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 as a geometric series in powers of . 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.
- A power series converges absolutely inside a disk of radius and diverges outside it; is the radius of convergence.
- The radius is computed by the Cauchy–Hadamard formula .
- 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 -transform of a discrete signal is literally a power series in , 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?
Let and let be a sequence of complex numbers. The formal expression
is called a power series centered at . Define
with the convention if the is , and if the is . The number is called the radius of convergence of the series. A function defined on an open set is called analytic at a point if there exists and a power series with radius of convergence at least such that
is analytic on if it is analytic at every point of . A function is holomorphic on if it is complex differentiable at every point of .
Intuition
Think of a power series as a "polynomial with infinitely many terms," built one power of at a time. Whether this infinite sum makes sense depends entirely on the size of the coefficients : if they shrink fast enough, the terms eventually decay geometrically for near , guaranteeing convergence; if they don't shrink fast enough, the terms can blow up once passes some threshold. That threshold is the radius of convergence , and the remarkable fact — proved below via a comparison to geometric series — is that convergence behavior is exactly dichotomous: absolute convergence for , divergence (terms don't even tend to ) for . Nothing can be said in general about the boundary circle 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 as an integral of around a circle, and expanding in a geometric series in converts that formula directly into a power series for , valid inside the circle.
Let be a power series and let
(with the conventions if the limsup is , if it is ). Then: 1. If , the series converges absolutely. 2. If , the terms do not tend to , so the series diverges. 3. For every , the series converges uniformly on the closed disk . Consequently, on the open disk the series defines a function that is continuous, and (as shown in the corollary below) holomorphic with derivative given by termwise differentiation.
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 ). Let satisfy . If there is nothing to prove (no such exists). Assume , possibly . Choose with (if , choose any ). Since , we have when ; when the limsup is for any finite . In either case, by definition of , there exists such that for all ,
Hence for ,
Since , this is a term of a convergent geometric series. By the comparison test, converges, and adding the finitely many terms (each a finite complex number) preserves convergence. Hence converges absolutely.
Part 2 (divergence outside ). Let satisfy . If there is no such . Assume . Then . By definition of as the supremum of subsequential limits, there is a subsequence along which ... more directly: since , there are infinitely many with
for infinitely many . Thus the terms do not converge to , so the series diverges (a necessary condition for convergence of any series is that its terms tend to ).
Part 3 (uniform convergence on closed subdisks). Fix . Choose with (possible since ; if pick any ). As in Part 1, there is such that for all . Then for every with and every ,
Since , is a convergent geometric series independent of . By the Weierstrass M-test, converges uniformly on .
Continuity. Each partial sum is a polynomial, hence continuous on . A uniform limit of continuous functions on a set is continuous on that set (standard argument: for in the disk, , and each piece is made small by uniform convergence and continuity of ). Since every point of lies in some closed subdisk with , the sum is continuous at every point of .
∎Let have radius of convergence . Then the series has the same radius of convergence , and is holomorphic on with there.
Same radius. Since as , we have (multiplying by a sequence tending to does not change a limsup: for any , eventually and , squeezing the limsup of the product between times the original limsup, and letting ). So 's radius of convergence is also (index shift does not affect the limsup either, by the same reasoning applied to the sequence ).
Differentiability. Fix and choose with . We show directly from the difference quotient, using uniform convergence on established above (this is a term-by-term limit interchange argument). For small enough that , write
Let , so . Using the algebraic identity with , , the bracket equals
Each term is again a telescoping sum bounded, for small enough that , by (apply the same factorization once more and bound each factor by ). Hence the bracket is bounded in absolute value by
Therefore
The series converges: it is (up to the same limsup argument as above, since is polynomial in and for any fixed polynomial factor ) a power series in with the same radius of convergence , evaluated at , hence convergent by Part 1 of Radius of Convergence and the Cauchy–Hadamard Formula (the theorem above). Call this convergent sum . Then
Hence is complex differentiable at with . Since was arbitrary, is holomorphic on with derivative .
∎Let be open and . Then is holomorphic on if and only if is analytic on . Moreover, if and is the largest disk centered at contained in , then equals its Taylor series
for all , and this series converges (at least) on that disk.
() Analytic implies holomorphic. This is immediate from the Lemma above: if is analytic at , it agrees with a convergent power series on some disk , and that lemma shows such a series defines a holomorphic function on its disk of convergence. Since analyticity at every point of gives, at each point, a local power series representation with positive radius, is complex differentiable at every point of , i.e. holomorphic.
() 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 . Since is open, choose with (a closed disk of some positive radius fits inside ). Let be the positively oriented circle , which lies in and is homotopic to a point in , so Cauchy's Integral Formula applies to (holomorphic on an open set containing ) for any with :
Fix such a and write , so that
using the geometric series formula , valid since gives and , so . This series in converges uniformly for (i.e. as ranges over the circle, is the constant ratio , so this is literally a fixed convergent geometric series of numbers, uniform trivially in ; more precisely, the partial sums converge uniformly in by the Weierstrass M-test with , a convergent geometric bound independent of ). Therefore
and since is continuous on the compact set (holomorphic functions are continuous, being complex differentiable), is bounded on , say for . The -th term is then bounded by , uniformly in ; the series of these bounds converges (geometric, ratio ), so by the Weierstrass M-test the series converges uniformly in on . 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
Define
These are well-defined complex numbers (independent of ), and we have shown
This exhibits as equal to a convergent power series on , so is analytic at . Since was arbitrary, is analytic on all of .
