IncrementConcentration #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The deterministic partition identity for the stream-increment L^p mass #
ABK26 proves e.kl.bounds.large by writing the cube average ⨍_{cu_l} |k_m - k_n|^p as the average of the subcube averages over the scale-m partition
of cu_l, and then applying p.concentration to that partition average. This
module proves the deterministic half of that step — the exact identity —
together with the law-carrier form of the cube observable that the
concentration step consumes.
What is proved #
regFieldLpMass p U a— the volume-normalizedL^pmass of a regular coefficient field on an observation set. This is the CoarseGraining-shaped cube observableX : Set (Vec d) → RegCoeffField d → ℝ; read at the increment field on a half-open triadic cube it is the cube average of the increment density (cubeAverage_streamIncrementLpDensity), i.e. the provedstreamIncrementLpMass.regFieldLpMass_translateSet— translating the observation set is the same as translating the field. This is the raw form of the covariance that CoarseGraining's restriction lane asks for (Ch04.IsRestrictionTranslationCovariant), one of the three structural hypotheses ofisBigO_gammaSigma_restrictionCenteredDescendantAverage_of_restrictionUnitRangeDependentLaw; the lane-shaped statement is carried by the measurable representativeregFieldLpMassRepofIncrementMassRepresentative.lean, together with the restriction locality (Ch04.IsRestrictionLocalRandomVariable) that the same module supplies. What that representative costs is exactly the measurability obstruction described in the gap note below.integrableOn_cubeSet_streamIncrementLpDensity— thex-side integrability of the density on a half-open triadic cube (the provedIncrementLpintegrability suite is inomega, and itsx-side lemma is stated on the open cube; CoarseGraining's partition identity needs the half-open one).streamIncrementLpMass_eq_descendantsAverage,streamIncrementLpMass_eq_descendantAverage_of_scale— the deterministic descendant identity, CoarseGraining'scubeAverage_eq_descendantsAverage_cubeAverage_of_integrableOninstantiated at the increment density, in both the depth-indexed and the scale-indexed form. The head + centered tail rewriting of that identity is not performed here. The raw centered tail is signed, so it does NOT satisfy the concentration interface'shT_nonnegdirectly; a consumer must passT := |mass − H|, to which theΓbound transfers sinceIsBigOWithis stated through the absolute tail event, and the provedIncrementLpGain.streamIncrementLpMass_head_taildoes exactly that.
The remaining gap for e.kl.bounds.large #
The concentration application itself is not proved, and needs exactly one more input, recorded here so the follow-up is bounded:
Measurable (regFieldLpMass p U)on the canonical carrier σ-algebra ofRegCoeffField d(equivalently, an a.e. representative of it in the sense of Ch04's restriction-lane centered-descendant-average theorem for an a.e.-equal local representative). Pointwise evaluationa ↦ a x i jis measurable, but the carrier σ-algebra is a join containing an uncountable-product part, so the integral overUof a nonlinear function of the values is not measurable for free. The canonical route is a countable local representative: on the (full-measure, because every increment field is continuous) set of continuous fields,⨍_U |a|^pis the limit of the triadic Riemann sumsdescendantsAverage U j (fun R => |cubeAverageMat R a|^p), and eachcubeAverageMat R ais a fixed multiple ofentryTestR i j (1_{cubeSet R}), henceLocalSigmaR- andRestrictionSigmaR-measurable.
: no rescaling achieves this for the manuscript's scale-m subcubes (unit
range and nonnegative subcube scale are incompatible); the local partition runs
at the coarser scale-(m+c) subcubes via Provider/Stream/IncrementLaw.lean's
scaledStreamIncrementLaw at 3^{m+c}, 3^c > 2 sqrt d, costing the
dimension-only 3^{(d/2)c}.
References #
- ABK26,
e.kl.bounds.large;p.concentration.
The L^p mass as an observable of the coefficient field #
The volume-normalized L^p mass of a regular coefficient field on an
observation set, measured in the exact Euclidean matrix operator norm. This is
the cube observable X : Set (Vec d) → RegCoeffField d → ℝ of the
p.concentration step.
Equations
- Algsuperdiff.Section3.Provider.Stream.regFieldLpMass p U a = (MeasureTheory.volume U).toReal⁻¹ * ∫ (x : HCPolySupport.Vec d) in U, HCPolySupport.Book.Ch02.matrixOperatorNorm (a.toFun x) ^ p
Instances For
The cube average of the increment density is the cube observable at the increment field, on the half-open cube used by CoarseGraining's partition identity.
Translation covariance of the observable #
The L^p mass observable commutes with spatial translation: translating
the observation set is the same as translating the field.
The L^p density of a stream increment is integrable on every half-open
triadic cube: it is continuous and the cube is bounded. The proved
IncrementLp integrability suite is in the sample omega; this is the
x-side statement, on the half-open cube used by CoarseGraining's partition
identity.
The deterministic descendant identity #
The deterministic descendant identity at the increment (depth form).
CoarseGraining's
cubeAverage_eq_descendantsAverage_cubeAverage_of_integrableOn, instantiated
at the increment L^p density: the cube mass on cu_l is the average of the
subcube masses over the depth-j descendants of cu_l.
The deterministic descendant identity at the increment (scale form).
This is the partition of cu_l into its scale-k subcubes, which for k = m
is exactly the partition used by e.kl.bounds.large.