Power Series and Radius of Convergence

⚡ Key Takeaways

Power series: an infinite series ∑n=0∞an(x−c)n\sum_{n=0}^\infty a_n (x-c)^n that behaves like an "infinite polynomial." Every such series has a radius of convergence R∈[0,∞]R \in [0,\infty] such that it converges absolutely for ∣x−c∣<R|x-c| < R and diverges for ∣x−c∣>R|x-c| > R. The number RR is computed by the Cauchy–Hadamard formula. Power series are the foundation of analytic function theory, Taylor expansions, generating functions, and the solution of differential equations. Central results due to Cauchy, Abel, Hadamard, and Weierstrass (19th century).

💡 The Core Insight

The convergence of a power series is governed by a single threshold RR. Inside the disk ∣x−c∣<R|x-c|<R the series converges absolutely and the geometric "tail control" ∣an(x−c)n∣∼(ρ/R)n|a_n(x-c)^n| \sim (\rho/R)^n for ρ<R\rho<R makes everything well-behaved (continuity, differentiability, integrability term-by-term). Outside the terms fail to even approach zero, so divergence is automatic. The boundary ∣x−c∣=R|x-c|=R is the genuinely subtle frontier where anything can happen. The magic is that RR depends only on the growth rate of ∣an∣1/n|a_n|^{1/n}, not on xx.

Formal Statement

DefinitionPower Series

A power series centered at c∈Rc \in \mathbb{R} (or C\mathbb{C}) with coefficients ana_n is the formal sum

1
f(x)=∑n=0∞an(x−c)n=a0+a1(x−c)+a2(x−c)2+⋯\quad f(x) = \sum_{n=0}^{\infty} a_n (x-c)^n = a_0 + a_1(x-c) + a_2(x-c)^2 + \cdots

Derivation hint: By definition; the symbols are ana_n (the nn-th coefficient, a fixed scalar), cc (the center), xx (the variable), nn (the summation index running over non-negative integers). The convergence set is S={x:the series [1] converges}S = \{x : \text{the series } [1] \text{ converges}\}. We always have c∈Sc \in S since at x=cx=c the series reduces to a0a_0.

DefinitionRadius and Interval of Convergence

The radius of convergence is

2
R=sup⁡{ r≥0:∑n=0∞an(x−c)n converges for some ∣x−c∣=r }\quad R = \sup\{\, r \ge 0 : \sum_{n=0}^\infty a_n (x-c)^n \text{ converges for some } |x-c|=r \,\}

with the conventions R=0R=0 (converges only at cc) and R=∞R=\infty (converges everywhere). The interval of convergence is the set SS itself, which is one of (c−R,c+R)(c-R,c+R), [c−R,c+R)[c-R,c+R), (c−R,c+R](c-R,c+R], or [c−R,c+R][c-R,c+R] over R\mathbb{R} — equal to the open interval together with whichever endpoints converge. Derivation hint: RR is defined as a supremum over radii of convergence; the four-fold interval cases arise because endpoint behavior is independent on each side.

TheoremCauchy–Hadamard Formula

For any power series [1][1], the radius of convergence is given by

3
1R=lim sup⁡n→∞∣an∣1/n\quad \frac{1}{R} = \limsup_{n\to\infty} |a_n|^{1/n}

with the conventions 1/0=∞1/0 = \infty and 1/∞=01/\infty = 0. Moreover the series converges absolutely for ∣x−c∣<R|x-c|<R and diverges for ∣x−c∣>R|x-c|>R. Derivation hint: Apply the root test to ∑∣an(x−c)n∣\sum |a_n(x-c)^n|; the nn-th root of the general term is ∣an∣1/n∣x−c∣|a_n|^{1/n}|x-c|, whose limsup is ∣x−c∣/R|x-c|/R.

TheoremRatio Form

If the limit exists, the radius of convergence may also be computed as

4
R=lim⁡n→∞∣anan+1∣\quad R = \lim_{n\to\infty} \left| \frac{a_n}{a_{n+1}} \right|

provided the ana_n are eventually nonzero and the limit (in [0,∞][0,\infty]) exists. This always agrees with [3][3] when the ratio limit exists, but the root formula [3][3] is universally valid. Derivation hint: Apply the ratio test to consecutive terms an+1(x−c)n+1/an(x−c)n=(an+1/an)(x−c)a_{n+1}(x-c)^{n+1} / a_n(x-c)^n = (a_{n+1}/a_n)(x-c); convergence requires ∣x−c∣<lim⁡∣an/an+1∣|x-c| < \lim|a_n/a_{n+1}|.

