Mathematics · Book 4 · Bachelor Year 2

University Mathematics — Year 2

University Mathematics — Year 2 · Bachelor Year 2

11Power Series

Power series are the best-behaved series of functions in mathematics: inside their disk of convergence they converge normally on compacts, may be differentiated and integrated term by term without a second thought, and their sums — analytic functions — are determined by their coefficients. This chapter proves that whole package and reclaims, honestly, every Taylor series of the Year 1 volume; generating functions close it with algebraic dividends.

11.1 Radius of convergence

Lemma 11.1 (Abel)

If the sequence (anz0n)(a_n z_0^n) is bounded for some z00z_0 \neq 0, then anzn\sum a_n z^n converges absolutely for every z<z0\abs z < \abs {z_0}, and normally on every disk zr<z0\abs z \leq r < \abs{z_0}.

Proof. With anz0nM\abs{a_n z_0^n} \leq M and zr\abs z \leq r:

anzn=anz0nzz0nM(rz0) ⁣n,\abs{a_n z^n} = \abs{a_n z_0^n}\,\Bigl|\frac{z}{z_0}\Bigr|^n \leq M\Bigl(\frac{r}{\abs{z_0}}\Bigr)^{\!n},

a convergent geometric bound, uniform on the disk.

Definition 11.2 (Radius of convergence)

The radius of convergence of anzn\sum a_n z^n is

R=sup{r0:(anrn) bounded}[0,+].R = \sup\{r \geq 0 : (a_n r^n) \text{ bounded}\} \in \intcc{0}{+\infty} .

By Lemma 11.1: absolute convergence for z<R\abs z < R (normal on compact subdisks), divergence — indeed unbounded terms — for z>R\abs z > R. On the boundary circle, anything can happen (Exercise 11.2). In practice RR is computed by d’Alembert’s ratio test on anzn\abs{a_n}\abs z^n or by comparison.

Example 11.3 (A radius with no ratio test)

What is the radius of sin(n)zn\sum \sin(n)\,z^n? The ratio sin(n+1)/sinn\abs{\sin(n+1)/\sin n} has no limit, but the definition works directly. R1R \geq 1: sinn1\abs{\sin n} \leq 1, so (sinnrn)(\sin n\cdot r^n) is bounded for every r<1r < 1 — indeed for r=1r = 1. R1R \leq 1: it suffices that sinn↛0\sin n \not\to 0. Suppose sinn0\sin n \to 0; the addition formula

sin(n+1)=sinncos1+cosnsin1\sin(n+1) = \sin n\cos 1 + \cos n\sin 1

would force cosn0\cos n \to 0 (solve for cosn\cos n: sin10\sin 1 \neq 0), contradicting sin2n+cos2n=1\sin^2 n + \cos^2 n = 1. So the terms sin(n)1n\sin(n)\,1^n do not tend to 00: the series diverges at z=1z = 1, and R1R \leq 1. Conclusion: R=1R = 1. Closing insight: the radius is a statement about anrn\abs{a_n}r^n being bounded — no limit of ratios is ever required, and boundedness arguments settle cases the ratio test cannot touch (compare the oscillating coefficients of Exercise 11.1).

Proposition 11.4 (Operations)

Let anzn\sum a_nz^n, bnzn\sum b_nz^n have radii Ra,RbR_a, R_b. Then, for z<min(Ra,Rb)\abs z < \min(R_a, R_b):

(an+bn)zn=anzn+bnzn,(anzn)(bnzn)=cnzn,cn=k=0nakbnk,\sum (a_n + b_n)z^n = \sum a_nz^n + \sum b_nz^n, \qquad \Bigl(\sum a_nz^n\Bigr)\Bigl(\sum b_nz^n\Bigr) = \sum c_n z^n, \quad c_n = \sum_{k=0}^{n} a_kb_{n-k},

both series having radius min(Ra,Rb)\geq \min(R_a, R_b). (The product is the Cauchy product, legitimate by absolute convergence and Theorem 7.14.)

Proof. The sum formula is the linearity of convergent series, and (an+bn)rn(a_n + b_n)r^n is bounded whenever both anrna_nr^n and bnrnb_nr^n are: radius min(Ra,Rb)\geq \min(R_a, R_b). For the product, fix z<min(Ra,Rb)\abs z < \min(R_a, R_b): both series converge absolutely there (Lemma 11.1), so the doubly indexed family (akzkblzl)k,l(a_kz^k\,b_lz^l)_{k,l} is summable, and Theorem 7.14 allows any grouping. Grouping by k+l=nk + l = n:

(kakzk)(lblzl)=n0(k+l=nakbl)zn=n0cnzn,\Bigl(\sum_k a_kz^k\Bigr)\Bigl(\sum_l b_lz^l\Bigr) = \sum_{n\geq0}\Bigl(\sum_{k+l=n}a_kb_l\Bigr)z^n = \sum_{n\geq0}c_nz^n ,

absolutely convergent for every such zz: the product series has radius min(Ra,Rb)\geq \min(R_a, R_b) as well.

Example 11.5 (A Cauchy square, cross-checked)

Square the geometric series: for x<1\abs x < 1, the coefficient of xnx^n in (xk)2\bigl(\sum x^k\bigr)^2 is cn=k+l=n11=n+1c_n = \sum_{k+l=n} 1\cdot1 = n + 1, so

1(1x)2=n0(n+1)xn.\frac{1}{(1-x)^2} = \sum_{n\geq0}(n+1)\,x^n .

Cross-check by term-by-term differentiation (Theorem 11.7 below): differentiating 11x=xn\frac{1}{1-x} = \sum x^n gives 1(1x)2=nxn1=(n+1)xn\frac{1}{(1-x)^2} = \sum nx^{n-1} = \sum(n+1)x^n — the same series by two unrelated mechanisms. Closing insight: when a coefficient identity looks mysterious, one of these two engines (convolution or differentiation) usually produces it in one line; the weekend problem’s question on (2kk)(2n2knk)=4n\sum\binom{2k}k\binom{2n-2k}{n-k} = 4^n runs the convolution engine at full power.

Example 11.6 (Multiplying by 11x\frac{1}{1-x} sums the coefficients)

A Cauchy product against the geometric series has a memorable meaning: for any anxn\sum a_nx^n of radius R>0R > 0 and x<min(R,1)\abs x < \min(R, 1),

11xn0anxn=n0(k=0nak)xn:\frac{1}{1-x}\sum_{n\geq0}a_nx^n = \sum_{n\geq0}\Bigl(\sum_{k=0}^{n}a_k\Bigr)x^n :

multiplication by 11x\frac{1}{1-x} replaces coefficients by their partial sums (convolve with the all-ones sequence). Instance: ex1x=nsnxn\dfrac{\eu^x}{1-x} = \sum_n s_n x^n with sn=kn1k!s_n = \sum_{k\leq n}\frac{1}{k!}, the partial sums of e\eu — compare Exercise 11.11, where the same product with ex\eu^{-x} encodes the derangement counts. Closing insight: operations on power series are operations on coefficient sequences in disguise (multiply by 11x\frac1{1-x}: sum; multiply by xx: shift; differentiate: multiply by nn and shift) — a dictionary the generating-functions chapter will read fluently.

