BesovNorms #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The four-term negative-norm display of Section 3.5 #
This module assembles the display e.Besov.norms.gradient of ABK26 for the
canonical maximizer on \cu_m from the four estimates already available in
this directory: the multiscale Poincare bridge, the per-scale defect estimate,
the summed large-scale split and the small-scale tail. Nothing about the
status of the lemma l.Besov.norms is asserted here.
The left-hand side is Carriers.scaledNegHMinusOne of the maximizer gradient
defect, that is
3^{-m} \| \nabla v(\cdot,\cu_m,p,q;\a) - (\s_*^{-1}(\cu_m)(q+\k(\cu_m)p)-p) \|_{\Hminusul(\cu_m)},
and the right-hand side is the printed four-term sum with one dimension-only
constant besovNormsConstant d.
Route #
sqrt_sum_sq_sum_le_sum_mul_sqrt_sum_sqis the Minkowski conversion(\sum_i (\sum_j w_j a_{ij})^2)^{1/2} \le \sum_j w_j (\sum_i a_{ij}^2)^{1/2}for nonnegative weights, proved by induction on thej-range from the two-term\ell^2triangle inequality, itself proved from the Cauchy--Schwarz inequality for finite sums. This is the conversion thatMultiscalePoincareBridge.leanstates but does not formalize: its conclusion aggregates the coordinates in\ell^2, while the printed displaye.msp.plus.split.beginis the\ell^1-of-\ell^2form.- At
(s,p,q) = (1,2,1)the depth-Nentry of the negative circ norm is the partial sum\sum_{j \le N+1} 3^{m-j} (\avsum_R |(u)_R|^2)^{1/2}(cubeBesovCircNormEntry_one_two_one, with the weight identified byMultiscalePoincareBridge.cubeBesovCircDepthWeight_one), so after the scale factor3^{-m}the summand is the printed3^{-(m-n)}term withn = m-j. sum_cubeBesovCircDepthAverage_maximizerGradientDefectidentifies the coordinate sum of the depth-jcirc averages of the gradient defect withdescendantsAverage Q j (parentCoarseScaleSeparationDeviationSq ...), the carrier ofLargeScaleSplit.lean. Averaging is linear in the coordinate, so the Euclidean length of the average vector is the coordinate sum of the squared scalar averages; the upstream Chapter 5 identitycubeAverageVec_canonicalMaximizerGradientDefectOnDependentFamily_eq_ch04supplies the Chapter 4 representative on each descendant.sum_range_multiscaleTerm_le_fourTermsplits the depth range at the base scale: depthsj \le m-L_0are the scalesn \in [L_0,m]and are bounded byLargeScaleSplit.sum_Icc_weighted_..., while depthsj > m-L_0are the scalesn < L_0and are bounded bySmallScaleTail.sum_range_smallScale_multiscaleTerm_le. The two upstream statements are on the identical summand, so the split is exact; the bound is uniform in the depth cutoffN.mul_sqrt_sum_sq_ciSup_lepasses from the partial circ norms to the circ norm itself. The circ norm is the supremum of the partial sums, which are monotone and, by the previous step, uniformly bounded; the limit therefore obeys the same bound. This is where the manuscript's bi-infinite sum\sum_{n=-\infty}^mis realized.scaledNegHMinusOne_maximizerGradientDefect_le_besovNormsSumcomposes the above with the bridge ofMultiscalePoincareBridge.leanand converts theℝ≥0∞-valued left-hand side byENNReal.ofReal.
Correspondence with the printed display #
C \lambda_{s,r}^{-1/2}(\cu_m;\a) \sum_{n=L_0}^m 3^{-(1-s)(m-n)} (\avsum_z J(z+\cu_n,p,q;\a) - J(\cu_m,p,q;\a))^{1/2}, realized withWeakNormsMaximizer.responseDefectAverageAtScale m n p q afor the bracket;C \sum_{n=L_0}^m 3^{-(m-n)} (\avsum_z | \s_*^{-1}(\cu_m)(q+\k(\cu_m)p) - \s_*^{-1}(z+\cu_n)(q+\k(z+\cu_n)p) |^2)^{1/2}, realized withLargeScaleSplit.coarseMatrixVariationSq;C \lambda_{s,r}^{-1/2}(\cu_m;\a) 3^{-(1-s)(m-L_0)} \| \s^{1/2} \nabla v \|_{\underline L^2(\cu_m)}, realized withSmallScaleTail.maximizerEnergyL2Norm;C 3^{-(m-L_0)} | \s_*^{-1}(\cu_m)(q+\k(\cu_m)p) - p |, realized as the square root ofvecNormSq (coarseScaleSeparation a ha (originCube d m) p q).
The manuscript constant C(d) is given the explicit value besovNormsConstant d = 2\sqrt 2 \cdot multiscalePoincareConstant d, which dominates the four
constants produced by the chain: 2 on the defect leg (\sqrt 2 from the
split times \sqrt 2 from the defect estimate), \sqrt 2 on the coarse-matrix
leg, and 2\sqrt 2 on both tails (\sqrt 2 from the triangle step times 2
from the geometric tail \rho/(1-\rho) \le 2). All four are multiplied by the
multiscale Poincare constant of the bridge.
Formalization readings #
The readings of Carriers.lean (the dual pairing is volume normalized; a vector
field's dual seminorm is the Euclidean \ell^2 aggregate of the scalar
seminorms of its coordinates) and of PerScaleDefect.lean (the manuscript index
set z \in 3^n\Zd \cap \cu_m is the set of triadic descendants at depth m-n,
and \avsum is descendantsAverage) are inherited unchanged. Two further
readings are specific to this module.
- The multiscale sum is the negative circ norm at
(s,p,q) = (1,2,1). The manuscript's right-hand side is\sum_{n=-\infty}^m 3^{-(m-n)} (\avsum_z |(f)_{z+\cu_n}|^2)^{1/2}. Here3^{-m} \cdot cubeBesovCircNorm Q 1 2 1 fis that sum: item 2 of the route proves that each partial sum of the circ norm is the printed sum truncated at a finite depth, with the same weight and the same average, and the circ norm is the supremum of those partial sums. Unlike inMultiscalePoincareBridge.lean, where only the weight half was formalized, the depth average and the depth sum are identified here in Lean, for the maximizer gradient defect. - The bi-infinite sum is a supremum of partial sums. The manuscript sums
over all
n \le m. The upstream circ norm issSupof the set of partial sums, which for a nonnegative summand is the value of the series, finite or not. The passage from the uniform bound on partial sums to the bound on the supremum ismul_sqrt_sum_sq_ciSup_leand uses monotone convergence of a bounded monotone real sequence; no summability is assumed, it is a consequence of the four-term bound.
The per-depth identification #
The per-depth identification. Summing the depth-j circ averages of the
coordinates of the maximizer gradient defect over the coordinate index gives the
descendant average of the squared deviation from the parent comparison
vector.
It is public because the l.J.bound.by.Besov assembly re-enters the chain at
this depth, before the coordinate aggregation.
The depth-indexed multiscale term #
Splitting the depth range at the base scale #
Reindexing the two ranges #
The four-term bound at every depth cutoff #
The four printed right-hand terms bound every partial multiscale sum.
The head of the depth range is discharged by the summed large-scale display and
the tail by the small-scale tail, on the identical summand.
It is public because the l.J.bound.by.Besov assembly bounds its own partial
multiscale sums by the same four terms.