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01 June 2026 · 7 min read · updated 13 June 2026

Series and Power Series

A power series is a polynomial of infinite degree, and within its radius of convergence it defines an infinitely differentiable function that is its own Taylor series. We prove absolute convergence implies convergence, prove the root test, prove the Cauchy-Hadamard formula for the radius of convergence, prove a power series may be differentiated term by term inside that radius, and use this to define the exponential function and establish its functional equation. This is where the exponential and trigonometric functions of the characteristic function come from.

  • 1 equation
  • 16 results
  • 8 connections
  • real-analysis
  • series
  • power-series
On this page▾
  • Series and absolute convergence
  • The radius of convergence
  • Term-by-term differentiation
  • The exponential function

7 min left

  • Series and absolute convergence1m
  • The radius of convergence1m
  • Term-by-term differentiation3m
  • The exponential function1m

A power series is the limit of its polynomial partial sums, and where it converges it defines a function as smooth as a polynomial and computable to any accuracy by truncation. The exponential, the sine, and the cosine are defined this way, and their series are what give meaning to the eitXe^{itX}eitX of a characteristic function. This post develops the convergence of series and of power series, proves that a power series can be differentiated term by term, and constructs the exponential, building on the completeness and differentiation of the earlier posts [1], [2].

#Series and absolute convergence

Definition1

The series ∑nan\sum_n a_n∑n​an​ converges to SSS when its partial sums sN=∑n=1Nans_N=\sum_{n=1}^N a_nsN​=∑n=1N​an​ converge to SSS. It converges absolutely when ∑n∣an∣\sum_n\abs{a_n}∑n​∣an​∣ converges.

Convergence is a statement about the sequence of partial sums, so the Cauchy criterion applies, and a series converges if and only if its partial-sum tails are small. Absolute convergence is the stronger and more useful condition.

Proposition2

An absolutely convergent series converges, and ∣∑nan∣≤∑n∣an∣\abs{\sum_n a_n}\le\sum_n\abs{a_n}∣∑n​an​∣≤∑n​∣an​∣.

Proof

For M>NM>NM>N the partial-sum increment is bounded by ∣sM−sN∣=∣∑n=N+1Man∣≤∑n=N+1M∣an∣\abs{s_M-s_N}=\abs{\sum_{n=N+1}^M a_n}\le\sum_{n=N+1}^M \abs{a_n}∣sM​−sN​∣=​∑n=N+1M​an​​≤∑n=N+1M​∣an​∣, which is the corresponding increment of the partial sums of ∑n∣an∣\sum_n\abs{a_n}∑n​∣an​∣. Since the latter series converges its increments tend to 000, so (sN)(s_N)(sN​) is Cauchy and converges by completeness. The inequality follows from ∣sN∣≤∑n=1N∣an∣\abs{s_N}\le\sum_{n=1}^N\abs{a_n}∣sN​∣≤∑n=1N​∣an​∣ by passing to the limit, using continuity of the absolute value.

The test that decides absolute convergence for power series is the root test, which compares the terms with a geometric series.

Theorem3

Let L=lim sup⁡n∣an∣1/nL=\limsup_n\abs{a_n}^{1/n}L=limsupn​∣an​∣1/n. If L<1L<1L<1 the series ∑nan\sum_n a_n∑n​an​ converges absolutely, and if L>1L>1L>1 it diverges.

Proof

If L<1L<1L<1, choose rrr with L<r<1L<r<1L<r<1. By definition of the limit superior, ∣an∣1/n≤r\abs{a_n}^{1/n}\le r∣an​∣1/n≤r for all large nnn, so ∣an∣≤rn\abs{a_n}\le r^n∣an​∣≤rn eventually, and ∑nrn\sum_n r^n∑n​rn converges as a geometric series with ratio below 111, so ∑n∣an∣\sum_n\abs{a_n}∑n​∣an​∣ converges by comparison. If L>1L>1L>1, then ∣an∣1/n≥1\abs{a_n}^{1/n}\ge 1∣an​∣1/n≥1 for infinitely many nnn, so ∣an∣≥1\abs{a_n}\ge 1∣an​∣≥1 infinitely often, the terms do not tend to 000, so the series cannot converge.

#The radius of convergence

A power series converges on an interval symmetric about its centre, and the root test computes its half-length exactly.