11.2 Regularity of the sum

Theorem 11.7 (Term-by-term calculus)

Let f(x)=n0anxnf(x) = \sum_{n\geq0} a_n x^n have radius R>0R > 0 (real variable x(R,R)x \in \intoo{-R}{R}).

  1. The derived series nanxn1\sum n\,a_n x^{n-1} has the same radius RR, and ff is C1C^1 with f(x)=n1nanxn1f'(x) = \sum_{n \geq 1} n a_n x^{n-1}. Iterating, ff is CC^\infty and

    an=f(n)(0)n!:a_n = \frac{f^{(n)}(0)}{n!} :

    the coefficients of a power series are unique (two series with the same sum near 00 have equal coefficients).

  2. Term-by-term primitive: ann+1xn+1\sum \frac{a_n}{n+1}x^{n+1} has radius RR and derivative ff.

Proof. Same radius: if (anrn)(a_nr^n) is bounded and r<rr' < r, then nanrn1=nranrn(rr)nn\abs{a_n} r'^{\,n-1} = \frac{n}{r'}\abs{a_nr^n} \bigl(\frac{r'}{r}\bigr)^n is bounded (indeed 0\to 0: geometric beats nn), so RRR' \geq R; conversely anxnxnanxn1\abs{a_n x^n} \leq \abs x \cdot n\abs{a_n}\abs x^{n-1} gives RRR \geq R'.

Differentiation: on [r,r]\intcc{-r}{r}, r<Rr < R, the derived series converges normally (nanrn1n\abs{a_n}r^{n-1} summable by the radius computation); the original converges at x=0x = 0: the differentiation theorem for series (Theorem 10.11) applies on every such segment, hence on (R,R)\intoo{-R}{R}. Iterating kk times and evaluating at 00: explicitly, the kk-th derived series is

f(k)(x)=nkn(n1)(nk+1)anxnk,f^{(k)}(x) = \sum_{n\geq k} n(n-1)\cdots(n-k+1)\,a_n\,x^{n-k},

and at x=0x = 0 every term with n>kn > k vanishes, leaving only the constant term k(k1)1akk(k-1)\cdots1\cdot a_k: f(k)(0)=k!akf^{(k)}(0) = k!\,a_k. Uniqueness of coefficients follows: two power series with the same sum near 00 have the same derivatives at 00, hence the same aka_k. Primitives: same radius by the same computation, and differentiate term by term back.

Example 11.8 (Evaluating a series at a point)

What is n1n22n\sum_{n\geq1}\dfrac{n^2}{2^n}? It is the sum n2xn\sum n^2x^n of Exercise 11.3 evaluated inside the disk, at x=12<1=Rx = \frac12 < 1 = R, where every manipulation used to derive the closed form was legitimate:

n1n2xn=x(1+x)(1x)3n1n22n=1232(12)3=3/41/8=6.\sum_{n\geq1} n^2x^n = \frac{x(1+x)}{(1-x)^3} \quad\Longrightarrow\quad \sum_{n\geq1}\frac{n^2}{2^n} = \frac{\frac12\cdot\frac32}{(\frac12)^3} = \frac{3/4}{1/8} = 6 .

Same engine, other dials: x=13x = \frac13 gives n23n=1343(2/3)3=32\sum\frac{n^2}{3^n} = \frac{\frac13\cdot\frac43}{(2/3)^3} = \frac32. Closing insight: a power-series identity is a machine, not a single formula — one derivation prices every numerical series n2qn\sum n^2q^n at once, for all q<1\abs q < 1; this is how the generating-functions chapter will compute expectations and variances wholesale.

Example 11.9 (The classics, this time honestly)

11x=xn\displaystyle\frac{1}{1 - x} = \sum x^n (R=1R = 1); integrating term by term (Theorem 11.7 (2)):

ln(1x)=n1xnn,arctanx=n0(1)nx2n+12n+1(x<1),-\ln(1 - x) = \sum_{n\geq1} \frac{x^n}{n}, \qquad \arctan x = \sum_{n \geq 0} \frac{(-1)^n x^{2n+1}}{2n+1} \quad (\abs x < 1),

the second in two steps: substitute x2-x^2 in the geometric series to get 11+x2=(1)nx2n\frac{1}{1+x^2} = \sum(-1)^nx^{2n} (radius 11, since x2<1    x<1\abs{x^2} < 1 \iff \abs x < 1), then take the term-by-term primitive vanishing at 00; both sides are primitives of the same function with the same value at 00, hence equal on (1,1)\intoo{-1}{1}. And exp\exp: the series E(x)=xnn!E(x) = \sum \frac{x^n}{n!} (R=R = \infty) satisfies E=EE' = E, E(0)=1E(0) = 1 by termwise differentiation, so E=expE = \exp by the Year 1 uniqueness. Every “standard expansion” of the Year 1 volume is now a theorem about its full power series.

Example 11.10 (A logarithm computed from inside the disk)

Evaluating ln(1x)=xnn-\ln(1-x) = \sum\frac{x^n}{n} at the interior point x=12x = \frac12:

n11n2n=ln2,\sum_{n\geq1}\frac{1}{n\,2^n} = \ln 2 ,

a fast-converging representation of ln2\ln 2 (ten terms already give 0.693060.69306\ldots against ln2=0.69314\ln 2 = 0.69314\ldots), far better than the alternating series 112+131 - \frac12 + \frac13 - \dots available only at the boundary. Closing insight: whenever a constant is reachable both at the rim and strictly inside the disk, the interior wins numerically — geometric decay against harmonic decay.

Example 11.11 (Differentiation preserves the radius, not the boundary)

The series n1xnn2\sum_{n\geq1}\frac{x^n}{n^2} has radius 11 and converges at both endpoints (1n2\sum\frac1{n^2} and its alternating twin). Its derived series,

n1xn1n,\sum_{n\geq1}\frac{x^{n-1}}{n} ,

has the same radius 11 — as Theorem 11.7 guarantees — but now diverges at x=1x = 1 (harmonic series) while still converging at x=1x = -1 (alternating). One more differentiation yields n2n1nxn2\sum_{n\geq2}\frac{n-1}{n}x^{n-2}, divergent at both ends (terms do not tend to 00). Closing insight: each differentiation multiplies the coefficients by nn, which never moves the radius (geometric beats polynomial) but eats one order of boundary decay; term-by-term calculus is an interior sport, and whatever happens on the rim must be re-examined — the weekend problem’s Abel–Tauber theory is exactly that re-examination.

