-to-right exactly as you would unpack a mathematical sentence: name → ambient types → automatically inferred structures → explicit hypotheses → conclusion → proof. Then read the proof top-to-bottom as transformations of the current goal.
- NameWhat reusable mathematical fact is being created?
- ParametersWhich symbols are arbitrary, and which structures are inferred by typeclass search?
- PropositionAfter the colon, translate the Lean expression back into a paper statement.
- Proof actionsAfter
by, ask what each tactic does to the mathematical goal—not only what syntax it uses.
Syntax used on this page
This glossary is filtered to syntax that actually occurs in the declaration above. Open a symbol only when you meet it, rather than memorizing Lean grammar in advance.
Source voice and ASTIS voice stay separate
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Lean statement
theorem integral_operator_normalizedGibbs_eq_zero_on_compactlySupportedC2
{n : ℕ}
{V f : EuclideanSpace ℝ (Fin (n + 1)) → ℝ}
(hV : ContDiff ℝ 1 V)
(hf : CompactlySupportedC2 f) :
∫ x, operator V f x ∂volume.withDensity
(fun x =>
(∫⁻ y, Measure.Gibbs.gibbsDensityENNReal V y ∂volume)⁻¹ *
Measure.Gibbs.gibbsDensityENNReal V x) = 0 := by
rw [TechnicalLemmas.Measure.GibbsIntegral.integral_withDensity_lintegral_inv_mul_gibbsDensityENNReal_eq_integral_lintegral_inv_mul_exp_smul_of_neZero
volume hV.continuous.measurable.aemeasurable]
simp_rw [operator, smul_eq_mul, mul_assoc]
rw [integral_const_mul]
rw [Langevin.integral_expNeg_langevinGenerator_rhs_eq_zero_of_contDiff_of_hasCompactSupport
hV hf.1 hf.2]
simp
/-- A semigroup satisfying the integrated-generator contract on the
compactly supported `C²` core preserves normalized Gibbs expectations on that
core.
This theorem composes the concrete Gibbs integration-by-parts identity with
the abstract semigroup-to-invariance bridge. The semigroup contract remains
an explicit hypothesis: no Langevin SDE, Markov semigroup, core closure, or
measure-determining extension is constructed here. -/
Open AutoSamplingTheory/TechnicalLemmas/StochasticProcesses/LangevinGenerator.lean:65published source at 7bcd37294df1
Proof architecture
Chewi Ch.1 Example 1.2.8 to Corollary 1.2.9: prove normalized Gibbs expectation of the displayed generator is zero on the C_c^2 test core
Lean proof walkthrough
- Read the quantified variables and typeclass brackets as part of the mathematical statement; inferred arguments are not missing assumptions.
- `rw` rewrites by an established identity.
- `simp` normalizes through registered definitional and theorem rewrites.
Why the statement has this shape
The declaration is kept at the reusable level recorded by its Registry tags and direct consumers. Explicit measures, spaces, wrappers, and regularity hypotheses expose interfaces that paper notation often infers. A theorem card explains those interfaces but never widens the compiled statement.
Hidden assumptions and non-claims
- Measurability is represented explicitly or must be supplied by a dependency.
- Pointwise support, topological support, and compact support retain distinct meanings.
- Almost-everywhere hypotheses depend on the stated measure and representative.
- Density statements retain normalization and absolute-continuity prerequisites.
- A Gibbs expression is not automatically a probability law or an invariant law.
- A formal generator display does not establish a closed operator domain.