Theorem4

For the power series ∑nanxn\sum_n a_n x^n∑n​an​xn, set R=1/lim sup⁡n∣an∣1/nR=1/\limsup_n\abs{a_n}^{1/n}R=1/limsupn​∣an​∣1/n, with R=∞R=\inftyR=∞ when the limit superior is 000 and R=0R=0R=0 when it is ∞\infty∞. The series converges absolutely for ∣x∣<R\abs x<R∣x∣<R and diverges for ∣x∣>R\abs x>R∣x∣>R. The number RRR is the radius of convergence.

Proof

Apply the root test to the series ∑nanxn\sum_n a_n x^n∑n​an​xn, whose terms have lim sup⁡n∣anxn∣1/n=∣x∣ lim sup⁡n∣an∣1/n=∣x∣/R\limsup_n\abs{a_n x^n}^{1/n}=\abs x\,\limsup_n\abs{a_n}^{1/n}=\abs x/Rlimsupn​∣an​xn∣1/n=∣x∣limsupn​∣an​∣1/n=∣x∣/R. This is below 111 exactly when ∣x∣<R\abs x<R∣x∣<R, giving absolute convergence there, and above 111 when ∣x∣>R\abs x>R∣x∣>R, giving divergence. When the limit superior is ∞\infty∞, so R=0R=0R=0, the computed value is ∞>1\infty>1∞>1 for every x≠0x\neq 0x=0, leaving only x=0x=0x=0 convergent, and when it is 000, so R=∞R=\inftyR=∞, the value is 0<10<10<1 for every xxx. The boundary ∣x∣=R\abs x=R∣x∣=R is left undecided, as it must be, since the behaviour there depends on the series.

#Term-by-term differentiation

Inside the radius the series defines a function, and that function is differentiable, with derivative the series differentiated term by term.

Lemma5

The differentiated series ∑nnanxn−1\sum_n n a_n x^{n-1}∑n​nan​xn−1 has the same radius of convergence as ∑nanxn\sum_n a_n x^n∑n​an​xn.

Proof

For x≠0x\neq 0x=0 the differentiated series is ∑n≥1nanxn−1=x−1∑n≥1nanxn\sum_{n\ge1} n a_n x^{n-1}=x^{-1}\sum_{n\ge1} n a_n x^n∑n≥1​nan​xn−1=x−1∑n≥1​nan​xn, and multiplication by the fixed nonzero factor x−1x^{-1}x−1 does not affect convergence, so ∑nnanxn−1\sum_n n a_n x^{n-1}∑n​nan​xn−1 and ∑nnanxn\sum_n n a_n x^n∑n​nan​xn converge for exactly the same xxx (both at x=0x=0x=0 trivially) and share a radius. That radius is governed by lim sup⁡n(n∣an∣)1/n=(lim⁡nn1/n)lim sup⁡n∣an∣1/n=lim sup⁡n∣an∣1/n\limsup_n(n\abs{a_n})^{1/n}=\big(\lim_n n^{1/n}\big)\limsup_n\abs{a_n}^{1/n}= \limsup_n\abs{a_n}^{1/n}limsupn​(n∣an​∣)1/n=(limn​n1/n)limsupn​∣an​∣1/n=limsupn​∣an​∣1/n, using n1/n→1n^{1/n}\to 1n1/n→1, which holds because log⁡(n1/n)=(log⁡n)/n→0\log(n^{1/n})=(\log n)/n\to 0log(n1/n)=(logn)/n→0. A convergent factor passes through the limit superior, so the two series share the value of lim sup⁡n∣an∣1/n\limsup_n \abs{a_n}^{1/n}limsupn​∣an​∣1/n and hence the radius RRR.

The passage to the derivative rests on a general principle about differentiating a limit, which the uniform convergence of the partial sums supplies.

Theorem6

Let gNg_NgN​ be differentiable on an interval with gN→fg_N\to fgN​→f pointwise and the derivatives gN′→hg_N'\to hgN′​→h uniformly. Then fff is differentiable with f′=hf'=hf′=h.