Example 11.12 (Splitting a series by residues — worked to the end)

Compute f(x)=n0x4n(4n)!f(x) = \sum_{n\geq0} \dfrac{x^{4n}}{(4n)!} in closed form. Both coshx=x2m(2m)!\cosh x = \sum \frac{x^{2m}}{(2m)!} and cosx=(1)mx2m(2m)!\cos x = \sum \frac{(-1)^m x^{2m}}{(2m)!} have radius \infty, so their average may be computed term by term:

coshx+cosx2=m01+(1)m2x2m(2m)!=m evenx2m(2m)!=n0x4n(4n)!=f(x).\frac{\cosh x + \cos x}{2} = \sum_{m\geq0}\frac{1 + (-1)^m}{2}\,\frac{x^{2m}}{(2m)!} = \sum_{m \text{ even}}\frac{x^{2m}}{(2m)!} = \sum_{n\geq0}\frac{x^{4n}}{(4n)!} = f(x) .

The filter 1+(1)m2\frac{1+(-1)^m}{2} keeps exactly the even mm: this is the real avatar of the roots-of-unity filter (the complex version, with in\iu^n, extracts residues modulo 44 in one stroke). Closing check: ff solves f=ff'''' = f with f(0)=1f(0) = 1, f(0)=f(0)=f(0)=0f'(0) = f''(0) = f'''(0) = 0 — differentiate the series four times (Theorem 11.7) and watch it reproduce itself; cosh+cos2\frac{\cosh + \cos}{2} satisfies the same data.

Definition 11.13 (Analytic functions)

ff is analytic at x0x_0 when it is the sum of a power series in (xx0)(x - x_0) on a neighborhood; on an interval, when at every point. Sums of power series are analytic inside their disk (rearrangement of the expansion — admitted at this level for re-centering, the case x0=0x_0 = 0 being Theorem 11.7). Analytic implies CC^\infty; the converse fails: the flat function e1/x2\eu^{-1/x^2} (Exercise 11.7).

Example 11.14 (Re-centering, and the radius as a distance)

Expand f(x)=11xf(x) = \frac{1}{1-x} around x0=12x_0 = \frac12: writing x=12+hx = \frac12 + h,

11x=112h=212h=n02n+1hn=n02n+1(x12) ⁣n,\frac{1}{1 - x} = \frac{1}{\frac12 - h} = \frac{2}{1 - 2h} = \sum_{n\geq0} 2^{n+1}\,h^n = \sum_{n\geq0} 2^{n+1}\Bigl(x - \frac12\Bigr)^{\!n},

valid for 2h<1\abs{2h} < 1, i.e. x12<12\abs{x - \frac12} < \frac12. The new radius is exactly the distance from the new center to the singularity x=1x = 1: re-centering shrinks (or grows) the disk to fit the nearest obstruction. Closing insight: this is the picture behind the definition of analyticity — one function, many local power series, each living on the largest disk avoiding the trouble; the Year 3 volume turns the heuristic “radius == distance to the nearest complex singularity” into a theorem.

Remark 11.15 (Common pitfalls)

(i) The ratio test is sufficient, not necessary: when an+1/an\abs{a_{n+1}/a_n} has no limit (Example 11.3, Exercise 11.1), go back to the definition: R=sup{r:(anrn)R = \sup\{r : (a_nr^n) bounded}\}. (ii) Nothing crosses the boundary for free: term-by-term differentiation and integration are theorems inside the open disk; at x=R\abs x = R each series must be re-examined (that is the whole subject of the weekend problem). (iii) Radius of a sum: min(Ra,Rb)\min(R_a, R_b) is only a lower bound — cancellations can enlarge it (an=1,bn=1a_n = 1, b_n = -1: sum identically 00, radius \infty). (iv) CC^\infty is not analytic: a convergent Taylor series may converge to the wrong function (Exercise 11.7); before writing f(x)=f(n)(0)n!xnf(x) = \sum \frac{f^{(n)}(0)}{n!}x^n, prove it — via an ODE (Method 11.17), a remainder estimate, or an integral formula.

Remark 11.16 (Where this is used)

Power series are the workhorse of three later chapters: the differential-equations chapter solves linear ODEs by injecting anxn\sum a_nx^n (the method box below, industrialized); the generating-functions chapter converts identities about probabilities into identities about power series and back; and the Year 3 volume makes the complex variable official, where analyticity becomes equivalent to complex differentiability and the “admitted re-centering” above gets its honest proof. The weekend problem explores the one place this chapter’s theorems stay silent: the boundary x=R\abs x = R itself.

Method 11.17 (Expanding via a differential equation)

To expand a function ff in a power series: find a linear ODE with polynomial coefficients satisfied by ff; inject anxn\sum a_nx^n; identify coefficients to get a recurrence for (an)(a_n); solve, and check radius and initial conditions. Example — the binomial series: f(x)=(1+x)αf(x) = (1+x)^\alpha satisfies (1+x)f=αf(1+x)f' = \alpha f, f(0)=1f(0) = 1; injecting gives (n+1)an+1=(αn)an(n+1)a_{n+1} = (\alpha - n)a_n, so an=(αn)a_n = \binom{\alpha}{n}, radius 11 (ratio test), and the sum, satisfying the same ODE with the same initial value, equals (1+x)α(1 + x)^\alpha by the uniqueness theorem for linear ODEs (Year 1 volume).

Example 11.18 (The method on a forced equation)

Solve y=y+xy' = y + x, y(0)=0y(0) = 0, by power series. Injecting y=anxny = \sum a_nx^n:

n0(n+1)an+1xn=n0anxn+x,\sum_{n\geq0}(n+1)a_{n+1}x^n = \sum_{n\geq0}a_nx^n + x ,

and identifying coefficients: a1=a0=0a_1 = a_0 = 0, 2a2=a1+1=12a_2 = a_1 + 1 = 1, and (n+1)an+1=an(n+1)a_{n+1} = a_n for n2n \geq 2. So a2=12!a_2 = \frac{1}{2!} and, by induction, an=1n!a_n = \frac{1}{n!} for every n2n \geq 2: radius \infty, and

y(x)=n2xnn!=ex1x.y(x) = \sum_{n\geq2}\frac{x^n}{n!} = \eu^x - 1 - x .

Check: y=ex1=y+xy' = \eu^x - 1 = y + x and y(0)=0y(0) = 0. Closing insight: the recurrence is the equation, coefficient by coefficient; the forcing term only perturbs finitely many initial coefficients, after which the homogeneous pattern takes over — a discrete shadow of “particular solution plus homogeneous solution”.

11.3 Generating functions

Example 11.19 (Fibonacci)

Let F(x)=n0FnxnF(x) = \sum_{n\geq0} F_n x^n (Fibonacci numbers, F0=0F_0 = 0, F1=1F_1 = 1). The recurrence Fn+2=Fn+1+FnF_{n+2} = F_{n+1} + F_n translates, multiplying by xn+2x^{n+2} and summing, into

F(x)x=xF(x)+x2F(x)F(x)=x1xx2,F(x) - x = x\,F(x) + x^2 F(x) \quad\Longrightarrow\quad F(x) = \frac{x}{1 - x - x^2} ,

valid where the series converges. The radius is 1φ\frac{1}{\varphi}: from Fnφn5F_n \sim \frac{\varphi^n}{\sqrt5} (Binet, next example — or the crude induction Fn2nF_n \leq 2^n plus the recurrence), the ratio test gives

Fn+1xn+1Fnxnφx,convergence iff x<1φ0.618.\frac{F_{n+1}\abs x^{n+1}}{F_n\abs x^n} \longrightarrow \varphi\abs x , \qquad\text{convergence iff } \abs x < \frac1\varphi \approx 0.618 .

