What happens at the boundary when a series has growing gaps?
Exponents doubling like 1, 2, 4, 8 leave bigger and bigger holes. The holes block continuation to every point of the circle. This happens even though the series converges nicely inside. The gap-free comparison series stays calm.
For example, imagine a πͺ staircase whose steps spread by 1, 2, 4, 8. The first steps are easy. Soon one step is too far, and the wall's end is out of reach.
N=5: inside the disc, S5β(0.5)β0.81642150902 converges fast β consistent with the radius-1 proof below.Show proof
Write f(z) as an ordinary power series βn=0ββanβzn: anβ=1 when n=2k and anβ=0 otherwise. The Cauchy-Hadamard formula gives R1β=limsupnββββ£anββ£1/n (with the conventions 1/0=β, 1/β=0).
Since β£anββ£1/nβ€1 for every nβ₯1 (at n=0, 1/n is undefined, so n=0 is excluded from the limsup argument), the limsup is at most 1.
But along the subsequence n=2k (kβ₯1) we have β£a2kββ£1/2k=11/2k=1, so the limsup is at least 1.
Hence the limsup equals 1 and R=1 β exactly 1.
So the series converges absolutely for β£zβ£<1, and diverges for β£zβ£>1 since the general term z2k does not tend to 0 (β£zβ£2kββ). The boundary β£zβ£=1 is where the test goes silent β exactly where the gap theorem speaks.
Prove by the Weierstrass M-test that T(z)=βk=0ββ(k+1)2zkβ converges uniformly on the closed unit disc β£zβ£β€1, so its sum extends continuously to the boundary.
Unlike the gap series, this sum is continuous on the closed disc, so β£zβ£=1 is not a natural boundary for the continuous extension (claiming no analytic singularity would go beyond this proof).
N=12: the dashed gray T12β stays calm at maxΞΈββ£T12ββ£β1.5551 β without gaps there is no blow-up at the boundary.Show proof
On β£zβ£β€1, βzk/(k+1)2ββ€1/(k+1)2=:Mkβ, and βMkβ=βk=1ββ1/k2=Ο2/6<β (the Basel problem). By the Weierstrass M-test, βzk/(k+1)2 converges uniformly on the closed disc β£zβ£β€1.
Each partial sum is a polynomial, hence continuous, and a uniform limit of continuous functions is continuous β so the sum T(z) is continuous on the whole closed disc.
That is, T extends continuously to the boundary β£zβ£=1: every boundary point is a point of continuity for the continuous extension.
That is exactly what this proof shows: continuity alone does not imply analytic extension or absence of an analytic singularity (for example T(z)=Li2β(z)/z extends continuously, yet z=1 is a singularity of Li2β).
T(z) and βz2k both have radius exactly 1 yet opposite fates β the gaps make the difference. The measurements agree: maxΞΈββ£T200β(0.99eiΞΈ)β£β1.6045<Ο2/6β1.6449, with no hint of blow-up near the boundary.
Sketch the key idea of the Hadamard gap theorem in 2β3 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.
N=12: 106 spikes crowd the boundary β below is the proof idea behind what this picture suggests (a sketch, not the complete proof).Show hint
Start with contradiction: suppose f(z)=βkβ₯0βz2k extended holomorphically past some boundary point ΞΆ (β£ΞΆβ£=1). Then there is a small disc D around ΞΆ on which a holomorphic function agrees with f inside β£zβ£<1 β so D pokes outside the unit circle.
Each new partial sum adds just one term yet leaps twice as far in degree (2k+1=2β 2k) β with no intermediate terms to interfere, a classical overconvergence lemma forces the sequence skβ to keep converging uniformly on all of D, including points with β£zβ£>1.
That lemma is the technical heart; it is stated here, not proved.
But at any point with β£z0ββ£>1, sk+1β(z0β)βskβ(z0β)=z02k+1β and β£z02k+1ββ£=β£z0ββ£2k+1ββ, so skβ(z0β) cannot converge β 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.