Power Series and Analyticity

Suppose a function is complex differentiable at every point of an open set. Can it be expanded as an infinite polynomial near each point? This question sits at the heart of complex analysis. Its answer, remarkably, is an unqualified yes. Real differentiability is a fragile local condition. It is compatible with wild, non-smooth behavior. Complex differentiability, by contrast, is extraordinarily rigid. It forces a function to be locally representable by a convergent power series. This equivalence — holomorphic if and only if analytic — is one of the central miracles of the subject. It explains why complex analysis feels so different from, and often so much cleaner than, real analysis. The bridge between these two notions is built from two pieces of machinery already in hand. The first is Cauchy's Integral Formula, which expresses the value of a holomorphic function at a point as a contour integral over a surrounding circle. The second is elementary facts about convergence of series. The strategy is to expand the Cauchy kernel 1/(ζ−z)1/(\zeta - z) as a geometric series in powers of zz. We then interchange a sum and an integral to produce a power series representation. Once we know every holomorphic function is locally a convergent power series, an avalanche of consequences follows. These include infinite differentiability, uniqueness of Taylor coefficients, the identity theorem, and Liouville's theorem, among others. This article develops the theory of power series carefully first. We cover radius of convergence, the Cauchy–Hadamard formula, and the basic analytic properties of series — term-by-term differentiability and continuity. Only then do we turn to the central theorem connecting analyticity to holomorphy. We treat convergence with full rigor. The subtleties of where a series converges, and how fast, are exactly what make the later theorem work. By the end, the reader will have a complete, self-contained proof that holomorphic functions are analytic. They will also have a clear picture of why the radius of convergence of the Taylor series at a point equals the distance to the nearest singularity. This sets the stage for Taylor Series of Holomorphic Functions and, further out, Laurent Series for functions with isolated singularities.

Key takeaways
  • A power series ∑an(z−z0)n\sum a_n(z-z_0)^n converges absolutely inside a disk of radius RR and diverges outside it; RR is the radius of convergence.
  • The radius is computed by the Cauchy–Hadamard formula 1/R=lim sup⁡n→∞∣an∣1/n1/R = \limsup_{n\to\infty} |a_n|^{1/n}.
  • Power series converge uniformly on closed subdisks, so they can be differentiated and integrated term by term inside the disk of convergence.
  • Every function holomorphic on an open set is represented, near each point, by a convergent power series — this is the analyticity theorem.
  • Conversely every convergent power series defines a holomorphic function on its disk of convergence, so holomorphic and analytic are the same class of functions in one complex variable.
  • Key idea: Cauchy's Integral Formula turns the Cauchy kernel into a geometric series, converting a contour integral into a power series that represents the function locally.

Where this lives today

The equivalence of holomorphy and analyticity underlies essentially every application of complex analysis. In pure mathematics, it is the foundation for the identity theorem (two analytic functions agreeing on a set with a limit point agree everywhere on a connected domain), analytic continuation, and the classification of singularities that leads to Laurent Series and residue calculus. In physics and engineering, power series expansions of holomorphic functions underlie perturbation theory in quantum mechanics and fluid dynamics, where physical quantities (wavefunctions, potentials) are often holomorphic in an auxiliary complex parameter, and their Taylor expansions give systematic approximation schemes with rigorously controlled radii of convergence. In signal processing, the ZZ-transform of a discrete signal is literally a power series in z−1z^{-1}, and questions of stability of digital filters reduce exactly to radius-of-convergence and pole-location questions of the type developed here. In numerical analysis, the radius of convergence of a Taylor series governs how far a Newton-like or series-based numerical method can be trusted before truncation error becomes unreliable. In algebraic geometry and number theory, formal and convergent power series are the basic local coordinates for analytic and complex-analytic varieties, and generating functions in combinatorics are power series whose radius of convergence encodes asymptotic growth rates of counted objects via the Cauchy–Hadamard formula itself.

Ask the tutor: How does the analyticity theorem shown here get used to prove the identity theorem for holomorphic functions?

DefinitionPower series, radius of convergence, analytic function

Let z0∈Cz_0 \in \mathbb{C} and let (an)n≥0(a_n)_{n \geq 0} be a sequence of complex numbers. The formal expression

∑n=0∞an(z−z0)n\sum_{n=0}^{\infty} a_n (z - z_0)^n

is called a power series centered at z0z_0. Define

R=1lim sup⁡n→∞∣an∣1/n∈[0,∞],R = \frac{1}{\limsup_{n\to\infty} |a_n|^{1/n}} \in [0, \infty],

with the convention R=∞R = \infty if the lim sup⁡\limsup is 00, and R=0R = 0 if the lim sup⁡\limsup is ∞\infty. The number RR is called the radius of convergence of the series. A function ff defined on an open set U⊆CU \subseteq \mathbb{C} is called analytic at a point z0∈Uz_0 \in U if there exists r>0r > 0 and a power series ∑an(z−z0)n\sum a_n (z - z_0)^n with radius of convergence at least rr such that

f(z)=∑n=0∞an(z−z0)nfor all z with ∣z−z0∣<r.f(z) = \sum_{n=0}^{\infty} a_n (z - z_0)^n \quad \text{for all } z \text{ with } |z - z_0| < r.

ff is analytic on UU if it is analytic at every point of UU. A function ff is holomorphic on UU if it is complex differentiable at every point of UU.