Why It Holds

ProofCauchy–Hadamard via the Root Test

We prove [3][3]. Let L=lim sup⁡n→∞∣an∣1/nL = \limsup_{n\to\infty} |a_n|^{1/n} and set R=1/LR = 1/L.

Step 1 — Set up the root test. Apply the root test to the series of absolute values ∑n=0∞∣an(x−c)n∣=∑n∣an∣ ∣x−c∣n\sum_{n=0}^\infty |a_n(x-c)^n| = \sum_n |a_n|\,|x-c|^n. The relevant quantity is

5
α:=lim sup⁡n→∞(∣an∣ ∣x−c∣n)1/n=∣x−c∣⋅lim sup⁡n→∞∣an∣1/n=∣x−c∣ L=∣x−c∣R.\quad \alpha := \limsup_{n\to\infty} \big( |a_n|\,|x-c|^n \big)^{1/n} = |x-c| \cdot \limsup_{n\to\infty} |a_n|^{1/n} = |x-c|\,L = \frac{|x-c|}{R}.

Derivation hint: ∣x−c∣|x-c| is a constant factor that pulls out of the limsup of an nn-th root; the remaining factor is the definition of LL.

Step 2 — Convergence when ∣x−c∣<R|x-c|<R. Then α=∣x−c∣/R<1\alpha = |x-c|/R < 1. The root test states that if lim sup⁡(term)1/n<1\limsup (\text{term})^{1/n} < 1 the series converges absolutely. Concretely, pick β\beta with α<β<1\alpha < \beta < 1; for all large nn we have ∣an∣∣x−c∣n≤βn|a_n||x-c|^n \le \beta^n, and ∑βn\sum \beta^n converges as a geometric series. By comparison, [1][1] converges absolutely.

Step 3 — Divergence when ∣x−c∣>R|x-c|>R. Then α>1\alpha > 1. By definition of lim sup⁡\limsup, infinitely many terms satisfy (∣an∣∣x−c∣n)1/n>1(|a_n||x-c|^n)^{1/n} > 1, i.e. ∣an(x−c)n∣>1|a_n(x-c)^n| > 1. The general term does not approach 00, so the series diverges (the nn-th term test).

Step 4 — Boundary undetermined. When ∣x−c∣=R|x-c| = R, α=1\alpha = 1 and the root test is inconclusive; both convergence and divergence are possible (see the examples). This establishes [2][2] and [3][3]. ■\blacksquare

∎
ProofTerm-by-Term Differentiation Inside R

A crucial consequence: inside the disk of convergence, ff is differentiable and

6
f′(x)=∑n=1∞n an(x−c)n−1,∣x−c∣<R,\quad f'(x) = \sum_{n=1}^\infty n\, a_n (x-c)^{n-1}, \qquad |x-c| < R,

and the differentiated series has the same radius RR. Derivation hint: lim sup⁡∣nan∣1/n=lim sup⁡n1/n∣an∣1/n=1⋅L=L\limsup |n a_n|^{1/n} = \limsup n^{1/n}|a_n|^{1/n} = 1\cdot L = L since n1/n→1n^{1/n}\to 1; so RR is unchanged. Equality of f′f' with the term-by-term derivative follows from uniform convergence of the differentiated series on each compact subdisk ∣x−c∣≤ρ<R|x-c|\le \rho < R (Weierstrass M-test), justifying interchange of limit and derivative.

∎
JH
Jacques Hadamard
1865–1963

Though primarily a pure mathematician, Hadamard's 1888 thesis crystallized the formula now bearing his name (with Cauchy), giving the exact radius of convergence via the lim sup⁡\limsup of ∣an∣1/n|a_n|^{1/n} — the first fully general statement, valid even when the ratio ∣an/an+1∣|a_n/a_{n+1}| has no limit. Hadamard also proved the Prime Number Theorem (1896, independently of de la Vallée Poussin), worked extensively on partial differential equations and the calculus of variations, and articulated the influential notion of a well-posed problem. His insight that the growth rate of coefficients alone dictates convergence transformed power series from a computational tool into a structural theory linking real analysis to complex function theory.

