Paper Step 4(B): whole-series high-frequency producer #
Paper: R-324 — §4.2 Step 4(B), whole-series high-frequency producer
The common-left Fourier argument is needed only when the canonical refined representative has a residual single. If both halves are full, the whole physical integral vanishes at a non-zero conserved external mode. This file records that dichotomy at the exact boundary required by the final capstone.
Keeping the residual input at the complete signed-series boundary is intentional: no selected-slot, first-high, cell, or contraction-wise triangle inequality occurs here. The analytic residual producer is supplied by the endpoint common-left Fourier identity, the grouped residual Fourier estimate, and the mixed-cutoff complete nested run imported above.
Absorbing the common-left Haar average #
Normalized common-left Haar average of a nonnegative auxiliary coefficient. The normalization is the paper's (non-probability) torus mass.
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One coordinate of a four-dimensional lattice mode carries at least half
of its Euclidean size. The factor two is exactly sqrt 4; the selected
coordinate itself is an honest maximum for the auxiliary sup norm.
At the high-frequency threshold, the inverse eighth power of a coordinate
carrying half the Euclidean norm is absorbed by the paper's central bracket.
The explicit constant is 2^8 * 2^4 = 4096.
The coordinate subgroup used by the one-dimensional Fourier estimate is literally the restriction of the canonical left-copy torus translation.
The complete grouped residual coefficient, translated as one signed family, is integrable against a torus character. This uses the repository's existing measurable and uniform-bound theorems for the whole residual sum; no primitive-coordinate triangle inequality is introduced here.
The full four-dimensional common-left Fourier coefficient of one grouped residual primitive sum.
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Averaging a function over one coordinate subgroup and over full torus
Haar gives exactly 2π times its original integral. This is the Fubini
normalization seam used twice below: once for the signed coefficient and once
for its nonnegative auxiliary majorant.
The interval-parameterized coordinate shift projects quasi-preservingly to full torus Haar.
Exact partial-Fourier decomposition of the normalized full-torus coefficient. The common coordinate is averaged only after the complete signed source has been formed.
Concrete exact decomposition of the grouped residual torus coefficient into one-dimensional coordinate Fourier coefficients.
Global grouped Step 4(B) Fourier estimate at one nonzero coordinate.
The 2π in the one-dimensional Fourier coefficient cancels exactly against
the coordinate-subgroup Haar average.
Coordinate-free form of the grouped Step 4(B) estimate, with the explicit finite-dimensional loss absorbed into a fixed scalar.
The canonical route coefficient is exactly the grouped residual torus coefficient at the doubled terminal root.
Joint integrability required by common-left Fubini follows from integrability on the terminal product carrier and quasi-measure-preservation of the common-translation projection.
Product Haar absorbs a normalized common-left average whenever the
remaining endpoint geometry is invariant under the same translation. This
is the positive Fubini seam between the global Fourier coefficient estimate
and completeNestedRunDensityWithCrossCutoff.
No norm or triangle inequality occurs here. The only analytic premise is joint integrability before exchanging the common translation with the two terminal configuration integrals.
The endpoint-erased inverse-square geometry is invariant under a common translation of every surviving coordinate in one completed half.
Exact mixed-cutoff transport to the initial nested run #
The terminal endpoint geometry with only the complete residual covariance
factor replaced by sigma. The two certified half traces, their scale
products, and both endpoint-erased inverse-square chains remain those of
rho, exactly as in paper Step 4(B).
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Pullback of the mixed-cutoff endpoint geometry to the literal initial nested-cross carrier.
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Exact mixed-cutoff counterpart of
initialNestedEndpointIntegratedGroupedMajorant_mul_coupling_eq.
No estimate occurs here. The equality only reindexes the completed terminal
pair, identifies its reconstruction with the initial nested reconstruction,
and unfolds the grouped residual product with cutoff sigma.
Integrated form of the exact mixed-cutoff transport. This is the form consumed by the scalar complete-run estimate after the endpoint norm has been taken once.
Integrability of the initial mixed grouped majorant. The only division
is by the strictly positive even power of lamEps; all scale products remain
as harmless finite constants.