Intuition

Think of a power series as a "polynomial with infinitely many terms," built one power of (z−z0)(z - z_0) at a time. Whether this infinite sum makes sense depends entirely on the size of the coefficients ana_n: if they shrink fast enough, the terms an(z−z0)na_n(z-z_0)^n eventually decay geometrically for zz near z0z_0, guaranteeing convergence; if they don't shrink fast enough, the terms can blow up once ∣z−z0∣|z - z_0| passes some threshold. That threshold is the radius of convergence RR, and the remarkable fact — proved below via a comparison to geometric series — is that convergence behavior is exactly dichotomous: absolute convergence for ∣z−z0∣<R|z - z_0| < R, divergence (terms don't even tend to 00) for ∣z−z0∣>R|z - z_0| > R. Nothing can be said in general about the boundary circle ∣z−z0∣=R|z-z_0|=R without more information. The deeper miracle is that this purely analytic notion of "locally a convergent power series" coincides exactly with the geometric/differential notion of holomorphy — a single complex derivative existing at every point. The engine that makes this work is Cauchy's Integral Formula: it lets us write f(z)f(z) as an integral of f(ζ)/(ζ−z)f(\zeta)/(\zeta - z) around a circle, and expanding 1/(ζ−z)1/(\zeta-z) in a geometric series in (z−z0)(z - z_0) converts that formula directly into a power series for ff, valid inside the circle.

Figure
Radius of convergence: absolute convergence inside, divergence outside
|z - z₀| < R (absolute convergence) |z - z₀| > R (terms → ∞, diverges) z₀ R boundary |z - z₀| = R: behavior not determined by R alone
TheoremCauchy–Hadamard formula and convergence of power series

Let ∑n=0∞an(z−z0)n\sum_{n=0}^{\infty} a_n(z-z_0)^n be a power series and let

R=1lim sup⁡n→∞∣an∣1/nR = \frac{1}{\limsup_{n \to \infty} |a_n|^{1/n}}

(with the conventions R=∞R=\infty if the limsup is 00, R=0R = 0 if it is ∞\infty). Then: 1. If ∣z−z0∣<R|z - z_0| < R, the series converges absolutely. 2. If ∣z−z0∣>R|z - z_0| > R, the terms an(z−z0)na_n(z-z_0)^n do not tend to 00, so the series diverges. 3. For every 0<ρ<R0 < \rho < R, the series converges uniformly on the closed disk D‾(z0,ρ)={z:∣z−z0∣≤ρ}\overline{D}(z_0, \rho) = \{z : |z-z_0| \le \rho\}. Consequently, on the open disk D(z0,R)D(z_0, R) the series defines a function that is continuous, and (as shown in the corollary below) holomorphic with derivative given by termwise differentiation.

Proof

We use the root test and a Weierstrass M-test argument; this is a direct comparison-with-geometric-series technique, entirely self-contained.

Part 1 (absolute convergence inside RR). Let zz satisfy ∣z−z0∣<R|z - z_0| < R. If R=0R = 0 there is nothing to prove (no such zz exists). Assume R>0R > 0, possibly R=∞R = \infty. Choose ρ\rho with ∣z−z0∣<ρ<R|z - z_0| < \rho < R (if R=∞R = \infty, choose any ρ>∣z−z0∣\rho > |z-z_0|). Since ρ<R\rho < R, we have 1/ρ>1/R=lim sup⁡n∣an∣1/n1/\rho > 1/R = \limsup_n |a_n|^{1/n} when R<∞R<\infty; when R=∞R=\infty the limsup is 0<1/ρ0 < 1/\rho for any finite ρ\rho. In either case, by definition of lim sup⁡\limsup, there exists NN such that for all n≥Nn \geq N,

∣an∣1/n<1ρ,i.e.∣an∣<ρ−n.|a_n|^{1/n} < \frac{1}{\rho}, \quad \text{i.e.} \quad |a_n| < \rho^{-n}.

Hence for n≥Nn \geq N,

∣an(z−z0)n∣<(∣z−z0∣ρ)n.|a_n (z-z_0)^n| < \left(\frac{|z - z_0|}{\rho}\right)^n.

Since ∣z−z0∣/ρ<1|z-z_0|/\rho < 1, this is a term of a convergent geometric series. By the comparison test, ∑n≥N∣an(z−z0)n∣\sum_{n \geq N} |a_n(z-z_0)^n| converges, and adding the finitely many terms n<Nn < N (each a finite complex number) preserves convergence. Hence ∑nan(z−z0)n\sum_n a_n(z-z_0)^n converges absolutely.

