Alphabeta Math
Pipeline-generated
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.

Analytic Hardy Spaces and Canonical Factorisation

1 · Prerequisites

2 · Summary

This page develops the analytic Hardy spaces Hp(D) on the unit disc and their canonical factorisation. The classes are defined in Analytic Hardy spaces on the unit disc by boundedness of the radial Lp means, with the p<1 quasi-norm made explicit; Radial p-means of a holomorphic function are nondecreasing proves that the radial means increase with the radius, so Hq⊆Hp for q>p with norm comparison, and identifies the norm as a limit.

The zero theory starts from Jensen's formula: The zero set of a Hardy function satisfies the Blaschke condition shows that the zeros of a nonzero Hp function satisfy the Blaschke condition. Normalized Blaschke factors and their products are studied in Blaschke factors and Blaschke products and Boundary values and zeros of a Blaschke product, which gives the exact zero sets, the bound ∣B∣≤1 and the unimodular boundary function, and F. Riesz factorization of a Hardy-space function factors f=Bg with a zero-free g of the same norm.

The canonical factors are defined in Inner, singular inner and outer functions: inner functions, singular inner functions Sμ built from finite positive measures, and outer functions [h] built from logarithmically integrable moduli. Their properties are proved in Properties of the singular functions Sμ, Properties of outer functions, and Zero-free inner functions are unimodular multiples of singular inner functions, and assembled into the inner-outer factorization f=λBSμF of Inner-outer factorisation of a Hardy-space function.

The boundary theory is Fatou's theorem, Fatou's boundary theorem for analytic Hardy spaces: nontangential limits exist almost everywhere, the radial functions converge in Lp for finite p, the boundary norm equals the Hp norm, and for p≥1 the function is the Poisson integral of its boundary values. Log-integrability of the boundary modulus is Log-integrability of the boundary values of a Hardy function, its Poisson-Jensen companion is Poisson-Jensen inequality for Hardy functions, and the H1 boundary measure is analysed in The F. and M. Riesz theorem and Cauchy representation of an H1 function from its boundary values.

The larger classes are treated next: the Nevanlinna class N(D) in The Nevanlinna class on the disc with the equivalent sup-mean criterion A harmonic majorant of log^+|F| exists exactly when the radial log^+ means are bounded, the quotient representation The Nevanlinna class is a bounded quotient class, internal Blaschke factorization Blaschke factorization of a Nevanlinna-class function and boundary values with log-integrability Boundary values and log-integrability of Nevanlinna-class functions; then the Smirnov class N+(D) in The Smirnov class on the disc, its quotient characterisation The Smirnov class is the class of quotients by outer bounded functions and the maximum principle N+∩Lp=Hp of A maximum principle for the Smirnov class: N+∩Lp=Hp.

Countable choice suffices for the definitions, Blaschke and outer properties, Nevanlinna and Smirnov results, the analytic Hardy boundary theorem and the F. and M. Riesz/Cauchy conclusions. The local special proofs are Bounded holomorphic disc functions have Poisson boundary data and Fatou limits under countable choice, Singular circle measures have Poisson integral tending nontangentially to zero almost everywhere, Finite positive circle measures admit a Lebesgue decomposition under countable choice, Complex circle measures have finite regular total variation under countable choice, and Finite complex circle measures are determined by Fourier coefficients and Poisson integrals. The zero-free inner representation and canonical factorisation retain their original explicit AC assumptions for the general Herglotz supplier. The examples companion is analytic-hardy-spaces-and-canonical-factorisation-examples.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

Analytic Hardy spaces on the unit disc

Definition

Assume countable choice. Let T=R/Z be the one-dimensional torus, identified with the Euclidean unit circle through φ([t])=e2πit, and let m be its normalized Haar measure, a probability measure on the compact metric space T (The one-dimensional torus and its normalized Haar integral). Let D:={ z∈C:∣z∣<1 } be the unit disc of The unit disc, the upper half-plane, and Blaschke factors, and let f:D→C be a function, holomorphic in the sense of Complex differentiability at a point, the complex derivative, holomorphic functions, and entire functions when required below. For 0≤r<1 write fr:T→C,fr(ζ):=f(rζ). If f is holomorphic, each fr is continuous, hence measurable with finite modulus; for 0<p<∞ the number (∫T∣f(rζ)∣p dm(ζ))1/p is therefore a well-defined element of [0,+∞), computed from the continuous representative of fr in the conventions of Complex Lp classes and Euclidean test-function conventions.

The classes Hp(D). For 0<p<∞ define Hp(D):={ f holomorphic on D: ∥f∥Hp:=sup⁡0≤r<1(∫T∣f(rζ)∣p dm(ζ))1/p<+∞ }, and for p=∞ define H∞(D):={ f holomorphic on D: ∥f∥∞:=sup⁡z∈D∣f(z)∣<+∞ }. Writing ur(ζ):=u(rζ) for any function u on D, the definition of H∞ is equivalently ∥f∥∞=sup⁡0≤r<1ess sup⁡T∣fr∣: a continuous function on the compact space T has the same supremum and essential supremum, because a nonempty open subset of T has positive m-measure, and every z∈D has the form rζ with r=∣z∣ and ζ∈T (The essential supremum of a measurable function with respect to a measure, The one-dimensional torus and its normalized Haar integral).

The (quasi-)norm assertions. For 1≤p≤∞, ∥⋅∥Hp is a norm on the complex vector space Hp(D). Homogeneity ∥λf∥Hp=∣λ∣ ∥f∥Hp for λ∈C and the triangle inequality ∥f+g∥Hp≤∥f∥Hp+∥g∥Hp follow by taking suprema over r of the corresponding statements for the Lp classes of the continuous functions fr,gr on the probability space (T,m) (Complex Holder, Minkowski, and the quotient norm); the case p=∞ is the elementary inequality between suprema of moduli, and ∥f∥∞=sup⁡r<1sup⁡ζ∣f(rζ)∣ holds because the radii and circle points range over D. All Hp(D) are closed under finite linear combinations: sums and scalar multiples of holomorphic functions are holomorphic (Complex differentiability at a point, the complex derivative, holomorphic functions, and entire functions), and the (quasi-)norm of a finite linear combination is finite by the inequalities just stated.

For 0<p<1, ∥⋅∥Hp is a quasi-norm, not a norm. For complex numbers a,b one has ∣a+b∣p≤∣a∣p+∣b∣p, because the power function is subadditive on [0,∞) when 0<p≤1: for x,y≥0 it suffices to prove (x+y)p≤xp+yp, which is trivial when y=0, and for y>0 and t=x/y≥0 is the claim (1+t)p≤1+tp; the function h(t):=1+tp−(1+t)p is continuous on [0,∞) with h(0)=0 and, for t>0, h′(t)=p (tp−1−(1+t)p−1)≥0 because p−1≤0 and t≤1+t, so h is nondecreasing and h≥0. Integrating at each radius gives ∫T∣f(rζ)+g(rζ)∣p dm(ζ)≤∫T∣f(rζ)∣p dm(ζ)+∫T∣g(rζ)∣p dm(ζ), and taking suprema over r yields ∥f+g∥Hpp≤∥f∥Hpp+∥g∥Hpp. Writing A:=∥f∥Hp, B:=∥g∥Hp and x:=A/(A+B) when A+B>0, the bound xp+(1−x)p≤21−p for 0≤x≤1 (the maximum of the concave left side is at x=1/2) gives Ap+Bp≤21−p(A+B)p, hence ∥f+g∥Hp≤21p−1(∥f∥Hp+∥g∥Hp), the quasi-norm statement; homogeneity and the case A+B=0 are immediate. The quasi-norm inequality for p<1 is the only place where the constant 21/p−1 enters, and no further structure (completeness, separability, duality) of these spaces is asserted here or used later.

The ordinary triangle inequality does fail for each 0<p<1. Put fn(z)=(1+z)n, gn(z)=(1−z)n for positive integers n, holomorphic polynomials (Complex polynomials are entire with the power-rule derivative, and rational functions are holomorphic wherever their denominator is nonzero). Any polynomial h is bounded on the closed disc, hence lies in Hp; the radial-means certifier Radial p-means of a holomorphic function are nondecreasing ↗ and uniform boundary continuity give ∥h∥Hpp=∫T∣h(ζ)∣pdm. Write An=∫∣fn∣pdm=∫∣gn∣pdm, using Haar invariance under ζ↦−ζ, and Dn=∫min⁡(∣fn∣p,∣gn∣p)dm. The already proved subadditivity gives ∣u+v∣p≥max⁡(∣u∣p,∣v∣p)−min⁡(∣u∣p,∣v∣p), hence ∫∣fn+gn∣pdm≥2An−2Dn. Since ∣1+ζ∣2+∣1−ζ∣2=4, Dn≤2np/2. The open set U={ζ∈T:∣1+ζ∣>3} contains 1, so c=m(U)>0 and An≥c 3np/2 (The one-dimensional torus and its normalized Haar integral). Thus Dn/An≤c−1((2/3)p/2)n→0 (For ∣r∣<1 the sequence rk is null, and for ∣r∣>1 the sequence ∣r∣k diverges to +∞). For sufficiently large n, Dn/An<1−2p−1, so ∥fn+gn∥Hpp>2pAn and ∥fn+gn∥Hp>2An1/p=∥fn∥Hp+∥gn∥Hp. This proves the claimed failure without any later factorization or outer-function existence result.

For p=∞, ∥f∥∞=0 immediately gives f≡0. For 0<p<∞, if ∥f∥Hp=0, then ∫T∣f(rζ)∣p dm(ζ)=0 for every 0≤r<1, so ∣fr∣p=0 m-almost everywhere (A nonnegative measurable function has integral 0 exactly when it vanishes almost everywhere), hence fr=0 everywhere since fr is continuous; taking r=∣z∣ for z≠0 and r=0 gives f≡0. Thus ∥⋅∥Hp is a genuine norm on Hp(D) for 1≤p≤∞ and a genuine quasi-norm for 0<p<1.

This item defines the classes and their (quasi-)norms only. The monotonicity of the radial p-means in r, and with it the containments Hq(D)⊆Hp(D) for q>p together with ∥f∥Hp≤∥f∥Hq, are proved in Radial p-means of a holomorphic function are nondecreasing ↗, which is the item that certifies this definition. No choice principle beyond countable choice is used.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Radial p-means of a holomorphic function are nondecreasing

Statement

Let f:D→C be holomorphic and let 0<p<∞. For all 0<r≤R<1, ∫T∣f(rζ)∣p dm(ζ)≤∫T∣f(Rζ)∣p dm(ζ). Consequently, for f∈Hp(D) the nondecreasing radial means satisfy ∥f∥Hpp=lim⁡r↑1∫T∣f(rζ)∣p dm(ζ), so that ∥f∥Hp=lim⁡r↑1∥fr∥Lp. Moreover, for 0<p<q≤∞ one has Hq(D)⊆Hp(D) and ∥f∥Hp≤∥f∥Hq for every f∈Hq(D).

Facts & Assumptions

Given: A holomorphic function f on D, an exponent 0<p<∞, radii 0<r≤R<1, and the function u:=∣f∣p.

[L1]

If f is not identically zero, then u=∣f∣p is subharmonic on D; f is smooth, hence continuous, so u is continuous on D (Positive powers of the modulus of a holomorphic function are subharmonic, Holomorphic functions are real analytic and smooth in their two real coordinates).

[L2]

For a subharmonic function u on D and a disc D(0,R)⋐D, the Poisson modification PD(0,R)u is harmonic on D(0,R) and satisfies PD(0,R)u≥u on D, where it is defined by boundary approximations ϕn↓u∣∂D(0,R) and the unique harmonic extensions hn of ϕn to the disc; when u is continuous on D(0,R)‾ one may take ϕn:=u∣∂D(0,R)+1/(n+1) for n≥0. If H is the Poisson extension of the continuous boundary datum u∣∂D(0,R), uniqueness gives hn=H+1/(n+1), so PD(0,R)u=H inside the disc (Poisson modification on a compactly contained disc, Poisson modification is subharmonic and majorizes the original function, The Poisson integral gives the unique continuous harmonic extension on the closed unit disc).

[L3]

For continuous boundary data ϕ on the circle of radius R, the function z↦∫TP(z/R,η) ϕ(Rη) dm(η)(∣z∣<R) is the unique harmonic extension of ϕ to D(0,R), continuous on the closed disc, where P is the Poisson kernel of the unit disc (The Poisson integral gives the unique continuous harmonic extension on the closed unit disc, The Poisson kernel on the unit disc, The Poisson integral of a finite complex boundary measure). In particular its value at z=0 is ∫Tϕ(Rη) dm(η), because P(0,η)=1.

[L4]

A harmonic function w on a neighbourhood of the closed disc D(0,r)‾ satisfies w(0)=∫Tw(rζ) dm(ζ), the circle mean-value property in the torus normalization (Plane harmonic functions satisfy the mean-value property, The circle and disc mean-value properties, The one-dimensional torus and its normalized Haar integral).

[L5]

On the probability space (T,m), for 0<p<q<∞ and measurable g one has (∫T∣g∣p dm)1/p≤(∫T∣g∣q dm)1/q. The case of an infinite right-hand side is immediate. Otherwise, for p≥1 use Lyapunov's moment inequality on a probability space; for p<1, apply Jensen's inequality for expectation to the integrable variable X=∣g∣q and the convex function φ(t)=−tp/q on [0,∞). Its composition is integrable because Xp/q≤1+X, and Jensen gives ∫∣g∣p dm≤(∫∣g∣q dm)p/q. For q=∞, integrating the almost-everywhere bound ∣g∣p≤∥g∥∞p gives the same comparison for every p>0.

[L6]

The classes Hp(D), 0<p≤∞, and their (quasi-)norms are defined by the suprema of the radial Lp means over 0≤r<1 (Analytic Hardy spaces on the unit disc).

Proof

technique · direct
1.1givenL1

Reduction and subharmonicity. If f≡0, then both sides of the asserted inequality vanish and the further claims are immediate, so assume f is not identically zero. Then u=∣f∣p is subharmonic on D and continuous, by [L1].

1.2L5

The Lp comparison. Let 0<p<q<∞ and let g be measurable on T. By [L5], ∥g∥Lp≤∥g∥Lq; and if q=∞, ∥g∥Lp≤∥g∥∞.

2.1step 1.1L2L3

The modification is the Poisson extension of the boundary data. Fix 0<R<1. By [L2] and continuity of u on D(0,R)‾ (a compact subset of D), the Poisson modification h:=PD(0,R)u is harmonic on D(0,R), satisfies h≥u on D, and is the Poisson extension of u∣∂D(0,R); hence by [L3], h(z)=∫TP(z/R,η) u(Rη) dm(η)(∣z∣<R),h(0)=∫Tu(Rη) dm(η).

2.2step 1.2L6algebra

Containment of the classes. Let 0<p<q≤∞ and f∈Hq(D); every radius r∈[0,1) satisfies ∥fr∥Lp≤∥fr∥Lq by step 1.2, and ∥fr∥Lq≤∥f∥Hq by the definition of the supremum when q<∞, while ∥fr∥Lq≤∥f∥Hq for q=∞ as well because ∣fr∣≤∥f∥H∞ pointwise. Taking suprema over r gives ∥f∥Hp≤∥f∥Hq<+∞, so f∈Hp(D) and the containment Hq(D)⊆Hp(D) holds with the asserted norm comparison.

3.1step 2.1L4algebra

Monotonicity of the means. Let 0<r≤R<1. The case r=R is an equality of the two integrals, so assume r<R. Step 2.1 gives h≥u on D(0,r) and h(0)=∫Tu(Rη) dm(η); since h is harmonic on D(0,R), hence on a neighbourhood of the closed disc D(0,r)‾ for r<R, integrating the inequality u(rζ)≤h(rζ) over T against m and applying the mean value property [L4] gives ∫T∣f(rζ)∣p dm(ζ)=∫Tu(rζ) dm(ζ)≤∫Th(rζ) dm(ζ)=h(0)=∫T∣f(Rη)∣p dm(η).

4.1step 1.1step 3.1L6algebra

The supremum is the limit. Let f∈Hp(D). Continuity of u=∣f∣p at 0 gives sup⁡ζ∈T∣u(rζ)−u(0)∣→0 as r↓0. Thus the mean inequality of step 3.1 also holds when the smaller radius is 0. The map r↦∫T∣f(rζ)∣p dm(ζ) is therefore nondecreasing on [0,1) and bounded by ∥f∥Hpp<+∞ by [L6]. A nondecreasing bounded real function on [0,1) has supremum equal to its limit as r↑1, so sup⁡0≤r<1(∫T∣f(rζ)∣p dm(ζ))1/p=lim⁡r↑1(∫T∣f(rζ)∣p dm(ζ))1/p, that is, ∥f∥Hp=lim⁡r↑1∥fr∥Lp.

5.1step 3.1step 4.1step 2.2∎

Assembly. The mean inequality is step 3.1, the limit description of the norm is step 4.1, and the containment together with the norm comparison is step 2.2; all were proved under the given hypotheses.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

The zero set of a Hardy function satisfies the Blaschke condition

Statement

Let f be holomorphic on D with f≢0, and suppose that lim inf⁡r↑1∫Tlog⁡∣f(rζ)∣ dm(ζ)<+∞, where log⁡∣f∣=−∞ at the zeros of f. This hypothesis holds in particular for every f∈Hp(D), 0<p≤∞: the logarithmic Jensen inequality and Radial p-means of a holomorphic function are nondecreasing give ∫Tlog⁡∣fr∣ dm≤log⁡∥f∥Hp for 0<p<∞ and ∫Tlog⁡∣fr∣ dm≤log⁡∥f∥∞ for p=∞. Let (an)n≥1 be the zeros of f in D repeated according to multiplicity. Then f has finite vanishing order m≥0 at the origin (with m=0 when f(0)≠0), and the nonzero zeros satisfy ∑n: an≠0log⁡1∣an∣<+∞,hence∑n≥1(1−∣an∣)<+∞. (The second inequality uses log⁡(1/x)≥1−x for 0<x≤1. The finite vanishing order at the origin contributes finitely many terms equal to 1 to the second sum and does not affect convergence of the nonzero part.)

Facts & Assumptions

Given: A holomorphic function f≢0 on D satisfying the displayed liminf hypothesis, its zero sequence (an) repeated with multiplicity, and (where used) the exponent p∈(0,∞].

[L1]

If f≢0, then f has a finite vanishing order at the origin: there are an integer m≥0 and a holomorphic g:D→C with f(z)=zmg(z) for all z∈D and g(0)≠0; the zeros of f are then the origin together with the zeros of g, with multiplicities, and f(r⋅) is holomorphic on a neighbourhood of the closed unit disc for every 0<r<1 (A holomorphic function equals its Taylor series throughout the largest centred disc in its domain, Identity theorem for holomorphic functions, Characterizations of removable singularities, Complex differentiability at a point, the complex derivative, holomorphic functions, and entire functions).

[L2]

Jensen's formula on a disc: if F is holomorphic on a neighbourhood of {∣z∣≤R}, F(0)≠0, and F has no zero on ∣z∣=R, then log⁡∣F(0)∣=12π∫02πlog⁡∣F(Reit)∣ dt−∑∣a∣<Rlog⁡R∣a∣, the sum over the zeros of F in ∣z∣<R with multiplicity; for a radius meeting boundary zeros the identity is recovered by taking r↑R through radii that avoid zeros on ∣z∣=r (Jensen's formula on a disc).

[L3]

Logarithmic Jensen inequality. For a measurable Y≥0 on the probability space (T,m) with ∫TY dm<+∞, one has ∫Tlog⁡Y dm≤log⁡∫TY dm, with both sides in [−∞,∞) and log⁡0:=−∞. Indeed, for gn:=max⁡(log⁡Y,−n) the convex Jensen inequality applied to gn and the convex function exp⁡ gives exp⁡(∫gn dm)≤∫exp⁡(gn) dm≤∫Y dm+e−n, and passing to the limit in n gives the claim (Jensen's integral inequality for a probability measure, Jensen's inequality for expectation, The one-dimensional torus and its normalized Haar integral).

[L4]

The classes Hp(D) and their norms are defined by suprema of radial Lp means; for f∈Hp, 0<p<∞, one has ∥fr∥Lp≤∥f∥Hp for every 0≤r<1 by definition of the supremum, and for p=∞, ∣f(z)∣≤∥f∥H∞ for all z (Analytic Hardy spaces on the unit disc, Radial p-means of a holomorphic function are nondecreasing).

[L5]

For 0<x≤1 one has log⁡(1/x)≥1−x; and for a sequence of nonnegative terms increasing to a limit, the sum of the limits is the limit of the sums (monotone convergence for series) (Monotone convergence for the integral).