Partial fractions on x1xx2\frac{x}{1 - x - x^2} and the geometric series re-derive Binet’s formula — generating functions industrialize linear recurrences.

Example 11.20 (Binet’s formula, carried out)

Let φ=1+52\varphi = \frac{1+\sqrt5}{2} and ψ=152\psi = \frac{1-\sqrt5}{2}, the roots of X2=X+1X^2 = X + 1; since φ+ψ=1\varphi + \psi = 1 and φψ=1\varphi\psi = -1,

1xx2=(1φx)(1ψx).1 - x - x^2 = (1 - \varphi x)(1 - \psi x) .

Partial fractions: seeking x(1φx)(1ψx)=A1φx+B1ψx\frac{x}{(1-\varphi x)(1-\psi x)} = \frac{A}{1 - \varphi x} + \frac{B}{1 - \psi x}, the constant term gives A+B=0A + B = 0 and the xx-coefficient AψBφ=1-A\psi - B\varphi = 1, so A(φψ)=1A(\varphi - \psi) = 1: A=15=BA = \frac{1}{\sqrt5} = -B. Two geometric series later,

F(x)=15n0(φnψn)xnFn=φnψn5F(x) = \frac{1}{\sqrt5}\sum_{n\geq0} \bigl(\varphi^n - \psi^n\bigr)x^n \quad\Longrightarrow\quad F_n = \frac{\varphi^n - \psi^n}{\sqrt5}

by uniqueness of coefficients (Theorem 11.7). Since ψ<1\abs\psi < 1, the term ψn5\frac{\psi^n}{\sqrt5} has absolute value <12< \frac12: FnF_n is the nearest integer to φn5\frac{\varphi^n}{\sqrt5}. Closing insight: the radius 1φ\frac1\varphi of FF is the reciprocal of the dominant root — growth of coefficients and radius of convergence are the same information read in opposite directions.

Example 11.21 (Catalan numbers)

The Catalan numbers CnC_n (number of triangulations, of bracketings, of Dyck paths, …) satisfy C0=1C_0 = 1 and Cn+1=k=0nCkCnkC_{n+1} = \sum_{k=0}^n C_kC_{n-k}. The generating function C(x)=CnxnC(x) = \sum C_nx^n then satisfies (Cauchy product!)

C(x)=1+xC(x)2C(x)=114x2x,C(x) = 1 + x\,C(x)^2 \quad\Longrightarrow\quad C(x) = \frac{1 - \sqrt{1 - 4x}}{2x} ,

choosing the root with C(0)=1C(0) = 1: solving the quadratic xC2C+1=0xC^2 - C + 1 = 0 gives the two candidates 1±14x2x\frac{1 \pm \sqrt{1-4x}}{2x}, and as x0x \to 0 the “++” root blows up like 1x\frac1x while the “-” root tends to 11 (expand 14x=12x+O(x2)\sqrt{1-4x} = 1 - 2x + O(x^2)) — only the minus sign can carry a power series with C0=1C_0 = 1. Expanding 14x\sqrt{1 - 4x} by the binomial series gives the closed form

Cn=1n+1(2nn),C_n = \frac{1}{n+1}\binom{2n}{n} ,

carried out in Exercise 11.8.

Remark 11.22 (Formal series versus convergent series)

Every generating-function computation above ends by invoking the uniqueness of coefficients, and that theorem lives inside a disk of positive radius: before “reading off” FnF_n or CnC_n, one must know R>0R > 0. A crude a priori bound suffices — Fn2nF_n \leq 2^n (immediate induction) gives R12R \geq \frac12 for Fibonacci; Cn4nC_n \leq 4^n (each Catalan number counts subsets of paths) gives R14R \geq \frac14. Beware the degenerate end of the scale: n!xn\sum n!\,x^n has radius 00, and manipulating it as a function is meaningless — identities involving such series belong to the formal calculus of coefficients, a purely algebraic game with its own (different) rules. At this level: always secure a positive radius first, then compute freely inside it.

Remark 11.23 (Perspectives within this volume)

Power series are one of the book’s two great expansion machines; the other is the Fourier series of the harmonic chapters, and comparing them is instructive. A power series is rigid: its coefficients are forced (an=f(n)(0)/n!a_n = f^{(n)}(0)/n!), its convergence is ruthless (normal inside, hopeless outside), and its sum is analytic — infinitely rigid (Definition 11.13). A Fourier series is supple: it represents merely piecewise-smooth signals, at the price of delicate convergence questions at the boundary of smoothness. The two theories meet in this chapter’s weekend problem: Cesàro and Abel summation, developed here for the boundary circle, return in the Fourier chapter as Fejér’s and Poisson’s kernels. Meanwhile the differential-equations chapter consumes power series directly (etA\eu^{tA}, series solutions), and the generating-functions chapter turns Example 11.19’s trick into a systematic calculus for probabilities.

11.4 Exercises

Exercise 11.1

Radii of convergence: n22nzn\sum \dfrac{n^2}{2^n}z^n;   zn(2nn)\;\sum \dfrac{z^n}{\binom{2n}{n}};   zn!\;\sum z^{n!};   (2+(1)n)nzn\;\sum \bigl(2 + (-1)^n\bigr)^n z^n.

Solution

Solution of Exercise 11.1.

n22nzn\sum \frac{n^2}{2^n}z^n: ratio (n+1)22n+12nn212\frac{(n+1)^2}{2^{n+1}}\cdot \frac{2^n}{n^2} \to \frac12: R=2R = 2.

zn(2nn)\sum \frac{z^n}{\binom{2n}{n}}: (2nn)4nπn\binom{2n}{n} \sim \frac{4^n}{\sqrt{\pi n}} (Example 6.14), so an14n\abs{a_n}^{-1} \approx 4^n up to polynomial factors: R=4R = 4 (ratio test: (2nn)(2n+2n+1)=(n+1)2(2n+1)(2n+2)14\frac{\binom{2n}{n}}{\binom{2n+2}{n+1}} = \frac{(n+1)^2}{(2n+1)(2n+2)} \to \frac14).

zn!\sum z^{n!}: coefficients ak=1a_k = 1 if k=n!k = n!, else 00. For z<1\abs z < 1, zn!\sum \abs z^{n!} converges (dominated by geometric); for z1\abs z \geq 1 the terms do not tend to 00: R=1R = 1.