Part 2 (divergence outside RR). Let zz satisfy ∣z−z0∣>R|z - z_0| > R. If R=∞R = \infty there is no such zz. Assume R<∞R < \infty. Then 1/∣z−z0∣<1/R=lim sup⁡n∣an∣1/n1/|z-z_0| < 1/R = \limsup_n |a_n|^{1/n}. By definition of lim sup⁡\limsup as the supremum of subsequential limits, there is a subsequence (nk)(n_k) along which ∣ank∣1/nk→L≥1/R|a_{n_k}|^{1/n_k} \to L \geq 1/R... more directly: since lim sup⁡n∣an∣1/n>1/∣z−z0∣\limsup_n |a_n|^{1/n} > 1/|z-z_0|, there are infinitely many nn with

∣an∣1/n>1∣z−z0∣,i.e.∣an(z−z0)n∣>1|a_n|^{1/n} > \frac{1}{|z - z_0|}, \quad \text{i.e.} \quad |a_n(z-z_0)^n| > 1

for infinitely many nn. Thus the terms an(z−z0)na_n(z-z_0)^n do not converge to 00, so the series ∑an(z−z0)n\sum a_n(z-z_0)^n diverges (a necessary condition for convergence of any series is that its terms tend to 00).

Part 3 (uniform convergence on closed subdisks). Fix 0<ρ<R0 < \rho < R. Choose ρ′\rho' with ρ<ρ′<R\rho < \rho' < R (possible since ρ<R\rho < R; if R=∞R = \infty pick any ρ′>ρ\rho' > \rho). As in Part 1, there is NN such that ∣an∣<(ρ′)−n|a_n| < (\rho')^{-n} for all n≥Nn \geq N. Then for every zz with ∣z−z0∣≤ρ|z - z_0| \leq \rho and every n≥Nn \geq N,

∣an(z−z0)n∣≤∣an∣ρn<(ρρ′)n=:Mn.|a_n (z - z_0)^n| \leq |a_n| \rho^n < \left(\frac{\rho}{\rho'}\right)^n =: M_n.

Since ρ/ρ′<1\rho/\rho' < 1, ∑nMn\sum_n M_n is a convergent geometric series independent of zz. By the Weierstrass M-test, ∑nan(z−z0)n\sum_n a_n(z - z_0)^n converges uniformly on D‾(z0,ρ)\overline{D}(z_0,\rho).

Continuity. Each partial sum SN(z)=∑n=0Nan(z−z0)nS_N(z) = \sum_{n=0}^N a_n(z-z_0)^n is a polynomial, hence continuous on C\mathbb{C}. A uniform limit of continuous functions on a set is continuous on that set (standard ε/3\varepsilon/3 argument: for z,wz, w in the disk, ∣f(z)−f(w)∣≤∣f(z)−SN(z)∣+∣SN(z)−SN(w)∣+∣SN(w)−f(w)∣|f(z)-f(w)| \le |f(z)-S_N(z)| + |S_N(z)-S_N(w)| + |S_N(w)-f(w)|, and each piece is made small by uniform convergence and continuity of SNS_N). Since every point of D(z0,R)D(z_0,R) lies in some closed subdisk D‾(z0,ρ)\overline{D}(z_0,\rho) with ρ<R\rho<R, the sum ff is continuous at every point of D(z0,R)D(z_0,R). ■\blacksquare

∎
LemmaTermwise differentiation of power series

Let f(z)=∑n=0∞an(z−z0)nf(z) = \sum_{n=0}^\infty a_n(z-z_0)^n have radius of convergence R>0R > 0. Then the series g(z)=∑n=1∞nan(z−z0)n−1g(z) = \sum_{n=1}^\infty n a_n (z-z_0)^{n-1} has the same radius of convergence RR, and ff is holomorphic on D(z0,R)D(z_0,R) with f′(z)=g(z)f'(z) = g(z) there.

Proof

Same radius. Since n1/n→1n^{1/n} \to 1 as n→∞n \to \infty, we have lim sup⁡n∣nan∣1/n=lim sup⁡n∣an∣1/n\limsup_n |na_n|^{1/n} = \limsup_n |a_n|^{1/n} (multiplying by a sequence tending to 11 does not change a limsup: for any ε>0\varepsilon>0, eventually n1/n<1+εn^{1/n} < 1+\varepsilon and n1/n>1−εn^{1/n}>1-\varepsilon, squeezing the limsup of the product between (1±ε)(1\pm\varepsilon) times the original limsup, and letting ε→0\varepsilon \to 0). So gg's radius of convergence is also RR (index shift n→n+1n \to n+1 does not affect the limsup either, by the same reasoning applied to the sequence (n+1)an+1(n+1)a_{n+1}).

Differentiability. Fix z∗∈D(z0,R)z^* \in D(z_0,R) and choose ρ\rho with ∣z∗−z0∣<ρ<R|z^*-z_0| < \rho < R. We show f′(z∗)=g(z∗)f'(z^*) = g(z^*) directly from the difference quotient, using uniform convergence on D‾(z0,ρ)\overline D(z_0,\rho) established above (this is a term-by-term limit interchange argument). For h≠0h \neq 0 small enough that z∗+h∈D(z0,ρ)z^*+h \in D(z_0,\rho), write

f(z∗+h)−f(z∗)h−g(z∗)=∑n=1∞an[(z∗+h−z0)n−(z∗−z0)nh−n(z∗−z0)n−1].\frac{f(z^*+h)-f(z^*)}{h} - g(z^*) = \sum_{n=1}^\infty a_n \left[\frac{(z^*+h-z_0)^n - (z^*-z_0)^n}{h} - n(z^*-z_0)^{n-1}\right].

