The half-step variant of the finite shift in Pan (2.23) #
The cutoff is y + 1/2, while both finite polynomials retain their complete
source coefficients. This is a boundary-safe variant, not a transcription of
the natural-cutoff integral. No Perron truncation estimate is assumed here.
The complete short-polynomial kernel at the real half-step cutoff.
Equations
- AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel f m H y A₁ A₂ k χ s = AnalyticNumberTheory.LargeSieve.panDyadicG f m A₁ A₂ k χ s * AnalyticNumberTheory.LargeSieve.panShortF₁ m H χ s * ↑(MathlibNt.SieveTheory.LiuWeight.liuPanPerronHalfStep y) ^ s / s
Instances For
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStep_pos · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.perronLine_verticalSection · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel_differentiableOn · compiled type and proof/definition references.
Exact rectangle identity, with the actual differential ds = i dt.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel_oriented_rectangle · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel_vertical_integrable · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel_horizontal_integrable · compiled type and proof/definition references.
Pointwise bounds use the actual source and prime polynomials.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel_horizontal_pointwise · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel_horizontal_integral_bound · compiled type and proof/definition references.
The finite shift before any specialization of the height.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel_finite_shift_bound · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStep_source_power_le · compiled type and proof/definition references.
This retains exactly exp (2 log² x); the fifth power merely bounds it.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStep_source_height_ge_fifth · compiled type and proof/definition references.
Uniform unnormalized error for the actual full-polynomial contour shift.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel_source_inverse_square · compiled type and proof/definition references.
The normalized dt integral, equivalently (2πi)⁻¹ ∫ kernel(s) ds.
Equations
- AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortIntegral f m H y A₁ A₂ k χ σ T = (↑(2 * Real.pi))⁻¹ * ∫ (t : ℝ) in -T..T, AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortKernel f m H y A₁ A₂ k χ (MathlibNt.SieveTheory.LiuWeight.liuPanPerronLine σ t)
Instances For
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortIntegral · compiled type and proof/definition references.
The normalized half-step shift has the same absolute constant 64.
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AnalyticNumberTheory.LargeSieve.ChenLiuCoprimeProducer.halfStepShortIntegral_source_inverse_square · compiled type and proof/definition references.