Proof

technique · direct
1.1givenL1algebra

Reduction at the origin. By [L1] write f(z)=zmg(z) with m≥0, g holomorphic on D and g(0)≠0; this m is the finite order of the zero of f at the origin, and f has no other zeros at the origin. For 0<r<1, ∫Tlog⁡∣f(rζ)∣ dm(ζ)=mlog⁡r+∫Tlog⁡∣g(rζ)∣ dm(ζ) (for m=0 this is the identity; for m≥1 it holds because log⁡∣rmζm∣=mlog⁡r is constant on the circle). Hence lim inf⁡r↑1∫Tlog⁡∣g(rζ)∣ dm(ζ)=lim inf⁡r↑1∫Tlog⁡∣f(rζ)∣ dm(ζ)<+∞, because mlog⁡r→0.

1.2L3algebra

The logarithmic Jensen inequality at each radius. Let F be holomorphic on a neighbourhood of the closed unit disc and not identically zero. Applying [L3] to Y:=∣F∣p with 0<p<∞, and noting ∫T∣F∣p dm=∥F∥Lpp<+∞ because F is continuous, gives ∫Tlog⁡∣F∣ dm=1p∫Tlog⁡∣F∣p dm≤1plog⁡∫T∣F∣p dm=log⁡∥F∥Lp. For p=∞, log⁡∣F∣≤log⁡∥F∥∞ pointwise, so ∫Tlog⁡∣F∣ dm≤log⁡∥F∥∞.

1.3givenL1L2algebra

Jensen's formula for g. Fix 0<r<1 such that no ∣an∣ equals r, and apply [L2] with R=1 to F:=g(r ⋅ ), whose zeros in ∣z∣<1 are the points an/r for those zeros an of f (equivalently of g) with 0<∣an∣<r: −∑0<∣an∣<rlog⁡r∣an∣=log⁡∣g(0)∣−∫Tlog⁡∣g(rζ)∣ dm(ζ).

2.1step 1.2L4

The Hp clause. Let f∈Hp(D). If p=∞, then for every 0<r<1 step 1.2 applied to fr and [L4] give ∫Tlog⁡∣f(rζ)∣ dm(ζ)≤log⁡∥fr∥∞≤log⁡∥f∥H∞<+∞, so the liminf hypothesis holds (when ∥f∥H∞=0 then f≡0, excluded). If 0<p<∞, the same steps give ∫Tlog⁡∣f(rζ)∣ dm(ζ)≤log⁡∥fr∥Lp≤log⁡∥f∥Hp<+∞.

2.2step 1.3L1L2algebra

Good radii and their limiting means. Jensen's formula in step 1.3, together with its boundary-zero limiting form in [L2], says that M(r):=∫log⁡∣g(rζ)∣dm=log⁡∣g(0)∣+∑0<∣an∣<rlog⁡(r/∣an∣) for every 0<r<1; a zero on the radius contributes zero in that limiting identity. Thus M(r) is nondecreasing. There are finitely many zero moduli in any closed subdisc, so a strictly increasing sequence of radii avoiding them and tending to 1 can be chosen recursively, for instance from the rational radii in successive intervals tending to 1. Monotonicity makes its means tend to lim inf⁡r↑1M(r). Along these radii, ∑0<∣an∣<rjlog⁡(rj/∣an∣)=M(rj)−log⁡∣g(0)∣ by step 1.3.

3.1step 2.2L1L5algebra

The Blaschke condition. In the identity of step 2.2 the left-hand side Sj:=∑0<∣an∣<rjlog⁡(rj/∣an∣) has nonnegative terms that increase with j and eventually include every nonzero zero, so Sj increases to S:=∑n:an≠0log⁡(1/∣an∣)∈[0,+∞]. By the choice of the radii, the right-hand side converges to L:=lim inf⁡r↑1∫Tlog⁡∣g(rζ)∣ dm(ζ)−log⁡∣g(0)∣, and L<+∞ by step 1.1; since Sj≥0 for every j, L≥0 as well, so L∈[0,+∞). As limits of the same identity, S=L<+∞. Since log⁡(1/x)≥1−x for 0<x≤1, also ∑n:an≠0(1−∣an∣)≤∑n:an≠0log⁡1∣an∣<+∞, and the zero at the origin contributes the finite amount m to the second sum; hence ∑n≥1(1−∣an∣)<+∞.

4.1step 1.1step 2.1step 1.3step 3.1∎

Assembly. Step 1.1 produces the finite order m of the zero at the origin and transfers the liminf hypothesis from f to g; step 2.1 verifies the hypothesis for Hp functions; steps 1.3–3.1 convert Jensen's formula for the dilated functions g(r ⋅ ) into convergence of the zero sum ∑log⁡(1/∣an∣) over the nonzero zeros, and then into the Blaschke condition ∑(1−∣an∣)<+∞.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

Blaschke factors and Blaschke products

Definition

For a∈D, let φa(z)=a−z1−a‾z be the published Blaschke factor of The unit disc, the upper half-plane, and Blaschke factors, a biholomorphic self-map of D by Blaschke factors are automorphisms of the disc. Define the normalized Blaschke factor ba(z):=a‾∣a∣ φa(z)  (a≠0),b0(z):=z. Since ∣a‾/∣a∣∣=1, each ba is holomorphic on an open neighbourhood of the closed disc (the denominator 1−a‾z does not vanish there), ba is zero-free on D except for the simple zero at a (the zero of φa), and ba(0)=a‾∣a∣ a=∣a∣≥0,∣ba(z)∣≤1(z∈D), the last inequality because φa maps D into itself. On the unit circle one has ∣ba(ζ)∣=1 for every ζ∈T (identified with the unit circle): for ∣ζ∣=1, ∣1−a‾ζ∣=∣ζ∣⋅∣ζ‾−a‾∣=∣a−ζ∣ by Conjugation is an involutive real-field automorphism, zz‾=∣z∣2, and modulus is definite, multiplicative, and subadditive and Real and imaginary parts, complex conjugation, and modulus, so ∣φa(ζ)∣=1.

Blaschke sequences and products. A sequence (an)n≥1 in D is a Blaschke sequence if ∑n(1−∣an∣)<+∞; its Blaschke product is the holomorphic product B(z):=∏n≥1ban(z), defined as the locally uniform limit of the partial products BN:=∏n≤Nban; for the empty sequence set B:=1. This definition is meaningful because the product converges normally on D in the sense of Normal convergence of holomorphic products: a Blaschke sequence satisfies ∣an∣→1, so for every compact K⊆D only finitely many an lie in K, and for every a∈D∖{0} and ∣z∣≤r<1 the identity 1−ba(z)=(1−∣a∣) 1+a‾∣a∣z1−a‾z,∣1−ba(z)∣≤(1−∣a∣)1+r1−r holds: the identity is a direct computation from ba=a‾∣a∣a−z1−a‾z using ∣a∣2=aa‾, and the estimate uses ∣1+a‾∣a∣z∣≤1+r and ∣1−a‾z∣≥1−r. For a=0, b0(z)=z and ∣1−b0(z)∣≤1+r=(1−∣0∣)(1+r)≤(1−∣0∣)(1+r)/(1−r), so the same estimate holds without dividing by ∣a∣. Hence ∑nsup⁡∣z∣≤r∣1−ban(z)∣≤1+r1−r∑n(1−∣an∣)<+∞. The published normal-convergence theorem therefore applies: the partial products converge locally uniformly to a holomorphic B that has exactly the zeros an with the multiplicity with which they occur, and satisfies ∣B(z)∣≤1 on D (Normally convergent products define holomorphic functions with the expected zeros). The limit does not depend on the enumeration of the sequence: the normal-convergence criterion is a condition on the set of factors, and for two enumerations and finite initial segments A,B containing a common block {1,…,N} the quotient ∏n∈Aban/∏n∈Bban deviates from 1 by at most a constant times the tail sum ∑n>Nsup⁡∣z∣≤r∣1−ban(z)∣, which tends to 0; hence the two partial-product sequences have the same locally uniform limit. The Blaschke sequence is reproduced by The zero set of a Hardy function satisfies the Blaschke condition from the zero set of a Hardy function. The boundary-modulus property ∣B∗∣=1 almost everywhere is not part of this definition; it is proved in Boundary values and zeros of a Blaschke product ↗.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Boundary values and zeros of a Blaschke product

Statement

Let (an)n≥1 be a Blaschke sequence with Blaschke product B=∏nban and partial products BN=∏n≤Nban. Then:

(i) ∣B(z)∣≤1 for every z∈D, and the zeros of B are exactly the points an, with multiplicity;

(ii) for every N, B/BN is the Blaschke product of the tail (an)n>N; it is holomorphic on D, satisfies ∣(B/BN)(z)∣≤1, and (B/BN)(0)=∏n>N∣an∣, a product that is eventually positive and tends to 1 as N→∞;

(iii) B has finite nontangential limits B∗(ζ) for m-almost every ζ∈T, and ∣B∗(ζ)∣=1 for m-almost every ζ. In particular B≢0.

Facts & Assumptions

Given: Countable choice and a Blaschke sequence (an)n≥1 with ∑n(1−∣an∣)<+∞, its Blaschke product B, and the partial products BN.

[L1]

The product converges normally: B is holomorphic on D with zeros exactly the an counted with multiplicity, and ∣B(z)∣≤1; for each N the quotient B/BN is the Blaschke product of the tail and is holomorphic with ∣B/BN∣≤1, while BN is holomorphic on a neighbourhood of the closed disc with ∣BN(ζ)∣=1 for every ζ∈T; also ba(0)=∣a∣ and ∣ba∣≤1 for every a∈D (Blaschke factors and Blaschke products, Normally convergent products define holomorphic functions with the expected zeros).

[L2]

Radii R and moduli: for the tail products, (B/BN)(0)=∏n>N∣an∣; since ∑n(1−∣an∣)<+∞ we have ∣an∣→1, so all but finitely many an have ∣an∣≥1/2, and for those log⁡(1/∣an∣)≤2(1−∣an∣); hence ∏n>N∣an∣=exp⁡(−∑n>Nlog⁡(1/∣an∣)) is eventually positive and tends to 1 as N→∞ (The zero set of a Hardy function satisfies the Blaschke condition, Blaschke factors and Blaschke products).

[L3]

If w is holomorphic on a neighbourhood of the closed disc of radius r<1, then ∣w(0)∣≤∫T∣w(rζ)∣ dm(ζ): ∣w∣ is subharmonic by Positive powers of the modulus of a holomorphic function are subharmonic with p=1, its Poisson modification on D(0,r) majorizes it and has the mean value of ∣w∣ on the circle at its centre, and for r=R this is the mean inequality for holomorphic functions of Radial p-means of a holomorphic function are nondecreasing (Poisson modification on a compactly contained disc, Poisson modification is subharmonic and majorizes the original function, Radial p-means of a holomorphic function are nondecreasing).

[L4]

Under countable choice every bounded holomorphic disc function has finite nontangential limits almost everywhere. (Bounded holomorphic disc functions have Poisson boundary data and Fatou limits under countable choice, The Axiom of Countable Choice (ACω))

[L5]

Domination and convergence: if ∣gr∣≤1 for all r and gr→g m-almost everywhere as r↑1, then ∫gr dm→∫g dm; the kernel has unit mass in the torus normalization and m is a probability measure (Dominated convergence, The Poisson kernel is positive, has total mass one, and concentrates at a boundary point, The one-dimensional torus and its normalized Haar integral).

Proof

technique · direct
1.1givenL1L2

Items (i) and (ii). [L1] gives ∣B∣≤1 with the stated zeros and the holomorphy and bound for B/BN. For each N the value at the origin is (B/BN)(0)=∏n>N∣an∣, whose factors are all nonzero once N exceeds the largest index with an=0. The tail need not be empty. By [L2] its product is eventually positive and tends to 1; for a finite sequence the empty tail equals 1.

2.1step 1.1L4

Nontangential limits exist and are bounded. Since ∣B∣≤1 and B is holomorphic, [L4] gives finite nontangential limits almost everywhere; hence B∗(ζ):=lim⁡Γ∋z→ζB(z) exists and satisfies ∣B∗(ζ)∣≤1 for m-almost every ζ.

2.2step 1.1L1L3algebra

The mean inequality for each tail. Fix N and 0<r<1. The function wN:=B/BN is holomorphic on a neighbourhood of the closed disc of radius r by [L1], so [L3] gives ∏n>N∣an∣=∣(B/BN)(0)∣≤∫T∣(B/BN)(rζ)∣ dm(ζ).

3.1step 1.1step 2.1step 2.2L1L5algebra

Letting the radius tend to the boundary. For m-almost every ζ one has B(rζ)→B∗(ζ) as r↑1, and BN extends continuously to D‾ with ∣BN(ζ)∣=1 on T by [L1], so (B/BN)(rζ)→B∗(ζ)/BN(ζ) along these radii, a limit of modulus ∣B∗(ζ)∣. Since ∣B/BN∣≤1, [L5] applies and gives ∏n>N∣an∣≤∫T∣B∗(ζ)∣ dm(ζ)≤1.

4.1step 3.1L2algebra∎

Conclusion. Letting N→∞ in step 3.1 and using that ∏n>N∣an∣→1 by [L2] gives 1≤∫T∣B∗∣ dm≤1, so ∫T∣B∗∣ dm=1; since ∣B∗∣≤1 m-almost everywhere, the nonnegative function 1−∣B∗∣ has integral 0, hence vanishes m-almost everywhere by A nonnegative measurable function has integral 0 exactly when it vanishes almost everywhere, that is, ∣B∗∣=1 m-almost everywhere. In particular the boundary function is not identically zero, so B≢0.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

F. Riesz factorization of a Hardy-space function

Statement

Let 0<p<∞, let f∈Hp(D) with f≢0, let (an)n≥1 be its zero sequence repeated with multiplicity and let B be the associated Blaschke product. Then g:=f/B extends holomorphically to D (removable singularities at the an), g has no zero in D, ∣f(z)∣≤∣g(z)∣ for every z∈D, and g∈Hp(D),∥g∥Hp=∥f∥Hp.

Facts & Assumptions

Given: A function f∈Hp(D) with 0<p<∞ and f≢0, its zero sequence (an) with multiplicity, the Blaschke product B, the partial products BN=∏n≤Nban and the quotients gN:=f/BN, together with g:=f/B where it is defined.

[L1]

The classes Hp(D) and their (quasi-)norms are defined by the suprema of radial Lp means, and ∥fr∥Lp≤∥f∥Hp for every 0≤r<1; the radial means of a holomorphic function are nondecreasing in the radius (Analytic Hardy spaces on the unit disc, Radial p-means of a holomorphic function are nondecreasing).

[L2]

The zero sequence of a nonzero Hp function satisfies the Blaschke condition ∑n(1−∣an∣)<+∞; hence B is a Blaschke product with ∣B∣≤1 and ∣ba∣≤1, and each finite product BN is holomorphic on a neighbourhood of the closed unit disc with ∣BN(ζ)∣=1 for every ζ∈T (The zero set of a Hardy function satisfies the Blaschke condition, Blaschke factors and Blaschke products, Boundary values and zeros of a Blaschke product).

[L3]

At a zero a occurring m≥1 times in the zero sequence, f has a zero of order at least m and B a zero of exactly order m, so g and each gN are holomorphic off the zero set and bounded near each an; a bounded holomorphic function on a punctured disc extends holomorphically across the puncture (Characterizations of removable singularities, Linearity, product, reciprocal, and quotient rules for complex derivatives, Complex differentiability at a point, the complex derivative, holomorphic functions, and entire functions).

[L4]

∣BN(z)∣≤1 on D, so ∣gN∣=∣f∣/∣BN∣≥∣f∣; the sequence (∣gN∣)N≥1 is nondecreasing at each point and converges to ∣g∣ (Blaschke factors and Blaschke products).

[L5]

Increasing sequences of nonnegative measurable functions may be integrated to the limit: if 0≤u1≤u2≤⋯ and uN↑u pointwise, then ∫uN dm↑∫u dm (Monotone convergence for the integral).

Proof

technique · direct
1.1givenL1L2L3

The Blaschke condition. By the Hp clause of [L2] applied to f∈Hp, the liminf hypothesis holds and ∑n(1−∣an∣)<+∞; hence B is a well-defined Blaschke product with ∣B∣≤1, each BN extends to the closed disc with ∣BN∣=1 on T, and each gN=f/BN is holomorphic on D by [L3].

1.2givenL1L2algebra

Bounding the N-th quotient. Fix 0<r<R<1, 0<ε<1 and N. By [L1] applied to the holomorphic function gN, ∫T∣gN(rζ)∣p dm(ζ)≤∫T∣gN(Rζ)∣p dm(ζ)=∫T∣f(Rζ)∣p∣BN(Rζ)∣p dm(ζ). Since BN is continuous on D‾ with ∣BN∣=1 on T by [L2], there is ρ<1 with ∣BN(Rζ)∣≥1−ε for all ζ∈T and all R∈(ρ,1); for such R, using [L1] again, ∫T∣gN(rζ)∣p dm(ζ)≤(1−ε)−p∫T∣f(Rζ)∣p dm(ζ)≤(1−ε)−p∥f∥Hpp.

2.1step 1.1L2L3L4algebra

The quotient. The function g=f/B is holomorphic off the zeros of B; at each a occurring m times, g is bounded near a and hence extends holomorphically by [L3], and g(a)≠0 because the order of the zero of f at a equals the multiplicity m with which a is listed. Thus g is holomorphic and zero-free on D, and ∣f∣≤∣g∣ because ∣B∣≤1.

3.1step 1.2step 2.1L1L4L5algebra

Passing to the limits in the correct order. Fix N and r<1. In step 1.2 choose R close enough to 1 for this N and ε, then let ε↓0. This gives ∫∣gN(rζ)∣pdm≤∥f∥Hpp, independently of N. The identities gN=baN+1gN+1 and ∣ba∣≤1 show that ∣gN∣p increases with N; off the zeros of B, gN=f/BN→f/B=g. A fixed circle contains only finitely many zeros, a null set, so monotone convergence [L5] gives ∫∣g(rζ)∣pdm≤∥f∥Hpp. Taking the supremum over r yields ∥g∥Hp≤∥f∥Hp. For finite or empty zero lists, the products stabilize, and the same argument gives B=1, g=f when the list is empty.

4.1step 1.1step 2.1step 3.1L1∎

Equality and assembly. Since ∣f∣≤∣g∣ pointwise by step 2.1, the radial means satisfy ∫T∣f(rζ)∣p dm≤∫T∣g(rζ)∣p dm for every r, so ∥f∥Hp≤∥g∥Hp by [L1]; combined with step 3.1 this gives ∥g∥Hp=∥f∥Hp with g∈Hp(D). Steps 1.1, 2.1 and 3.1 together prove all the asserted clauses.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

Inner, singular inner and outer functions

Definition

Assume countable choice. Let T be the one-dimensional torus with its normalized Haar measure m, identified with the Euclidean unit circle through φ([t])=e2πit (The one-dimensional torus and its normalized Haar integral), and let D be the unit disc (The unit disc, the upper half-plane, and Blaschke factors).

The Cauchy kernel. For ζ∈T (regarded as a point of the unit circle) and z∈D put K(z,ζ):=ζ+zζ−z. For fixed z the function ζ↦K(z,ζ) is continuous on the compact torus with ∣K(z,ζ)∣≤1+∣z∣1−∣z∣,Re⁡K(z,ζ)=1−∣z∣2∣ζ−z∣2=P(z,ζ)>0, where P is the Poisson kernel of The Poisson kernel on the unit disc under the identification of The Poisson integral of a finite complex boundary measure; for fixed ζ the function z↦K(z,ζ) is holomorphic on C∖{ζ}.

(a) Inner functions. A holomorphic θ:D→C is inner if θ∈H∞(D) and ∣θ∗(ζ)∣=1 for m-almost every ζ∈T, where θ∗ is its nontangential boundary function (Analytic Hardy spaces on the unit disc). Every Blaschke product is inner, and a Blaschke product has ∣B∣≤1 on D (Boundary values and zeros of a Blaschke product). An inner function also satisfies ∣θ∣≤1 on D; this is the case p=∞ of the bounded-holomorphic boundary-norm identity under countable choice proved in Bounded holomorphic disc functions have Poisson boundary data and Fatou limits under countable choice, and no inner function is assumed here to have any particular product form.

(b) Singular inner functions. For a finite positive Borel measure μ on T define Sμ(z):=exp⁡(−∫TK(z,ζ) dμ(ζ))(z∈D). If μ is singular with respect to m (written μ⊥m), Sμ is called a singular inner function. The function Sμ is well defined and holomorphic on D, has no zeros, satisfies ∣Sμ(z)∣=e−P[μ](z)≤1 and Sμ(0)=e−μ(T)>0; these properties and the boundary behaviour are proved in Properties of the singular functions Sμ ↗.

