An function orthogonal to all of vanishes
ProvedCauchyRiemannIndex.eq_zero_of_forall_integral_inner_eq_zerodualityfunctional-analysismeasure-theory
Let be a -finite measure, a complete real inner product space and . If satisfies
then in .
The pairing therefore separates the points of . This is the injectivity half of the duality between and , and it is used to identify annihilators of subspaces of inside .
Formalization Note. is Lp E p μ with Fact (1 ≤ p) and p ≠ ⊤, and likewise for . No relation between and is assumed; the integral is the Bochner integral of , which is by convention when that function is not integrable.
Preamble
import Mathlib.MeasureTheory.Function.LpSpace.Basic import Mathlib.MeasureTheory.Integral.Bochner.Basic import Mathlib.Analysis.InnerProductSpace.Basic
Formal statement
namespace CauchyRiemannIndex
open MeasureTheory
open scoped ENNReal
/-- Let `μ` be σ-finite, `E` a complete real inner product space and `1 ≤ p, q < ∞`. If
`g ∈ L^q(μ; E)` satisfies `∫ ⟨f, g⟩ dμ = 0` for every `f ∈ L^p(μ; E)`, then `g = 0`. -/
theorem eq_zero_of_forall_integral_inner_eq_zero {α E : Type*} [MeasurableSpace α]
(μ : Measure α) [SigmaFinite μ] [NormedAddCommGroup E] [InnerProductSpace ℝ E]
[CompleteSpace E] (p q : ℝ≥0∞) [Fact (1 ≤ p)] [Fact (1 ≤ q)] (hp : p ≠ ⊤) (hq : q ≠ ⊤)
(g : Lp E q μ) (hg : ∀ f : Lp E p μ, ∫ x, inner ℝ (f x) (g x) ∂μ = 0) : g = 0 := by
sorry
end CauchyRiemannIndex
Source
Standard; see e.g. H. Brezis, Functional Analysis, Sobolev Spaces and Partial Differential Equations, Springer 2011, Section 4.3