Let w=z∗−z0w = z^* - z_0, so ∣w∣<ρ|w| < \rho. Using the algebraic identity un−vn=(u−v)∑k=0n−1ukvn−1−ku^n - v^n = (u-v)\sum_{k=0}^{n-1}u^kv^{n-1-k} with u=w+hu = w+h, v=wv=w, the bracket equals

∑k=0n−1(w+h)kwn−1−k−nwn−1=∑k=0n−1[(w+h)k−wk]wn−1−k.\sum_{k=0}^{n-1} (w+h)^k w^{n-1-k} - n w^{n-1} = \sum_{k=0}^{n-1}\left[(w+h)^k - w^k\right]w^{n-1-k}.

Each term (w+h)k−wk(w+h)^k - w^k is again a telescoping sum bounded, for ∣h∣|h| small enough that ∣w+h∣≤ρ|w+h| \le \rho, by k∣h∣ρk−1k|h|\rho^{k-1} (apply the same factorization once more and bound each factor by ρk−1\rho^{k-1}). Hence the bracket is bounded in absolute value by

∑k=0n−1k∣h∣ρk−1ρn−1−k=∣h∣ρn−2∑k=0n−1k=∣h∣ρn−2n(n−1)2.\sum_{k=0}^{n-1} k|h|\rho^{k-1}\rho^{n-1-k} = |h|\rho^{n-2}\sum_{k=0}^{n-1}k = |h|\rho^{n-2}\frac{n(n-1)}{2}.

Therefore

∣f(z∗+h)−f(z∗)h−g(z∗)∣≤∣h∣∑n=2∞∣an∣n(n−1)2ρn−2.\left|\frac{f(z^*+h)-f(z^*)}{h} - g(z^*)\right| \leq |h| \sum_{n=2}^\infty |a_n| \frac{n(n-1)}{2}\rho^{n-2}.

The series ∑n∣an∣n(n−1)ρn−2/2\sum_n |a_n| n(n-1)\rho^{n-2}/2 converges: it is (up to the same limsup argument as above, since n(n−1)/2n(n-1)/2 is polynomial in nn and x1/n→1x^{1/n}\to1 for any fixed polynomial factor x=x(n)x=x(n)) a power series in ρ\rho with the same radius of convergence RR, evaluated at ρ<R\rho < R, hence convergent by Part 1 of Radius of Convergence and the Cauchy–Hadamard Formula (the theorem above). Call this convergent sum C<∞C < \infty. Then

∣f(z∗+h)−f(z∗)h−g(z∗)∣≤C∣h∣→0 as h→0.\left|\frac{f(z^*+h)-f(z^*)}{h} - g(z^*)\right| \leq C|h| \to 0 \text{ as } h \to 0.

Hence ff is complex differentiable at z∗z^* with f′(z∗)=g(z∗)f'(z^*) = g(z^*). Since z∗∈D(z0,R)z^* \in D(z_0,R) was arbitrary, ff is holomorphic on D(z0,R)D(z_0,R) with derivative gg. ■\blacksquare

∎
TheoremEquivalence of holomorphy and analyticity

Let U⊆CU \subseteq \mathbb{C} be open and f:U→Cf: U \to \mathbb{C}. Then ff is holomorphic on UU if and only if ff is analytic on UU. Moreover, if z0∈Uz_0 \in U and D(z0,R)⊆UD(z_0,R) \subseteq U is the largest disk centered at z0z_0 contained in UU, then ff equals its Taylor series

f(z)=∑n=0∞f(n)(z0)n!(z−z0)nf(z) = \sum_{n=0}^\infty \frac{f^{(n)}(z_0)}{n!}(z-z_0)^n

for all z∈D(z0,R)z \in D(z_0,R), and this series converges (at least) on that disk.

Proof

(⇐\Leftarrow) Analytic implies holomorphic. This is immediate from the Lemma above: if ff is analytic at z0z_0, it agrees with a convergent power series on some disk D(z0,r)D(z_0,r), and that lemma shows such a series defines a holomorphic function on its disk of convergence. Since analyticity at every point of UU gives, at each point, a local power series representation with positive radius, ff is complex differentiable at every point of UU, i.e. holomorphic.

(⇒\Rightarrow) Holomorphic implies analytic. This is the substantial direction; we use Cauchy's Integral Formula together with the geometric series and the uniform-convergence machinery above (a Cauchy kernel expansion argument). Fix z0∈Uz_0 \in U. Since UU is open, choose R>0R>0 with D‾(z0,R)⊆U\overline{D}(z_0,R) \subseteq U (a closed disk of some positive radius fits inside UU). Let γ\gamma be the positively oriented circle ∣ζ−z0∣=R|\zeta - z_0| = R, which lies in UU and is homotopic to a point in UU, so Cauchy's Integral Formula applies to ff (holomorphic on an open set containing D‾(z0,R)\overline D(z_0,R)) for any zz with ∣z−z0∣<R|z-z_0|<R:

f(z)=12πi∮γf(ζ)ζ−z dζ.f(z) = \frac{1}{2\pi i}\oint_\gamma \frac{f(\zeta)}{\zeta - z}\,d\zeta.

