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An outer function with a prescribed power of a vanishing modulus

Example

Let 0<α<∞ and let h(ζ):=∣1−ζ∣α for ζ∈T (identified with the unit circle). Then log⁡h∈L1(T,m) and h∈L∞(T,m)⊆Lp for every p, and the associated outer function is [h](z)=(1−z)α, the principal branch normalized by [h](0)=1. Hence ∣[h]∗(ζ)∣=∣1−ζ∣α=h(ζ) for every ζ≠1, [h]∈H∞(D) with ∥[h]∥∞=2α, and [h] is outer; for α∉N the function [h] is not rational. The identity ∫TK(z,ζ)log⁡∣1−ζ∣ dm(ζ)=log⁡(1−z) (principal branch) is the computation that produces the outer function: its real part is log⁡∣1−z∣=P[log⁡∣1−ζ∣](z) because the power series log⁡(1−z)=−∑n≥1zn/n has boundary real part log⁡∣1−ζ∣ with Fourier coefficients −1/(2∣n∣), n≠0.

Facts & Assumptions

Given: A parameter 0<α<∞ and the function h=∣1−ζ∣α on T.

[F1]

The zero-free function 1−w has a holomorphic logarithm L on the simply connected disc, normalized by L(0)=0. Its derivative is L′(w)=−1/(1−w); successive derivatives at zero give L(n)(0)=−(n−1)! for n≥1. Taylor expansion therefore gives L(w)=−∑n≥1wn/n, locally uniformly, and Re⁡L(w)=log⁡∣1−w∣. Since 1−w lies in the right half-plane, this normalized logarithm is the principal branch. (A nonvanishing holomorphic function on a homologically simply connected domain has a holomorphic logarithm, Star-shaped plane domains are homologically simply connected, A holomorphic logarithm is a primitive of the logarithmic derivative, A holomorphic function equals its Taylor series throughout the largest centred disc in its domain, A complex power series converges absolutely and uniformly on every closed subdisc strictly inside its disc of convergence)

[F2]

Jensen's formula gives log⁡∣F(0)∣=12π∫02πlog⁡∣F(reiθ)∣ dθ when F is holomorphic and zero-free on a neighbourhood of {∣w∣≤r}; applied to F(w)=1−rw this gives ∫Tlog⁡∣1−rζ∣ dm(ζ)=0 for every 0<r<1 (Jensen's formula on a disc, The one-dimensional torus and its normalized Haar integral).

[F3]

The kernel K(z,ζ)=(ζ+z)/(ζ−z) has Re⁡K=P(z,ζ) and expansion K(z,ζ)=1+2∑n≥1znζ−n; P(z,⋅) has total mass 1 and is bounded for fixed z (The Poisson kernel on the unit disc, The Poisson integral of a finite complex boundary measure, The Poisson kernel is positive, has total mass one, and concentrates at a boundary point, Inner, singular inner and outer functions).

[F4]

The outer function [h]=exp⁡(∫Klog⁡h dm) satisfies ∣[h]∗∣=h a.e. and, if h∈L∞, [h]∈H∞ with ∣[h]∣≤∥h∥∞; it is determined by h up to a unimodular constant (Properties of outer functions, Inner, singular inner and outer functions).

[F5]

For 1/2≤r<1 and ∣ζ∣=1, ∣1−rζ∣2=(1−r)2+r∣1−ζ∣2≥∣1−ζ∣2/2, while ∣1−rζ∣≤2. Hence ∣log⁡∣1−rζ∣∣≤C(1+∣1−ζ∣−1/2) for a fixed constant C: use ∣log⁡t∣≤C′(1+t−1/2) for 0<t≤2. This is an integrable bound, since for ∣θ∣≤π, ∣1−eiθ∣=2∣sin⁡(θ/2)∣≥2∣θ∣/π, and ∫0πθ−1/2dθ<∞. Dominated convergence therefore applies to log⁡∣1−rζ∣ and its bounded weighted variants as r↑1. (Dominated convergence, The one-dimensional torus and its normalized Haar integral)

[F6]

A nonzero rational function R=P/Q has near 1 the form (z−1)mg(z) with integer m and g holomorphic and nonzero at 1: factor the numerator and denominator into their finite powers of z−1, then divide the remaining nonvanishing polynomials. (Complex polynomials are entire with the power-rule derivative, and rational functions are holomorphic wherever their denominator is nonzero)

Verification

1.1givenF2F5algebra

The logarithm log⁡∣1−ζ∣ is integrable with zero mean. By [F2] and [F5], ∫Tlog⁡∣1−ζ∣ dm=lim⁡r↑1∫Tlog⁡∣1−rζ∣ dm=0. Moreover log⁡∣1−ζ∣∈L1: its positive part is bounded by log⁡2, and its negative part is integrable by the bound of [F5].

2.1step 1.1F1F2F3F5algebra

Fourier coefficients and the holomorphic kernel. For 0<r<1, the power series in [F1] shows that log⁡∣1−rζ∣ has Fourier coefficients −rn/(2n) at ±n and zero mean. By the L1 limit in [F5], the function u(ζ)=log⁡∣1−ζ∣ has u^(0)=0 and u^(±n)=−1/(2n). The holomorphic kernel is K(z,ζ)=1+2∑n≥1znζ−n, uniformly convergent in ζ for fixed ∣z∣<1. Multiplication by u∈L1 and termwise integration are legitimate under the uniform convergence, so ∫TK(z,ζ)u(ζ) dm(ζ)=u^(0)+2∑n≥1znu^(n)=−∑n≥1zn/n=log⁡(1−z), the holomorphic branch with value zero at the origin. Its real part is log⁡∣1−z∣.

3.1step 2.1F3algebra

The outer function is (1−z)α. Since log⁡h=αlog⁡∣1−ζ∣∈L1 by step 1.1, the outer function is well defined and, by step 2.1, [h](z)=exp⁡(∫TK(z,ζ)log⁡h(ζ) dm(ζ))=exp⁡(αlog⁡(1−z))=(1−z)α, the principal branch, with [h](0)=1.

4.1step 3.1F4algebra

Modulus and H∞ membership. Since 0≤h≤2α, the function h lies in L∞(T,m)⊆Lp for every p, and [F4] gives [h]∈H∞ with ∣[h]∣≤2α and ∣[h]∗∣=h a.e.; explicitly ∣(1−z)α∣=∣1−z∣α≤2α on D with equality along z→−1, so ∥[h]∥∞=2α. On the boundary, for every ζ≠1 the principal branch is continuous and ∣(1−ζ)α∣=∣1−ζ∣α=h(ζ); combined with the a.e. identity this gives ∣[h]∗∣=h off the single point 1.

5.1step 3.1F6algebra∎

Non-rationality for non-integer α. If α∉N and (1−z)α agreed on D with a rational function R, then R has a finite integer order m at 1, obtained by factoring its numerator and denominator into their powers of z−1. Because R(x)=(1−x)α→0 along real x↑1, this order is positive, so R is holomorphic near 1. But near z=1 the principal branch behaves as (1−z)α, which is not of the form (1−z)mg(z) with m∈Z and g holomorphic and nonzero at 1 unless α∈Z (compare the growth of (1−z)α−m along real z→1−: it tends to 0 for α>m and to +∞ for α<m); a rational function has such a finite-order behaviour at each of its singularities, so α∈N, a contradiction.

Depends on

Used by

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Sources