Alphabeta Math
PropositionStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedprecheck passaudited 2026-09-30
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Entire-function order agrees with maximum-modulus order

Statement

For an entire function f, define M(r,f)=max⁡∣z∣=r∣f(z)∣,m0(r,f)=12π∫02πlog⁡+∣f(reit)∣ dt,T0(r,f)=m0(r,f)+N(r,∞;f)=m0(r,f). For every nonconstant entire f and 0<r<R, T0(r,f)≤log⁡+M(r,f)≤R+rR−r T0(R,f). Its Nevanlinna order ρ(f) and lower order λ(f) from Order and lower order from the Nevanlinna characteristic agree with lim sup⁡r→∞log⁡(log⁡+M(r,f))log⁡r,lim inf⁡r→∞log⁡(log⁡+M(r,f))log⁡r, respectively; these limits are taken for sufficiently large r with log⁡+M(r,f)>1.

Facts & Assumptions

Given: A nonconstant entire f on C and the chordal characteristic and order conventions of Counting, chordal proximity and characteristic and Order and lower order from the Nevanlinna characteristic.

[F1]

T(r,h)=m(r,∞;h)+N(r,∞;h), and m(r,∞;h) is the circular mean of 12log⁡(1+∣h∣2) (Counting, chordal proximity and characteristic).

[F2]

The Poisson–Jensen identity on ∣z∣≤R subtracts the zero Green terms and adds the pole Green terms; at a boundary divisor the identity is interpreted by the limit through regular radii (Poisson–Jensen formula for a meromorphic function on a disc).

[F3]

For nonconstant meromorphic f, T(r,f)>1 for all sufficiently large r (Order and lower order from the Nevanlinna characteristic).

[F4]

An entire function equals its Taylor series throughout its largest centred disc; for f entire this gives f(z)=∑n≥0anzn for every z∈C (A holomorphic function equals its Taylor series throughout the largest centred disc in its domain).

[F5]

If M bounds ∣f∣ on ∣z∣=r, then each Taylor coefficient an satisfies ∣an∣≤M/rn (Cauchy's inequalities bound the Taylor coefficients by the circle supremum).

[F6]

Every nonempty subset of N has a least element (The well-ordering principle), used to select the first nonzero positive Taylor index.

Proof

technique · Compare the chordal characteristic with $T_0=m_0+N_\infty$, bound the maximum modulus above by Poisson–Jensen, and squeeze both logarithmic limits after setting $R=2r$
1.1F1algebra

For every finite w, log⁡+∣w∣≤12log⁡(1+∣w∣2)≤log⁡+∣w∣+12log⁡2. Since an entire function has no poles, [F1] gives T0(r,f)=m0(r,f) and 0≤T(r,f)−T0(r,f)≤c, where c=12log⁡2<1.

1.2F4F5F6givenalgebra

By [F4], write f(z)=∑n≥0anzn on C. Since f is nonconstant, let k≥1 be the least index with ak≠0. Applying [F5] on the radius-r circle, with any larger holomorphy radius such as 2r, gives ∣ak∣≤M(r,f)/rk. Thus M(r,f)≥∣ak∣rk and log⁡+M(r,f)→∞; in particular log⁡+M(r,f)>1 for all sufficiently large r.

2.1F1step 1.1algebra

On ∣z∣=r, log⁡+∣f(z)∣≤log⁡+M(r,f). Averaging gives T0(r,f)=m0(r,f)≤log⁡+M(r,f).

2.2F1F2step 1.1algebra

Fix 0<r<R. For ∣z∣=r with f(z)≠0, [F2] and the absence of poles give log⁡∣f(z)∣≤(2π)−1∫02πPR(z,t)log⁡+∣f(Reit)∣ dt, since every zero Green term is nonnegative. Indeed ∣R2−b‾z∣2−R2∣z−b∣2=(R2−∣z∣2)(R2−∣b∣2)>0, so GR(z,b)>0. Also 0<PR(z,t)≤(R+∣z∣)/(R−∣z∣)≤(R+r)/(R−r). If f(z)=0, its log⁡+ is zero, so the same bound for log⁡+∣f(z)∣ holds trivially. Taking the supremum over ∣z∣=r yields log⁡+M(r,f)≤R+rR−rm0(R,f)=R+rR−rT0(R,f). For a zero on the outer circle, pass through the boundary-radius limit in [F2]; m0(s,f) is continuous in s because f is continuous on compact annuli.

3.1F1F3step 1.1step 1.2step 2.1step 2.2algebra∎

Put L(r)=log⁡+M(r,f). From steps 2.1–2.2 with R=2r, T0(r,f)≤L(r)≤3T0(2r,f). By [F3] and step 1.1, T0(r,f)≥T(r,f)−c>1−c>0 for all sufficiently large r, while step 1.2 gives L(r)>1 there. Thus the logarithms are defined, log⁡T(r,f)−log⁡T0(r,f)=O(1) by the mean-value bound on [1−c,∞), and log⁡T0(r,f)log⁡r≤log⁡L(r)log⁡r≤log⁡3log⁡r+log⁡T0(2r,f)log⁡r. Replacing r by 2r leaves both limsup and liminf of log⁡T0(r,f)/log⁡r unchanged because log⁡(2r)/log⁡r→1; the additive log⁡3/log⁡r and the bounded log⁡T−log⁡T0 terms vanish after division by log⁡r. The squeeze proves both asserted order equalities.

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