Building Intuition

🧠 Intuition

Think of ∣an(x−c)n∣|a_n(x-c)^n| as a race between two factors. The coefficients ∣an∣|a_n| try to blow the terms up (if they grow), while the powers ∣x−c∣n|x-c|^n either help (if ∣x−c∣<1|x-c|<1) or hurt (if ∣x−c∣>1|x-c|>1). The radius RR is the precise value of ∣x−c∣|x-c| at which these forces exactly balance:

  • If ∣x−c∣<R|x-c| < R, the powers shrink fast enough to crush whatever growth ∣an∣|a_n| has — the terms decay geometrically, like a convergent geometric series with ratio ∣x−c∣/R<1|x-c|/R < 1.
  • If ∣x−c∣>R|x-c| > R, the powers grow faster than the coefficients can be tamed, the terms blow up, and the series has no chance.

The number ∣an∣1/n|a_n|^{1/n} measures the "average geometric growth rate per term" of the coefficients; its reciprocal is exactly the distance at which the powers can offset that growth. This is why RR depends only on the coefficients, never on xx.

Figure
Convergence behavior on the real line: absolute convergence inside, divergence outside, indeterminate at the endpoints.

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c c−R c+R absolute convergence |x−c| < R diverges diverges ? convergence ? convergence endpoints must be tested individually

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Worked Examples

ExampleThe Exponential Series — Infinite Radius

Given: f(x)=∑n=0∞xnn!\displaystyle f(x) = \sum_{n=0}^\infty \frac{x^n}{n!}, so an=1/n!a_n = 1/n!, c=0c = 0.

Step 1 — Ratio form [4][4].

∣anan+1∣=1/n!1/(n+1)!=(n+1)!n!=n+1.\left|\frac{a_n}{a_{n+1}}\right| = \frac{1/n!}{1/(n+1)!} = \frac{(n+1)!}{n!} = n+1.

Step 2 — Take the limit.

R=lim⁡n→∞(n+1)=∞.R = \lim_{n\to\infty}(n+1) = \infty.

Step 3 — Interpret. The series converges absolutely for every real (and complex) xx. There are no endpoints to test since R=∞R=\infty.

R=∞,interval of convergence =(−∞,∞)\boxed{R = \infty, \qquad \text{interval of convergence } = (-\infty,\infty)}

This is consistent with f(x)=exf(x) = e^x being defined and analytic everywhere.

ExampleEndpoints Differ — A Logarithmic Series

Given: f(x)=∑n=1∞xnn\displaystyle f(x) = \sum_{n=1}^\infty \frac{x^n}{n}, so an=1/na_n = 1/n, c=0c = 0.

Step 1 — Radius via ratio.

R=lim⁡n→∞∣anan+1∣=lim⁡n→∞1/n1/(n+1)=lim⁡n→∞n+1n=1.R = \lim_{n\to\infty}\left|\frac{a_n}{a_{n+1}}\right| = \lim_{n\to\infty}\frac{1/n}{1/(n+1)} = \lim_{n\to\infty}\frac{n+1}{n} = 1.

So the open interval is (−1,1)(-1,1).

Step 2 — Test the right endpoint x=1x = 1. The series becomes ∑1/n\sum 1/n, the harmonic series, which diverges.

Step 3 — Test the left endpoint x=−1x = -1. The series becomes ∑(−1)n/n\sum (-1)^n/n, the alternating harmonic series, which converges (conditionally, by the alternating series test).

R=1,interval of convergence =[−1,1)\boxed{R = 1, \qquad \text{interval of convergence } = [-1, 1)}

This illustrates that the two endpoints can — and often do — behave completely differently. (Indeed f(x)=−ln⁡(1−x)f(x) = -\ln(1-x), whose singularity at x=1x=1 explains the divergence there.)

Common Misconceptions

⚠️ Common mistake

The ratio test is not always applicable. The formula R=lim⁡∣an/an+1∣R = \lim |a_n/a_{n+1}| requires the limit to exist. For series with gaps (e.g. only even powers) or oscillating coefficient ratios, the limit may fail. The Cauchy–Hadamard formula [3][3] with the limsup is the universally correct tool. Also note: convergence at ∣x−c∣=R|x-c|=R tells you nothing about the other endpoint or about absolute vs. conditional convergence — each boundary point must be checked by hand.