Proof

Fix a point aaa and form the difference quotients φN(x)=gN(x)−gN(a)x−a\varphi_N(x)=\dfrac{g_N(x)-g_N(a)}{x-a}φN​(x)=x−agN​(x)−gN​(a)​ for x≠ax\neq ax=a. For two indices the mean value theorem applied to gN−gMg_N-g_MgN​−gM​ gives a point ξ\xiξ with φN(x)−φM(x)=gN′(ξ)−gM′(ξ)\varphi_N(x)-\varphi_M(x)=g_N'(\xi)-g_M'(\xi)φN​(x)−φM​(x)=gN′​(ξ)−gM′​(ξ), so ∣φN(x)−φM(x)∣≤sup⁡∣gN′−gM′∣\abs{\varphi_N(x)-\varphi_M(x)}\le\sup\abs{ g_N'-g_M'}∣φN​(x)−φM​(x)∣≤sup∣gN′​−gM′​∣, a bound independent of xxx. Since gN′→hg_N'\to hgN′​→h uniformly the right side tends to 000, so (φN)(\varphi_N)(φN​) is uniformly Cauchy and converges uniformly to φ(x)=f(x)−f(a)x−a\varphi(x)=\frac{f(x)-f(a)}{x-a}φ(x)=x−af(x)−f(a)​. Each φN\varphi_NφN​ has the limit gN′(a)g_N'(a)gN′​(a) as x→ax\to ax→a, so the iterated-limit (Moore-Osgood) theorem applies, its two hypotheses being the uniform convergence φN→φ\varphi_N\to\varphiφN​→φ just shown and the existence of each inner limit lim⁡x→aφN(x)=gN′(a)\lim_{x\to a}\varphi_N(x)=g_N'(a)limx→a​φN​(x)=gN′​(a). With lim⁡NgN′(a)=h(a)\lim_N g_N'(a)=h(a)limN​gN′​(a)=h(a) existing by hypothesis it permits exchanging that limit with the limit in NNN, so

lim⁡x→aφ(x)=lim⁡Nlim⁡x→aφN(x)=lim⁡NgN′(a)=h(a).(1)\lim_{x\to a}\varphi(x)=\lim_N\lim_{x\to a}\varphi_N(x)=\lim_N g_N'(a)=h(a). \tag{1}x→alim​φ(x)=Nlim​x→alim​φN​(x)=Nlim​gN′​(a)=h(a).(1)

The left side is by definition f′(a)f'(a)f′(a), so f′(a)=h(a)f'(a)=h(a)f′(a)=h(a).

Corollary7

Inside its radius of convergence a power series f(x)=∑nanxnf(x)=\sum_n a_n x^nf(x)=∑n​an​xn is differentiable with f′(x)=∑nnanxn−1f'(x)=\sum_n n a_n x^{n-1}f′(x)=∑n​nan​xn−1, and by iteration it is infinitely differentiable and equals its own Taylor series, with an=f(n)(0)/n!a_n=f^{(n)}(0)/n!an​=f(n)(0)/n!.

Proof

Fix r<Rr<Rr<R and work on ∣x∣≤r\abs x\le r∣x∣≤r. The partial sums sN(x)=∑n≤Nanxns_N(x)=\sum_{n\le N}a_n x^nsN​(x)=∑n≤N​an​xn are polynomials with sN′(x)=∑n≤Nnanxn−1s_N'(x)=\sum_{n\le N}n a_n x^{n-1}sN′​(x)=∑n≤N​nan​xn−1, and these derivatives converge uniformly on ∣x∣≤r\abs x\le r∣x∣≤r, since ∣nanxn−1∣≤n∣an∣rn−1\abs{n a_n x^{n-1}}\le n\abs{a_n}r^{n-1}​nan​xn−1​≤n∣an​∣rn−1 and ∑nn∣an∣rn−1\sum_n n\abs{a_n}r^{n-1}∑n​n∣an​∣rn−1 converges by Lemma 5 and absolute convergence at r<Rr<Rr<R. By Theorem 6, fff is differentiable on ∣x∣<r\abs x<r∣x∣<r with f′=∑nnanxn−1f'=\sum_n n a_n x^{n-1}f′=∑n​nan​xn−1, and since r<Rr<Rr<R was arbitrary this holds on ∣x∣<R\abs x<R∣x∣<R. By Lemma 5 the derivative f′=∑n≥1nanxn−1f'=\sum_{n\ge1} n a_n x^{n-1}f′=∑n≥1​nan​xn−1 is itself a power series of radius RRR, so the argument reapplies to f′f'f′ and, by induction, f(k)f^{(k)}f(k) exists as a power series of radius RRR for every kkk. Then f(k)(x)=∑n≥kn(n−1)⋯(n−k+1)anxn−kf^{(k)}(x)=\sum_{n\ge k} n(n-1)\cdots(n-k+1)a_n x^{n-k}f(k)(x)=∑n≥k​n(n−1)⋯(n−k+1)an​xn−k, and evaluating the kkk-th derivative at x=0x=0x=0 leaves only the constant term k! akk!\,a_kk!ak​, so ak=f(k)(0)/k!a_k=f^{(k)}(0)/k!ak​=f(k)(0)/k!, the Taylor coefficients.