The preceding integrability statement transported back to the completed two-half terminal carrier.
The coefficient-free spatial geometry in the parametric two-half endpoint majorant.
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Specialization of the generic Haar-absorption identity to the exact coefficient-free geometry emitted by the parametric endpoint majorant.
Integrability companion to the preceding Haar-absorption identity.
The joint T4 × terminal function is integrated first in the common-left
Haar parameter; normalization by the fixed torus mass is then harmless.
The same absorption identity on the literal initial nested carrier used by the exact four-endpoint collapse and by the mixed-cutoff run.
The Haar-averaged endpoint geometry is integrable on the literal initial
nested carrier. This is the missing Integrable premise for the first legal
post-collapse norm comparison.
Real-valued form of the preceding integrability statement. The
complex-valued initialNestedPullback is only an implementation detail of
the exact endpoint-density API.
The complete positive auxiliary residual sum evaluated on the reconstructed
terminal pair. This is the sole coefficient that changes from rho to the
analytic cross cutoff sigma; the endpoint geometry is untouched.
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Translating the completed left terminal tuple is exactly the canonical left-copy translation of the doubled root, on the genuine support of the grouped residual sum.
On the terminal product carrier, coefficient-free endpoint geometry times the complete auxiliary residual sum is definitionally the mixed-cutoff grouped endpoint majorant (up to reassociation of scalar products).
The mixed endpoint geometry supplies the joint integrability needed for the common-left Haar/Fubini step.
Common-left Haar absorption followed by the exact terminal-to-nested reindexing. The result is precisely the mixed-cutoff grouped majorant read by the Steps 2--3 complete-run identity; no pointwise comparison between the original and auxiliary cutoff is used.
Real-valued common-left Haar absorption on the literal nested carrier. This is the scalar identity used after the first legal endpoint norm.
Pointwise coefficient estimate on the actual completed route packages. This is the exact input expected by the coefficient-parametric endpoint majorant.
Minimal signed endpoint/Fourier certificate #
Uniform absorption of the grouped Fourier loss #
Fixed base which absorbs the endpoint mass normalization, the explicit
4096, the eighth-degree order loss, and the three copies per order of the
cutoff derivative majorant.
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The whole grouped Fourier loss is exponential in the ambient order and
therefore fits into the 2m power already present in the inserted primitive
majorant.
Optional abstract certificate for the exact downstream information produced by the common-left endpoint calculation for one residual schedule.
This interface is useful for independent consumers, but it is not an assumption of the final proof chain: the unconditional producer below constructs the physical estimate directly.
canonicalCommonLeftIdentity is the signed Haar/Fubini identity and occurs
before any norm. commonLeftCoefficient_le_auxiliary is the grouped
Fourier-to-auxiliary estimate. The coefficient-parametric endpoint theorem
then gives the first legal endpoint-density norm, and its weighted integral
is discharged by the mixed-cutoff complete nested run.
- leftOrder : ℕ
- rightOrder : ℕ
- crossOrder : ℕ
- measure : MeasureTheory.Measure X
- originalCoefficient : X → ℂ
- commonLeftCoefficient : X → ℂ
- auxiliaryCoefficientMajorant : X → ℝ
- mixedCutoffMajorant : X → ℝ
- exactEndpointCollapse : ↑(lamEps 1 epsilon) ^ (2 * (self.leftOrder + self.rightOrder)) * r324RefinedPhysicalIntegral rho epsilon m alpha beta p = ∫ (x : X), self.endpointDensityWithCoefficient self.originalCoefficient x ∂self.measure
- canonicalCommonLeftIdentity : ∫ (x : X), self.endpointDensityWithCoefficient self.originalCoefficient x ∂self.measure = ∫ (x : X), self.endpointDensityWithCoefficient self.commonLeftCoefficient x ∂self.measure
- commonLeftCoefficient_le_auxiliary : (fun (x : X) => ‖self.commonLeftCoefficient x‖) ≤ᵐ[self.measure] self.auxiliaryCoefficientMajorant
- coefficientParametricEndpointDensity_le_mixedCutoffMajorant : (fun (x : X) => ‖self.commonLeftCoefficient x‖) ≤ᵐ[self.measure] self.auxiliaryCoefficientMajorant → (fun (x : X) => ‖self.endpointDensityWithCoefficient self.commonLeftCoefficient x‖) ≤ᵐ[self.measure] self.mixedCutoffMajorant