CounterexampleRatio Test Failure on a Lacunary Series

Consider

f(x)=∑n=0∞x2n=x+x2+x4+x8+x16+⋯f(x) = \sum_{n=0}^\infty x^{2^n} = x + x^2 + x^4 + x^8 + x^{16} + \cdots

Here the coefficient of xkx^k is ak=1a_k = 1 if kk is a power of 22 and ak=0a_k = 0 otherwise. The ratio ∣ak/ak+1∣|a_k/a_{k+1}| is undefined infinitely often (division by zero), so [4][4] cannot be used. But Cauchy–Hadamard [3][3] still works: lim sup⁡k∣ak∣1/k=1\limsup_k |a_k|^{1/k} = 1 (since ∣ak∣1/k|a_k|^{1/k} is either 11 or 00, and equals 11 infinitely often), giving R=1R = 1. Moreover, the unit circle ∣x∣=1|x|=1 is a natural boundary: ff cannot be analytically continued past it at any boundary point — a phenomenon invisible to the radius alone.

Connections

connection

Power series sit at the crossroads of several theories:

  • A function equal to its Taylor Series on a neighborhood is precisely an analytic function; power series are the local building blocks of Analytic Functions.
  • Over C\mathbb{C}, the radius of convergence equals the distance from the center to the nearest singularity, tying RR to Complex Analysis and the residue theory of poles and branch points.
  • Generating Functions in combinatorics are power series whose coefficients encode counting sequences; RR controls the asymptotic growth of those sequences via an∼R−na_n \sim R^{-n}.
  • The Frobenius method solves linear Ordinary Differential Equations by assuming power-series solutions and recovering recurrences for the ana_n.
  • Uniform Convergence on compact subdisks (via the Weierstrass M-test) is the engine that legitimizes term-by-term differentiation [6][6] and integration.

Real-World Applications

🔬 Where this appears

Historical Development

⏳ History
- 1668–1671 — Nicolaus Mercator and Isaac Newton develop series for ln⁡(1+x)\ln(1+x) and the generalized binomial series, pioneering power series as a computational engine.
- 1715 — Brook Taylor publishes the Taylor expansion (anticipated by Gregory and Newton), expressing functions as power series in a single point.
- 1748 — Euler's Introductio in analysin infinitorum treats power series formally and freely, deriving countless identities (often without convergence concerns).
- 1821 — Augustin-Louis Cauchy's Cours d'analyse rigorously defines convergence and introduces the root test, laying groundwork for what becomes the Cauchy–Hadamard formula.
- 1826 — Niels Henrik Abel proves Abel's theorem on boundary continuity (∑anxn→∑an\sum a_n x^n \to \sum a_n as x→R−x\to R^- when the endpoint series converges) and corrects loose 18th-century practice.
- 1851–1860s — Weierstrass builds analytic function theory on power series as the primitive objects, proving uniform convergence properties and the M-test that justify term-by-term operations.
- 1888 — Jacques Hadamard, in his doctoral thesis, states the general formula 1/R=lim sup⁡∣an∣1/n1/R = \limsup |a_n|^{1/n}, valid without assuming the ratio limit exists.
- 1892 — Hadamard's gap theorem on natural boundaries shows lacunary series cannot be continued past ∣x∣=R|x|=R.
- 20th c. — The theory generalizes to power series over C\mathbb{C}, Banach spaces (formal/analytic functional calculus), and pp-adic fields, with the radius concept persisting throughout.

Subtleties & Limits

open-problem

Several frontiers remain genuinely deep even beyond undergraduate scope:

  • Boundary behavior is largely undetermined in general: while Abel's theorem handles convergent endpoints and Tauberian theorems give partial converses, classifying exactly which boundary points of a given series converge can be intractable. Carleson's theorem (1966) on almost-everywhere convergence of Fourier series is a celebrated hard result in this circle of ideas.
  • Divergent yet useful series. Many physical expansions have R=0R = 0 (asymptotic series). Borel summation and resurgence theory (Écalle) extract meaning from such series; understanding which divergent series are "resummable" and how is active research.
  • Natural boundaries. Determining whether a power series with a given coefficient pattern has the unit circle as a natural boundary — and the fine structure of singularities on it — connects to the Fabry gap theorem and remains delicate.
  • Several complex variables. The single radius RR becomes a domain of convergence with intricate (logarithmically convex) geometry; the theory of domains of holomorphy and pseudoconvexity is a rich modern subject.

See Also

Taylor Series · Analytic Functions · Limit Superior and Limit Inferior · Root and Ratio Tests · Geometric Series · Uniform Convergence · Complex Analysis · Generating Functions · Ordinary Differential Equations · Fourier Series