(c) Outer functions. For a nonnegative measurable h:T→[0,+∞] with log⁡h∈L1(T,m) (Complex Lp classes and Euclidean test-function conventions) define the outer function [h](z):=exp⁡(∫TK(z,ζ) log⁡h(ζ) dm(ζ))(z∈D), where log⁡h is extended by −∞ where h=0. The integral is absolutely convergent because ∣K(z,ζ)∣≤1+∣z∣1−∣z∣ and ∣log⁡h∣∈L1. To see holomorphy without any Lp hypothesis on h, expand K(z,ζ)=1+2∑n≥1znζ−n: its geometric tail is uniformly bounded on ∣z∣≤r<1, so termwise integration against log⁡h gives a power series whose coefficients have modulus at most 2∥log⁡h∥1. It is holomorphic on D (A complex power series converges absolutely and uniformly on every closed subdisc strictly inside its disc of convergence, A complex function is holomorphic if and only if it is analytic). Its exponential [h] is holomorphic and zero-free, with log⁡∣[h](z)∣=P[log⁡h](z),[h](0)=exp⁡(∫Tlog⁡h dm)>0, by The complex exponential is entire and its complex derivative is itself and exp⁡(x+iy)=ex(cos⁡y+isin⁡y), ∣exp⁡(x+iy)∣=ex, and eiπ+1=0, and depends only on the m-class of h. If h∈Lp(T,m) for some 0<p≤∞, then [h]∈Hp(D) and ∣[h]∗∣=h m-almost everywhere, with log⁡∣[h]∗∣=log⁡h a.e.; these additional properties are proved in Properties of outer functions ↗.

A holomorphic f on D with finite nontangential boundary values f∗ almost everywhere and log⁡∣f∗∣∈L1(T,m) is called outer if f=eiγ[ ∣f∗∣ ] for some γ∈R. Equivalently, log⁡∣f(z)∣=P[log⁡∣f∗∣](z) for every z∈D: the representation implies the equality by the displayed identity; conversely, the equality makes the holomorphic quotient f/[ ∣f∗∣ ] have modulus one throughout the disc, hence it is a unimodular constant by Local maximum modulus principle. Thus the outer function with the prescribed modulus and this interior equality is determined up to a unimodular constant, and [h](0)>0 fixes its normalization.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Properties of outer functions

Statement

Let 0<p≤∞, let h≥0 be measurable on T with log⁡h∈L1(T,m) and h∈Lp(T,m), and let [h] be the outer function of Inner, singular inner and outer functions. Then:

(i) [h] is holomorphic and zero-free on D with [h](0)=exp⁡(∫log⁡h dm)>0, and for p<∞ ∣[h](z)∣p≤P[hp](z)(z∈D); hence [h]∈Hp(D) with ∥[h]∥Hp≤∥h∥p, while for p=∞ one has ∣[h]∣≤∥h∥∞ and [h]∈H∞(D).

(ii) ∣[h]∗(ζ)∣=h(ζ) for m-almost every ζ∈T.

(iii) If h1=h2 m-almost everywhere then [h1]=[h2].

(iv) If g∈Hp(D) satisfies g≢0, ∣g∗∣=h m-almost everywhere and the outer equality log⁡∣g(z)∣=P[log⁡h](z) for all z∈D, then g=eiγ[h] for some γ∈R; in particular the outer function with prescribed boundary modulus is determined up to a unimodular constant.

Facts & Assumptions

Given: Countable choice and a nonnegative measurable h on T with log⁡h∈L1(T,m) and h∈Lp(T,m), and the outer function [h]=exp⁡L, L(z):=∫TK(z,ζ)log⁡h(ζ) dm(ζ).

[L1]

K(z,ζ)=(ζ+z)/(ζ−z) satisfies Re⁡K(z,ζ)=P(z,ζ), the Poisson kernel; P(z,⋅) is a probability density on T with ∫P(z,ζ)dm(ζ)=1, and for fixed z the integrals ∫∣K(z,ζ)∣ ∣f(ζ)∣dm(ζ) are finite for f∈L1 with ∫∣K(z,ζ)∣∣f∣dm≤1+∣z∣1−∣z∣∥f∥1 (Inner, singular inner and outer functions, The Poisson kernel on the unit disc, The Poisson kernel is positive, has total mass one, and concentrates at a boundary point, The Poisson integral of a finite complex boundary measure, Complex Holder, Minkowski, and the quotient norm).

[L2]

The expansion K(z,ζ)=1+2∑n≥1znζ−n converges absolutely and locally uniformly on ∣z∣<1, ∣ζ∣=1, so with cn:=∫ζ−nlog⁡h dm the series L(z)=∫log⁡h dm+2∑n≥1cnzn has ∣cn∣≤∥log⁡h∥1 and converges locally uniformly; its sum is holomorphic by the published power-series theorem, and exp⁡ of a holomorphic function is holomorphic and never zero, with ∣ew∣=eRe⁡w (A complex power series converges absolutely and uniformly on every closed subdisc strictly inside its disc of convergence, A complex function is holomorphic if and only if it is analytic, The complex exponential by its power series, The complex exponential is entire and its complex derivative is itself, exp⁡(x+iy)=ex(cos⁡y+isin⁡y), ∣exp⁡(x+iy)∣=ex, and eiπ+1=0).

[L3]

Jensen's inequality for the expectation with respect to the probability measure P(z,ζ)dm(ζ) and the convex exponential: e∫P(z,ζ) t(ζ) dm(ζ)≤∫P(z,ζ)et(ζ) dm(ζ) for real t with both t and et integrable against this probability measure (Jensen's inequality for expectation, Jensen's integral inequality for a probability measure).

[L4]

Tonelli's theorem for nonnegative and Fubini's theorem for L1 functions on the product of the probability space (T,m) with itself, and the translation invariance of m making ∫P(rζ,η) dm(ζ)=1 for every fixed η (Tonelli's theorem for nonnegative measurable functions on a sigma-finite product, Fubini's theorem for L^1 functions on a sigma-finite product, The Poisson kernel is positive, has total mass one, and concentrates at a boundary point, The one-dimensional torus and its normalized Haar integral).

[L5]

Under countable choice the Poisson integral of an L1 datum converges to that datum nontangentially almost everywhere. A nonzero Hardy function is in N and therefore has finite nontangential boundary limits under CC. (Fatou limits for Poisson extensions of L1 boundary data, Boundary values and log-integrability of Nevanlinna-class functions, The Nevanlinna class on the disc, The Axiom of Countable Choice (ACω))

[L6]

A holomorphic function of constant modulus on a domain is constant (maximum principle), and ∣uv∣=∣u∣∣v∣ (Local maximum modulus principle, Conjugation is an involutive real-field automorphism, zz‾=∣z∣2, and modulus is definite, multiplicative, and subadditive).

Proof

technique · direct
1.1givenL2algebra

Holomorphy, zero-freeness and the value at the origin. By [L2] the function L is holomorphic on D with L(0)=∫log⁡h dm∈R, so [h]=eL is holomorphic and zero-free with [h](0)=e∫log⁡h dm>0 (finite because log⁡h∈L1).

2.1step 1.1L1L2L3algebra

The pointwise bound. Let p<∞ and fix z∈D. Since Re⁡L(z)=∫P(z,ζ)log⁡h(ζ) dm(ζ) by [L1], put t:=plog⁡h, choosing a finite real representative on the null exceptional set. Both t and et=hp are integrable against P(z,ζ)dm(ζ) because log⁡h∈L1, h∈Lp, and the fixed kernel is bounded by [L1]. Jensen's inequality [L3] therefore gives ∣[h](z)∣p=epRe⁡L(z)=e∫P(z,ζ) plog⁡h(ζ) dm(ζ)≤∫TP(z,ζ)h(ζ)p dm(ζ)=P[hp](z). For p=∞, log⁡h≤log⁡∥h∥∞ m-almost everywhere (with ∥h∥∞>0 because log⁡h∈L1), so Re⁡L(z)=∫Plog⁡h dm≤log⁡∥h∥∞ and ∣[h](z)∣≤∥h∥∞.

2.2step 1.1L6algebra

Uniqueness up to a unimodular constant. Assume g∈Hp, g≢0, ∣g∗∣=h a.e. and log⁡∣g(z)∣=P[log⁡h](z) for all z. Then log⁡∣g∣=log⁡∣[h]∣ on D by step 1.1 and [L1], so the holomorphic zero-free function g/[h] has constant modulus 1; by [L6] it is a constant of modulus one, that is, g=eiγ[h] for some γ∈R.

3.1step 2.1L4algebra

Membership in Hp. For p<∞ and 0<r<1, integrating the bound of step 2.1 over the circle and applying Tonelli's theorem [L4] to the nonnegative integrand gives ∫T∣[h](rζ)∣p dm(ζ)≤∫T(∫TP(rζ,η) dm(ζ))h(η)p dm(η)=∥h∥pp, because the inner integral equals the unit mass of the kernel by translation invariance. Taking the supremum over r gives [h]∈Hp(D) with ∥[h]∥Hp≤∥h∥p; for p=∞ step 2.1 gives [h]∈H∞ with ∥[h]∥∞≤∥h∥∞.

4.1step 3.1L1L5algebra

Boundary modulus. Since log⁡∣[h]∣=Re⁡L=P[log⁡h] by [L1], the harmonic Fatou theorem for the L1 datum log⁡h gives log⁡∣[h](z)∣→log⁡h(ζ) as z→ζ within every cone, at m-almost every ζ. By step 3.1, [h]∈Hp, so by [L5] it has nontangential limits [h]∗ m-almost everywhere; at every point where both statements hold, taking moduli gives ∣[h]∗(ζ)∣=h(ζ). This proves (ii), and (iii) is immediate from the definition of [h] as an integral against dm.

5.1step 1.1step 3.1step 4.1step 2.2∎

Assembly. Steps 1.1, 2.1 and 3.1 give (i), step 4.1 gives (ii) and (iii), and step 2.2 gives (iv). All four clauses are proved under the stated hypotheses.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Singular circle measures have Poisson integral tending nontangentially to zero almost everywhere

Statement

Assume countable choice. Let μ be a finite positive Borel measure on T singular with respect to normalized Haar measure m. Then, for m-almost every ζ∈T and every A>1, lim⁡z→ζ, z∈ΓA(ζ)P[μ](z)=0. The zero measure is allowed.

Facts & Assumptions

Given: Countable choice, the finite positive singular measure μ, and the normalized circle conventions.

[F1]

Under countable choice, finite Borel measures on the compact metric circle are regular. Singularity supplies a Borel set E with m(E)=0 and μ(T∖E)=0. For every ε>0, inner regularity provides a compact K⊆E with μ(T∖K)<ε. The Haar measure is a probability measure. (Locally finite Borel measures on second-countable LCH spaces are regular, The one-dimensional torus and its normalized Haar integral, The Axiom of Countable Choice (ACω))

[F2]

For each finite regular positive Borel measure ρ, the circle maximal function satisfies m{MTρ>λ}≤3ρ(T)/λ for λ>0. Moreover NA(P[ρ])≤(A+1)2MTρ for A>1. Both results assume countable choice. (The circle maximal function is weak type one one for finite measures, Poisson nontangential maximal function is controlled by circle maximal averages, The circle maximal function and nontangential approach regions)

[F3]

Restrictions are measures and remain finite regular Borel measures here by [F1]. The kernel is (1−∣z∣2)/∣η−z∣2, and the Poisson integral is linear in its measure. (Restriction of a measure to a measurable set, The restriction of a measure to a measurable set is a measure, The Poisson kernel on the unit disc, The Poisson integral of a finite complex boundary measure)

Proof

1.1F1F3givenconstructalgebra

Fix ε>0 and choose the compact null set K in [F1]. Split μ=μK+ρ, its restrictions to K and its complement; then ρ(T)<ε. At a circle point ζ∉K, compactness gives d=dist⁡(ζ,K)>0 if K is nonempty. For ∣z−ζ∣<d/2, [F3] gives P[μK](z)≤4d−2(1−∣z∣2)μ(T)⟶0. If K is empty, this integral is already zero. This limit holds along every approach within the disc, not only a radius.

2.1F1F2step 1.1constructalgebra

Fix A>1 and t>0, and let BA,t be the circle points where the nontangential limsup of P[μ] in ΓA is greater than t. For ζ∉K, step 1.1 and positivity imply that this limsup is the limsup for P[ρ]. Thus [F2] gives BA,t⊆K ∪ {MTρ>t/(A+1)2}. The right side is Borel and has Haar measure at most 3(A+1)2ε/t. Since ε is arbitrary, BA,t has Haar outer measure zero. This argument does not assume measurability of the cone limsup.

3.1F1F2step 2.1algebra∎

For each integer j≥2 and k≥1, apply step 2.1 with A=j and t=1/k. A set of outer measure zero is contained in a Borel null set: choose Borel supersets of mass less than 2−l and intersect them, using countable choice. By countable choice choose these null supersets for the countable pairs (j,k) and take their union, a Borel null set. Outside that union, positivity gives limsup zero in every cone of integer aperture j≥2, hence the limit zero there. Every cone of aperture A>1 is contained in one with integer aperture j>A, so the same full-measure set works for all A. For μ=0 the integral is identically zero throughout.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Finite positive circle measures admit a Lebesgue decomposition under countable choice

Statement

Assume countable choice. Every finite positive Borel measure μ on T has a unique decomposition μ=w m+μs, where w≥0 is Borel measurable and integrable for normalized Haar measure m, and μs is a finite positive Borel measure carried by an m-null Borel set. The density w is unique up to m-almost-everywhere equality. The zero measure is allowed.

Facts & Assumptions

Given: Countable choice and the finite positive measure μ on the circle, whose Haar measure has mass one.

[F1]

Under countable choice, real L2(ν) is a Hilbert space for every measure space, with inner product ∫fg dν. Every bounded real linear functional has a representing vector for this pairing. Cauchy-Schwarz bounds integrals of products of square-integrable functions. (L2 with the integral pairing is a Hilbert space, Riesz representation for Hilbert spaces, Cauchy-Schwarz inequality for L2, The Axiom of Countable Choice (ACω))

[F2]

The integral is linear on integrable real functions, increasing nonnegative functions integrate to their limit, and a nonnegative function has integral zero exactly when it vanishes almost everywhere. (The Lebesgue integral is linear on L1(μ), Monotone convergence for the integral, A nonnegative measurable function has integral 0 exactly when it vanishes almost everywhere)

[F3]

Restrictions to Borel sets are measures. Being carried by a null Borel set is the meaning of singularity here; Haar measure is a probability measure. (Restriction of a measure to a measurable set, The restriction of a measure to a measurable set is a measure, A positive, signed, or complex measure concentrated on a measurable set, The one-dimensional torus and its normalized Haar integral)

Proof

1.1F1F3givenconstructalgebra

Set ν=μ+m, a finite positive measure on the circle Borel sigma-algebra. The functional Λ(f)=∫f dm on real L2(ν) is well-defined: a ν-null set is m-null since m≤ν, and Cauchy-Schwarz gives ∫∣f∣ dm≤(∫∣f∣2 dm)1/2≤∥f∥L2(ν). By [F1] there is a real Borel representative h∈L2(ν) with Λ(f)=∫fh dν. Every Borel indicator lies in this L2, so m(E)=∫Eh dν(E Borel).

2.1F2step 1.1constructalgebra

This identity forces 0≤h≤1 ν-almost everywhere. On Ek={h<−1/k} the integral is at most −ν(Ek)/k but equals the nonnegative m(Ek), hence ν(Ek)=0. On Dk={h>1+1/k} it is at least (1+1/k)ν(Dk) but m(Dk)≤ν(Dk), so ν(Dk)=0. Clip h into [0,1] on the countable union of these null Borel sets. The identity remains true. By linearity, μ(E)=ν(E)−m(E)=∫E(1−h) dν.

3.1F2F3step 1.1step 2.1constructalgebra

Put N={h=0}, and define w=(1−h)/h on T∖N and w=0 on N. Step 1.1 gives m(N)=0. Its indicator identity implies ∫v dm=∫vh dν for every nonnegative Borel v: first for simple functions by linearity, then for arbitrary nonnegative functions by increasing simple approximation and [F2]. Applying it to v=w1E gives ∫Ew dm=∫E∖N(1−h) dν=μ(E∖N). In particular w is integrable, with integral at most μ(T). Set μs=ν∣N=μ∣N by step 2.1. It is positive, finite and carried by the m-null Borel set N, and the displayed identity proves μ=w m+μs.

4.1F2step 3.1algebra∎

For uniqueness, suppose also μ=v m+ρs with the stated properties. Choose null Borel carriers for μs and ρs and let A be their union. For every Borel E⊆T∖A, equality of the two measures gives ∫E(w−v) dm=0. Testing the sets where w−v>1/k or v−w>1/k proves w=v almost everywhere outside A, hence everywhere almost surely. The density measures are equal, and subtraction then gives μs=ρs. For μ=0, positivity forces both parts zero. Countable choice was used only for the Hilbert-space interface [F1]; all other constructions use explicit measurable formulas.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Bounded holomorphic disc functions have Poisson boundary data and Fatou limits under countable choice

Statement

Assume countable choice. Let f be bounded and holomorphic on D, and set M=sup⁡z∈D∣f(z)∣. Then there is a unique φ∈L∞(T,m) with f=P[φ]. It satisfies ∥φ∥∞=M, and f has nontangential limit φ(ζ) for almost every ζ within every cone ΓA(ζ), A>1. The zero function is allowed.

Facts & Assumptions

Given: Countable choice, bounded holomorphic f, and its finite bound M.

[F1]
[F2]

Under countable choice, Parseval identifies the squared L2 norm with the sum of the squared Fourier coefficients, and every square-summable bilateral coefficient sequence comes from a unique L2 class. (The Parseval identity for Fourier series, Riesz–Fischer: the Fourier coefficient map is onto the space of square-summable families, The Axiom of Countable Choice (ACω))

[F3]

Haar measure is a probability measure; Holder gives L2⊆L1. The Poisson kernel is (1−∣z∣2)/∣ζ−z∣2, and P[φ](z)=∫P(z,ζ)φ(ζ) dm(ζ). For any L1 datum its Poisson integral converges nontangentially almost everywhere to that datum under countable choice. (The one-dimensional torus and its normalized Haar integral, Complex Holder, Minkowski, and the quotient norm, The Poisson kernel on the unit disc, The Poisson kernel is positive, has total mass one, and concentrates at a boundary point, The Poisson integral of a finite complex boundary measure, Fatou limits for Poisson extensions of L1 boundary data)

Proof

1.1F1F2F3givenconstructalgebra

For 0<r<1, [F1] identifies the Fourier coefficients of fr as cnrn for n≥0 and zero for n<0, by uniform termwise integration and character orthogonality. By [F2], for each N, ∑n=0N∣cn∣2r2n≤∫T∣f(rζ)∣2 dm≤M2. Let r↑1 at this fixed finite N, then take the supremum in N: ∑n≥0∣cn∣2≤M2. Riesz-Fischer in [F2] gives a unique φ∈L2 with coefficients cn for n≥0 and zero for n<0.

2.1F1F3step 1.1algebra

This datum is in L1 by [F3]. The geometric identity, for ∣z∣<1 and ∣ζ∣=1, gives P(z,ζ)=1+∑n≥1(znζ−n+z‾nζn). The series converges absolutely uniformly in ζ at each fixed z, with total absolute bound 1+2∑n≥1∣z∣n<∞. Its integral against φ therefore converges termwise, since the error is bounded by its uniform norm times ∥φ∥1. Using its prescribed Fourier coefficients yields P[φ](z)=∑n≥0cnzn=f(z).

3.1F3step 2.1algebra∎

By [F3], f=P[φ] has the asserted nontangential limits. Since ∣f(z)∣≤M, passing to these limits gives ∣φ∣≤M almost everywhere, so φ∈L∞. Conversely positivity and unit mass of the kernel give ∣f(z)∣≤∥φ∥∞, hence M=∥φ∥∞. If another bounded datum ψ has P[ψ]=f, its nontangential limits are ψ by [F3]; the same limits give ψ=φ almost everywhere. If M=0 then f=0 and every coefficient and the unique datum are zero, so all claims remain valid. Only countable choice, in [F2] and [F3], has been used.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Complex circle measures have finite regular total variation under countable choice

Statement

Assume countable choice. Every finite-valued countably additive complex Borel measure ν on T has ∣ν∣(T)<∞, and ∣ν∣ is a finite regular positive Borel measure. The zero complex measure is allowed. No Hahn or Jordan decomposition is required.