- weightedMixedCutoffMajorant_integrable : MeasureTheory.Integrable (fun (x : X) => lamEps 1 epsilon ^ (2 * self.crossOrder) * self.mixedCutoffMajorant x) self.measure
- weightedMixedCutoffMajorant_integral_le : ∫ (x : X), lamEps 1 epsilon ^ (2 * self.crossOrder) * self.mixedCutoffMajorant x ∂self.measure ≤ paperFourthOrderModeDecay alpha * paperFourthOrderModeDecay beta * eighthOrderFrequencyDecay (epsilon ^ 2 * ‖z4EuclideanFrequency (alpha + beta)‖) * (epsilon⁻¹ ^ 8 * ∫ (z : T4), primitiveInsertedMajorant primitiveConstant 1 epsilon supportConstant m z ∂paperMeasure)
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Optional schedule-uniform certificate interface. A concrete instance would combine canonical endpoint averaging, the grouped residual Fourier-to-auxiliary estimate, and the mixed-cutoff run. The final unconditional route does not consume this interface as a hypothesis.
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The concrete certificate is assembled after choosing the canonical routes as follows.
Xis the literal initial nested-coordinate function space ofleft.bound.twoHalfTerminal right.bound, with product paper measure.endpointDensityWithCoefficientisnestedEndpointProductDensityWithCoefficientafter pulling a two-terminal coefficient back alongterminalProductPiMeasurableEquivNested.originalCoefficientisleft.bound.crossCoefficient right.bound pi;commonLeftCoefficientis itsr324CommonLeftFourierCoefficientatalpha + beta. The canonical route package supplies the signed integral identity before the first norm.auxiliaryCoefficientMajorantis the common-left Haar average ofr324ResidualPrimitiveSumProduct rho.auxiliaryCutoff. The grouped global Fourier theorem supplies its pointwise coefficient bound, including the eighth-order central decay and the absorbablem^8 C^(3m)loss.mixedCutoffMajorantis the coefficient-parametric endpoint majorant with that auxiliary coefficient. Common-translation invariance of product Haar turns its integral intocompleteNestedRunDensityWithCrossCutoff; the mixed complete-run theorem and the existing reachable-scale ledger then supply the final weighted integral field.
Thus the certificate has no selected-slot, cell, word, or contraction-local norm, and its fields correspond one-for-one to the paper's endpoint collapse, common translation, derivative estimate, and Steps 2--3 nested run.
The analytic residual target in the physical-integral normalization used by the exact two-half endpoint packages. This is the convenient output of the common-left Fourier / mixed-cutoff nested-run proof.
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Unconditional Step 4(B) producer in the physical normalization. This is a whole-series implementation of the paper's high-frequency gain: complete both signed endpoint routes, apply the common-left Fourier identity before taking a norm, use the coefficient-parametric endpoint majorant once, Haar-average the complete residual family, and finally run the already closed Steps 2--3 majorant. It is mathematically equivalent at the public estimate boundary, but is not the paper's literal single-high-slot presentation.
The optional abstract signed endpoint/Fourier certificate suffices to close the residual physical estimate. This adapter is not on the final unconditional proof path.
The genuinely residual part of paper Step 4(B), still at the complete signed open-series boundary. This is the precise target of the common-left Fourier calculation; the full/full branch is discharged structurally below.
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Exact covariance reassembly transports a physical-integral estimate to the complete signed open series without any triangle inequality.
Adding the structurally vanishing full/full branch turns the residual common-left estimate into the public complete-series Step 4(B) producer.
Existential adapter from the residual common-left Fourier estimate to the final assembly.
One-step adapter from the exact endpoint/Fourier proof's physical normalization to the public complete signed-series producer.
Unconditional paper Step 4(B) producer consumed by the final assembly.
Optional abstract assembly: a uniform common-left endpoint certificate also implies the public Step 4(B) producer. The stable final theorem above instead uses the unconditional physical producer directly.