Bounded Cauchy differentiation between closed disks #
The operator integrates on a circle of radius σ - ρ centered at each point
of the smaller disk. It is defined on all continuous outer-disk functions;
on holomorphic inputs it agrees with the actual complex derivative.
Disk: an abbreviation for ↥(closedBall c r).
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Inclusion, bundling toFun, continuous_toFun.
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- NavierStokes.CauchyRestriction.inclusion c h = { toFun := fun (z : NavierStokes.CauchyRestriction.Disk c ρ) => ⟨↑z, ⋯⟩, continuous_toFun := ⋯ }
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Restriction linear, bundling toFun, map_add, map_smul.
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- One or more equations did not get rendered due to their size.
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Restriction continuous linear map, given by (restrictionLinear c h).mkContinuous 1 (by intro f simpa only [one_mul] using norm_restrictionLinear_le c h f).
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Sample, bundling toFun, continuous_toFun.
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- NavierStokes.CauchyRestriction.sample c hgap θ = { toFun := fun (z : NavierStokes.CauchyRestriction.Disk c ρ) => ⟨↑z + circleMap 0 (σ - ρ) θ, ⋯⟩, continuous_toFun := ⋯ }
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Integrand, given by weight (σ - ρ) θ • f.comp (sample c hgap θ).
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- NavierStokes.CauchyRestriction.integrand c hgap f θ = NavierStokes.CauchyRestriction.weight (σ - ρ) θ • f.comp (NavierStokes.CauchyRestriction.sample c hgap θ)
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Cauchy map, given by (2 * Real.pi * I : ℂ)⁻¹ • ∫ θ : ℝ in (0)..(2 * Real.pi), integrand c hgap f θ.
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Derivative continuous linear map as an element of C(Disk c σ, E) →L[ℂ] C(Disk c ρ, E).
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- NavierStokes.CauchyRestriction.derivativeCLM c hgap = { toFun := NavierStokes.CauchyRestriction.cauchyMap c hgap, map_add' := ⋯, map_smul' := ⋯ }.mkContinuous (σ - ρ)⁻¹ ⋯
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Use any holomorphic extension agreeing with the continuous outer-disk input.
Of continuous on, given by ⟨fun z => F z, hF.domRestrict⟩.
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- NavierStokes.CauchyRestriction.ofContinuousOn c r F hF = { toFun := fun (z : NavierStokes.CauchyRestriction.Disk c r) => F ↑z, continuous_toFun := ⋯ }
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Agreement with the actual derivative under holomorphy in the open disk and continuity on its closure. No smoothness of the derivative is assumed.
On holomorphic data, further restriction of the derivative does not depend on which smaller target disk was used to construct the Cauchy integral.
Restricting the source disk also gives the same derivative on common smaller disks, provided the source represents a holomorphic function.