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The disc Bergman kernel from its monomial basis, with a reproducing check

Example

In A2(D) with Lebesgue area measure the functions ek(z)=(k+1)/π zk, k≥0, form a complete orthonormal system, and

KD(z,w)=∑k≥0k+1πzkw‾k=1π(1−zw‾)2.

The reproducing property is checked directly on the monomials: for every k≥0 and w∈D,

∫Dek(z)KD(z,w)‾ dλ(z)=ek(w).

Facts & Assumptions

[A1]

The only choice assumption is ACω (The Axiom of Countable Choice (ACω)), inherited through the Bergman Hilbert-space, kernel and expansion suppliers; no full Axiom of Choice is used.

[F1]

The monomials zk, k≥0, have squared norms ∥zk∥A2(D)2=π/(k+1) and the normalized monomials form a complete orthonormal system of A2(D) (Weighted monomial integrals and monomial norms for the disc, ball and polydisc, Monomials form complete orthogonal systems of the Bergman spaces of the disc, the ball and the polydisc).

[F2]

For every complete orthonormal system (ej) of A2(Ω) one has KΩ(z,w)=∑jej(z)ej(w)‾, the finite-subset sums converge in A2(Ω) to KΩ(⋅,w), and the series converges absolutely and uniformly on compact subsets (A2(Ω) is closed, and the Bergman kernel is the sum over any complete orthonormal system).

[F3]

The disc Bergman kernel is KD(z,w)=1π(1−zw‾)2 and it satisfies the reproducing identity ⟨f,KD(⋅,w)⟩=f(w) for every f∈A2(D) (Bergman kernels of the disc, ball and polydisc, and Szegő kernels of the disc and ball, Reproducing property, Bergman projection and the extremal characterization).

[F4]

The integral pairing is continuous in its second variable: ∣⟨f,g⟩∣≤∥f∥2∥g∥2 (Cauchy–Schwarz: ∣⟨x,y⟩∣≤∥x∥ ∥y∥, with equality exactly for dependent pairs, The Bergman space A2(Ω) and the Bergman kernel).

[F5]

Natural powers are defined recursively, so zk and ∣z∣2k=zkz‾ k have their stated meanings (Integer powers in the complex field).

Verification

technique · direct, using the complete orthonormal monomial system

Given: ACω, the unit disc with Lebesgue area measure, and k≥0, w∈D.

1.1A1F1F5given

By [F1] the family ek(z)=(k+1)/π zk is a complete orthonormal system of A2(D), with ∥zk∥22=π/(k+1); since z,w∈D we have ∣zw‾∣<1 for the geometric series.

2.1A1F1F2F3step 1.1

By [F2] applied to this complete orthonormal system, KD(z,w)=∑k≥0ek(z)ek(w)‾=1π∑k≥0(k+1)(zw‾)k, and by [F3] this sum equals 1π(1−zw‾)2; this is the displayed series identity.

3.1A1F1F2F4step 2.1

Fix k and w. The holomorphic Fourier sums TN:=∑j≤Nej(w)‾ej converge in A2(D) to KD(⋅,w) by [F2]. Continuity of the pairing [F4] gives ∫Dek(z)KD(z,w)‾ dλ(z)=lim⁡N⟨ek,TN⟩. For N≥k, conjugate-linearity in the second variable and orthonormality give ⟨ek,TN⟩=∑j≤Nej(w)⟨ek,ej⟩=ek(w). This proves the reproducing integral.

4.1A1F1F2F3F4step 2.1step 3.1∎

Step 2.1 identifies the displayed series with the disc Bergman kernel of [F3], and step 3.1 verifies the reproducing identity on every monomial. Since the monomial span is dense by [F1] and both sides of the reproducing identity are continuous in the first variable by [F4], the check extends to all of A2(D) and agrees with the general reproducing theorem.

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