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Reproducing property, Bergman projection and the extremal characterization

Statement

Assume ACω (The Axiom of Countable Choice (ACω)), let m≥1, and let Ω⊆Cm be a nonempty open set. Write kw=KΩ(⋅,w) for the Riesz section at w∈Ω, and let P:L2(Ω)→A2(Ω) be the Hilbert orthogonal projection. Then for every w∈Ω:

  1. For every f∈A2(Ω), f(w)=⟨f,kw⟩=∫Ωf(z)KΩ(z,w)‾ dλΩ(z).
  2. For every f∈L2(Ω), Pf(w)=⟨f,kw⟩=∫Ωf(z)KΩ(z,w)‾ dλΩ(z); P is linear, self-adjoint and contractive, and Pf=f for f∈A2(Ω).
  3. KΩ(w,w)=∥kw∥22=sup⁡{∣f(w)∣2:f∈A2(Ω),∥f∥2≤1} and ∣f(w)∣2≤KΩ(w,w)∥f∥22 for every f∈A2(Ω). If kw≠0, the maximizers in the supremum are exactly λkw/∥kw∥2 with ∣λ∣=1; if kw=0, every member of the closed unit ball attains the supremum, which is 0.

Facts & Assumptions

[A1]

The only choice principle is ACω, inherited through the Bergman Hilbert-space structure and the orthogonal-decomposition and projection suppliers; no full Axiom of Choice is used (The Axiom of Countable Choice (ACω)).

[F1]

A2(Ω) is a closed complex linear subspace of the Hilbert space L2(Ω), with the first-variable-linear integral pairing and unique holomorphic representatives (The Bergman space A2(Ω) and the Bergman kernel, A2(Ω) is closed, and the Bergman kernel is the sum over any complete orthonormal system).

[F2]

For a closed subspace M of a Hilbert space, each x has a unique decomposition x=PMx+(x−PMx) with PMx∈M and x−PMx∈M⊥; PM is the Hilbert orthogonal projection and is the identity on M (Orthogonal decomposition by a closed subspace, The Hilbert orthogonal projection onto a closed subspace).

[F3]

The Hilbert orthogonal projection is linear, self-adjoint and contractive (Hilbert projections are linear, self-adjoint and contractive).

[F4]

Evaluation at w has unique Riesz representer kw∈A2(Ω), f(w)=⟨f,kw⟩, and KΩ(z,w)=kw(z) (The Bergman space A2(Ω) and the Bergman kernel).

[F5]

Cauchy–Schwarz gives ∣⟨f,kw⟩∣≤∥f∥2∥kw∥2, with equality exactly when the pair is linearly dependent (Cauchy–Schwarz: ∣⟨x,y⟩∣≤∥x∥ ∥y∥, with equality exactly for dependent pairs).

Proof

technique · direct, using the Riesz representation and orthogonal projection

Given: ACω, a nonempty open Ω⊆Cm, its Bergman space A2(Ω), and w∈Ω.

1.1A1F1F4given

By [F4], evaluation at w is represented by kw=KΩ(⋅,w), so for each f∈A2(Ω), f(w)=⟨f,kw⟩=∫Ωf(z)kw(z)‾ dλΩ(z). The definition KΩ(z,w)=kw(z) gives the stated reproducing integral.

1.2A1F1F2F3given

By [F1], A2(Ω) is a closed subspace of L2(Ω), so [F2] defines its unique orthogonal projection P. The projection lemma [F3] gives linearity, self-adjointness and contractivity; [F2] also gives Pf=f for f∈A2(Ω).

2.1A1F1F2F4step 1.1step 1.2given

For f∈L2(Ω), [F2] gives f−Pf∈A2(Ω)⊥ and kw∈A2(Ω) by [F4]. Hence ⟨f−Pf,kw⟩=0. Applying step 1.1 to Pf∈A2(Ω) and using linearity in the first variable, Pf(w)=⟨Pf,kw⟩=⟨f,kw⟩; expanding kw(z) as KΩ(z,w) gives the displayed integral.

3.1A1F1F4F5step 1.1given∎

Applying step 1.1 to kw gives KΩ(w,w)=kw(w)=⟨kw,kw⟩=∥kw∥22. For any f∈A2(Ω), [F4] and [F5] imply ∣f(w)∣2≤∥f∥22∥kw∥22, so the supremum over the unit ball is at most ∥kw∥22. If kw≠0, the unit vector kw/∥kw∥2 attains this bound. Any other maximizer must give equality in [F5], hence is linearly dependent on kw; its norm must be 1, so it is exactly λkw/∥kw∥2 with ∣λ∣=1. If kw=0, step 1.1 gives f(w)=0 for every f∈A2(Ω), so the supremum is 0 and every function in the unit ball attains it.

Depends on

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Sources