(2+(1)n)nzn\sum (2 + (-1)^n)^n z^n: coefficients 3n3^n (even nn) and 11 (odd nn). Boundedness of anrna_nr^n requires 3r13r \leq 1; and r<13r < \frac13 works: R=13R = \frac13.

Exercise 11.2

Show that zn\sum z^n, znn\sum \frac{z^n}{n}, znn2\sum \frac{z^n}{n^2} all have radius 11 but behave differently at z=1z = 1 and z=1z = -1: divergence/divergence, divergence/convergence, convergence/convergence.

Solution

Solution of Exercise 11.2.

All three have radius 11 (ratio test). At z=1z = 1: 1\sum 1 diverges; 1n\sum\frac1n diverges; 1n2\sum\frac{1}{n^2} converges. At z=1z = -1: (1)n\sum(-1)^n diverges; (1)nn\sum\frac{(-1)^n}{n} converges (alternating); (1)nn2\sum\frac{(-1)^n}{n^2} converges (absolutely). Boundary behavior is invisible to the radius.

Exercise 11.3

Compute the sums, for x<1\abs x < 1:

n0nxn,n0n2xn,n0x2n+12n+1.\sum_{n\geq0} n x^n, \qquad \sum_{n\geq0} n^2 x^n, \qquad \sum_{n\geq0} \frac{x^{2n+1}}{2n+1} .
Solution

Solution of Exercise 11.3.

From 11x=xn\frac{1}{1-x} = \sum x^n, differentiate and multiply by xx (Theorem 11.7):

nxn=x(1x)2.\sum n x^n = \frac{x}{(1-x)^2} .

Differentiate once more, multiply by xx again:

n2xn=x ⁣d ⁣dx(x(1x)2)=x(1+x)(1x)3.\sum n^2 x^n = x\,\frac{\dd}{\dd x}\Bigl(\frac{x}{(1-x)^2}\Bigr) = \frac{x(1 + x)}{(1-x)^3} .

Third sum: it is the odd part of ln(1x)-\ln(1 - x):

n0x2n+12n+1=ln(1x)+ln(1+x)2=12ln1+x1x=artanhx.\sum_{n\geq0} \frac{x^{2n+1}}{2n+1} = \frac{-\ln(1-x) + \ln(1+x)}{2} = \frac12 \ln\frac{1+x}{1-x} = \operatorname{artanh} x .

Exercise 11.4 ★★

Expand in power series at 00, with radius: 1(1x)(2x)\dfrac{1}{(1-x)(2-x)} (partial fractions);   ln(1+x+x2)\;\ln(1 + x + x^2) (write 1+x+x2=1x31x1 + x + x^2 = \frac{1 - x^3}{1 - x}).

Solution

Solution of Exercise 11.4.

Partial fractions: 1(1x)(2x)=11x12x=xn12(x2)n\frac{1}{(1-x)(2-x)} = \frac{1}{1-x} - \frac{1}{2 - x} = \sum x^n - \frac12\sum \bigl(\frac x2\bigr)^n:

1(1x)(2x)=n0(112n+1)xn,R=1.\frac{1}{(1-x)(2-x)} = \sum_{n\geq0} \Bigl(1 - \frac{1}{2^{n+1}}\Bigr)x^n, \qquad R = 1 .

ln(1+x+x2)=ln1x31x=ln(1x3)ln(1x)=n1xnnm1x3mm\ln(1 + x + x^2) = \ln\frac{1 - x^3}{1 - x} = \ln(1 - x^3) - \ln(1 - x) = \sum_{n\geq1}\frac{x^n}{n} - \sum_{m\geq1}\frac{x^{3m}}{m}: the coefficient of xnx^n is 1n\frac1n if 3n3 \nmid n, and 1n3n=2n\frac1n - \frac{3}{n} = -\frac2n if 3n3 \mid n. Radius 11 (the nearest obstruction: the series for ln(1x3)\ln(1-x^3)).

Exercise 11.5 ★★

Prove that f(x)=n1Hnxn=ln(1x)1xf(x) = \sum_{n\geq1} H_n x^n = -\dfrac{\ln(1 - x)}{1 - x} for x<1\abs x < 1, where HnH_n is the harmonic number (Cauchy product of xn\sum x^n and xnn\sum \frac{x^n}{n}).

Solution

Solution of Exercise 11.5.

Cauchy product of m0xm\sum_{m \geq 0} x^m (coefficients 11) and k1xkk\sum_{k\geq1} \frac{x^k}{k} (coefficients 1k\frac1k, k1k \geq 1), both absolutely convergent for x<1\abs x < 1: the coefficient of xnx^n in the product is k=1n1k1=Hn\sum_{k=1}^{n} \frac1k \cdot 1 = H_n. Hence

(xm)(xkk)=11x(ln(1x))=n1Hnxn.\Bigl(\sum x^m\Bigr)\Bigl(\sum \frac{x^k}{k}\Bigr) = \frac{1}{1-x}\cdot\bigl(-\ln(1-x)\bigr) = \sum_{n\geq1} H_n x^n .

Exercise 11.6 ★★

Solve by generating function the recurrence u0=1u_0 = 1, un+1=2un+nu_{n+1} = 2u_n + n: compute U(x)=unxnU(x) = \sum u_nx^n in closed form, decompose, and read off un=2n+1n1u_n = 2^{n+1} - n - 1.

Solution

Solution of Exercise 11.6.

Multiply the recurrence by xn+1x^{n+1} and sum (x<12\abs x < \frac12):

U(x)1=2xU(x)+n0nxn+1=2xU(x)+x2(1x)2,U(x) - 1 = 2x\,U(x) + \sum_{n\geq0} n\,x^{n+1} = 2x\,U(x) + \frac{x^2}{(1-x)^2} ,

using Exercise 11.3. Hence

U(x)=112x(1+x2(1x)2)=12x+2x2(12x)(1x)2.U(x) = \frac{1}{1 - 2x}\Bigl(1 + \frac{x^2}{(1-x)^2}\Bigr) = \frac{1 - 2x + 2x^2}{(1-2x)(1-x)^2} .

Partial fractions (cover-up at x=12x = \frac12 gives coefficient 22; at the double pole x=1x = 1, coefficient 1-1; the middle coefficient vanishes by evaluating at x=0x = 0):

U(x)=212x1(1x)2.U(x) = \frac{2}{1-2x} - \frac{1}{(1 - x)^2} .

Expanding both:

un=22n(n+1)=2n+1n1.u_n = 2\cdot 2^n - (n + 1) = 2^{n+1} - n - 1 .

(Check: u0=1u_0 = 1, u1=2u0+0=2=42u_1 = 2u_0 + 0 = 2 = 4 - 2.)

Exercise 11.7 ★★

Let f(x)=e1/x2f(x) = \eu^{-1/x^2} for x0x \neq 0, f(0)=0f(0) = 0. Prove that ff is CC^\infty on R\R with f(n)(0)=0f^{(n)}(0) = 0 for all nn (show by induction that f(n)(x)=Pn(1x)e1/x2f^{(n)}(x) = P_n\bigl(\frac1x\bigr) \eu^{-1/x^2} for polynomials PnP_n, and use the growth comparison). Conclude that ff is not analytic at 00: its Taylor series at 00 converges — to the wrong function.

