Lp Extension #
Part of the Caffarelli–Kohn–Nirenberg partial regularity proof.
Submodule of Lᵖ classes whose representatives also belong to L².
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- One or more equations did not get rendered due to their size.
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Representative-level operator data sufficient to construct a bounded continuous Lᵖ extension.
- T : (Parabolic.Vec3 → ℝ) → Parabolic.Vec3 → ℝ
Operator on scalar representatives to be extended from the Lᵖ–L² intersection.
- measurable {f : Parabolic.Vec3 → ℝ} : MeasureTheory.MemLp f 2 MeasureTheory.volume → Measurable (self.T f)
- output_mem {f : Parabolic.Vec3 → ℝ} : MeasureTheory.MemLp f p MeasureTheory.volume → MeasureTheory.MemLp f 2 MeasureTheory.volume → MeasureTheory.MemLp (self.T f) p MeasureTheory.volume
- congr_ae {f g : Parabolic.Vec3 → ℝ} : MeasureTheory.MemLp f 2 MeasureTheory.volume → MeasureTheory.MemLp g 2 MeasureTheory.volume → f =ᵐ[MeasureTheory.volume] g → self.T f =ᵐ[MeasureTheory.volume] self.T g
- add_ae {f g : Parabolic.Vec3 → ℝ} : MeasureTheory.MemLp f 2 MeasureTheory.volume → MeasureTheory.MemLp g 2 MeasureTheory.volume → self.T (f + g) =ᵐ[MeasureTheory.volume] self.T f + self.T g
- smul_ae (c : ℝ) {f : Parabolic.Vec3 → ℝ} : MeasureTheory.MemLp f 2 MeasureTheory.volume → self.T (c • f) =ᵐ[MeasureTheory.volume] c • self.T f
- bound {f : Parabolic.Vec3 → ℝ} (hf : MeasureTheory.MemLp f p MeasureTheory.volume) (hf₂ : MeasureTheory.MemLp f 2 MeasureTheory.volume) : ‖MeasureTheory.MemLp.toLp (self.T f) ⋯‖ ≤ C * ‖MeasureTheory.MemLp.toLp f hf‖
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Linear operator on the dense Lᵖ–L² intersection induced by the extension data.
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- CKN.Foundation.Euclidean.lpInterL2Map h = { toFun := fun (u : ↥(CKN.Foundation.Euclidean.lpInterL2Submodule p)) => MeasureTheory.MemLp.toLp (h.T ↑↑↑u) ⋯, map_add' := ⋯, map_smul' := ⋯ }
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Continuous extension of the bounded operator from the dense Lᵖ–L² intersection.
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Measurable representative of the extended operator, defined as zero outside its Lᵖ domain.
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- One or more equations did not get rendered due to their size.
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Pointwise presentation of the continuous Lᵖ extension.
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Sum of the componentwise extended operators acting on a tensor source.
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- CKN.Foundation.Euclidean.lpExtensionTensorOperator hp h G x = ∑ i : Fin 3, ∑ j : Fin 3, CKN.Foundation.Euclidean.lpExtensionOperator hp (h i j) (G i j) x
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View a function belonging to both Lᵖ and L² as an element of the intersection submodule.
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- CKN.Foundation.Euclidean.lpInterL2Input hf hf₂ = ⟨MeasureTheory.MemLp.toLp f hf, ⋯⟩
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Continuous linear pairing against a fixed function in the conjugate Lᵖ space.