Fix such a zz and write ζ−z=(ζ−z0)−(z−z0)\zeta - z = (\zeta - z_0) - (z-z_0), so that

1ζ−z=1(ζ−z0)(1−z−z0ζ−z0)=1ζ−z0∑n=0∞(z−z0ζ−z0)n,\frac{1}{\zeta - z} = \frac{1}{(\zeta-z_0)\left(1 - \frac{z-z_0}{\zeta - z_0}\right)} = \frac{1}{\zeta - z_0}\sum_{n=0}^\infty \left(\frac{z-z_0}{\zeta-z_0}\right)^n,

using the geometric series formula 11−w=∑n≥0wn\frac{1}{1-w} = \sum_{n\ge0}w^n, valid since ζ∈γ\zeta \in \gamma gives ∣ζ−z0∣=R|\zeta - z_0| = R and ∣z−z0∣<R|z-z_0|<R, so ∣w∣:=∣z−z0ζ−z0∣=∣z−z0∣R<1|w| := \left|\frac{z-z_0}{\zeta-z_0}\right| = \frac{|z-z_0|}{R} < 1. This series in ww converges uniformly for ζ∈γ\zeta \in \gamma (i.e. as ζ\zeta ranges over the circle, ∣w∣|w| is the constant ratio ∣z−z0∣/R<1|z-z_0|/R < 1, so this is literally a fixed convergent geometric series of numbers, uniform trivially in ζ\zeta; more precisely, the partial sums converge uniformly in ζ\zeta by the Weierstrass M-test with Mn=(∣z−z0∣/R)nM_n = (|z-z_0|/R)^n, a convergent geometric bound independent of ζ\zeta). Therefore

f(ζ)ζ−z=∑n=0∞f(ζ)(z−z0)n(ζ−z0)n+1,\frac{f(\zeta)}{\zeta - z} = \sum_{n=0}^\infty \frac{f(\zeta)(z-z_0)^n}{(\zeta-z_0)^{n+1}},

and since ff is continuous on the compact set γ\gamma (holomorphic functions are continuous, being complex differentiable), ff is bounded on γ\gamma, say ∣f(ζ)∣≤M|f(\zeta)| \leq M for ζ∈γ\zeta \in \gamma. The nn-th term is then bounded by M(∣z−z0∣/R)n/RM(|z-z_0|/R)^n/R, uniformly in ζ∈γ\zeta \in \gamma; the series of these bounds converges (geometric, ratio <1<1), so by the Weierstrass M-test the series ∑nf(ζ)(z−z0)n(ζ−z0)n+1\sum_n \frac{f(\zeta)(z-z_0)^n}{(\zeta - z_0)^{n+1}} converges uniformly in ζ\zeta on γ\gamma. Uniform convergence permits interchange of the (contour) integral and the infinite sum — this is justified because a uniformly convergent series of continuous functions on a rectifiable curve of finite length may be integrated term by term (the partial sums converge uniformly to the full sum, and integration against a fixed finite-length curve is a continuous linear functional with respect to the sup norm, so it commutes with uniform limits). Hence

f(z)=12πi∮γ∑n=0∞f(ζ)(z−z0)n(ζ−z0)n+1 dζ=∑n=0∞(12πi∮γf(ζ)(ζ−z0)n+1 dζ)(z−z0)n.f(z) = \frac{1}{2\pi i}\oint_\gamma \sum_{n=0}^\infty \frac{f(\zeta)(z-z_0)^n}{(\zeta - z_0)^{n+1}}\,d\zeta = \sum_{n=0}^\infty \left(\frac{1}{2\pi i}\oint_\gamma \frac{f(\zeta)}{(\zeta-z_0)^{n+1}}\,d\zeta\right)(z-z_0)^n.

Define

an:=12πi∮γf(ζ)(ζ−z0)n+1 dζ.a_n := \frac{1}{2\pi i}\oint_\gamma \frac{f(\zeta)}{(\zeta-z_0)^{n+1}}\,d\zeta.

These are well-defined complex numbers (independent of zz), and we have shown

f(z)=∑n=0∞an(z−z0)nfor all ∣z−z0∣<R.f(z) = \sum_{n=0}^\infty a_n(z-z_0)^n \quad \text{for all } |z - z_0| < R.

This exhibits ff as equal to a convergent power series on D(z0,R)D(z_0,R), so ff is analytic at z0z_0. Since z0∈Uz_0 \in U was arbitrary, ff is analytic on all of UU.

Identification of coefficients with Taylor coefficients. By the Lemma (termwise differentiation), applied repeatedly to f(z)=∑nan(z−z0)nf(z) = \sum_n a_n(z-z_0)^n on D(z0,R)D(z_0,R), we get for every k≥0k \geq 0,

f(k)(z)=∑n=k∞n(n−1)⋯(n−k+1)an(z−z0)n−kf^{(k)}(z) = \sum_{n=k}^\infty n(n-1)\cdots(n-k+1)a_n (z-z_0)^{n-k}

(each differentiation is justified by the Lemma, applied to the previous derivative series, which itself is a power series with the same radius RR). Evaluating at z=z0z = z_0 kills every term except n=kn=k, giving f(k)(z0)=k! akf^{(k)}(z_0) = k! \, a_k, i.e.

ak=f(k)(z0)k!.a_k = \frac{f^{(k)}(z_0)}{k!}.