Solution

Solution of Exercise 11.7.

Induction: f(x)=2x3e1/x2f'(x) = \frac{2}{x^3}\eu^{-1/x^2}, and if f(n)(x)=Pn(1x)e1/x2f^{(n)}(x) = P_n(\tfrac1x)\eu^{-1/x^2} then

f(n+1)(x)=(1x2Pn(1x)+2x3Pn(1x))e1/x2:f^{(n+1)}(x) = \Bigl(-\frac{1}{x^2}\,P_n'\Bigl(\frac1x\Bigr) + \frac{2}{x^3}\,P_n\Bigl(\frac1x\Bigr)\Bigr)\eu^{-1/x^2} :

again of the stated form. At 00: difference quotients f(n)(h)h=1hPn(1h)e1/h20\frac{f^{(n)}(h)}{h} = \frac1h P_n(\frac1h)\eu^{-1/h^2} \to 0 as h0h \to 0, since Q(u)eu20Q(u)\,\eu^{-u^2} \to 0 as u±u \to \pm\infty for any polynomial QQ (exponential beats powers): by induction all f(n)(0)f^{(n)}(0) exist and vanish, and each f(n)f^{(n)} is continuous at 00 by the same limit. So fCf \in C^\infty with zero Taylor series at 00; the Taylor series sums to 0f0 \neq f: not analytic at 00.

Exercise 11.8 ★★★

Complete Example 11.21: expand 14x\sqrt{1 - 4x} with the binomial series, showing

(1/2n+1)(4)n+1=2n+1(2nn),\binom{1/2}{n+1}(-4)^{n+1} = -\frac{2}{n+1}\binom{2n}{n},

and deduce Cn=1n+1(2nn)C_n = \frac{1}{n+1}\binom{2n}{n}; determine the radius of convergence of C(x)C(x) and the asymptotics of CnC_n via Stirling.

Solution

Solution of Exercise 11.8.

Binomial series: 14x=k0(1/2k)(4x)k\sqrt{1-4x} = \sum_{k\geq0} \binom{1/2}{k}(-4x)^k. For k=n+11k = n + 1 \geq 1:

(1/2n+1)(4)n+1=12(121)(12n)(n+1)!(4)n+1=(1)n13(2n1)2n+1(n+1)!(4)n+1=2n+1(2n)!n!n!,\begin{align*} \binom{1/2}{n+1}(-4)^{n+1} &= \frac{\frac12\bigl(\frac12 - 1\bigr)\cdots\bigl(\frac12 - n\bigr)}{(n+1)!}\,(-4)^{n+1}\\ &= \frac{(-1)^n\,1\cdot3\cdots(2n-1)}{2^{n+1}(n+1)!}\,(-4)^{n+1} = -\frac{2}{n+1}\cdot\frac{(2n)!}{n!\,n!} , \end{align*}

using 13(2n1)=(2n)!2nn!1\cdot3\cdots(2n-1) = \frac{(2n)!}{2^n n!}. Hence

C(x)=114x2x=12xn02n+1(2nn)xn+1=n01n+1(2nn)xn:C(x) = \frac{1 - \sqrt{1-4x}}{2x} = \frac{1}{2x}\sum_{n\geq0}\frac{2}{n+1}\binom{2n}{n}x^{n+1} = \sum_{n\geq0} \frac{1}{n+1}\binom{2n}{n}\,x^n :

Cn=1n+1(2nn)C_n = \frac{1}{n+1}\binom{2n}{n}. Radius: 14\frac14 (the binomial series in 4x4x). Asymptotics via Example 6.14:

Cn4nπ  n3/2.C_n \sim \frac{4^n}{\sqrt{\pi}\; n^{3/2}} .

Exercise 11.9 ★★★

(Abel’s radial limit theorem, special case) Suppose an\sum a_n converges. Prove that limx1nanxn=nan\lim_{x \to 1^-} \sum_{n} a_n x^n = \sum_n a_n. (Abel summation: with AnA_n the partial sums and A=limAnA = \lim A_n, write anxn=(1x)Anxn\sum a_nx^n = (1 - x)\sum A_n x^n; then anxnA=(1x)(AnA)xn\sum a_nx^n - A = (1-x)\sum (A_n - A)x^n, split the sum at a large NN.) Application: (1)n1n=ln2\sum \frac{(-1)^{n-1}}{n} = \ln 2 and (1)n2n+1=π4\sum \frac{(-1)^n}{2n+1} = \frac\pi4, re-proved from the power series.

Solution

Solution of Exercise 11.9.

With An=knakAA_n = \sum_{k \leq n} a_k \to A: Abel summation gives, for 0x<10 \leq x < 1,

n=0anxn=(1x)n=0Anxn\sum_{n=0}^{\infty} a_n x^n = (1 - x)\sum_{n=0}^{\infty} A_n x^n

(both sides converge: (An)(A_n) is bounded; and the identity follows from an=AnAn1a_n = A_n - A_{n-1} and reindexing). Since (1x)xn=1(1 - x)\sum x^n = 1:

nanxnA=(1x)n(AnA)xn.\sum_n a_nx^n - A = (1-x)\sum_{n} (A_n - A)x^n .

Given ε\varepsilon, choose NN with AnAε\abs{A_n - A} \leq \varepsilon for n>Nn > N; then

anxnA(1x)nNAnA+ε(1x)n>Nxn(1x)CN+ε,\Bigl|\sum a_nx^n - A\Bigr| \leq (1-x)\sum_{n \leq N}\abs{A_n - A} + \varepsilon(1 - x)\sum_{n > N}x^n \leq (1-x)\,C_N + \varepsilon ,

and letting x1x \to 1^-: limsup ε\leq \varepsilon for all ε\varepsilon. Hence the radial limit is AA.

Applications: (1)n1n\sum \frac{(-1)^{n-1}}{n} converges (alternating), and for x<1x < 1 its power series sums to ln(1+x)\ln(1 + x): by Abel, the sum is ln2\ln 2. Likewise (1)n2n+1x2n+1=arctanx\sum\frac{(-1)^n}{2n+1}x^{2n+1} = \arctan x gives π4\frac\pi4 at x=1x = 1 — the Year 1 integral proofs, now structural.

Exercise 11.10

Show that n1xnn(n+1)=1+1xxln(1x)\displaystyle\sum_{n\geq1}\frac{x^n}{n(n+1)} = 1 + \frac{1-x}{x}\,\ln(1-x) for 0<x<10 < \abs x < 1, determine the radius, and check that the convergence is normal on [1,1]\intcc{-1}{1}; verify that the value at x=1x = 1 predicted by continuity agrees with the telescoping sum 1n(n+1)=1\sum \frac{1}{n(n+1)} = 1.