#The exponential function

Definition8

The exponential is exp⁡(x)=∑n=0∞xnn!\exp(x)=\sum_{n=0}^\infty\dfrac{x^n}{n!}exp(x)=∑n=0∞​n!xn​, a series with radius of convergence ∞\infty∞ since ∣1/n!∣1/n→0\abs{1/n!}^{1/n}\to 0∣1/n!∣1/n→0.

Proposition9

The exponential satisfies exp⁡′=exp⁡\exp'=\expexp′=exp, exp⁡(0)=1\exp(0)=1exp(0)=1, and the functional equation exp⁡(x+y)=exp⁡(x)exp⁡(y)\exp(x+y)=\exp(x)\exp(y)exp(x+y)=exp(x)exp(y).

Proof

Differentiating term by term with Corollary 7, exp⁡′(x)=∑n≥1nxn−1n!=∑n≥1xn−1(n−1)!=exp⁡(x)\exp'(x)=\sum_{n\ge 1}\frac{n x^{n-1}}{n!} =\sum_{n\ge 1}\frac{x^{n-1}}{(n-1)!}=\exp(x)exp′(x)=∑n≥1​n!nxn−1​=∑n≥1​(n−1)!xn−1​=exp(x), and exp⁡(0)=1\exp(0)=1exp(0)=1 from the constant term. For the functional equation, fix yyy and let u(x)=exp⁡(x+y)exp⁡(−x)u(x)=\exp(x+y)\exp(-x)u(x)=exp(x+y)exp(−x), whose derivative is u′(x)=exp⁡(x+y)exp⁡(−x)−exp⁡(x+y)exp⁡(−x)=0u'(x)=\exp(x+y)\exp(-x)-\exp(x+y)\exp(-x)=0u′(x)=exp(x+y)exp(−x)−exp(x+y)exp(−x)=0 by the product and chain rules with exp⁡′=exp⁡\exp'=\expexp′=exp, so uuu is constant by the mean value theorem, equal to its value u(0)=exp⁡(y)u(0)=\exp(y)u(0)=exp(y). Thus exp⁡(x+y)exp⁡(−x)=exp⁡(y)\exp(x+y)\exp(-x)=\exp(y)exp(x+y)exp(−x)=exp(y), and taking y=0y=0y=0 shows exp⁡(−x)=1/exp⁡(x)\exp(-x)=1/\exp(x)exp(−x)=1/exp(x), so exp⁡(x+y)=exp⁡(x)exp⁡(y)\exp(x+y)=\exp(x)\exp(y)exp(x+y)=exp(x)exp(y).

With the exponential in hand the trigonometric functions are its even and odd parts on the imaginary axis, eix=cos⁡x+isin⁡xe^{ix}=\cos x+i\sin xeix=cosx+isinx, and the same term-by-term calculus gives their derivatives and identities. The power series is the bridge from the algebra of polynomials to the transcendental functions of analysis, and the term-by-term differentiation proved here is what turns formal manipulation of infinite sums into rigorous calculus. The exponential series in particular is the function the characteristic function evaluates at imaginary arguments, and its functional equation is the reason characteristic functions of independent sums multiply.

[1]
W. Rudin, Principles of Mathematical Analysis, 3rd ed. McGraw-Hill, 1976.
[2]
S. Abbott, Understanding Analysis, 2nd ed. Springer, 2015.

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cite
@misc{series-and-power-series,
  author = {Zac Kienzle},
  title  = {Series and Power Series},
  year   = {2026},
  month  = {06},
  url    = {https://zackienzle.com/blog/series-and-power-series}
}