This shows the power series obtained from Cauchy's formula is exactly the Taylor series of ff at z0z_0, and it converges to ff on the disk D(z0,R)D(z_0,R) for every RR with D‾(z0,R)⊆U\overline{D}(z_0,R)\subseteq U; taking the supremum of all such admissible RR recovers the statement for the largest disk D(z0,R)⊆UD(z_0,R)\subseteq U (any point of that open disk lies in some smaller closed disk contained in UU, to which the above argument applies). ■\blacksquare

∎
CorollaryInfinite differentiability of holomorphic functions

If ff is holomorphic on an open set UU, then ff has complex derivatives of all orders on UU, and each derivative f(k)f^{(k)} is itself holomorphic on UU.

The proof is immediate: locally, ff equals a convergent power series, and by the Lemma such a series may be differentiated term by term any number of times, each time yielding another convergent power series (hence another holomorphic function) on the same disk.

Worked examples

Example 1 — a series with an asymmetric coefficient pattern. Consider

f(z)=∑n=0∞n2+35n (z−2i)n.f(z) = \sum_{n=0}^\infty \frac{n^2 + 3}{5^n}\, (z-2i)^n.

Here z0=2iz_0 = 2i and an=(n2+3)/5na_n = (n^2+3)/5^n. We compute the radius of convergence via Cauchy–Hadamard:

∣an∣1/n=(n2+3)1/n5.|a_n|^{1/n} = \frac{(n^2+3)^{1/n}}{5}.

Since n2+3→∞n^2 + 3 \to \infty polynomially, (n2+3)1/n→1(n^2+3)^{1/n} \to 1 as n→∞n \to \infty (any sequence of the form p(n)1/np(n)^{1/n} for a polynomial pp with positive leading coefficient tends to 11: write (n2+3)1/n=e1nln⁡(n2+3)(n^2+3)^{1/n} = e^{\frac{1}{n}\ln(n^2+3)}, and ln⁡(n2+3)n→0\frac{\ln(n^2+3)}{n}\to 0 since ln⁡\ln grows slower than any positive power of nn). Hence

lim sup⁡n→∞∣an∣1/n=15,R=5.\limsup_{n\to\infty}|a_n|^{1/n} = \frac{1}{5}, \qquad R = 5.

So this series converges absolutely for ∣z−2i∣<5|z - 2i| < 5 and diverges for ∣z−2i∣>5|z-2i|>5; by the theorem it defines a function holomorphic on the disk D(2i,5)D(2i, 5). Let's verify termwise differentiation concretely at one asymmetric point, say z=2i+1z = 2i + 1 (so w:=z−z0=1w := z - z_0 = 1, well inside ∣w∣<5|w|<5). The derivative series is

f′(z)=∑n=1∞n⋅n2+35n(z−2i)n−1,f'(z) = \sum_{n=1}^\infty n\cdot\frac{n^2+3}{5^n}(z-2i)^{n-1},

which at z=2i+1z = 2i+1 becomes the numerical series ∑n=1∞n(n2+3)5n\sum_{n=1}^\infty \frac{n(n^2+3)}{5^n}. This converges (ratio test: (n+1)((n+1)2+3)5n+1/n(n2+3)5n→15<1\frac{(n+1)((n+1)^2+3)}{5^{n+1}} \Big/ \frac{n(n^2+3)}{5^n} \to \frac{1}{5} < 1), consistent with the Lemma's guarantee that the differentiated series shares the radius R=5R=5 and converges throughout ∣w∣<5|w|<5, in particular at w=1w=1.

Example 2 — recovering Taylor coefficients from a rational function via Cauchy's formula, then checking against direct expansion. Let U=C∖{3}U = \mathbb{C}\setminus\{3\} and f(z)=13−zf(z) = \dfrac{1}{3-z}, holomorphic on UU. Expand ff about z0=1z_0 = 1 (an asymmetric, off-center choice, not the origin). Via the theorem's construction. The largest disk centered at 11 contained in UU has radius R=∣3−1∣=2R = |3-1| = 2 (distance to the removed point 33). By the theorem, for ∣z−1∣<2|z-1|<2,

f(z)=∑n=0∞an(z−1)n,an=12πi∮∣ζ−1∣=rf(ζ)(ζ−1)n+1 dζ(0<r<2).f(z) = \sum_{n=0}^\infty a_n(z-1)^n, \qquad a_n = \frac{1}{2\pi i}\oint_{|\zeta - 1|=r} \frac{f(\zeta)}{(\zeta-1)^{n+1}}\,d\zeta \quad (0<r<2).

