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LeanPool.Superdiffusion.Algsuperdiff.Section3.Provider.BadEvents.ObservableSwapPayoff

ObservableSwapPayoff #

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

What the observable body swap buys: the two pointwise payoffs #

Two obstructions that were recorded as structural in the tree were obstructions of that representative choice only, and both dissolve. This module proves the two consequences.

The lower leg's grid domination, now pointwise in the sample #

Its module docstring recorded the resulting quantifier gap as the lower leg's open hgrid conjunct, and named the fix — "a pointwise-valid representative for Observable.cutoffLowerEllipticityInv (i.e. a change in the observable layer)". That change has now been made, so the equality descends at every sample point: cutoffLowerEllipticityInv_eq_top_add_gridSum, and with it the for all omega, for all L form cutoffLowerEllipticityInv_forall_le_top_add_gridSum. The quantifier order the pointwise dominates clause of Probability.IsLowerIntegerFamilyOrliczWithWitness demands is available.

(b) The off-centre transport of the lower family relation #

The centered-cube transport of the hcg anchoring is definitional after the observable body swap: both observables reduce to the same clamped literal. Earlier scope notes, including the corresponding note in Provider/Tail/TailSqrt.lean, said the off-centre half admitted "no defeq escape", because the only proved translate identity (LambdaCovariance.lambdaSq_cutoff_translateCutoffSample) is a pathwise equality read at a different sample, while the exported observables carried no pointwise information at all.

They do now. The exported observables are the literals on the source range, so the pathwise covariance applies to them directly:

cubeLowerEllipticityInv M Q L s hs q omega
  = Observable.cutoffLowerEllipticityInv M Q.scale L s hs q
      (translateCutoffSample (triadicCubeShift Q) omega)  ,

at every sample point and every cutoff index, with one shift vector triadicCubeShift Q independent of L. Composing with the law invariance Cutoff.map_translateCutoffSample_cutoffSampleLaw (through Provider.Stream.isBigOWith_comp_translateCutoffSample) transports the whole IsLowerIntegerFamilyOrliczWithWitness package from the centered cube to an arbitrary triadic cube of the same scale, with the witness Y replaced by Y ∘ translateCutoffSample (triadicCubeShift Q) and with b, A, L0 and the tail profile unchanged. This is the per-translate producer of the hcg binder of EllipticityBranchLow.lean.

Scope. The local result transports the statement from the centered cube to a translate. The frozen Algsuperdiff.Frozen.Section3.coarse_ellipticity_bounds is now proved, but it is not applied in this transport module; the hcg binder of EllipticityBranchLow.lean remains a conditional A binder. A downstream assembly can now discharge it at the centered cube and use this result at every translate of that scale, which is exactly the manuscript's own stationarity reduction (applied). The upper (Lambda) leg is not transported here: only the lower covariance lambdaSq_cutoff_translateCutoffSample is proved, and the Lambda twin would need the upperLeft analogue of coarseSigmaStarInvMatrixNorm_cutoff_translateCutoffSample, which is not.

Main results #

References #

(b) The off-centre identification #

The pathwise off-centre identification, at the literal. The literal inverse lower ellipticity on an arbitrary triadic cube Q is the centered literal at the same scale, read at the sample translated by the base point of Q. This is LambdaCovariance.lambdaSq_cutoff_translateCutoffSample written at the Section 3 observable layer.

The pathwise off-centre identification, at the exported observable. On the source range 0 < s the clamp is inert on both sides, so the covariance of the literals is inherited verbatim. Before the body swap no such statement was available at the exported observables: they were Classical.choose-selected representatives, and no pointwise identity of an off-centre representative with anything was proved.

(b) The transport of the lower family relation to a translate #

The off-centre witness-level transport. A lower-integer-family weak-Orlicz relation for the centered observable at scale Q.scale, with witness Y, gives the same relation for the general-cube observable at Q, with the translated witness Y ∘ translateCutoffSample (triadicCubeShift Q), the same deterministic shift b, the same amplitude A, the same lower index L0 and the same tail profile.

The off-centre transport, in the shape the hcg binder is stated in. The conclusion of p.cg.ellipticity.bounds at the centered cube of scale Q.scale implies the same conclusion at Q. This is the manuscript's own stationarity reduction at the observable layer.

The per-translate hcg producer. One centered instance of p.cg.ellipticity.bounds at scale n yields the binder of EllipticityBranchLow.lean at every scale-n descendant of Q, which is exactly what ABK26 applies and justifies.