Plain-English statement
- Remainder measurability transported from the normalized Brownian coordinate law. This cycle-194 lower_2 bridge discharges the downstream `hRemainderMeas` shape once the source correspondence has supplied measurability under the normalized scalar-coordinate law. The law transport uses only the already compiled standard-Gaussian coordinate-law bridge and the variance packaging bridge; domination and integrability remain separate leaves.
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Lean statement
theorem selectedWeakTestRemainderMeasOfStdGaussianVectorLaw
{Test E : Type*} [NormedAddCommGroup E] [InnerProductSpace Real E]
[FiniteDimensional Real E] [MeasurableSpace E] [BorelSpace E]
(variance : Test → E → Fin (Module.finrank Real E) → NNReal)
(normalizedVectorLaw : Test → E → MeasureTheory.Measure E)
(normalizedCoordinateLaw :
Test → E → Fin (Module.finrank Real E) → MeasureTheory.Measure Real)
(normalizedRemainder :
Test → E → Fin (Module.finrank Real E) → Real → Real)
(testRegular : Prop)
(hNormalizedRemainderMeas :
testRegular →
∀ φ x i,
MeasureTheory.AEStronglyMeasurable
(normalizedRemainder φ x i)
(normalizedCoordinateLaw φ x i))
(hNormalizedVectorLaw :
testRegular →
∀ φ x, normalizedVectorLaw φ x = ProbabilityTheory.stdGaussian E)
(hCoordinateLawDef :
testRegular →
∀ φ x i,
normalizedCoordinateLaw φ x i =
(normalizedVectorLaw φ x).map
(fun y : E => inner Real ((stdOrthonormalBasis Real E) i) y))
(hVarianceDef :
testRegular →
∀ φ x i,
(variance φ x i : Real) =
ProbabilityTheory.variance (id : Real → Real)
(normalizedCoordinateLaw φ x i)) :
testRegular →
∀ φ x i,
MeasureTheory.AEStronglyMeasurable
(fun z : Real => normalizedRemainder φ x i z)
(ProbabilityTheory.gaussianReal (0 : Real) (variance φ x i)) := by
intro htests φ x i
have hNormalizedCoordinateLaw :
testRegular →
∀ φ x i,
normalizedCoordinateLaw φ x i =
ProbabilityTheory.gaussianReal (0 : Real) (1 : NNReal) :=
selectedWeakTestNormalizedCoordinateLawOfStdGaussianVectorLaw
normalizedVectorLaw normalizedCoordinateLaw testRegular
hNormalizedVectorLaw hCoordinateLawDef
have hVarianceOne :
testRegular →
∀ φ x i, variance φ x i = (1 : NNReal) :=
selectedWeakTestNormalizedVarianceDefOfGaussianRealUnitLaw
variance normalizedCoordinateLaw testRegular hVarianceDef
hNormalizedCoordinateLaw
simpa [hNormalizedCoordinateLaw htests φ x i,
hVarianceOne htests φ x i]
using hNormalizedRemainderMeas htests φ x i
/-- Remainder domination transported from the normalized Brownian coordinate law.
This cycle-194 bridge narrows the downstream `hRemainderBound` leaf to the
same source-side normalized scalar-coordinate law used for the remainder
measurability bridge. It only rewrites the ambient measure using the compiled
standard-Gaussian coordinate-law bridge and the variance packaging bridge;
integrability of the dominating bound remains a separate leaf.
-/
Proof architecture
discharge hRemainderMeas in the active Brownian/Ito Taylor moment backend
Lean proof walkthrough
- Read the quantified variables and typeclass brackets as part of the mathematical statement; inferred arguments are not missing assumptions.
- `intro` introduces quantified hypotheses into the local proof context.
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- `simpa` closes the goal after a controlled simplification of a typed result.
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.
- Integrability is an input or proved output; a displayed integral alone does not supply it.
- Almost-everywhere hypotheses depend on the stated measure and representative.