Via direct algebra (to check). Write 3−z=(3−1)−(z−1)=2−(z−1)=2(1−z−12)3 - z = (3-1) - (z-1) = 2 - (z-1) = 2\left(1 - \frac{z-1}{2}\right), so

f(z)=12⋅11−z−12=12∑n=0∞(z−12)n=∑n=0∞12n+1(z−1)n,f(z) = \frac{1}{2}\cdot\frac{1}{1 - \frac{z-1}{2}} = \frac{1}{2}\sum_{n=0}^\infty \left(\frac{z-1}{2}\right)^n = \sum_{n=0}^\infty \frac{1}{2^{n+1}}(z-1)^n,

valid exactly when ∣z−1∣/2<1|z-1|/2 < 1, i.e. ∣z−1∣<2|z-1|<2 — matching R=2R=2 exactly, as predicted since the nearest singularity of ff (the pole at z=3z=3) is at distance 22 from z0=1z_0=1. Cross-check via Taylor's formula. Since f(n)(z)=n!(3−z)n+1f^{(n)}(z) = \dfrac{n!}{(3-z)^{n+1}} (check: f(z)=(3−z)−1f(z)=(3-z)^{-1}, f′(z)=(3−z)−2f'(z) = (3-z)^{-2}, and inductively f(n)(z)=n!(3−z)−(n+1)f^{(n)}(z) = n!(3-z)^{-(n+1)}), we get

f(n)(1)n!=1(3−1)n+1=12n+1,\frac{f^{(n)}(1)}{n!} = \frac{1}{(3-1)^{n+1}} = \frac{1}{2^{n+1}},

exactly matching an=1/2n+1a_n = 1/2^{n+1} found by direct algebra, confirming the theorem's identification an=f(n)(z0)/n!a_n = f^{(n)}(z_0)/n!.

Counterexamplewhy complex differentiability, not just partial derivatives existing, is needed

The theorem crucially uses complex differentiability (holomorphy), not merely that a function is smooth when viewed as a map R2→R2\mathbb{R}^2 \to \mathbb{R}^2. If we only assume real differentiability of u,vu,v (writing f=u+ivf = u+iv) without the Cauchy–Riemann equations, analyticity can fail completely. Consider f(z)=zˉ=x−iyf(z) = \bar z = x - iy. As a map R2→R2\mathbb{R}^2\to\mathbb{R}^2 this is smooth (linear, even), with continuous partial derivatives of all orders — it is about as regular as a real function can be. But ff is nowhere complex differentiable: for h→0h\to 0 along the real axis, f(z+h)−f(z)h=z+h‾−zˉh=hˉh=1\frac{f(z+h)-f(z)}{h} = \frac{\overline{z+h}-\bar z}{h} = \frac{\bar h}{h} = 1, while along the imaginary axis h=ith = it, hˉh=−itit=−1\frac{\bar h}{h} = \frac{-it}{it} = -1. The difference quotient has no limit, so f′(z)f'(z) does not exist at any zz. Consequently ff cannot be represented near any point by a convergent power series ∑an(z−z0)n\sum a_n(z-z_0)^n: such a series, by the Lemma, would automatically be holomorphic (complex differentiable) on its disk of convergence, contradicting the nowhere-differentiability of zˉ\bar z. This shows the hypothesis "ff holomorphic," meaning genuinely complex differentiable and not merely real-smooth, is indispensable in the theorem: dropping it (replacing it with mere real smoothness) allows functions with no local power series representation at all.

Scope, edge cases & common traps

SituationWhat happens
R=0R = 0Series converges only at z=z0z=z_0; defines no function on any open set, hence witnesses no analyticity there
R=∞R = \inftySeries converges on all of C\mathbb{C} (entire function), e.g. ∑zn/n!=ez\sum z^n/n!= e^z
zz on the boundary circle ∣z−z0∣=R|z-z_0|=RCauchy–Hadamard says nothing; behavior must be checked case by case (e.g. ∑zn\sum z^n diverges everywhere on ∣z∣=1|z|=1, ∑zn/n2\sum z^n/n^2 converges everywhere on ∣z∣=1|z|=1)
Radius from the theorem vs. domain of ffRR equals the distance from z0z_0 to the nearest point not in the domain of holomorphy, not necessarily the "natural" domain one first writes down
Real-variable smoothnessInfinitely differentiable real functions need not be analytic (e.g. e−1/x2e^{-1/x^2}); this pathology cannot occur for holomorphic functions, by the theorem above

The mathematician behind it

Origins · 1 minAugustin-Louis Cauchy and how this was discovered
AC
Augustin-Louis Cauchy
1789–1857 · Founder of rigorous complex analysis and the integral formula that bears his name

Cauchy, working in Paris in the 1820s, built the theory of complex integration essentially from scratch, proving the integral theorem and integral formula that make the equivalence of holomorphy and analyticity provable. He was notoriously prolific — he has more theorems, formulas, and concepts named after him than perhaps any other mathematician — and equally notorious for the speed and sometimes casualness with which he published, occasionally at the expense of rigor that later mathematicians (Weierstrass among them) had to repair. Nonetheless the core architecture of complex analysis, integral formula, residue calculus, and the power series expansion theorem, is fundamentally his.