Identification of coefficients with Taylor coefficients. By the Lemma (termwise differentiation), applied repeatedly to on , we get for every ,
(each differentiation is justified by the Lemma, applied to the previous derivative series, which itself is a power series with the same radius ). Evaluating at kills every term except , giving , i.e.
This shows the power series obtained from Cauchy's formula is exactly the Taylor series of at , and it converges to on the disk for every with ; taking the supremum of all such admissible recovers the statement for the largest disk (any point of that open disk lies in some smaller closed disk contained in , to which the above argument applies).
∎If is holomorphic on an open set , then has complex derivatives of all orders on , and each derivative is itself holomorphic on .
The proof is immediate: locally, 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
Here and . We compute the radius of convergence via Cauchy–Hadamard:
Since polynomially, as (any sequence of the form for a polynomial with positive leading coefficient tends to : write , and since grows slower than any positive power of ). Hence
So this series converges absolutely for and diverges for ; by the theorem it defines a function holomorphic on the disk . Let's verify termwise differentiation concretely at one asymmetric point, say (so , well inside ). The derivative series is
which at becomes the numerical series . This converges (ratio test: ), consistent with the Lemma's guarantee that the differentiated series shares the radius and converges throughout , in particular at .
Example 2 — recovering Taylor coefficients from a rational function via Cauchy's formula, then checking against direct expansion. Let and , holomorphic on . Expand about (an asymmetric, off-center choice, not the origin). Via the theorem's construction. The largest disk centered at contained in has radius (distance to the removed point ). By the theorem, for ,
Via direct algebra (to check). Write , so
valid exactly when , i.e. — matching exactly, as predicted since the nearest singularity of (the pole at ) is at distance from . Cross-check via Taylor's formula. Since (check: , , and inductively ), we get
exactly matching found by direct algebra, confirming the theorem's identification .
The theorem crucially uses complex differentiability (holomorphy), not merely that a function is smooth when viewed as a map . If we only assume real differentiability of (writing ) without the Cauchy–Riemann equations, analyticity can fail completely. Consider . As a map this is smooth (linear, even), with continuous partial derivatives of all orders — it is about as regular as a real function can be. But is nowhere complex differentiable: for along the real axis, , while along the imaginary axis , . The difference quotient has no limit, so does not exist at any . Consequently cannot be represented near any point by a convergent power series : such a series, by the Lemma, would automatically be holomorphic (complex differentiable) on its disk of convergence, contradicting the nowhere-differentiability of . This shows the hypothesis " 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
| Situation | What happens |
|---|---|
| Series converges only at ; defines no function on any open set, hence witnesses no analyticity there | |
| Series converges on all of (entire function), e.g. | |
| on the boundary circle | Cauchy–Hadamard says nothing; behavior must be checked case by case (e.g. diverges everywhere on , converges everywhere on ) |
| Radius from the theorem vs. domain of | equals the distance from to the nearest point not in the domain of holomorphy, not necessarily the "natural" domain one first writes down |
| Real-variable smoothness | Infinitely differentiable real functions need not be analytic (e.g. ); 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
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.
Why does the radius of convergence only depend on a limsup of and not on the actual limit?
Not every sequence converges — it may oscillate — so an ordinary limit might not exist. The always exists (possibly ) for any bounded-below real sequence, because it is defined as the limit of the (necessarily monotonic, hence convergent) sequence of suprema as . Using rather than 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 real function converges back to that function?
Not necessarily — this is one of the sharpest differences between real and complex analysis. A real function can have a Taylor series that converges everywhere but to the wrong function, or converges only at the center. The standard example (extended by ) is real-analytic nowhere near : all its derivatives vanish at , so its Taylor series is identically , yet for . 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 .
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 as an integral of , which is precisely what allows expanding the kernel as a geometric series in . The mean value property (a consequence of the same formula, restricted to ) 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 rather than just an open disk, in the proof of holomorphic implies analytic?
We need to be holomorphic on an open set containing the closed disk and its boundary circle so that Cauchy's Integral Formula, together with continuity/boundedness of on the compact curve , applies rigorously. If we only had an open disk without control on a neighborhood of its boundary, we could not guarantee is even defined on , 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 exists (finite or infinite), it equals , so 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 satisfying (so ) produces, by the Lemma, a genuinely holomorphic function on — coefficients need no special extra property beyond controlling this limsup. Conversely, by the analyticity theorem, that function's own Taylor coefficients at recover exactly the we started with (), so the correspondence between convergent power series and holomorphic germs is a genuine bijection, not merely a one-way construction.