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LeanPool.Superdiffusion.Algsuperdiff.Section3.Provider.CoarseEllipticity.DoubledPairingCross

DoubledPairingCross #

Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.

The cross term of Step 2 by the depth-zero Besov identity #

Source display in ABK26: the cross-term estimate of Step 2 of l.approximate.recurrence.formula,

P_z . fint_{z+cu_n} bfA_m tilde S_z
  <= C | bfAhom^{1/2} P_z | Lambda-tilde 3^n [ bfAhom^{1/2} bfF_z ]_{H^1(z+cu_n)} .

The route #

The manuscript reaches this display by Cauchy--Schwarz in the bfA_m-form followed by e.bound.one.cube.by.lambdas. That term is the plain cube average:

cubeBesovNegativeVectorPartialSeminormTwo Q s 0 u = || fint_Q u || ,

recorded here as cubeBesovNegativeVectorPartialSeminormTwo_zero. Hence any envelope Bu of the finite-depth negative seminorms of bfA_0^{-1/2} bfA_m tilde S_z already controls its cube average, and the cross term follows from Cauchy--Schwarz alone. Strictly fewer inputs than the printed route: no one-cube ellipticity comparison is spent here.

The statement below is gauge-neutral: it is proved for an arbitrary block vector P and an arbitrary block field Y. A caller instantiates it at P:= bfAhom^{1/2} P_z and Y:= bfAhom^{-1/2} bfA_m tilde S_z after applying DoubledPairingGauge.blockVecDot_blockGaugeDown_blockGaugeUp, so that normP becomes the manuscript's |bfAhom^{1/2} P_z| in the component-sum rendering. That instantiation is not performed here.

Binders #

Bu is a caller-supplied envelope of the finite-depth negative seminorms. No smallness, moment, measurability or integrability proposition occurs: everything below is pointwise linear algebra and one identity of the seminorm at depth zero.

Scope #

No anchor, frozen theorem or external input is consumed, and there is no sorry.

The depth-zero identity #

The cross term #

The cross term by the depth-zero route.

| P . fint_Q Y |  <=  blockVecNormSum P * Bu

for any envelope Bu of the finite-depth negative q = 2 Besov seminorms of the two legs of Y. Per the only ingredients are the depth-zero identity and Cauchy--Schwarz.