Facts & Assumptions

Given: Countable choice and a complex Borel measure ν:B(T)→C.

[F1]

A complex measure is finite-valued and countably additive on every given disjoint sequence. Its total variation is the supremum of sums ∑j∣ν(Ej)∣ over countable Borel partitions of a set. (A complex measure is a finite-valued countably additive set function, The total variation |nu|(E) from countable measurable partitions, The Axiom of Countable Choice (ACω))

[F2]

A finite family of nonempty sets has a choice function without a choice axiom. (Every natural-number-indexed list of nonempty sets has a choice function on its family of values)

[F3]

Under CC, Borel measures finite on compact sets on a second-countable LCH space are regular. The circle is compact and metrizable. (Locally finite Borel measures on second-countable LCH spaces are regular, The one-dimensional torus and its normalized Haar integral)

Proof

1.1F1givenconstructalgebra

For every supplied disjoint Borel sequence (Dj), ∑j∣ν(Dj)∣ is finite. To see this directly from [F1], split the real parts into their nonnegative and negative index groups. On each group, replace other cells by the empty set; [F1] says the complex series converges to the finite measure of that group's union. Its real part therefore has a finite sum of terms of one sign. Thus ∑j∣Re⁡ν(Dj)∣<∞. The two imaginary sign groups give ∑j∣Im⁡ν(Dj)∣<∞ as well. Since ∣z∣≤∣Re⁡z∣+∣Im⁡z∣, the asserted absolute sum is finite. Empty groups cause zero sums.

2.1F1step 1.1givenconstructalgebra

Suppose ∣ν∣(T)=∞. For each n≥0 there is a finite ordered Borel partition Pn with sum of absolute measures greater than 2n: take a finite initial portion of a countable partition whose sum exceeds that threshold, and append its complement. CC supplies the sequence (Pn). Let Qn be the finite common refinement of P0,…,Pn, ordered lexicographically by their cell indices; empty cells may be retained. For Borel E put Sn(E)=∑C∈Qn∣ν(E∩C)∣,V(E)=sup⁡nSn(E). Refinement and the triangle inequality make Sn(E) nondecreasing, and V(T)=∞. For any fixed m, refinement gives Sn(E)=∑C∈QmSn(E∩C) for n≥m; passing to the limit in this finite sum gives V(E)=∑C∈QmV(E∩C).

3.1F1step 1.1step 2.1constructalgebra

Define a nested sequence deterministically, starting with E0=T and index m0=−1. Given V(Ek)=∞, take the least n>mk for which Sn(Ek)>∣ν(Ek)∣+2. Among the finitely many cells of Qn contained in Ek, choose the first C with V(C)=∞, possible by the finite-sum identity in step 2.1. Set Ek+1=C, mk+1=n, and retain all other cells of the refinement inside Ek as side cells Dk,j. Here Ek is a cell of the previous refinement for k>0, so the new cells partition it. Write sk=∑j∣ν(Dk,j)∣. Finite additivity gives ∣ν(C)∣≤∣ν(Ek)∣+sk, while Sn(Ek)=∣ν(C)∣+sk, hence sk≥Sn(Ek)−∣ν(Ek)∣2>1. Side cells from different stages are disjoint, since later parents lie in the retained nested child. Concatenating the prescribed finite ordered side lists is a disjoint countable Borel sequence with total absolute sum ∑ksk=∞, contradicting step 1.1. The recursion uses least natural numbers and first indices in supplied finite lists; it spends no dependent choice. Therefore ∣ν∣(T)<∞.

4.1F1F2step 3.1constructalgebra

We also prove that variation is a measure directly. It has value zero on the empty set. Let E=⨆jEj be a supplied disjoint Borel union. Every piece has finite variation by step 3.1, since its partitions extend to partitions of the circle by appending the complement. For fixed N and epsilon, choose partitions of the first N+1 pieces within ε/(N+1) of their variation suprema; [F2] supplies these finitely many choices. Concatenate their cells and append the remainder of E. The resulting partition gives ∣ν∣(E)≥∑j=0N∣ν∣(Ej)−ε. Let epsilon decrease to zero and then N increase to infinity. Conversely, for every partition (Bl) of E, countable additivity gives ∣ν(Bl)∣≤∑j∣ν(Bl∩Ej)∣. Summing and interchanging the two nonnegative series yields ∑l∣ν(Bl)∣≤∑j∣ν∣(Ej). Taking the supremum over partitions proves the reverse bound. Thus ∣ν∣ is a finite positive Borel measure.

5.1F3step 3.1step 4.1algebra∎

Step 4.1 and the finiteness from step 3.1 meet [F3], which gives regularity on the circle. For nu zero all sums are zero. CC was used only for the independent partition sequence in step 2.1 and the regularity theorem; the recursive refinement is deterministic and the measure proof uses only finite choice.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Finite complex circle measures are determined by Fourier coefficients and Poisson integrals

Statement

Assume countable choice. If two complex Borel circle measures μ,ν have μ^(n)=ν^(n) for every integer n, then μ=ν. Moreover P[μ]=P[ν] on the disc implies μ=ν. For every complex Borel measure, every 0<r<1 and every integer n, (P[μ])r^(n)=r∣n∣μ^(n). The zero measures are allowed.

Facts & Assumptions

Given: Countable choice and two complex Borel measures on the circle.

[F1]

Under CC their total variations, and the variation of their difference, are finite regular positive Borel measures. Integration against a complex measure satisfies ∣∫u dσ∣≤∫∣u∣ d∣σ∣. (Complex circle measures have finite regular total variation under countable choice, Integrals against signed or complex measures are bounded by total variation, The Axiom of Countable Choice (ACω))

[F2]

The trigonometric polynomials are uniformly dense in C(T,C) under CC. Their coefficients are integrals against the characters, which are orthonormal for normalized Haar measure. (Trigonometric polynomials are uniformly dense in continuous functions on the torus, Fourier coefficients and trigonometric polynomials on the torus, The trigonometric characters are orthonormal in L2 of the torus, The one-dimensional torus and its normalized Haar integral)

[F3]

The kernel is P(z,η)=(1−∣z∣2)/∣η−z∣2, and P[μ] is its integral against μ. The circle is a compact metric space. (The Poisson kernel on the unit disc, The Poisson integral of a finite complex boundary measure, The one-dimensional torus and its normalized Haar integral)

Proof

1.1F1F2givenconstructalgebra

Set σ=μ−ν, a complex measure by countable additivity. If its Fourier coefficients vanish, its integral against every trigonometric polynomial is zero. Given a continuous u, [F2] supplies polynomials arbitrarily close to u uniformly; [F1] bounds ∣∫(u−p)dσ∣ by ∥u−p∥∞∣σ∣(T). Therefore ∫u dσ=0 for every continuous u.

1.2F1F2F3algebra

For z=rζ, the geometric-series identity yields P(rζ,η)=∑k∈Zr∣k∣ζkη−k. At fixed r<1 this is uniformly absolutely convergent in both circle variables, with bound 1+2∑k≥1rk. Integrating first against μ is justified by [F1] and the uniform error bound, and produces the uniformly convergent circle series ∑kr∣k∣μ^(k)ζk, since ∣μ^(k)∣≤∣μ∣(T). Integrating this series against ζ−ndm and using [F2] gives the stated coefficient formula.

2.1F1F3step 1.1constructalgebra

Fix a Borel E and ε>0. Regularity in [F1] gives a compact K⊆E and open U⊇E with ∣σ∣(U∖K)<ε. There is a continuous 0≤u≤1 equal to one on K and zero outside U. Explicitly, if K is empty take u=0; if U is the circle take u=1; otherwise use u(x)=d(x,T∖U)d(x,T∖U)+d(x,K). The two sets are disjoint closed sets, so the denominator is positive at each x; distances are continuous because ∣d(x,A)−d(y,A)∣≤d(x,y) for a nonempty set A. Thus ∣1E−u∣≤1U∖K. Step 1.1 and [F1] give ∣σ(E)∣=∣∫(1E−u)dσ∣<ε. Hence σ(E)=0 for every E, proving Fourier uniqueness.

3.1step 2.1step 1.2algebra∎

If P[μ]=P[ν], fix r=1/2 in step 1.2. Every factor r∣n∣ is strictly positive, so all Fourier coefficients agree. Step 2.1 gives μ=ν. Zero measures and zero variation cause no division by a measure mass anywhere in the proof.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Properties of the singular functions Sμ

Statement

Assume countable choice, as in the defining circle and singular-function conventions. Let μ be a finite positive Borel measure on T and let Sμ(z)=exp⁡(−∫TK(z,ζ) dμ(ζ)). Then Sμ is holomorphic and zero-free on D, log⁡∣Sμ∣=−P[μ], ∣Sμ∣≤1, and Sμ(0)=e−μ(T)∈(0,1]. Moreover Sμ has finite nontangential limits Sμ∗(ζ) for m-almost every ζ∈T, with ∣Sμ∗∣=e−lim⁡r↑1P[μ](rζ), and the following are equivalent:

(i) μ⊥m; (ii) ∣Sμ∗∣=1 m-almost everywhere; (iii) P[μ](rζ)→0 for m-almost every ζ∈T.

Consequently Sμ is a singular inner function exactly when μ⊥m.

Facts & Assumptions

Given: Countable choice and a finite positive Borel measure μ on the torus T with normalized Haar measure m, the kernel K(z,ζ)=(ζ+z)/(ζ−z) and the function Sμ=e−H with H(z):=∫TK(z,ζ) dμ(ζ).

[L1]

K is continuous and bounded on T for fixed z, Re⁡K(z,ζ)=P(z,ζ) is the Poisson kernel, and ∫TP(z,ζ) dm(ζ)=1; the Poisson integral P[μ](z)=∫P(z,ζ) dμ is harmonic with P[μ]≥0 and P[μ](0)=μ(T) (Inner, singular inner and outer functions, The Poisson kernel on the unit disc, The Poisson kernel is positive, has total mass one, and concentrates at a boundary point, The Poisson integral of a finite complex boundary measure).

[L2]

The expansion K(z,ζ)=1+2∑n≥1znζ−n converges absolutely and locally uniformly for ∣z∣<1, ∣ζ∣=1, so termwise integration against the finite measure μ exhibits H as a locally uniform limit of holomorphic polynomials, hence holomorphic on D; exp⁡ of a holomorphic function is holomorphic, and the exponential is never zero (A complex power series converges absolutely and uniformly on every closed subdisc strictly inside its disc of convergence, Inner, singular inner and outer functions, The complex exponential by its power series).

[L3]

Under countable choice, every bounded holomorphic disc function has finite nontangential limits almost everywhere. (Bounded holomorphic disc functions have Poisson boundary data and Fatou limits under countable choice)

[L4]

Under countable choice every finite positive Borel circle measure has a decomposition μ=h m+μs with integrable Borel h≥0 and μs carried by a Haar-null Borel set. (Finite positive circle measures admit a Lebesgue decomposition under countable choice, A positive, signed, or complex measure concentrated on a measurable set)

[L5]

The Poisson integral of h∈L1(T,m) converges to h(ζ) at m-almost every ζ within every cone ΓA(ζ), A>1 (Fatou limits for Poisson extensions of L1 boundary data).

[L6]

For a finite positive singular circle measure, its Poisson integral tends nontangentially to zero almost everywhere under countable choice. The proof uses compact approximation of its singular carrier and the weak maximal estimate; no small-closure assertion for an open set is used. (Singular circle measures have Poisson integral tending nontangentially to zero almost everywhere)

Proof

technique · direct
1.1givenL1L2algebra

Holomorphy, modulus and value at the origin. By [L2] the function H is holomorphic on D with Re⁡H=P[μ] by [L1]; hence Sμ=e−H is holomorphic and zero-free, ∣Sμ(z)∣=e−Re⁡H(z)=e−P[μ](z)≤1 because P[μ]≥0, and Sμ(0)=e−H(0)=e−μ(T)∈(0,1]. Also log⁡∣Sμ∣=−P[μ].

2.1step 1.1L1L3L4L5L6algebra

Nontangential limits. By step 1.1, Sμ is bounded holomorphic, so [L3] gives finite nontangential limits Sμ∗ almost everywhere. To identify their modulus, decompose μ=h m+μs by [L4]. The Poisson integral is the sum P[h]+P[μs] by [L1]; [L5] gives P[h]→h nontangentially almost everywhere, and [L6] gives P[μs]→0. On their common full-measure set, P[μ]→h, so continuity of the real exponential in the identity of step 1.1 gives ∣Sμ∗∣=e−h=e−lim⁡r↑1P[μ](rζ). The radial limit agrees with the cone limits.

2.2step 1.1L6

(i) implies (iii). If μ⊥m, [L6] gives P[μ](z)→0 within every cone at almost every circle point, hence in particular along radii. Thus (iii) holds, including μ=0.

3.1step 2.1algebra

(iii) implies (ii). If P[μ](rζ)→0 for m-almost every ζ, then step 2.1 gives ∣Sμ∗(ζ)∣=e0=1 for m-almost every ζ, which is (ii).

3.2step 2.1L4L5algebra

(ii) implies (i). Assume (ii) and decompose μ=h m+μs as in [L4]. Since h≥0, one has P[h]≤P[μ] pointwise, and by [L5], P[h](rζ)→h(ζ) for m-almost every ζ. By step 2.1, (ii) says P[μ](rζ)→0 a.e.; hence 0≤h(ζ)≤lim inf⁡rP[μ](rζ)=0 a.e., so h=0 m-almost everywhere. Therefore μ=μs is concentrated on an m-null set, that is, μ⊥m, which is (i).

4.1step 1.1step 2.1step 2.2step 3.2algebra∎

Assembly. Step 1.1 gives holomorphy, zero-freeness, the modulus identity and the value at 0; step 2.1 gives the a.e. nontangential limits and the displayed modulus formula; steps 2.2, 3.1 and 3.2 prove (i)⇒(iii)⇒(ii)⇒(i), so the three conditions are equivalent. By the definition of singular inner function, Sμ is a singular inner function exactly when μ⊥m, i.e. exactly when the equivalent conditions hold.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Zero-free inner functions are unimodular multiples of singular inner functions

Statement

Assume the Axiom of Choice. Let S be holomorphic and zero-free on D with ∣S∣≤1, and suppose that its boundary function satisfies ∣S∗∣=1 m-almost everywhere (equivalently, S is an inner function without zeros). Then there are a unique λ∈T and a unique finite positive measure μ⊥m with S=λ Sμ,Sμ(z)=exp⁡(−∫TK(z,ζ) dμ(ζ)). With the normalizations Sμ(0)=e−μ(T)>0 and λ=S(0)/Sμ(0), the pair (λ,μ) is unique. In particular Sμ is the singular inner function of μ, and every inner function is, up to a unimodular constant, the product of a Blaschke product and a singular inner function.

Facts & Assumptions

Given: The Axiom of Choice, hence countable choice (The Axiom of Choice, The Axiom of Countable Choice (ACω)); a zero-free holomorphic S on D with ∣S∣≤1 and ∣S∗∣=1 m-almost everywhere; and, where asserted, an inner function θ.

[L1]

S zero-free means log⁡∣S∣ is harmonic on D, so u:=−log⁡∣S∣=−Re⁡log⁡S is a nonnegative harmonic function with u(0)=−log⁡∣S(0)∣<+∞; the kernel K(z,ζ)=(ζ+z)/(ζ−z) is holomorphic in z with Re⁡K=P (A nonvanishing holomorphic function on a homologically simply connected domain has a holomorphic logarithm, Holomorphic functions are real analytic and smooth in their two real coordinates, The C2 real and imaginary parts of a holomorphic function satisfy Laplace's equation and form a harmonic-conjugate pair, Star-shaped plane domains are homologically simply connected, Inner, singular inner and outer functions, Plane harmonic functions).

[L2]

Herglotz representation: every nonnegative harmonic u on D is u=P[μ] for a unique finite nonnegative regular Borel measure μ with μ(T)=u(0), and conversely P[μ] is nonnegative harmonic (Positive harmonic boundary measures and compact normalized families).

[L3]

The functions H(z):=∫TK(z,ζ) dμ(ζ) are holomorphic on D with Re⁡H=P[μ], and Sμ=e−H is holomorphic, zero-free, with ∣Sμ∣=e−P[μ] and Sμ(0)=e−μ(T); Sμ is a singular inner function exactly when μ⊥m (Properties of the singular functions Sμ, Inner, singular inner and outer functions).

[L4]

Maximum modulus: a holomorphic function on a domain with constant modulus is constant; a holomorphic function on a domain whose modulus has an interior maximum is constant (Local maximum modulus principle).

[L5]

For θ∈H∞ with ∣θ∗∣=1 a.e. (an inner function), one has ∣θ∣≤1 on D and ∥θ∥∞=1, by the boundary-norm identity of the Fatou theorem for analytic H∞; the zero sequence of θ satisfies the Blaschke condition, and θ/B for the Blaschke product of its zeros is holomorphic and zero-free with nontangential boundary modulus 1 a.e., while its modulus is bounded by 1 by the maximum principle on expanding discs ∣z∣<R with ∣BN(Rζ)∣→1 (Fatou's boundary theorem for analytic Hardy spaces, The zero set of a Hardy function satisfies the Blaschke condition, Boundary values and zeros of a Blaschke product, F. Riesz factorization of a Hardy-space function, Blaschke factors and Blaschke products, Local maximum modulus principle).

Proof

technique · direct
1.1givenL1L2

The measure of the modulus. By [L1] the function u=−log⁡∣S∣ is nonnegative harmonic with u(0)<+∞, so [L2] provides a unique finite nonnegative regular Borel measure μ with u=P[μ], μ(T)=u(0).

2.1step 1.1L3L4algebra

S is a unimodular constant times Sμ. Let H be the holomorphic function with Re⁡H=P[μ]=u from [L3]. Then ∣S(z)eH(z)∣=∣S(z)∣eRe⁡H(z)=e−u(z)eu(z)=1(z∈D), so the holomorphic function SeH has constant modulus 1; by [L4] it is a constant λ with ∣λ∣=1, that is, S=λe−H=λSμ.

3.1step 2.1L3algebra

Singularity of μ. Since ∣S∗∣=1 a.e. and ∣λ∣=1, the relation S=λSμ passes to the a.e. boundary values: ∣Sμ∗∣=1 a.e. By the equivalence of [L3], this forces μ⊥m.

4.1step 2.1step 3.1L2L3algebra

Uniqueness. If S=λSμ=λ′Sμ′ with unimodular λ,λ′ and finite positive μ,μ′⊥m, then taking moduli gives log⁡∣S∣=−P[μ]=−P[μ′], so P[μ]=P[μ′] and the uniqueness clause of the Herglotz representation [L2] gives μ=μ′; then λ=S(0)/Sμ(0)=λ′.

4.2step 2.1step 3.1L5algebra

Every inner function factors. Let θ be an inner function. The inner function cannot be identically zero, because its boundary modulus is 1 almost everywhere. Let (an) be its zero sequence with multiplicity and B its Blaschke product. By [L5] the sequence is a Blaschke sequence, and S:=θ/B is holomorphic, zero-free, satisfies ∣S∣≤1 and has ∣S∗∣=1 a.e. By steps 1.1, 2.1 and 3.1 there are λ∈T and μ⊥m with S=λSμ, so θ=B⋅S=λ B Sμ: up to the unimodular constant λ, θ is the product of the Blaschke product B and the singular inner function Sμ.

5.1step 2.1step 3.1step 4.1step 4.2∎

Assembly. Steps 1.1, 2.1 and 3.1 produce the representation S=λSμ with μ⊥m for a zero-free S, step 4.1 proves the asserted uniqueness, and step 4.2 gives the factorisation of a general inner function.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Fatou's boundary theorem for analytic Hardy spaces

Statement

Assume countable choice. Let 0<p≤∞ and f∈Hp(D) (the zero function is allowed in (a)–(c)).

(a) For m-almost every ζ∈T the nontangential limit f∗(ζ):=lim⁡z→ζ, z∈ΓA(ζ)f(z) exists and is finite for every A>1, and f∗∈Lp(T,m) with ∥f∗∥p≤∥f∥Hp.

(b) If p<∞ then ∥fr−f∗∥p→0 as r↑1 and ∥f∗∥p=∥f∥Hp; for p=∞, ∥f∗∥∞=∥f∥∞ and the radial functions converge to f∗ weak-star against L1(T,m).

(c) If 1≤p≤∞ then f=P[f∗], the Poisson integral of its boundary function; for p=1 it says that the analytic h1 representing measure of f is the absolutely continuous measure f∗m, proved here without the F. and M. Riesz theorem, from the a.e. limits and the L1 convergence in (b).

Facts & Assumptions

Given: Countable choice, 0<p≤∞ and f∈Hp(D).