Solution

Solution of Exercise 11.10.

Both xnn\sum\frac{x^n}{n} and xnn+1\sum\frac{x^n}{n+1} have radius 11, and 1n(n+1)=1n1n+1\frac{1}{n(n+1)} = \frac1n - \frac1{n+1}, so for 0<x<10 < \abs x < 1:

n1xnn(n+1)=ln(1x)1xn1xn+1n+1=ln(1x)ln(1x)xx=1+1xxln(1x).\sum_{n\geq1}\frac{x^n}{n(n+1)} = -\ln(1-x) - \frac1x\sum_{n\geq1}\frac{x^{n+1}}{n+1} = -\ln(1-x) - \frac{-\ln(1-x) - x}{x} = 1 + \frac{1-x}{x}\ln(1-x) .

Radius 11; and xn/(n(n+1)),[1,1]=1n(n+1)\norm{x^n/(n(n+1))}_{\infty,\intcc{-1}1} = \frac{1}{n(n+1)} is summable: normal convergence on [1,1]\intcc{-1}{1}, so the sum is continuous there. As x1x \to 1^-, (1x)ln(1x)0(1-x)\ln(1-x) \to 0 and the closed form tends to 11 — in agreement with the telescoping value 1n(n+1)=limN(11N+1)=1\sum\frac{1}{n(n+1)} = \lim_N\bigl(1 - \frac{1}{N+1}\bigr) = 1 at x=1x = 1.

Exercise 11.11 ★★

(Derangements) Let DnD_n be the number of permutations of nn objects without fixed point (D0=1D_0 = 1). Sorting the permutations of {1,,n}\{1, \dots, n\} by their fixed-point set gives n!=k=0n(nk)Dnkn! = \sum_{k=0}^{n}\binom nk D_{n-k}. Multiply by xnn!\frac{x^n}{n!}, sum, and recognize a Cauchy product to obtain the exponential generating function

n0Dnxnn!=ex1x(x<1),\sum_{n\geq0} D_n\,\frac{x^n}{n!} = \frac{\eu^{-x}}{1-x} \qquad (\abs x < 1),

then read off the closed form Dnn!=k=0n(1)kk!\dfrac{D_n}{n!} = \sum_{k=0}^{n}\dfrac{(-1)^k}{k!} and the limit Dnn!e1\dfrac{D_n}{n!} \to \eu^{-1}.

Solution

Solution of Exercise 11.11.

Sorting the n!n! permutations by their fixed-point set: choosing the kk fixed points ((nk)\binom nk ways) and deranging the other nkn - k objects gives n!=k=0n(nk)Dnkn! = \sum_{k=0}^n\binom nk D_{n-k}. Dividing by n!n!:

1=k=0n1k!Dnk(nk)!,1 = \sum_{k=0}^{n}\frac{1}{k!}\cdot\frac{D_{n-k}}{(n-k)!} ,

which says exactly that the Cauchy product of ex=xkk!\eu^x = \sum\frac{x^k}{k!} and D(x)=Dnxnn!D(x) = \sum D_n\frac{x^n}{n!} is xn=11x\sum x^n = \frac{1}{1-x}. Both factors converge absolutely for x<1\abs x < 1 (Dnn!D_n \leq n!, so DD is dominated by the geometric series): the product identity is legitimate (Proposition 11.4), and

D(x)=ex1x.D(x) = \frac{\eu^{-x}}{1-x} .

Cauchy product of ex=(1)kxkk!\eu^{-x} = \sum\frac{(-1)^kx^k}{k!} and xm\sum x^m: the coefficient of xnx^n is k=0n(1)kk!\sum_{k=0}^{n}\frac{(-1)^k}{k!}, and by uniqueness of power series coefficients (Theorem 11.7):

Dnn!=k=0n(1)kk!ne1:\frac{D_n}{n!} = \sum_{k=0}^{n}\frac{(-1)^k}{k!} \xrightarrow[n\to\infty]{} \eu^{-1} :

about 37%37\% of all permutations are derangements, whatever nn.

Exercise 11.12 ★★★

Prove, with the binomial series of Method 11.17, that

114x=n0(2nn)xn(x<14),\frac{1}{\sqrt{1 - 4x}} = \sum_{n\geq0}\binom{2n}{n}x^n \qquad \Bigl(\abs x < \frac14\Bigr),

and deduce, by squaring (Cauchy product against 114x=4nxn\frac{1}{1-4x} = \sum 4^nx^n), the convolution identity

k=0n(2kk)(2n2knk)=4n.\sum_{k=0}^{n}\binom{2k}{k}\binom{2n-2k}{n-k} = 4^n .
Solution

Solution of Exercise 11.12.

Binomial series with α=12\alpha = -\frac12 at 4x-4x:

(1/2n)(4)n=(12)(32)(2n12)n!(4)n=13(2n1)2nn!4n=(2n)!2nn!2nn!=(2nn),\binom{-1/2}{n}(-4)^n = \frac{\bigl(-\frac12\bigr)\bigl(-\frac32\bigr)\cdots \bigl(-\frac{2n-1}2\bigr)}{n!}(-4)^n = \frac{1\cdot3\cdots(2n-1)}{2^n\,n!}\,4^n = \frac{(2n)!}{2^n n!}\cdot\frac{2^n}{n!} = \binom{2n}{n},

using 13(2n1)=(2n)!2nn!1\cdot3\cdots(2n-1) = \frac{(2n)!}{2^nn!}. Hence (14x)1/2=(2nn)xn(1-4x)^{-1/2} = \sum\binom{2n}nx^n for 4x<1\abs{4x} < 1. Squaring (Cauchy product, legitimate by absolute convergence) and comparing with 114x=4nxn\frac{1}{1-4x} = \sum 4^nx^n: the coefficient of xnx^n in the square is k=0n(2kk)(2n2knk)\sum_{k=0}^n\binom{2k}k\binom{2n-2k}{n-k}, and uniqueness of coefficients gives

k=0n(2kk)(2n2knk)=4n.\sum_{k=0}^{n}\binom{2k}{k}\binom{2n-2k}{n-k} = 4^n .

11.5 Problem: Abel, Tauber, and the boundary of convergence

Problem 11.1

Inside the disk of convergence everything is easy; all the drama of power series happens on the boundary. This problem builds the boundary theory in the real variable: Abel’s theorem in its uniform form, its converse under Tauber’s condition, the Cesàro–Abel hierarchy of summation methods (with Frobenius’ theorem), term-by-term integration up to the boundary with classical constants as dividends, and finally the rigidity of analytic functions — the identity theorem. Throughout, (an)(a_n) is a real sequence, f(x)=n0anxnf(x) = \sum_{n\geq0} a_nx^n, and An=a0++anA_n = a_0 + \dots + a_n.

Part I — Abel’s theorem, uniformly. Assume in this part that an\sum a_n converges, and set rn=knakr_n = \sum_{k\geq n} a_k (so rn0r_n \to 0 and an=rnrn+1a_n = r_n - r_{n+1}).

