SN(z)=∑k=0Nz2k (gap ratio exactly 2): plotting ∣SN(reiθ)∣ for r∈{0.90,0.95,0.99}, spikes erupt at more and more angles as N grows — a gappy series with radius exactly 1 is singular at every point of the unit circle. The gap-free contrast ∑zk/(k+1)2 stays calm.
nknk+1=2k2k+1=2>1,R1=n→∞limsup∣an∣1/n=1
θmax∣S12(0.99eiθ)∣≈6.3139
Examples & Exercises
Prove by the Cauchy-Hadamard root test that f(z)=∑k=0∞z2k has radius of convergence exactly 1.
f(z)=n=0∑∞anzn,an=1(n=2k),an=0otherwise
R1=n→∞limsup∣an∣1/n=1⇒R=1
N=5: inside the disc, S5(0.5)≈0.81642150902 converges fast — consistent with the radius-1 proof below.Show proof
Write f(z) as an ordinary power series ∑n=0∞anzn: an=1 when n=2k and an=0 otherwise. The Cauchy-Hadamard formula gives R1=limsupn→∞∣an∣1/n (with the conventions 1/0=∞, 1/∞=0).
Since ∣an∣1/n≤1 for every n, the limsup is at most 1. But along the subsequence n=2k we have ∣a2k∣1/2k=11/2k=1, so the limsup is at least 1. Hence the limsup equals 1 and R=1 — exactly 1.
So the series converges absolutely for ∣z∣<1, and diverges for ∣z∣>1 since the general term z2k does not tend to 0 (∣z∣2k→∞). The boundary ∣z∣=1 is where the test goes silent — exactly where the gap theorem speaks.
Prove by the Weierstrass M-test that T(z)=∑k=0∞(k+1)2zk converges uniformly on the closed unit disc ∣z∣≤1, so its sum extends continuously to the boundary. Without gaps, no natural boundary appears.
(k+1)2zk≤(k+1)21=Mk,k=0∑∞Mk=6π2<∞
θmax∣T200(0.99eiθ)∣≈1.6045<1.65<6π2
N=12: the dashed gray T12 stays calm at maxθ∣T12∣≈1.5551 — without gaps there is no blow-up at the boundary.Show proof
On ∣z∣≤1, zk/(k+1)2≤1/(k+1)2=:Mk, and ∑Mk=∑k=1∞1/k2=π2/6<∞ (the Basel problem). By the Weierstrass M-test, ∑zk/(k+1)2 converges uniformly on the closed disc ∣z∣≤1.
Each partial sum is a polynomial, hence continuous, and a uniform limit of continuous functions is continuous — so the sum T(z) is continuous on the whole closed disc. That is, T extends continuously to the boundary ∣z∣=1: every boundary point is a point of continuity, so there is not a single singularity there.
T(z) and ∑z2k both have radius exactly 1 yet opposite fates — the gaps make the difference. The measurements agree: maxθ∣T200(0.99eiθ)∣≈1.6045<π2/6≈1.6449, with no hint of blow-up near the boundary.
Sketch the key idea of the Hadamard gap theorem in 2–3 steps: assuming a holomorphic extension past the boundary, explain the mechanism by which the gaps force a contradiction. State explicitly in your answer that this is a sketch of the idea, not the complete proof.
sk(z)=j=0∑kz2j,sk+1(z)−sk(z)=z2k+1
∣z0∣>1⇒∣z0∣2k+1→∞
N=12: 106 spikes crowd the boundary — below is the proof idea behind what this picture suggests (a sketch, not the complete proof).Show proof
Start with contradiction: suppose f(z)=∑k≥0z2k extended holomorphically past some boundary point ζ (∣ζ∣=1). Then there is a small disc D around ζ on which a holomorphic function agrees with f inside ∣z∣<1 — so D pokes outside the unit circle.
[IDEA — the step not proved here] Gap-forced overconvergence: the partial sums sk(z)=∑j=0kz2j converge to f on ∣z∣<1, hence to the extension on D∩{∣z∣<1}. Each new partial sum adds just one term yet leaps twice as far in degree (2k+1=2⋅2k) — with no intermediate terms to interfere, a classical overconvergence lemma forces the sequence sk to keep converging uniformly on all of D, including points with ∣z∣>1. That lemma is the technical heart; it is stated here, not proved.
But at any point with ∣z0∣>1, sk+1(z0)−sk(z0)=z02k+1 and ∣z02k+1∣=∣z0∣2k+1→∞, so sk(z0) cannot converge — a contradiction. Hence no holomorphic extension past any boundary point exists, and every point of the unit circle is singular. To stress again: this is the idea (the skeleton) of the proof, not the complete proof.