[F1]

A nonzero Hardy function belongs to N and has finite nonzero nontangential boundary values f∗ under CC, with f∗∈Lp and ∥f∗∥p≤∥f∥Hp. Its logarithm is integrable and log⁡∣f(z)∣≤P[log⁡∣f∗∣](z). A bounded holomorphic function has the CC Poisson representation and equality of infinity norms. (Boundary values and log-integrability of Nevanlinna-class functions, Log-integrability of the boundary values of a Hardy function, Poisson-Jensen inequality for Hardy functions, Bounded holomorphic disc functions have Poisson boundary data and Fatou limits under countable choice, The Axiom of Countable Choice (ACω), The circle maximal function and nontangential approach regions)

[F2]

Convex Jensen for the positive unit-mass Poisson kernel gives exp⁡(pP[u])≤P[epu] for an integrable real u with integrable exponential. The kernel is positive and its circle mass is one. (Jensen's inequality for expectation, The Poisson kernel is positive, has total mass one, and concentrates at a boundary point, The Poisson kernel on the unit disc, The Poisson integral of a finite complex boundary measure)

[F3]

Poisson extension contracts L1 and positivity preserves pointwise order; for bounded datum v, P[v]≤∥v∥∞. Tonelli applies to nonnegative integrands. The integral of an L1 function is absolutely continuous with respect to the measure, which also follows directly by splitting it into a bounded truncation and its small L1 tail. (Poisson extension is an Lp contraction and converges in finite Lp, Tonelli's theorem for nonnegative measurable functions on a sigma-finite product, The Poisson kernel is positive, has total mass one, and concentrates at a boundary point)

[F4]

Dominated convergence and Fatou apply to nonnegative measurable functions. Holder on the probability circle gives ∥v∥1≤∥v∥p for 1≤p≤∞. Radial means define the Hardy norm and increase with the radius. (Dominated convergence, Fatou's lemma, Complex Holder, Minkowski, and the quotient norm, Analytic Hardy spaces on the unit disc, Radial p-means of a holomorphic function are nondecreasing)

[F5]

Holomorphic f equals its locally uniformly convergent Taylor series. Fourier coefficients use the orthonormal circle characters. For each fixed interior z the Poisson kernel has the uniformly absolutely convergent geometric expansion 1+∑n≥1(znζ−n+z‾nζn). (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, Fourier coefficients and trigonometric polynomials on the torus, The trigonometric characters are orthonormal in L2 of the torus, The Poisson kernel on the unit disc)

[F6]

An L1 density first defines a countably additive complex measure by dominated convergence. Its finite positive regular variation is supplied under CC by the local circle-variation lemma. The direct simple-integral and phase-approximation proof of the density formula then gives total variation equal to its absolute density integral; no general Hahn/Jordan existence assertion is used. Under CC finite complex circle measures are uniquely determined by their Poisson integral. (A complex L^1 density defines a complex measure whose total variation is |h| dmu, Complex circle measures have finite regular total variation under countable choice, Finite complex circle measures are determined by Fourier coefficients and Poisson integrals)

[F7]

Under CC, m{MTv>t}≤3∥v∥1/t for L1 data and NA(P[v])≤(A+1)2MTv. For a nonnegative measurable function, its squared integral is ∫0∞2t m{v>t}dt; the same formula for finite truncations and monotone convergence handles extended values. (The circle maximal function is weak type one one for finite measures, Poisson nontangential maximal function is controlled by circle maximal averages, The circle maximal function and nontangential approach regions, For 0 < p < infinity, the layer-cake formula computes the integral of |f|^p from the distribution function, Monotone convergence for the integral)

Proof

1.1F1F2F6givenconstructalgebra

For f identically zero take the zero boundary function; every assertion is immediate, including the unique zero density measure by [F6]. Otherwise [F1] supplies the finite nontangential boundary values and the Lp bound in (a) under CC. For finite p put h=∣f∗∣p∈L1. The Poisson logarithmic inequality and [F2] give ∣f(z)∣p≤P[h](z). For p infinity [F1] already gives the Poisson representation and equality of infinity norms.

2.1step 1.1F3F4constructalgebra

Uniform integrability for finite p. For M≥1 write h=hM+tM, where hM=min⁡(h,M) and tM=(h−M)+. Since h is integrable, ∥tM∥1→0 by [F4]. For every Borel E and every radius r, positivity and [F3] give ∫E∣fr∣pdm≤∫EPrh dm≤Mm(E)+∥tM∥1. The same truncation bounds ∫Eh dm. Therefore both ∣fr∣p uniformly in r and h have arbitrarily small integrals on sets of sufficiently small Haar measure. The inequality ∣a−b∣p≤cp(∣a∣p+∣b∣p), with cp=1 for p≤1 and cp=2p−1 for p≥1, gives the same uniform integrability for er=∣fr−f∗∣p.

2.2step 1.1F4algebra

The infinity case. The equal infinity norms and Poisson representation are in step 1.1. For any a in L1, a(fr−f∗) tends to zero almost everywhere and is bounded by 2∥f∥∞∣a∣, an integrable function. Dominated convergence [F4] gives ∫afrdm→∫af∗dm, exactly the stated weak-star convergence.

3.1step 1.1step 2.1F2F3F4algebra

Strong convergence for finite p. The radial limits in step 1.1 give er→0 almost everywhere. For each eta>0 the indicators of {er>η} tend to zero almost everywhere, so [F4] gives m{er>η}→0. Given epsilon>0, choose delta>0 by step 2.1 so that ∫Eerdm<ε/2 for every r whenever m(E)<δ. Take eta=epsilon/2. For r sufficiently near one the exceptional superlevel has measure below delta, so ∫erdm≤η+∫{er>η}erdm<ε. This argument along every sequence r tending to one proves ∥fr−f∗∥p→0, including p<1. Also step 1.1 and unit kernel mass give ∫∣fr∣pdm≤∫hdm for every r by Tonelli; the supremum and the reverse inequality in (a) yield ∥f∥Hp=∥f∗∥p.

4.1step 3.1F4F5F6algebra

Poisson representation for finite p≥1. Holder [F4] and step 3.1 give L1 convergence of fr to f∗. Write f(z)=∑n≥0cnzn by [F5]. At each r>0 the Fourier coefficients of fr are cnrn for nonnegative n and zero for negative n, by uniform Taylor convergence and orthogonality. L1 convergence passes every Fourier coefficient to the limit, so f∗^(n)=cn for n nonnegative and zero for n negative. Integrate the uniformly absolutely convergent kernel expansion of [F5] against the L1 datum f∗; the uniform error is bounded in integral by its supremum times ∥f∗∥1. The result is P[f∗](z)=∑n≥0cnzn=f(z), proving (c). For p=1, [F6] makes f∗m a finite complex representing measure; any other such measure has the same Poisson integral and is equal to it by [F6]. Its total variation is ∥f∗∥1=∥f∥H1.

5.1step 1.1step 3.1step 2.2step 4.1algebra

Steps 1.1, 3.1, 2.2 and 4.1 prove every clause (a)–(c). All prior AC instances remain covered by the stronger CC conclusion. CC is used by the boundary and Fourier/measure uniqueness suppliers; the uniform integrability and convergence deduction is completely supplied in steps 2.1–3.1.

6.1step 1.1step 3.1F1F2F3F4F7algebra∎

Ancillary maximal bound in the included source. Fix A>1. The superlevel set of NAf at t is the union, over interior z with ∣f(z)∣>t, of the open circle sets {ζ:∣z−ζ∣<A(1−∣z∣)}, so it is Borel measurable. First let u≥0 be in L2 on the circle, hence in L1 by [F4]. For t>0 split u=min⁡(u,t/2)+(u−t/2)+. The first summand has maximal function at most t/2, while subadditivity of averages gives {MTu>t}⊆{MT(u−t/2)+>t/2}. The weak bound in [F7] therefore gives m{MTu>t}≤6t∫{u>t/2}u dm. Apply layer-cake to min⁡(MTu,K), then Tonelli to this nonnegative bound, and finally let K increase to infinity by [F7]. This yields ∫(MTu)2dm≤12∫0∞∫{u>t/2}u dm dt=24∫u2dm. For finite p>0 put q=p/2 and u=∣f∗∣q∈L2. The same Poisson-Jensen and convexity argument as step 1.1 gives ∣f(z)∣q≤P[u](z); applying [F7] gives (NAf)q≤(A+1)2MTu. Since p/q=2, ∥NAf∥pp≤24(A+1)4∫∣f∗∣pdm=24(A+1)4∥f∥Hpp. Thus ∥NAf∥p≤241/p(A+1)4/p∥f∥Hp. For p infinity, NAf≤∥f∥∞ everywhere. All these estimates include f zero and imply the maximal function is finite almost everywhere for finite p.

Remark

The maximal estimate in step 6.1 also closes the maximal-bound clause of the included Garnett source Theorem3.1. It is an additional consequence; clauses (a)–(c) of the Statement retain their full original conclusions.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Log-integrability of the boundary values of a Hardy function

Statement

Let 0<p≤∞ and f∈Hp(D) with f≢0, with its nontangential boundary function f∗ supplied by Boundary values and log-integrability of Nevanlinna-class functions. Then log⁡∣f∗∣∈L1(T,m); equivalently ∫Tlog⁡∣f∗∣ dm>−∞. In particular f∗≠0 m-almost everywhere, and if f∗=0 on a set of positive m-measure then f≡0.

Facts & Assumptions

Given: Countable choice, 0<p≤∞ and a nonzero f∈Hp(D).

[F1]

Hardy membership bounds the radial p-means for finite p and the interior supremum for p infinity. On the probability circle, log⁡+t≤tp/p for p>0. Uniformly bounded radial logarithmic means are equivalent to Nevanlinna membership under countable choice. (Analytic Hardy spaces on the unit disc, The Nevanlinna class on the disc, A harmonic majorant of log^+|F| exists exactly when the radial log^+ means are bounded, The one-dimensional torus and its normalized Haar integral, The Axiom of Countable Choice (ACω))

[F2]

Under countable choice every nonzero Nevanlinna function has finite nonzero nontangential boundary values almost everywhere and an integrable boundary logarithm. (Boundary values and log-integrability of Nevanlinna-class functions)

[F3]

Fatou's lemma bounds the integral of a nonnegative pointwise limit by the limit inferior of the integrals. (Fatou's lemma)

Proof

1.1F1givenalgebra

If p<∞, [F1] gives sup⁡r∫log⁡+∣fr∣dm≤∥f∥Hpp/p<∞. If p=∞, log⁡+∣f∣≤log⁡+∥f∥∞, a constant harmonic majorant. In both cases f∈N(D) by [F1], including functions with origin zeros or no zeros; no zero enumeration or general Hardy boundary theorem is used.

2.1step 1.1F2F3algebra

Apply [F2] to the nonzero f. It gives the finite nontangential boundary function f∗ and log⁡∣f∗∣∈L1. For finite p, [F3] applied along radii to ∣fr∣p also gives ∫∣f∗∣pdm≤∥f∥Hpp; for p infinity, limits preserve the bound ∣f∗∣≤∥f∥∞. Thus the same boundary function is in the asserted Lp class under CC alone.

3.1step 2.1F1algebra

The positive boundary logarithmic part is integrable by the Lp bound and log⁡+t≤tp/p (or the uniform bound at infinity). Hence finiteness of the lower logarithmic integral is equivalent to integrability of its negative part, and so to absolute logarithmic integrability. Both are given by step 2.1.

4.1step 2.1step 3.1algebra∎

An integrable real logarithm is finite almost everywhere, so f∗≠0 almost everywhere. If the boundary function of a Hardy function vanishes on a positive-measure set, it cannot be nonzero by step 2.1; it must therefore be the zero function. This proves all original logarithmic and uniqueness claims under the existing CC class conventions.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Poisson-Jensen inequality for Hardy functions

Statement

Let 0<p≤∞ and f∈Hp(D) with f≢0, with boundary function f∗∈Lp as in Boundary values and log-integrability of Nevanlinna-class functions; by Log-integrability of the boundary values of a Hardy function one has log⁡∣f∗∣∈L1(T,m). Then for every z∈D log⁡∣f(z)∣≤P[log⁡∣f∗∣](z):=∫TP(z,ζ) log⁡∣f∗(ζ)∣ dm(ζ), with the convention log⁡0=−∞. In particular log⁡∣f∣ is majorized on D by the harmonic function P[log⁡∣f∗∣], and equality holds for every z whenever f is outer in the sense of Inner, singular inner and outer functions.

Facts & Assumptions

Given: Countable choice, 0<p≤∞, a nonzero f∈Hp(D), its boundary function f∗ with log⁡∣f∗∣∈L1(T,m), a point z∈D with f(z)≠0, and radii R∈(∣z∣,1).

[L1]

A nonzero Hardy function lies in N and has finite nonzero nontangential boundary values under countable choice, with f∗∈Lp and log⁡∣f∗∣∈L1. In particular radial limits exist almost everywhere. The elementary estimate log⁡+t≤tq/q holds for every q>0. No strong Lp convergence is assumed in this proof. (Boundary values and log-integrability of Nevanlinna-class functions, Log-integrability of the boundary values of a Hardy function, Analytic Hardy spaces on the unit disc, The Nevanlinna class on the disc, The Axiom of Countable Choice (ACω))

[L2]

fR(w):=f(Rw) is holomorphic on a neighbourhood of the closed unit disc, and F(w):=fR(φz(w)) likewise, where φz(w)=z−w1−z‾w is the Blaschke factor; F(0)=f(Rz) and F has finitely many zeros in the open disc (The unit disc, the upper half-plane, and Blaschke factors, Blaschke factors are automorphisms of the disc).

[L3]

Jensen's formula: for F holomorphic on a neighbourhood of the closed unit disc with F(0)≠0, log⁡∣F(0)∣=12π∫02πlog⁡∣F(eiθ)∣ dθ−∑jlog⁡1∣wj∣, the sum over the zeros wj of F in the open unit disc with multiplicity; if F meets a boundary zero the identity is recovered by limits (Jensen's formula on a disc).

[L4]

Change of variables on the circle: φz maps T bijectively onto itself with ∣φz′(ζ)∣=1−∣z∣2∣1−z‾ζ∣2=P(z,ζ), so 12π∫02πG(φz(eiθ)) dθ=∫TG(ζ)P(z,ζ) dm(ζ) for every integrable G on T (Blaschke factors are automorphisms of the disc, The Poisson kernel on the unit disc, The unit disc, the upper half-plane, and Blaschke factors, Conjugation is an involutive real-field automorphism, zz‾=∣z∣2, and modulus is definite, multiplicative, and subadditive).

[L5]

For an L1 real datum its Poisson integral is harmonic; the Poisson kernel has unit mass and is a bounded positive continuous weight at each fixed interior z. Dominated convergence applies to bounded truncated logarithms, and Fatou's lemma to their nonnegative weighted negative parts. (The Poisson integral of a finite complex boundary measure, The Poisson kernel is positive, has total mass one, and concentrates at a boundary point, Dominated convergence, Fatou's lemma)

[L6]

A holomorphic f is outer exactly when log⁡∣f(z)∣=P[log⁡∣f∗∣](z) for all z (Inner, singular inner and outer functions).

Proof

technique · direct
1.1givenL2L3L4algebra

The Jensen inequality. Assume first f(z)≠0 and take R<1 sufficiently close to 1 that f(Rz)≠0, which follows from continuity and f(z)≠0. By [L2] the function F(w)=fR(φz(w)) is holomorphic on a neighbourhood of the closed unit disc with F(0)=f(Rz)≠0; applying [L3] and dropping the nonnegative zero terms gives log⁡∣f(Rz)∣≤12π∫02πlog⁡∣fR(φz(eiθ))∣ dθ (if F has boundary zeros, use the limiting form of [L3]). By the change of variables [L4], the right side equals ∫Tlog⁡∣fR(ζ)∣P(z,ζ) dm(ζ)=∫TP(z,ζ)log⁡∣f(Rζ)∣ dm(ζ).

1.2givenalgebra

The case f(z)=0. If f(z)=0, then log⁡∣f(z)∣=−∞≤P[log⁡∣f∗∣](z) by the convention on log⁡0; the inequality holds trivially.

1.3L1L5givenalgebra

Positive logarithmic parts converge in L1. For finite p set C=∥f∥Hpp, so ∫∣fR∣pdm≤C and ∫∣f∗∣pdm≤C by [L1]. Given ε>0, choose L>0 large enough that log⁡t≤εtp for all t>eL; indeed [L1] with q=p/2 gives log⁡t/tp≤(2/p)t−p/2 for t≥1, and it suffices to take L with (2/p)e−Lp/2≤ε. Writing uR=log⁡+∣fR∣, u∗=log⁡+∣f∗∣, the tails satisfy ∫(uR−L)+dm≤εC,∫(u∗−L)+dm≤εC. The truncated functions min⁡(uR,L) converge almost everywhere to min⁡(u∗,L) and are bounded by L, so [L5] gives L1 convergence by dominated convergence. Therefore lim sup⁡R↑1∥uR−u∗∥1≤2εC, and letting epsilon decrease to zero proves the claim. For p infinity, all positive logarithms are bounded by log⁡+∥f∥∞, so dominated convergence applies directly. These limit statements hold along every sequence tending to one, hence for the stated radial limit.

2.1step 1.1step 1.2step 1.3L1L5algebra

Pass to the Jensen inequality. For f(z) nonzero, let R increase to one in step 1.1. Its left side tends to log⁡∣f(z)∣. The weight P(z,⋅) is bounded by [L5], so step 1.3 gives convergence of the weighted positive logarithmic integrals. Fatou's lemma gives ∫P(z,ζ)log⁡−∣f∗(ζ)∣dm≤lim inf⁡R↑1∫P(z,ζ)log⁡−∣f(Rζ)∣dm. Subtracting this inequality from the positive-part limit bounds the limsup of the Jensen right side by P[log⁡∣f∗∣](z). This quantity is finite by [L1] and the bounded weight, so log⁡∣f(z)∣≤P[log⁡∣f∗∣](z). Step 1.2 covers zeros of f. Only CC boundary existence and the logarithmic tail estimate were used; no AC Hardy representation is invoked.

3.1step 1.1step 2.1L6algebra∎

Equality for outer functions. If f is outer, then by [L6] the identity log⁡∣f(z)∣=P[log⁡∣f∗∣](z) holds for every z, so equality holds in the Poisson-Jensen inequality; thus the inequality is an identity for all nonzero outer functions.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Inner-outer factorisation of a Hardy-space function

Statement

Assume the Axiom of Choice. Let 0<p≤∞ and let f∈Hp(D) with f≢0, with boundary function f∗∈Lp and log⁡∣f∗∣∈L1. Then there exist a constant λ∈T, a Blaschke product B (the product of the normalized Blaschke factors of the zeros of f), a finite positive measure μ⊥m with associated singular inner function Sμ, and the outer function F:=[ ∣f∗∣ ], such that f=λ B Sμ F, with F∈Hp and ∥F∥Hp≤∥f∥Hp, and: B is determined by the zeros of f; F is the unique outer function with F(0)>0 and ∣F∗∣=∣f∗∣ a.e.; μ is the unique finite positive singular measure with Sμ(0)>0 and f/(BSμF) constant of modulus 1; and λ is that constant. The factorization is unique in this normalized sense.

Facts & Assumptions

Given: The Axiom of Choice, hence countable choice; 0<p≤∞ and f∈Hp(D), f≢0.

[L1]

Fatou boundary theorem and log-integrability: f∗∈Lp exists a.e., ∥f∗∥p=∥f∥Hp for p<∞ (with the L∞/weak-star version at p=∞), and log⁡∣f∗∣∈L1 with f∗≠0 a.e. (Fatou's boundary theorem for analytic Hardy spaces, Log-integrability of the boundary values of a Hardy function, Analytic Hardy spaces on the unit disc).

[L2]

Outer functions: F:=[ ∣f∗∣ ] is holomorphic, zero-free, F(0)=exp⁡(∫log⁡∣f∗∣)>0, ∣F∗∣=∣f∗∣ a.e., and F∈Hp with ∥F∥Hp≤∥f∗∥p=∥f∥Hp for p<∞ (and F∈H∞, ∣F∣≤∥f∗∥∞ for p=∞); an outer function with a prescribed boundary modulus and positive value at 0 is unique (Properties of outer functions, Inner, singular inner and outer functions).

[L3]

For finite p, Riesz factorization gives f=Bg with B the Blaschke product of the zeros of f, g zero-free holomorphic with ∥g∥Hp=∥f∥Hp; B is determined by the zeros of f, and ∣B∗∣=1 a.e. (F. Riesz factorization of a Hardy-space function, Blaschke factors and Blaschke products, Boundary values and zeros of a Blaschke product).

