How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
An outer function with a prescribed power of a vanishing modulus
Example
Let and let for (identified with the unit circle). Then and for every , and the associated outer function is , the principal branch normalized by . Hence for every , with , and is outer; for the function is not rational. The identity (principal branch) is the computation that produces the outer function: its real part is because the power series has boundary real part with Fourier coefficients , .
Facts & Assumptions
Given: A parameter and the function on .
The zero-free function has a holomorphic logarithm on the simply connected disc, normalized by . Its derivative is ; successive derivatives at zero give for . Taylor expansion therefore gives , locally uniformly, and . Since 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)
Jensen's formula gives when is holomorphic and zero-free on a neighbourhood of ; applied to this gives for every (Jensen's formula on a disc, The one-dimensional torus and its normalized Haar integral).
The kernel has and expansion ; has total mass and is bounded for fixed (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).
The outer function satisfies a.e. and, if , with ; it is determined by up to a unimodular constant (Properties of outer functions, Inner, singular inner and outer functions).
For and , , while . Hence for a fixed constant : use for . This is an integrable bound, since for , , and . Dominated convergence therefore applies to and its bounded weighted variants as . (Dominated convergence, The one-dimensional torus and its normalized Haar integral)
A nonzero rational function has near the form with integer and holomorphic and nonzero at : factor the numerator and denominator into their finite powers of , 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
The logarithm is integrable with zero mean. By [F2] and [F5], . Moreover : its positive part is bounded by , and its negative part is integrable by the bound of [F5].
Fourier coefficients and the holomorphic kernel. For , the power series in [F1] shows that has Fourier coefficients at and zero mean. By the limit in [F5], the function has and . The holomorphic kernel is , uniformly convergent in for fixed . Multiplication by and termwise integration are legitimate under the uniform convergence, so , the holomorphic branch with value zero at the origin. Its real part is .
The outer function is . Since by step 1.1, the outer function is well defined and, by step 2.1, the principal branch, with .
Modulus and membership. Since , the function lies in for every , and [F4] gives with and a.e.; explicitly on with equality along , so . On the boundary, for every the principal branch is continuous and ; combined with the a.e. identity this gives off the single point .
Non-rationality for non-integer . If and agreed on with a rational function , then has a finite integer order at , obtained by factoring its numerator and denominator into their powers of . Because along real , this order is positive, so is holomorphic near . But near the principal branch behaves as , which is not of the form with and holomorphic and nonzero at unless (compare the growth of along real : it tends to for and to for ); a rational function has such a finite-order behaviour at each of its singularities, so , a contradiction.
Depends on
- Inner, singular inner and outer functions
- Properties of outer functions
- The one-dimensional torus and its normalized Haar integral
- 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
- A complex power series converges absolutely and uniformly on every closed subdisc strictly inside its disc of convergence
- Jensen's formula on a disc
- Dominated convergence
- The complex exponential by its power series
- Complex polynomials are entire with the power-rule derivative, and rational functions are holomorphic wherever their denominator is nonzero
- Analytic Hardy spaces on the unit disc
- 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
Used by
Dependency tree · two levels
143 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- R. K. Srivastava, Lecture Notes on Hardy Spaces (MA650, IIT Guwahati), §5.10, §6.2 (standard reference, not scraped)
- J. B. Garnett, Bounded Analytic Functions, revised first edition, Chapter II §4 (standard reference, not scraped)