History
- 1814 — Cauchy presents early work on complex integrals to the Paris Academy.
- 1825 — Cauchy publishes the memoir establishing what is now Cauchy's Integral Theorem for contour integrals.
- 1831 — Cauchy, in Turin, derives the power series expansion of a holomorphic function from the integral formula, essentially the theorem proved here.
- 1841 — Weierstrass independently develops the power-series approach to complex analysis, emphasizing analyticity as the foundational definition.
- 1851 — Riemann's dissertation gives the geometric/differential-equation viewpoint (Cauchy–Riemann equations), completing the triad of equivalent perspectives on holomorphic functions.
Why does the radius of convergence only depend on a limsup of ∣an∣1/n|a_n|^{1/n} and not on the actual limit?

Not every sequence ∣an∣1/n|a_n|^{1/n} converges — it may oscillate — so an ordinary limit might not exist. The lim sup⁡\limsup always exists (possibly +∞+\infty) for any bounded-below real sequence, because it is defined as the limit of the (necessarily monotonic, hence convergent) sequence of suprema sup⁡n≥N∣an∣1/n\sup_{n\ge N}|a_n|^{1/n} as N→∞N\to\infty. Using lim sup⁡\limsup rather than lim⁡\lim makes the Cauchy–Hadamard formula universally applicable, and the proof of the dichotomy (converge inside, diverge outside) goes through using only limsup properties, so no generality is lost by not assuming the ordinary limit exists.

Does the theorem say a power series always converges on its full "natural" domain?

No — the theorem gives a disk of convergence, and the domain of the underlying holomorphic function may be far larger, but the series itself is only guaranteed to converge to that function within a disk bounded by the nearest singularity to the center. Outside that disk the series generally diverges even though the function it represents may extend, via a different formula or a different expansion point, well beyond the disk (this phenomenon is called analytic continuation, built on the identity theorem that follows from this equivalence).

Is it true that a real power series representing a C∞C^\infty real function converges back to that function?

Not necessarily — this is one of the sharpest differences between real and complex analysis. A real C∞C^\infty function can have a Taylor series that converges everywhere but to the wrong function, or converges only at the center. The standard example e−1/x2e^{-1/x^2} (extended by f(0)=0f(0)=0) is real-analytic nowhere near 00: all its derivatives vanish at 00, so its Taylor series is identically 00, yet f(x)≠0f(x)\ne 0 for x≠0x\ne0. In the complex setting the analyticity theorem rules this out entirely: complex differentiability alone (not even requiring it a priori at nearby points beyond an open set) forces genuine convergence back to ff.

What role does Cauchy's Integral Formula play that couldn't be replaced by, say, the mean value property alone?

Cauchy's Integral Formula gives an explicit closed-form expression for f(z)f(z) as an integral of f(ζ)/(ζ−z)f(\zeta)/(\zeta-z), which is precisely what allows expanding the kernel 1/(ζ−z)1/(\zeta-z) as a geometric series in (z−z0)(z-z_0). The mean value property (a consequence of the same formula, restricted to z=z0z=z_0) only gives the value at the center of a circle in terms of a boundary average — it does not, by itself, supply the algebraic structure of the Cauchy kernel needed to generate all the higher-order Taylor coefficients simultaneously.

Why must we choose a closed disk D‾(z0,R)⊆U\overline D(z_0,R)\subseteq U rather than just an open disk, in the proof of holomorphic implies analytic?

We need ff to be holomorphic on an open set containing the closed disk and its boundary circle γ\gamma so that Cauchy's Integral Formula, together with continuity/boundedness of ff on the compact curve γ\gamma, applies rigorously. If we only had an open disk without control on a neighborhood of its boundary, we could not guarantee ff is even defined on γ\gamma, let alone bounded there, which the proof needs to apply the Weierstrass M-test and justify the term-by-term integration.

Can the radius of convergence be computed using the ratio test instead of Cauchy–Hadamard?

Yes, when the ratio limit exists: if lim⁡n→∞∣an+1/an∣\lim_{n\to\infty} |a_{n+1}/a_n| exists (finite or infinite), it equals lim sup⁡n∣an∣1/n\limsup_n|a_n|^{1/n}, so R=lim⁡n∣an/an+1∣R = \lim_n |a_n/a_{n+1}| in that case. The ratio test is often computationally easier (as in Example 1's differentiated series check), but Cauchy–Hadamard via limsup is the universally valid formula, since the ratio limit may fail to exist even when the root limsup does.

Does every convergent power series arise from some holomorphic function via Taylor's formula, or could the coefficients be arbitrary?

Any sequence (an)(a_n) satisfying lim sup⁡∣an∣1/n<∞\limsup|a_n|^{1/n}<\infty (so R>0R>0) produces, by the Lemma, a genuinely holomorphic function on D(z0,R)D(z_0,R) — coefficients need no special extra property beyond controlling this limsup. Conversely, by the analyticity theorem, that function's own Taylor coefficients at z0z_0 recover exactly the ana_n we started with (an=f(n)(z0)/n!a_n = f^{(n)}(z_0)/n!), so the correspondence between convergent power series and holomorphic germs is a genuine bijection, not merely a one-way construction.

Before this

Where this leads