[L4]

Poisson-Jensen inequality: for the zero-free g∈Hp one has log⁡∣g(z)∣≤P[log⁡∣g∗∣](z) for every z, with equality when g is outer (Poisson-Jensen inequality for Hardy functions).

[L5]

Zero-free inner functions are singular inner functions: a holomorphic zero-free S with ∣S∣≤1 and ∣S∗∣=1 a.e. satisfies S=λ′Sμ with unique λ′∈T and unique finite positive μ⊥m, normalized by Sμ(0)>0 (Zero-free inner functions are unimodular multiples of singular inner functions).

[L6]

A holomorphic function of constant modulus is constant. In particular, a function holomorphic near a closed disc is bounded by its boundary maximum: an interior maximum exceeding the boundary maximum would force it to be constant (Local maximum modulus principle).

Proof

technique · direct
1.1givenL1L2L3

Put F:=[ ∣f∗∣ ]. By [L1] and [L2], it is holomorphic, zero-free and outer, with F(0)>0, ∣F∗∣=∣f∗∣ almost everywhere, F∈Hp and ∥F∥Hp≤∥f∥Hp. For finite p, [L3] gives f=Bg with g zero-free and ∥g∥Hp=∥f∥Hp. For p=∞, apply [L3] with exponent 1 (bounded f belongs to H1) to obtain the same holomorphic zero-free quotient g=f/B.

2.1step 1.1L1L3L6algebra

For p=∞, fix N and 0<ε<1. The holomorphic quotient gN=f/BN on every radius-R circle sufficiently near 1 satisfies ∣gN∣≤(1−ε)−1∥f∥∞, since BN is continuous on the closed disc with unit boundary modulus. The boundary maximum principle [L6] gives the same bound inside that circle. Let ε↓0, then N→∞ off the zeros of B, where gN→g; continuity extends the bound to those zeros. Thus ∥g∥∞≤∥f∥∞, and ∣B∣≤1 gives equality. In every case [L1] now supplies g∗, so f∗=B∗g∗ and ∣B∗∣=1 yield ∣g∗∣=∣f∗∣ almost everywhere.

3.1step 1.1step 2.1L2L4L5algebra

The quotient is a zero-free inner function. Let S:=g/F, holomorphic and zero-free because both factors are. By [L4] applied to g, log⁡∣g∣≤P[log⁡∣g∗∣]=log⁡∣F∣ on D, since log⁡∣F∣=P[log⁡∣F∗∣]=P[log⁡∣g∗∣]; hence ∣S∣≤1. On the boundary, ∣S∗∣=∣g∗∣/∣F∗∣=1 a.e. By [L5] there are λ′∈T and a unique finite positive μ⊥m with S=λ′Sμ and Sμ(0)>0.

4.1step 1.1step 3.1L2L3L5L6

The factorization and its uniqueness. Substituting gives f=Bg=BFS=λ′ B Sμ F, which is the asserted factorization. Uniqueness: B is determined by the zeros of f by [L3]; ∣F∗∣=∣f∗∣ a.e., F outer and F(0)>0 determine F by [L2]; then S=f/(BF) is determined, and its representation λ′Sμ with Sμ(0)>0 is unique by [L5]; hence λ=λ′ is determined, and writing λ for λ′ gives the stated normalized factorization.

5.1step 1.1step 3.1step 4.1∎

Assembly. Steps 1.1, 3.1 and 4.1 produce the factorization f=λBSμF with the asserted bounds and prove that the normalized factors B,F,Sμ and the constant λ are uniquely determined.

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6.1-sol)Open item page →

The Nevanlinna class on the disc

Definition

Assume countable choice. Write T, m and D for the torus with its normalized Haar measure and the unit disc (The one-dimensional torus and its normalized Haar integral), and put log⁡+x:=max⁡{log⁡x,0} for x>0, with log⁡+0:=0.

A holomorphic function f:D→C (Complex differentiability at a point, the complex derivative, holomorphic functions, and entire functions) belongs to the Nevanlinna class N(D) if the subharmonic function log⁡+∣f∣ has a harmonic majorant on D, that is, if there is a harmonic function h on D with log⁡+∣f(z)∣≤h(z)(z∈D). Since log⁡+∣f∣≥0, any such majorant satisfies h≥0 on D; the function log⁡+∣f∣ is subharmonic: it is zero if f≡0, and otherwise log⁡∣f∣ is subharmonic and log⁡+∣f∣=max⁡(log⁡∣f∣,0) is a finite maximum of subharmonic functions, with log⁡∣f∣=−∞ at the zeros of f (The logarithm of the modulus of a holomorphic function is subharmonic, Subharmonic functions on plane domains). Constant functions are harmonic, so every bounded holomorphic function lies in N(D).

Equivalent sup-mean form. A holomorphic f belongs to N(D) if and only if sup⁡0<r<1∫Tlog⁡+∣f(rζ)∣ dm(ζ)<+∞. The forward direction is the mean value property of a harmonic majorant: if log⁡+∣f∣≤h with h harmonic, then ∫Tlog⁡+∣f(rζ)∣ dm(ζ)≤∫Th(rζ) dm(ζ)=h(0) for every 0<r<1 (Plane harmonic functions satisfy the mean-value property); the converse is the Poisson-modification and increasing-Harnack construction of A harmonic majorant of log^+|F| exists exactly when the radial log^+ means are bounded, which is quoted here as the well-definedness statement for the two equivalent forms. Both forms are used in this pair: the majorant form in The Nevanlinna class is a bounded quotient class and Boundary values and log-integrability of Nevanlinna-class functions, the sup-mean form in Blaschke factorization of a Nevanlinna-class function.

The Hardy classes are contained in N(D). Every Hp(D), 0<p≤∞, is contained in N(D) (Analytic Hardy spaces on the unit disc). For 0<p<∞ one has log⁡+x≤xp/p for every x≥0: the inequality is trivial for x≤1, and for x≥1 it follows from ddx(xp/p−log⁡x)=xp−1−1/x≥0 and its value at x=1 is 1/p>0. Hence ∫Tlog⁡+∣f(rζ)∣ dm(ζ)≤1p∫T∣f(rζ)∣p dm(ζ)≤1p∥f∥Hpp<+∞ for every 0<r<1, so the sup-mean form of membership holds and f∈N(D). For p=∞ one has log⁡+∣f∣≤log⁡+∥f∥H∞ pointwise, because ∣f(z)∣≤∥f∥H∞ and log⁡+ is nondecreasing; the constant function h:=log⁡+∥f∥H∞ is harmonic with log⁡+∣f∣≤h, so f∈N(D) directly by the majorant form. (For ∥f∥H∞<1 the constant majorant is 0, which is why the bound is written with log⁡+ on both sides.)

This is the disc Nevanlinna class of holomorphic functions. No result from Nevanlinna value-distribution theory for meromorphic functions on C is used in this pair. No choice principle beyond countable choice is used.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

A harmonic majorant of log^+|F| exists exactly when the radial log^+ means are bounded

Statement

Let F:D→C be holomorphic and put u:=log⁡+∣F∣. Then u has a harmonic majorant on D if and only if sup⁡0<r<1∫Tlog⁡+∣F(rζ)∣ dm(ζ)<+∞. The forward implication is immediate from the mean value property of a harmonic majorant; the converse is the Poisson-modification construction below.

Facts & Assumptions

Given: A holomorphic function F on the unit disc D, the function u=log⁡+∣F∣=max⁡(log⁡∣F∣,0) with log⁡∣F(z)∣=−∞ at zeros of F, the number C:=sup⁡0<r<1∫Tu(rζ) dm(ζ) where it occurs, and the radii rn:=1−1/(n+1)↑1, n≥1 of the converse construction.

[L1]

If F≢0, then log⁡∣F∣ is subharmonic on D, and a finite maximum of subharmonic functions is subharmonic; subharmonic functions are upper semicontinuous by definition. Hence u=max⁡(log⁡∣F∣,0) is subharmonic and upper semicontinuous; for F≡0 the same holds because u=0. In both cases u≥0 everywhere (The logarithm of the modulus of a holomorphic function is subharmonic, Positive linear combinations and finite maxima preserve subharmonicity, Subharmonic functions on plane domains).

[L2]

Since u is upper semicontinuous on D, on every circle ∂D(0,r) the boundary data ur are upper semicontinuous and bounded above, its average is a well-defined element of [−∞,∞), and there exist boundary approximations ϕn↓u∣∂D(0,r) by continuous functions; the associated harmonic functions hn on D(0,r), continuous on D(0,r)‾, with boundary values ϕn exist uniquely by the Poisson boundary-value theorem, and the Poisson modification PD(0,r)u is PD(0,r)u=inf⁡nhn on D(0,r) (Upper semicontinuous functions are Borel and their circle averages are defined, Poisson modification on a compactly contained disc, The Poisson integral gives the unique continuous harmonic extension on the closed unit disc).

[L3]

The Poisson modification Hr:=PD(0,r)u is well defined, subharmonic on D, harmonic on D(0,r), satisfies Hr≥u on D and equals u outside D(0,r); moreover hn≥Hr≥u on D(0,r) for every boundary approximation (Poisson modification is subharmonic and majorizes the original function).

[L4]

Every plane harmonic function h satisfies the circle mean-value property h(a)=12π∫02πh(a+Reit) dt for every closed disc D(a,R)‾ in its domain (Plane harmonic functions satisfy the mean-value property, The circle and disc mean-value properties). For a continuous G on T one has ∫TG dm=∫[0,1)G(e2πit) dt=12π∫02πG(eis) ds, the last step by the linear change of variables s=2πt (The one-dimensional torus and its normalized Haar integral, The Poisson integral of a finite complex boundary measure, A C^1 diffeomorphism satisfies the change-of-variables formula for L^1 functions); in particular ∫Tu(rζ) dm(ζ)=12π∫02πu(reis) ds.

[L6]

(Minimum principle.) If k is harmonic on a bounded domain Ω and continuous on Ω‾, then inf⁡Ω‾k=inf⁡∂Ωk (Maximum and minimum principles for plane harmonic functions).

[L7]

(Harnack.) A positive harmonic function k on a neighbourhood of D(a,R)‾ satisfies k(z)≤R+ρR−ρk(a) for ∣z−a∣=ρ<R. If (kn) is an increasing sequence of harmonic functions on a domain Ω, then either kn→+∞ pointwise on Ω, or kn converges locally uniformly on Ω to a harmonic limit (Positive harmonic functions on a disc satisfy Harnack's inequality, An increasing harmonic sequence converges locally uniformly to a harmonic limit or diverges to +infinity).

Proof

technique · direct
1.1givenL4algebra

Forward implication. Suppose h is a harmonic majorant of u on D, i.e. h is harmonic and h≥u. Fix 0<r<1; h is harmonic on a neighbourhood of D(0,r)‾, so integrating u(rζ)≤h(rζ) over T and applying the mean-value property in torus form gives ∫Tu(rζ) dm(ζ)≤∫Th(rζ) dm(ζ)=h(0)<+∞. Taking the supremum over r gives the stated bound, so the forward implication holds.

1.2givenL1

If F≡0, then u=0, its radial means are zero and the zero harmonic function is a majorant, so both conditions hold. Assume henceforth F≢0. The function u=log⁡+∣F∣ is subharmonic and nonnegative by [L1]. It is also continuous: F is continuous and x↦log⁡+x, with value 0 at x=0, is continuous on [0,∞).

2.1step 1.2L2L3L4algebra

The modifications and their values at the origin. Since u is continuous by step 1.2, in [L2] choose the specific boundary approximants ϕn=u∣∂D(0,r)+1/n. Their extensions are hn=Pr[u]+1/n, by uniqueness and linearity of the Dirichlet solution. Thus Hr=PD(0,r)u=Pr[u], continuous on the closed radius-r disc, harmonic inside, with boundary value u and Hr≥u by [L3]. Its mean value at the origin is Hr(0)=∫Tu(rζ) dm(ζ) by [L4].

3.1step 2.1L3L6algebra

Monotonicity in the radius. Let 0<r<ρ<1. On ∂D(0,r), Hr=u by step 2.1 whereas Hρ≥u by [L3]. Both are harmonic on D(0,r) and continuous on its closure, so their difference is nonnegative there by the minimum principle [L6]. Hence Hρ≥Hr on D(0,r).

3.2step 2.1L3L7algebra

Harnack bounds for the converse. Suppose C<∞. For ∣z∣<R<r<1, apply [L7] to Hr+ε on the radius-R disc and let ε↓0. Using step 2.1 gives 0≤Hr(z)≤(R+∣z∣)(R−∣z∣)−1C. Letting R↑r yields Hr(z)≤(r+∣z∣)(r−∣z∣)−1C. In particular, for any fixed ∣z∣<r0<1, these values are uniformly bounded for r≥r0, by (r0+∣z∣)(r0−∣z∣)−1C.

4.1step 2.1step 3.1L3L7algebra

Construction of the harmonic majorant. Put rn:=1−1/(n+1) for n≥1 and Hn:=Hrn. Fix R<1. For all n with rn>R, the function Hn is harmonic on a neighbourhood of D(0,R)‾ (namely on D(0,rn)), and by step 3.1 the sequence (Hn)n≥nR is increasing on D(0,R); it is bounded at the origin by C by step 2.1, so the increasing Harnack convergence principle [L7] provides a harmonic function H(R) on D(0,R) with Hn→H(R) locally uniformly there. For R<R′<1 the two limits H(R) and H(R′) agree on D(0,R) by uniqueness of pointwise limits of the same sequence, so there is a single harmonic function H on D with Hn→H locally uniformly on D. For each fixed z∈D and all n with rn>∣z∣ one has Hn(z)≥u(z) by [L3], and (Hn(z)) is eventually nondecreasing by step 3.1, so H(z)=lim⁡nHn(z)≥u(z). Hence H is a harmonic majorant of u on D.

5.1step 1.1step 1.2step 4.1L1∎

Assembly. If a harmonic majorant exists, step 1.1 bounds the radial u-means by its value at the origin, so the supremum is finite. Conversely, if the supremum is finite and equal to C, step 4.1 constructs a harmonic majorant H of u on D; the construction uses the subharmonicity and upper semicontinuity of u from step 1.2 together with the Poisson modifications, so both implications hold.

TheoremStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

The Nevanlinna class is a bounded quotient class

Statement

For a holomorphic f:D→C the following are equivalent:

(i) f∈N(D);

(ii) there exist g,h∈H∞(D) with h zero-free in D and f=g/h, where in addition g and h may be chosen with ∣g∣≤1 and ∣h∣≤1.

The pair (g,h) is not unique: if φ∈H∞ is zero-free then (gφ,hφ) is another representation of the same f, and no uniqueness is asserted. This proof is choice-free: neither the Axiom of Choice nor countable choice is used.

Facts & Assumptions

Given: A holomorphic function f on the unit disc D, and where asserted a representation f=g/h with g,h∈H∞(D) and h zero-free.

[L1]

The class N(D) consists of the holomorphic f for which log⁡+∣f∣ has a harmonic majorant on D, and H∞(D) consists of the bounded holomorphic functions, with ∥g∥∞=sup⁡D∣g∣; every h∈H∞ with ∣h∣≤1 satisfies ∣h∣≤1 and −log⁡∣h∣≥0 pointwise (The Nevanlinna class on the disc, Analytic Hardy spaces on the unit disc).

[L2]

Products and quotients by a nowhere-zero holomorphic function are holomorphic, and the complex exponential is holomorphic and never zero. On the simply connected disc, a zero-free h has a holomorphic logarithm L; holomorphic functions are smooth and their real components harmonic, so log⁡∣h∣=Re⁡L is harmonic. These are choice-free analytic interfaces. (Linearity, product, reciprocal, and quotient rules for complex derivatives, The complex exponential by its power series, A nonvanishing holomorphic function on a homologically simply connected domain has a holomorphic logarithm, Holomorphic functions are real analytic and smooth in their two real coordinates, The C2 real and imaginary parts of a holomorphic function satisfy Laplace's equation and form a harmonic-conjugate pair, Star-shaped plane domains are homologically simply connected)

[L3]

The unit disc is a star-shaped plane domain, hence homologically simply connected; every harmonic function on a homologically simply connected complex domain has a harmonic conjugate there (Star-shaped plane domains are homologically simply connected, Harmonic conjugates exist on homologically simply connected plane domains, Harmonic conjugates).

Proof

technique · direct
1.1givenL1L2algebra

(ii) implies (i). Assume f=g/h with g,h∈H∞(D) and h zero-free. Put λ:=max⁡{∥g∥∞,∥h∥∞,1} and replace (g,h) by (g/λ,h/λ); this leaves f=g/h unchanged and gives ∣g∣≤1 and ∣h∣≤1 on D. Then H:=log⁡+∥g∥∞−log⁡∣h∣ is harmonic on D, because log⁡∣h∣ is harmonic and the first term is constant, and H≥0 because ∣h∣≤1; moreover, at every point where log⁡∣f∣>0 one has log⁡∣f∣=log⁡∣g∣−log⁡∣h∣≤log⁡∥g∥∞−log⁡∣h∣≤H, while where log⁡∣f∣≤0 one has log⁡+∣f∣=0≤H. Hence log⁡+∣f∣≤H with H harmonic on D, so f∈N(D).

1.2givenL1L2L3

(i) implies (ii). Assume f∈N(D) and let h0 be a harmonic majorant of log⁡+∣f∣ on D; then h0≥log⁡+∣f∣≥0 on D. By [L3] there is a harmonic conjugate h~0 of h0 on D, and h:=exp⁡(−h0−ih~0) is holomorphic, zero-free and satisfies ∣h∣=e−h0≤1 on D; hence h∈H∞(D) with ∣h∣≤1.

2.1step 1.2L1L2algebra

The companion numerator. With h as in step 1.2 put g:=fh. Then g is holomorphic on D, and for every z with f(z)≠0, ∣g(z)∣=∣f(z)∣e−h0(z)=elog⁡∣f(z)∣−h0(z)≤elog⁡+∣f(z)∣−h0(z)≤1, while ∣g(z)∣=0≤1 at the zeros of f; here we used log⁡∣f∣≤log⁡+∣f∣≤h0. Thus g∈H∞(D) with ∣g∣≤1, and f=g/h because h is zero-free. This proves (i)⇒(ii) with both functions bounded by 1.

3.1step 1.1step 1.2step 2.1L2algebra∎

Assembly and non-uniqueness. Step 1.1 proves (ii)⇒(i) and steps 1.2 and 2.1 prove (i)⇒(ii), with the normalization ∣g∣≤1, ∣h∣≤1 established in each direction; hence (i) and (ii) are equivalent. If f=g/h with h zero-free and φ∈H∞ is zero-free, then gφ,hφ∈H∞, hφ is zero-free and (gφ)/(hφ)=g/h=f, so the representation is not unique. The construction used only the harmonic conjugate and the exponential, both choice-free, so neither the Axiom of Choice nor countable choice is used.

Remark

The choice-free assertion concerns this direct bounded-function/majorant equivalence: the raw membership clauses of the two definitions are used, and neither completeness nor a boundary representation of their function spaces is invoked. Their other, countable-choice conventions do not enter this construction.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Blaschke factorization of a Nevanlinna-class function

Statement

Let f∈N(D) with f≢0, let (an)n≥1 be its zero sequence repeated with multiplicity and let B be the associated Blaschke product. Then (an) is a Blaschke sequence, so B is a Blaschke product in the sense of Blaschke factors and Blaschke products, the quotient g:=f/B extends holomorphically to D (removable singularities at the an), g has no zeros in D, ∣f(z)∣≤∣g(z)∣ for every z∈D, and g∈N(D).

Facts & Assumptions

Given: A function f∈N(D), f≢0, a harmonic majorant h0≥0 of log⁡+∣f∣, the zero sequence (an) with multiplicity, and the constants N(r):=#{n:∣an∣<r} and S:=∑n(1−∣an∣).

[L1]

Membership f∈N(D) means that log⁡+∣f∣ has a harmonic majorant, and the equivalent sup-mean form holds; conversely a holomorphic F with sup⁡0<r<1∫Tlog⁡+∣F(rζ)∣ dm(ζ)<+∞ lies in N(D) (The Nevanlinna class on the disc, A harmonic majorant of log^+|F| exists exactly when the radial log^+ means are bounded).

[L2]

If F≢0 is holomorphic on D and lim inf⁡r↑1∫Tlog⁡∣F(rζ)∣ dm(ζ)<+∞, then the zero sequence of F satisfies ∑n(1−∣cn∣)<+∞ (The zero set of a Hardy function satisfies the Blaschke condition).

[L3]

For a Blaschke sequence the product B is holomorphic with zeros exactly the an counted with multiplicity and ∣B∣≤1 on D (Blaschke factors and Blaschke products, Boundary values and zeros of a Blaschke product).

[L4]

If F is holomorphic on the punctured disc 0<∣z−a∣<ρ and bounded there, then F extends holomorphically across a; a holomorphic function has a zero of finite order at an isolated zero, and F/B is holomorphic off the zero set of B (Characterizations of removable singularities, Linearity, product, reciprocal, and quotient rules for complex derivatives, Blaschke factors and Blaschke products).

[L5]

Mean value of the logarithm of a linear factor: for every c∈C, ∫Tlog⁡∣ζ−c∣ dm(ζ)=log⁡+∣c∣. For ∣c∣<1 this is ∫Tlog⁡∣1−c‾ζ∣ dm(ζ), the mean of the harmonic function log⁡∣1−c‾w∣ over the unit circle, which equals its value log⁡1=0 at the centre; for ∣c∣>1 it is log⁡∣c∣+∫Tlog⁡∣1−ζ/c∣ dm(ζ)=log⁡∣c∣ by the same mean value property. For ∣c∣=1, apply the boundary-zero limiting form of Jensen to 1−c‾w, whose value at zero is one; its boundary logarithm is log⁡∣ζ−c∣. Here the harmonic functions are real parts of holomorphic functions on a neighbourhood of D‾, and the torus integral agrees with the circle average (Jensen's formula on a disc, A holomorphic function equals its average on every circle inside a larger concentric holomorphy disc, Plane harmonic functions satisfy the mean-value property, The circle and disc mean-value properties, The one-dimensional torus and its normalized Haar integral).

[L6]

If 0≤g1≤g2≤⋯ are measurable with gn↑g pointwise, then ∫gn dm↑∫g dm; moreover for a sequence of nonnegative measurable functions Fatou's inequality ∫lim inf⁡ngn dm≤lim inf⁡n∫gn dm holds (Monotone convergence for the integral, Fatou's lemma).

[L7]

Elementary estimates: log⁡(1/x)≤2(1−x) for 1/2≤x≤1, and log⁡(1/r)≤2(1−r) for 1/2≤r≤1; log⁡+∣g∣≤log⁡+∣f∣+log⁡(1/∣B∣) where B≠0, when g=f/B and ∣B∣≤1. [algebra]

Proof

technique · direct
1.1givenL1L2L3L5

The zero sequence satisfies the Blaschke condition. For every 0<r<1, monotonicity of the integral and log⁡∣f∣≤log⁡+∣f∣≤h0 give ∫Tlog⁡∣f(rζ)∣ dm(ζ)≤∫Th0(rζ) dm(ζ)=h0(0)<+∞ by the mean value property; hence the liminf hypothesis of [L2] holds and ∑n(1−∣an∣)<+∞, so (an) is a Blaschke sequence and B is a well-defined Blaschke product with ∣B∣≤1.

1.2givenL5algebra

The logarithm of one factor. Let a∈D and 0<r<1 with r≠∣a∣. Since ∣ba(rζ)∣=∣a−rζ∣/∣1−a‾rζ∣ and ∫Tlog⁡∣1−a‾rζ∣ dm(ζ)=0 by the mean value property of the zero-free harmonic function log⁡∣1−a‾rw∣ on a neighbourhood of D‾, [L5] gives ∫Tlog⁡1∣ba(rζ)∣ dm(ζ)=log⁡1r−∫Tlog⁡∣ζ−ar∣ dm(ζ)=log⁡1r−log⁡+∣a∣r={log⁡1r,∣a∣<r,log⁡1∣a∣,∣a∣>r.

2.1step 1.1L3L4algebra

The quotient. Put g:=f/B, holomorphic on the complement of the zero set of B. At a point a occurring m≥1 times in the zero sequence, B has a zero of order m and f a zero of order at least m (the sequence lists all zeros with multiplicity), so g is bounded near a and extends holomorphically there by [L4]; hence g extends holomorphically to all of D. Since the zeros of B are exactly the an and g is holomorphic at those points with g≠0 there — the multiplicity of the numerator's zero is exactly exhausted when the sequence is repeated with multiplicity — g has no zero in D; and ∣g∣=∣f∣/∣B∣≥∣f∣ off that zero set because ∣B∣≤1, with the inequality extending to the zeros by continuity.

2.2step 1.2L6L7algebra

The mean of −log⁡∣Br∣ at non-exceptional radii. Fix 0<r<1 with r∉{∣an∣}. The partial sums ∑n≤N−log⁡∣ban(rζ)∣ are nonnegative and increase to −log⁡∣B(rζ)∣ (the product converges and each factor has modulus ≤1), so the monotone convergence theorem [L6] and step 1.2 give ∫Tlog⁡1∣B(rζ)∣ dm(ζ)=∑n∫Tlog⁡1∣ban(rζ)∣ dm(ζ)=N(r)log⁡1r+∑∣an∣>rlog⁡1∣an∣=:R(r), where N(r)<+∞ because (an) has no accumulation point in {∣z∣<r} and the sum is finite: only finitely many zeros have ∣an∣<1/2, while the remaining terms obey log⁡1∣an∣≤2(1−∣an∣) by [L7].

3.1step 2.2L7algebra

Bound at non-exceptional radii. For r≥1/2, R(r)≤2N(r)(1−r)+2S≤2S+2S=4S, because N(r)(1−r)≤∑∣an∣<r(1−∣an∣)≤S and by [L7].

4.1step 2.2step 3.1L6algebra

Exceptional radii. Let r∈[1/2,1) be arbitrary and choose a sequence rk↓r with r<rk<1 and rk∉{∣an∣} for all k (the exceptional set is countable and has no accumulation point below 1). The functions ζ↦−log⁡∣B(rkζ)∣ are nonnegative and converge pointwise m-almost everywhere to −log⁡∣B(rζ)∣: for ζ outside the finite set where B(rζ)=0, continuity of B gives B(rkζ)→B(rζ)≠0. Fatou's inequality [L6] and step 3.1 therefore give ∫Tlog⁡1∣B(rζ)∣ dm(ζ)≤lim inf⁡k∫Tlog⁡1∣B(rkζ)∣ dm(ζ)≤4S.

5.1step 2.1step 4.1L1L7algebra

The quotient lies in N(D). Since g=f/B and ∣B∣≤1, [L7] gives log⁡+∣g∣≤log⁡+∣f∣+log⁡(1/∣B∣). For 1/2≤r<1, steps 2.2, 3.1 and 4.1 and the majorant bound of step 1.1 give ∫Tlog⁡+∣g(rζ)∣ dm(ζ)≤h0(0)+4S; for 0≤r≤1/2 the holomorphic function g is continuous on the compact disc ∣z∣≤1/2, so ∫Tlog⁡+∣g(rζ)∣ dm(ζ)≤log⁡+(sup⁡∣z∣≤1/2∣g(z)∣)<+∞. Hence sup⁡0<r<1∫Tlog⁡+∣g(rζ)∣ dm(ζ)<+∞, and the sup-mean criterion [L1] shows that log⁡+∣g∣ has a harmonic majorant, that is, g∈N(D).

6.1step 1.1step 2.1step 5.1∎

Assembly. Step 1.1 produces the Blaschke sequence and the product B; step 2.1 produces the holomorphic zero-free extension g=f/B with ∣f∣≤∣g∣; and steps 1.2–3.1 verify the sup-mean criterion for g, giving g∈N(D).

TheoremStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Boundary values and log-integrability of Nevanlinna-class functions

Statement

Assume countable choice, as in the defining Nevanlinna and circle conventions. Let f∈N(D) with f≢0. Then f has finite nontangential limits f∗(ζ) for m-almost every ζ∈T, and log⁡∣f∗∣∈L1(T,m); in particular f∗≠0 m-almost everywhere.

Facts & Assumptions

Given: Countable choice and a nonzero f∈N(D).

[F1]

A Nevanlinna function is a quotient f=g/h with bounded holomorphic g,h, h zero-free, and both bounded by one. This construction uses a harmonic conjugate of a majorant and its exponential, without Herglotz representation. (The Nevanlinna class is a bounded quotient class, The Nevanlinna class on the disc)

[F2]

Under countable choice a bounded holomorphic disc function has finite nontangential limits almost everywhere. The same full-measure set works for all cone apertures. (Bounded holomorphic disc functions have Poisson boundary data and Fatou limits under countable choice, The Axiom of Countable Choice (ACω))

[F3]

A nonzero holomorphic function has a finite order at zero, factors there as zmq0 with q0(0)≠0, and has isolated zeros. Holomorphic functions are continuous, and closed bounded annuli in the plane are compact. Jensen's formula on a smaller disc with no boundary zeros gives ∫log⁡∣q0(rζ)∣ dm≥log⁡∣q0(0)∣. Haar measure is normalized to mass one. (The order of a zero is the exponent in its local holomorphic factorization, Identity theorem for holomorphic functions, Zeros of a nonzero holomorphic function are isolated, Heine-Borel in Rn: with the Euclidean metric a subset of Rn is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line, Complex differentiability at a point implies continuity there, Jensen's formula on a disc, The one-dimensional torus and its normalized Haar integral)

[F4]

For nonnegative measurable functions, the integral of the pointwise limit inferior is at most the limit inferior of the integrals. (Fatou's lemma)

Proof

1.1F1F2givenconstruct

Apply [F1] to write f=g/h with ∣g∣,∣h∣≤1 and h zero-free. Both g and h are nonzero functions, since f≢0. By [F2] they have finite nontangential limits g∗,h∗ almost everywhere. We must prove h∗≠0 and the integrability of both boundary logarithms before dividing.

1.2F2F3F4givenconstructalgebra

Let q be any bounded nonzero holomorphic disc function, with bound M>0. By [F3], its origin order m is finite; the quotient q0=q/zm off zero extends holomorphically to the disc with q0(0)≠0. Its zeros on each closed annulus compactly inside the disc are finite: all open neighborhoods containing at most one zero cover the annulus, by continuity at nonzeros and isolatedness at zeros. Compactness in [F3] gives a finite subcover, bounding the number of zeros by its finite size. For every j≥2, choose rj∈(1−1/j,1−1/(j+1)) whose circle contains no zero; only finitely many radii in this interval are forbidden. Countable choice supplies this sequence. Jensen applied to q0 gives ∫log⁡∣q(rjζ)∣ dm=mlog⁡rj+∫log⁡∣q0(rjζ)∣ dm≥mlog⁡(1/2)+log⁡∣q0(0)∣=:c>−∞. Meanwhile log⁡+∣q(rjζ)∣≤log⁡+M=:C. Consequently ∫log⁡−∣q(rjζ)∣ dm≤C−c. The nontangential limits q∗ of [F2] include radial limits; Fatou [F4] applied to the negative parts, with value +∞ at a zero boundary limit, gives ∫log⁡−∣q∗∣ dm≤C−c<∞. The positive part is bounded by C. Thus log⁡∣q∗∣∈L1 and q∗≠0 almost everywhere. This also covers m=0, a zero-free q and a nonzero constant.

2.1step 1.1step 1.2algebra

Apply step 1.2 separately to g and h. On the common full-measure set where their finite nonzero boundary limits exist, the quotient has finite nontangential limit f∗=g∗/h∗. It is nonzero there, and log⁡∣f∗∣=log⁡∣g∗∣−log⁡∣h∗∣∈L1, by the triangle inequality for the two integrable logarithms. This identifies the complex limit directly, without inferring it from a modulus limit.

3.1step 1.1step 1.2step 2.1algebra∎

Step 2.1 proves the entire assertion. Only countable choice has been used: in the bounded-holomorphic boundary supplier [F2] and the sequence of good Jensen radii in step 1.2. No general positive-harmonic measure representation or full-AC decomposition is needed. The excluded zero function nevertheless has the obvious zero boundary function, a convention used by the class definitions without assigning it an integrable logarithm.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

The Smirnov class on the disc

Definition

Assume countable choice. The Smirnov class N+(D) contains 0 and consists otherwise of the nonzero f∈N(D) such that, with f∗ the boundary function of Boundary values and log-integrability of Nevanlinna-class functions (so that log⁡∣f∗∣∈L1(T,m), extended by −∞ where f∗=0), log⁡∣f(z)∣≤P[log⁡∣f∗∣](z)for every z∈D. For the zero function, the boundary function is zero; we interpret both sides of the displayed inequality as −∞. Its boundary logarithm is not an L1 datum, and the finite-measure Poisson construction is used only for nonzero functions. The Poisson integral for the nonzero case is the one of The Poisson integral of a finite complex boundary measure.

By the Poisson-Jensen inequality of Poisson-Jensen inequality for Hardy functions, every f∈Hp(D), 0<p≤∞, lies in N+(D) by the displayed inequality; hence Hp(D)⊆N+(D)⊆N(D)(0<p≤∞), the second inclusion being part of the definition.

Equivalently, N+(D) is the class of quotients g/h with g,h∈H∞(D) and h outer (and then h may be normalized by h(0)>0); this equivalence is proved in The Smirnov class is the class of quotients by outer bounded functions ↗. The class N+ is a complex vector space, as certified using the quotient characterization just proved by The Smirnov class is the class of quotients by outer bounded functions ↗, its justified_by supplier. Indeed, for nonzero fj=gj/hj with bounded holomorphic numerators and bounded outer denominators, h1h2 is bounded and outer: its boundary logarithm is the sum of the two integrable boundary logarithms, and its interior log-modulus is their Poisson integral by linearity, in the outer convention of Inner, singular inner and outer functions. Thus f1+f2=(g1h2+g2h1)/(h1h2) has bounded numerator and bounded outer denominator. If the numerator is zero, the sum is the already included zero function; otherwise the characterization gives membership in N+. Scalar multiplication uses the same denominator and numerator cgj, including c=0. This certification is not used in the proof of the quotient characterization, which depends only on the displayed defining inequality.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

The Smirnov class is the class of quotients by outer bounded functions

Statement

Let f be holomorphic on D with f≢0. Then f∈N+(D) if and only if there are g,h∈H∞(D) with h outer (equivalently log⁡∣h∗∣∈L1 and log⁡∣h(z)∣=P[log⁡∣h∗∣](z) for all z) such that f=g/h. Moreover h may be chosen with h(0)>0 and ∣h∣≤1, and the representation is not unique: (g,h) may be replaced by (gφ,hφ) for any bounded outer φ∈H∞.

Facts & Assumptions

Given: Countable choice and a holomorphic f≢0 on D; in the forward direction its boundary function f∗ with log⁡∣f∗∣∈L1.

[L1]

The Smirnov class N+(D)⊆N(D) consists of the f with log⁡∣f(z)∣≤P[log⁡∣f∗∣](z) for all z, where f∗ is the a.e. boundary function with log⁡∣f∗∣∈L1 (The Smirnov class on the disc, Boundary values and log-integrability of Nevanlinna-class functions).

[L2]

Bounded quotients of Nevanlinna functions: if g,h∈H∞ with h zero-free then f=g/h is holomorphic and lies in N(D); and for nonzero F∈H∞, log⁡∣F∣≤P[log⁡∣F∗∣] with log⁡∣F∗∣∈L1 (The Nevanlinna class is a bounded quotient class, Poisson-Jensen inequality for Hardy functions, The Nevanlinna class on the disc).

[L3]

If H≥0 has log⁡H∈L1, the outer function [H] is holomorphic and zero-free, with log⁡∣[H]∣=P[log⁡H] and [H](0)=exp⁡(∫log⁡H)>0. In particular, for φ≥0 in L1, h=[e−φ] satisfies log⁡∣h∣=−P[φ]≤0, hence ∣h∣≤1. Products of bounded outer functions remain bounded and outer, by adding their integrable boundary logarithms and their Poisson log-modulus identities. (Properties of outer functions, Inner, singular inner and outer functions)

[L5]

A zero-free factor multiplies numerator and denominator without changing the quotient; products of H∞ functions are in H∞ (The Nevanlinna class is a bounded quotient class).

Proof

technique · direct
1.1givenL1L2algebra

Quotients by outer bounded functions lie in N+. Assume f=g/h with g,h∈H∞, h outer and h≢0. By [L2], f is holomorphic and in N(D), and log⁡∣g∣≤P[log⁡∣g∗∣], while outer-ness of h gives log⁡∣h∣=P[log⁡∣h∗∣]; subtracting the two displays gives, using linearity of the Poisson integral, log⁡∣f∣=log⁡∣g∣−log⁡∣h∣≤P[log⁡∣g∗∣−log⁡∣h∗∣]=P[log⁡∣f∗∣], with the identification f∗=g∗/h∗ a.e. and log⁡∣f∗∣=log⁡∣g∗∣−log⁡∣h∗∣∈L1 by [L2]. Hence f∈N+(D) by [L1].

2.1step 1.1L1L3algebra

A Smirnov function is such a quotient. Assume f∈N+(D), so by [L1] log⁡∣f∗∣∈L1 and log⁡∣f∣≤P[log⁡∣f∗∣]. Put φ:=log⁡+∣f∗∣+1≥1, an L1 function, and h:=[e−φ]. By [L3], h is outer with 0<h(0)=e−∫φ≤e−1<1 and ∣h∣=e−P[φ]≤1, so h∈H∞ and h is outer. Let g:=fh, holomorphic on D. Then log⁡∣g∣=log⁡∣f∣−P[φ]≤P[log⁡∣f∗∣]−P[φ]=P[log⁡∣f∗∣−log⁡+∣f∗∣−1]=P[−log⁡− ⁣∣f∗∣−1]≤−1, because −log⁡−∣f∗∣−1≤−1 pointwise, and the Poisson integral of a function ≤−1 is ≤−1. Hence ∣g∣≤e−1<1 and g∈H∞(D), while f=g/h with h outer, h(0)>0, ∣h∣≤1.

3.1step 1.1step 2.1L3L5algebra

Non-uniqueness and normalization. If f=g/h with g,h∈H∞ and h outer, and φ∈H∞ is outer, both products gφ,hφ are bounded holomorphic by [L5]. The denominator is outer by [L3] and is zero-free. Therefore (gφ)/(hφ)=f is another representation with an outer denominator. Taking, for example, the constant outer multiplier 2 gives a distinct pair, so the representation is not unique. Step 2.1 already constructs a denominator with h(0)>0 and ∣h∣≤1. A merely zero-free bounded multiplier preserves the quotient but need not preserve an outer denominator.

4.1step 1.1step 2.1step 3.1∎

Assembly. Step 1.1 proves the backward implication, steps 2.1 and 3.1 the forward implication with the stated normalization, and step 3.1 records the non-uniqueness. This proves the equivalence of membership in N+(D) with the quotient representation.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

A maximum principle for the Smirnov class: N+∩Lp=Hp

Statement

Let 0<p≤∞ and let f∈N+(D) with boundary function f∗ (as in Boundary values and log-integrability of Nevanlinna-class functions). If f∗∈Lp(T,m) then f∈Hp(D) and ∥f∥Hp=∥f∗∥p(0<p<∞),∥f∥∞=∥f∗∥∞. Consequently a function of N+(D) lies in Hp(D) exactly when its boundary function lies in Lp, with equality of norms; this is written N+∩Lp=Hp. (The statement is false with N in place of N+: the reciprocal 1/Sμ of a nonconstant singular inner function lies in N with unimodular boundary values, but is not bounded on D and hence not in H∞.)

Facts & Assumptions

Given: Countable choice, 0<p≤∞ and f∈N+(D) whose boundary function satisfies f∗∈Lp(T,m).

[L1]

For nonzero f, N+ membership means f∈N(D), log⁡∣f∗∣∈L1 and log⁡∣f(z)∣≤P[log⁡∣f∗∣](z) for all z; and fr→f∗ m-almost everywhere (The Smirnov class on the disc, Boundary values and log-integrability of Nevanlinna-class functions).

[L2]

Convex Jensen for the probability density P(z,ζ)dm(ζ): for the convex function t↦ept and an integrable real u with epu∈L1(P dm), ep∫P(z,ζ)u(ζ)dm(ζ)≤∫P(z,ζ)epu(ζ)dm(ζ); in particular with u=log⁡∣f∗∣ one has ∣f(z)∣p≤P[∣f∗∣p](z) whenever log⁡∣f∗∣∈L1 and ∣f∗∣p∈L1 (Jensen's inequality for expectation, The Poisson integral of a finite complex boundary measure, The Smirnov class on the disc).

[L3]

Fubini-Tonelli on the product of the probability space (T,m) with itself, and ∫TP(rζ,η)dm(ζ)=1 for every fixed η; ∥⋅∥Hp is the supremum of the radial Lp means, nondecreasing in the radius (Fubini's theorem for L^1 functions on a sigma-finite product, Tonelli's theorem for nonnegative measurable functions on a sigma-finite product, Radial p-means of a holomorphic function are nondecreasing, Analytic Hardy spaces on the unit disc).

[L4]

Fatou's lemma: ∫lim inf⁡rgr dm≤lim inf⁡r∫gr dm for nonnegative measurable gr (Fatou's lemma).

[L5]

For a nonzero finite positive singular measure μ, Sμ is zero-free, ∣Sμ∣≤1, Sμ(0)=e−μ(T)<1, and ∣Sμ∗∣=1 almost everywhere under CC. Its reciprocal is holomorphic with log⁡∣1/Sμ∣=P[μ]≥0, hence belongs to N. If the reciprocal were bounded, its boundary modulus one and the CC bounded-holomorphic norm identity would force ∣1/Sμ∣≤1, contradicting 1/Sμ(0)>1. Thus it is not bounded; no divergence claim at every support point is required. (Properties of the singular functions Sμ, Bounded holomorphic disc functions have Poisson boundary data and Fatou limits under countable choice, Inner, singular inner and outer functions, Boundary values and log-integrability of Nevanlinna-class functions)

Proof

technique · direct
1.1givenL1L2L3algebra

If f≡0, its boundary function and every asserted norm are zero, so all conclusions hold. Assume henceforth f≢0. The case p<∞: Hp membership and the bound ∥f∥Hp≤∥f∗∥p. Assume p<∞ and f∗∈Lp. By [L1], log⁡∣f∗∣∈L1 and log⁡∣f(z)∣≤P[log⁡∣f∗∣](z), so [L2] (applied with u=log⁡∣f∗∣, for which epu=∣f∗∣p∈L1) gives ∣f(z)∣p≤P[∣f∗∣p](z) for every z∈D. Integrating over the circle ∣z∣=r and using Tonelli's theorem and the unit mass of the kernel [L3] gives ∫T∣f(rζ)∣p dm(ζ)≤∫T∣f∗∣p dm for every r<1; hence f is holomorphic with bounded radial means, that is f∈Hp(D), and ∥f∥Hp≤∥f∗∥p.

2.1step 1.1L1L3L4algebra

The reverse inequality by Fatou. By [L1], f(rζ)→f∗(ζ) m-almost everywhere; Fatou's lemma [L4] applied to the nonnegative functions ∣fr∣p gives ∥f∗∥pp=∫∣f∗∣p dm≤lim inf⁡r∫∣fr∣p dm≤sup⁡r∫∣fr∣p dm=∥f∥Hpp, using the definition of the Hp norm as a supremum [L3]. Together with step 1.1 this gives ∥f∥Hp=∥f∗∥p.

2.2step 1.1L1algebra

The case p=∞. If f∗∈L∞, then log⁡∣f∗∣≤log⁡∥f∗∥∞ a.e., so P[log⁡∣f∗∣]≤log⁡∥f∗∥∞ and the defining inequality of [L1] gives ∣f(z)∣≤∥f∗∥∞ for every z, that is f∈H∞ with ∥f∥∞≤∥f∗∥∞. Conversely, f∗ is an a.e. limit of the radial functions fr, so ∣f∗∣≤sup⁡z∈D∣f(z)∣=∥f∥∞ a.e. and ∥f∗∥∞≤∥f∥∞; hence ∥f∥∞=∥f∗∥∞.

3.1step 1.1step 2.1step 2.2L5∎

Assembly and sharpness for N. Steps 1.1, 2.1 and 2.2 prove N+∩Lp=Hp with equality of norms for every 0<p≤∞: if f∈N+ and f∗∈Lp then f∈Hp with the stated norm identity, and the reverse inclusion Hp⊆N+ is in the definition of N+. The sharpness assertion is [L5]: the reciprocal of a nonconstant singular inner function lies in N with unimodular boundary values, so N∩L∞≠H∞, showing that the maximum principle fails for N.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Analytic Poisson integrals are exactly the measures with vanishing negative coefficients

Statement

Assume countable choice, as in the circle conventions. Let μ be a finite complex Borel measure on T and let μ^(n):=∫Tζ−n dμ(ζ),n∈Z, where exponents are read through the identification φ([t])=e2πit of T with the Euclidean unit circle, so that ζ−n is the character e−n(ζ) of Fourier coefficients and trigonometric polynomials on the torus. The following are equivalent:

(i) P[μ] is holomorphic on D;

(ii) P[μ](z)=∑n≥0μ^(n)zn for ∣z∣<1, the power series obtained from the Poisson kernel expansion, with no negative powers of z;

(iii) μ^(n)=0 for every n<0.

When these hold, P[μ]∈H1(D) with ∥P[μ]∥H1≤∣μ∣(T), and its Taylor coefficients are the μ^(n), n≥0.

Facts & Assumptions

Given: Countable choice and a finite complex Borel measure μ on T, its Poisson integral P[μ], and the coefficients μ^(n)=∫Te−n dμ, n∈Z.

[L1]

Setting T=R/Z identified with the Euclidean unit circle through φ([t])=e2πit, the Poisson kernel is P(z,ζ)=P(z,φ(ζ))=(1−∣z∣2)/∣φ(ζ)−z∣2 for z∈D, ζ∈T, and P[μ](z)=∫TP(z,ζ) dμ(ζ); for z=reiϕ one has P(z,eit)=Pr(t−ϕ)=(1−r2)/(1−2rcos⁡(t−ϕ)+r2) (The Poisson integral of a finite complex boundary measure, The Poisson kernel on the unit disc, The one-dimensional torus and its normalized Haar integral).

[L2]

The kernel is strictly positive with unit mass: Pr(θ)>0 and 12π∫02πPr(θ) dθ=1 for 0≤r<1 (The Poisson kernel is positive, has total mass one, and concentrates at a boundary point).

[L3]

Characters satisfy ekel=ek+l, ∣ek∣=1, ek‾=e−k, ek=φk, and they are orthonormal: ∫Tekel‾ dm=δkl (Fourier coefficients and trigonometric polynomials on the torus, The trigonometric characters are orthonormal in L2 of the torus).

[L4]

Under CC every complex circle measure has finite regular total variation, and integration obeys ∣∫u dμ∣≤∫∣u∣d∣μ∣. In particular ∣μ∣(E)≤∣μ∣(T)<∞. (Complex circle measures have finite regular total variation under countable choice, Integrals against signed or complex measures are bounded by total variation, The Axiom of Countable Choice (ACω))

[L5]

Fubini's theorem applies to functions integrable for a product of sigma-finite measures, and Tonelli's theorem applies to nonnegative product-measurable functions (Fubini's theorem for L^1 functions on a sigma-finite product, Tonelli's theorem for nonnegative measurable functions on a sigma-finite product).

[L6]

A holomorphic function equals its Taylor series throughout the largest centred open disc contained in its domain, and the sum of a complex power series is analytic, hence holomorphic, on its open disc of convergence; a complex power series converges absolutely and uniformly on every closed subdisc strictly inside its disc of convergence (A holomorphic function equals its Taylor series throughout the largest centred disc in its domain, The sum of a complex power series is analytic throughout its open disc of convergence, A complex function is holomorphic if and only if it is analytic, A complex power series converges absolutely and uniformly on every closed subdisc strictly inside its disc of convergence).

[L7]

The classes Hp(D) with their (quasi-)norms are those of Analytic Hardy spaces on the unit disc; in particular ∥f∥H1=sup⁡0≤r<1∫T∣f(rζ)∣ dm(ζ) (Analytic Hardy spaces on the unit disc, Complex differentiability at a point, the complex derivative, holomorphic functions, and entire functions).

Proof

technique · direct
1.1L1L3algebra

Expansion of the kernel. Fix z∈D and ζ∈T, put ξ:=φ(ζ)∈C, so that ∣ξ∣=1 and ξ−1=ξ‾, and put w:=zξ−1, so ∣w∣=∣z∣<1. Dividing numerator and denominator of (ξ+z)/(ξ−z) by ξ and using P(z,ζ)=Re⁡[(ξ+z)/(ξ−z)] gives P(z,ζ)=Re⁡[(1+w)/(1−w)]; since (1+w)/(1−w)=1+2∑n≥1wn for ∣w∣<1, and wn=znξ−n=zne−n(ζ) while w‾ n=z‾ nξn=z‾ nen(ζ), taking real parts yields P(z,ζ)=1+∑n≥1(zne−n(ζ)+z‾ nen(ζ)), a series that converges absolutely and uniformly in ζ∈T for fixed z, because ∣zne−n(ζ)∣+∣z‾ nen(ζ)∣=2∣z∣n and ∑n∣z∣n<∞.

1.2L4L6algebra

(ii) implies (i). Assume (ii) and put g(z):=∑n≥0μ^(n)zn. Since ∣μ^(n)∣≤∣μ∣(T) for every n, the series converges for ∣z∣<1; its sum g is analytic on the open unit disc by [L6] and hence holomorphic there by A complex function is holomorphic if and only if it is analytic, and (ii) says P[μ]=g. Thus (i) holds.

1.3L1L2L4L5algebra

The H1 bound. For every z∈D and every radius 0<r<1, [L1] and [L4] give ∣P[μ](z)∣≤∫TP(z,ζ) d∣μ∣(ζ) and hence, integrating over the circle z=rζ′ against m, ∫T∣P[μ](rζ′)∣ dm(ζ′)≤∫T(∫TP(rζ′,η) dm(ζ′))d∣μ∣(η)=∣μ∣(T); the interchange is Tonelli's theorem applied to the nonnegative product-measurable integrand (ζ′,η)↦P(rζ′,η), and the inner integral equals the unit mass of the kernel by [L2] together with translation invariance of m, the substitution showing ∫TP(rζ′,η) dm(ζ′)=12π∫02πPr(θ) dθ=1.

2.1step 1.1L1L3L4algebra

Termwise integration and the two-sided expansion. For fixed z∈D the partial sums of the series of step 1.1 converge uniformly on T to the continuous function ζ↦P(z,ζ), so integrating term by term against the finite complex measure μ gives P[μ](z)=μ(T)+∑n≥1((∫Te−n dμ)zn+(∫Ten dμ)z‾ n)=∑n≥0μ^(n) zn+∑n<0μ^(n) z‾ −n, since μ(T)=∫e0 dμ=μ^(0) and, for n≥1, ∫en dμ=μ^(−n) by the substitution m=−n. This identity holds for every finite complex Borel measure μ and every z∈D.

3.1step 2.1L3L4algebra

Fourier coefficients of the radial traces. Fix 0<r<1 and m∈Z, and regard a torus element ζ′ also as the unit-circle point φ(ζ′), writing ζ′ n:=en(ζ′). Since φ(ζ′)‾ ∣n∣=φ(ζ′)−∣n∣=e−∣n∣(ζ′), evaluating step 2.1 at z=rφ(ζ′) gives P[μ](rζ′)=∑n≥0μ^(n)rnζ′ n+∑n<0μ^(n)r∣n∣ζ′ n=∑n∈Zμ^(n)r∣n∣ζ′ n, a series that converges uniformly in ζ′∈T because ∑n∣μ^(n)∣r∣n∣≤∣μ∣(T)∑nr∣n∣<∞ by [L4]; the function ζ′↦P[μ](rζ′) is therefore continuous and its m-th Fourier coefficient is ∫TP[μ](rζ′)e−m(ζ′) dm(ζ′)=∑n∈Zμ^(n)r∣n∣∫Ten−m dm=μ^(m) r∣m∣, by termwise integration and orthonormality.

4.1step 2.1step 3.1L3L4algebra

Equivalence of (ii) and (iii). If (iii) holds, the second sum in the expansion of step 2.1 vanishes termwise, so P[μ](z)=∑n≥0μ^(n)zn for every ∣z∣<1, which is (ii). Conversely assume (ii). For m<0 and 0<r<1, the right side of (ii) is the uniformly convergent series ∑k≥0μ^(k)rkζ′ k on T (uniform convergence as in step 3.1, using ∣μ^(k)∣≤∣μ∣(T)), so integrating it against e−m and using orthonormality gives ∫TP[μ](rζ′)e−m(ζ′) dm(ζ′)=0; by step 3.1 this equals μ^(m)r∣m∣, hence μ^(m)=0 for every m<0, which is (iii).

4.2step 3.1L4L6algebra

(i) implies (iii), and the Taylor coefficients. Assume (i). By [L6] the holomorphic function P[μ] equals its Taylor series P[μ](z)=∑k≥0akzk throughout D, and this series converges uniformly on the closed subdisc ∣z∣≤r for every fixed 0<r<1. Fix such an r and m∈Z. Evaluating at z=rφ(ζ′) gives the uniformly convergent series P[μ](rζ′)=∑k≥0akrkζ′ k; integrating against e−m and using orthonormality, its m-th Fourier coefficient is amrm when m≥0 and 0 when m<0. Comparing with the identity of step 3.1 gives amrm=μ^(m)rm for m≥0, so am=μ^(m) for every m≥0 (take any r∈(0,1)), and 0=μ^(m)r∣m∣ for m<0, so μ^(m)=0 for every m<0, which is (iii).

5.1step 4.1step 1.2step 4.2step 1.3L7∎

Assembly. Steps 4.1, 1.2 and 4.2 prove that (i), (ii) and (iii) are equivalent: (ii) and (iii) are equivalent by step 4.1, (ii) implies (i) by step 1.2, and (i) implies (iii) by step 4.2, while (iii) implies (ii) again by step 4.1. If the equivalent conditions hold, then by step 4.2 the Taylor coefficients of P[μ] are am=μ^(m) for m≥0, its holomorphy is (i), and step 1.3 gives sup⁡0<r<1∫T∣P[μ](rζ′)∣dm(ζ′)=:∥P[μ]∥H1≤∣μ∣(T)<+∞ by [L7], so P[μ]∈H1(D) with the asserted bound.

TheoremStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

The F. and M. Riesz theorem

Statement

Assume countable choice, as in the circle and Hardy conventions. Let μ be a finite complex Borel measure on T whose Fourier coefficients μ^(n)=∫Tζ−n dμ(ζ) vanish for every n<0. Then μ is absolutely continuous with respect to m. More precisely, f:=P[μ] is holomorphic on D and lies in H1(D), and if f∗ is the boundary function of the Fatou theorem for analytic H1 then μ=f∗m; consequently ∣μ∣(T)=∥f∗∥1=∥f∥H1.

Facts & Assumptions

Given: Countable choice and a finite complex Borel measure μ on the circle with μ^(n)=0 for every n<0; put f=P[μ].

[F1]

The analytic Poisson coefficient criterion gives f holomorphic and in H1, with ∥f∥H1≤∣μ∣(T). Under CC complex circle measures have finite regular total variation. (Analytic Poisson integrals are exactly the measures with vanishing negative coefficients, Complex circle measures have finite regular total variation under countable choice, The Axiom of Countable Choice (ACω))

[F2]

The CC analytic Hardy boundary theorem gives f∗∈L1, finite nontangential limits, ∥fr−f∗∥1→0 and ∥f∗∥1=∥f∥H1. (Fatou's boundary theorem for analytic Hardy spaces, Analytic Hardy spaces on the unit disc)

[F3]

The circle Fourier coefficients of (P[μ])r are r∣n∣μ^(n), and equality of all Fourier coefficients determines a complex circle measure under CC. Fourier coefficients of L1 functions are bounded linear integrals. (Finite complex circle measures are determined by Fourier coefficients and Poisson integrals, Fourier coefficients and trigonometric polynomials on the torus)

[F4]

An L1 density h defines a complex measure h m by dominated convergence. Its known finite positive variation is supplied by the local CC circle-variation lemma; the direct unit-bounded simple-integral and phase-approximation argument gives ∣hm∣(E)=∫E∣h∣dm. (A complex L^1 density defines a complex measure whose total variation is |h| dmu, Complex circle measures have finite regular total variation under countable choice)

Proof

1.1F1F2given

By [F1], f=P[μ] is holomorphic and in H1. By [F2] it has the L1 boundary function f∗ with radial L1 convergence and the exact H1 norm. This covers f zero as well.

2.1step 1.1F3F4constructalgebra

Let ν=f∗m, a finite complex measure by [F4]. For each integer n, [F3] gives fr^(n)=r∣n∣μ^(n). L1 convergence in step 1.1 implies fr^(n)→f∗^(n), since the character has modulus one. Letting r increase to one yields ν^(n)=f∗^(n)=μ^(n). Fourier uniqueness [F3] gives μ=ν=f∗m, so μ≪m. No general h1 measure-existence theorem is invoked; the measure mu was already given.

3.1step 1.1step 2.1F2F4algebra∎

By [F4] and step 2.1, ∣μ∣(T)=∫∣f∗∣dm=∥f∗∥1. Step 1.1 gives ∥f∗∥1=∥f∥H1, proving the full norm identity. Holomorphy, boundary representation, absolute continuity and all stated equalities have now been established under CC.

CorollaryStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Cauchy representation of an H1 function from its boundary values

Statement

Assume countable choice, as in the Hardy and circle conventions. Let f∈H1(D) and let μ be the unique finite complex Borel measure on T with f=P[μ]. Then μ≪m and μ=f∗m for the boundary function f∗ of the Fatou theorem, and for every z∈D f(z)=P[f∗](z)=∫TP(z,ζ)f∗(ζ) dm(ζ)=12πi∮Tf∗(ζ)ζ−z dζ. Moreover ∥f∥H1=∥f∗∥1=∣μ∣(T) and ∥fr−f∗∥1→0 as r↑1.

Facts & Assumptions

Given: Countable choice and f∈H1(D).

[F1]

The CC analytic Hardy boundary theorem gives f∗∈L1, f=P[f∗], ∥fr−f∗∥1→0 and ∥f∗∥1=∥f∥H1. Its analytic H1 representing measure exists and is unique under CC. (Fatou's boundary theorem for analytic Hardy spaces, Analytic Hardy spaces on the unit disc, The Axiom of Countable Choice (ACω))

[F2]

The density measure f∗m is countably additive by dominated convergence; its finite positive variation is supplied by the local CC circle-variation lemma, and the direct density formula gives total variation integral ∫∣f∗∣dm, and finite complex circle measures with equal Poisson integrals are equal under CC. (A complex L^1 density defines a complex measure whose total variation is |h| dmu, Complex circle measures have finite regular total variation under countable choice, Finite complex circle measures are determined by Fourier coefficients and Poisson integrals)

[F3]

Cauchy's integral formula applies on every radius-r circle with |z|<r<1. The torus parametrization is ζ=e2πit with dm=dt. (Cauchy's integral formula on a circle compactly contained in a disc of holomorphy, The one-dimensional torus and its normalized Haar integral)

[F4]

The Poisson integral is the kernel integral against the boundary datum. L1 convergence and uniform convergence of bounded weights imply convergence of their integrals, by the estimate ∣∫(vrwr−vw)dm∣≤∥vr−v∥1∥wr∥∞+∥v∥1∥wr−w∥∞. (The Poisson integral of a finite complex boundary measure)

Proof

1.1F1F2givenconstructalgebra

Apply [F1] and set μ=f∗m. By [F2] it is a finite complex representing measure for f, and its total variation is ∥f∗∥1=∥f∥H1. Every other finite complex representing measure has the same Poisson integral, so [F2] proves it equals mu. Thus the unique measure in the Statement is exactly this absolutely continuous density measure, including mu zero when f zero.

2.1step 1.1F1F4algebra

By [F1] and [F4], f=P[f∗]=∫P(z,ζ)f∗(ζ)dm, and ∥fr−f∗∥1→0. Together with step 1.1 this gives the full Poisson, absolute-continuity, uniqueness and norm assertions under CC.

3.1step 2.1F3F4algebra

The Cauchy formula. Fix z∈D and r∈(∣z∣,1). The function f is holomorphic on a neighbourhood of the closed disc of radius r, so [F3] gives f(z)=12πi∮∣ζ∣=rf(ζ)ζ−z dζ. Writing the circle integral in the torus parametrization, this equals ∫Trζrζ−zf(rζ) dm(ζ) (the factor rζ is dζ2πi dm). As r↑1, the weights rζrζ−z converge uniformly on T to ζζ−z and are uniformly bounded for r≥(1+∣z∣)/2, because ∣rζ−z∣≥r−∣z∣≥(1−∣z∣)/2>0; together with ∥fr−f∗∥1→0 from step 2.1, [F4] gives f(z)=∫Tζζ−zf∗(ζ) dm(ζ)=12πi∮Tf∗(ζ)ζ−z dζ, the last equality being the same parametrization at r=1.

4.1step 1.1step 2.1step 3.1∎

Assembly. Step 1.1 gives μ=f∗m with the norm identity, step 2.1 gives f=P[f∗]=∫P(z,ζ)f∗dm and the L1 convergence of the radial functions, and step 3.1 gives the Cauchy representation of f by its boundary values.

5 · Examples, counterexamples and false statements

None yet.

Sources