  1. Prove, by summation by parts, that for all 0x10 \leq x \leq 1 and NMN \leq M:

    n=NManxn2supnNrn.\Bigl|\sum_{n=N}^{M} a_n x^n\Bigr| \leq 2\sup_{n \geq N}\,\abs{r_n} .
  2. Deduce that anxn\sum a_nx^n converges uniformly on [0,1]\intcc{0}{1}, that its sum is continuous there, and recover the radial limit of Exercise 11.9: f(x)anf(x) \to \sum a_n as x1x \to 1^-.
  3. (Abel’s theorem for Cauchy products) Let an=A\sum a_n = A, bn=B\sum b_n = B and suppose the Cauchy product cn\sum c_n, cn=kakbnkc_n = \sum_{k} a_kb_{n-k}, converges, with sum CC. Prove C=ABC = AB (inside the disk the product identity holds by Proposition 11.4; let x1x \to 1^-).
  4. Show the hypothesis matters: for an=bn=(1)nn+1a_n = b_n = \frac{(-1)^n}{\sqrt{n+1}}, both series converge, yet cn2(n+1)n+21\abs{c_n} \geq \frac{2(n+1)}{n+2} \geq 1 (bound each factor (k+1)(nk+1)\sqrt{(k+1)(n-k+1)} by AM–GM): the Cauchy product of two convergent series may diverge.
  5. (A dividend of Exercise 11.5) Show that (ln(1x))2=2n1Hnn+1xn+1\bigl(\ln(1-x)\bigr)^2 = 2\sum_{n\geq1} \frac{H_n}{n+1}x^{n+1} on (1,1)\intoo{-1}{1}, check that (Hnn+1)n1\bigl(\frac{H_n}{n+1}\bigr)_{n\geq1} decreases to 00, and conclude with Abel:

    n1(1)n+1Hnn+1=(ln2)22.\sum_{n\geq1} (-1)^{n+1}\,\frac{H_n}{n+1} = \frac{(\ln 2)^2}{2} .

Part II — Tauber’s converse. Call an\sum a_n Abel-summable to LL when f(x)Lf(x) \to L as x1x \to 1^-.

  1. Show that (1)n\sum (-1)^n is Abel-summable to 12\frac12 yet divergent: Abel’s theorem has no unconditional converse.
  2. (Cesàro lemma) If un0u_n \to 0 then u1++uNN0\frac{u_1 + \dots + u_N}{N} \to 0 (split the sum at a fixed mm).
  3. Assume now nan0n\,a_n \to 0 and f(x)Lf(x) \to L. With xN=11Nx_N = 1 - \frac1N, prove the two estimates

    n=0Nan(1xNn)1Nn=1Nnan,n>NanxNnsupn>N(nan)\Bigl|\sum_{n=0}^{N} a_n\bigl(1 - x_N^n\bigr)\Bigr| \leq \frac{1}{N}\sum_{n=1}^{N} n\,\abs{a_n}, \qquad \Bigl|\sum_{n>N} a_n x_N^n\Bigr| \leq \sup_{n>N}\bigl(n\abs{a_n}\bigr)

    (for the first, 1xnn(1x)1 - x^n \leq n(1-x); for the second, an1Nsupm>Nmam\abs{a_n} \leq \frac{1}{N}\sup_{m>N} m\abs{a_m} and xNnN\sum x_N^n \leq N).

  4. Conclude Tauber’s theorem: if nan0n\,a_n \to 0 and an\sum a_n is Abel-summable to LL, then an\sum a_n converges to LL.
  5. (The easy Tauberian for positive coefficients) If an0a_n \geq 0 and ff is bounded on [0,1)\intco{0}{1}, show that an\sum a_n converges and an=limx1f(x)\sum a_n = \lim_{x\to1^-} f(x) (bound nNanxnf(x)\sum_{n\leq N}a_nx^n \leq f(x) and let x1x \to 1^-, then use Abel).

Part III — Cesàro means and Frobenius’ theorem. Call an\sum a_n Cesàro-summable to LL when σN=A0++AN1NL\sigma_N = \frac{A_0 + \dots + A_{N-1}}{N} \to L.

  1. Show that a convergent series is Cesàro-summable to its sum (question 7 applied to AnLA_n - L).
  2. Compute the Cesàro value of (1)n\sum(-1)^n and check it agrees with the Abel value 12\frac12 of question 6.
  3. With Sn=A0++An=(n+1)σn+1S_n = A_0 + \dots + A_n = (n+1)\,\sigma_{n+1}, prove the two identities, for 0x<10 \leq x < 1:

    f(x)=(1x)2n0(n+1)σn+1xn,(1x)2n0(n+1)xn=1.f(x) = (1-x)^2\sum_{n\geq0}(n+1)\,\sigma_{n+1}x^n, \qquad (1-x)^2\sum_{n\geq0}(n+1)x^n = 1 .
  4. (Frobenius) Deduce: if σNL\sigma_N \to L then f(x)Lf(x) \to L as x1x \to 1^- — Cesàro-summable implies Abel-summable, to the same value (subtract the two identities and split the sum at a large NN, as in Exercise 11.9).
  5. Show that the hierarchy

    convergent    Cesaˋro-summable    Abel-summable\text{convergent} \;\Longrightarrow\; \text{Ces\`aro-summable} \;\Longrightarrow\; \text{Abel-summable}

    is strict at both arrows: question 6 for the first; for the second, show that (1)n(n+1)\sum(-1)^n(n+1) is Abel-summable to 14\frac14 (compute ff) but not Cesàro-summable (compute σN\sigma_N separately for even and odd NN).

Part IV — Integrating to the boundary.

  1. Suppose anxn\sum a_nx^n converges on [0,1)\intco{0}{1} and ann+1\sum \frac{a_n}{n+1} converges. Prove that the improper integral 01f\int_0^1 f exists and

    01(n0anxn) ⁣dx=n0ann+1\int_0^1 \Bigl(\sum_{n\geq0} a_nx^n\Bigr)\dd x = \sum_{n\geq0}\frac{a_n}{n+1}

    (the primitive F(x)=ann+1xn+1F(x) = \sum\frac{a_n}{n+1}x^{n+1} is continuous at 11 by Part I).

  2. Let η=n1(1)n1n2\eta = \sum_{n\geq1}\frac{(-1)^{n-1}}{n^2}. Show 01ln(1+x)x ⁣dx=η\int_0^1 \frac{\ln(1+x)}{x}\dd x = \eta and, by splitting even and odd indices in the absolutely convergent 1n2\sum \frac1{n^2}, that η=12n11n2\eta = \frac12\sum_{n\geq1}\frac{1}{n^2}. (The Fourier chapter’s weekend problem evaluates 1n2=π26\sum\frac1{n^2} = \frac{\pi^2}{6}.)
  3. Prove

    n0(1)n3n+1=01 ⁣dx1+x3=13(ln2+π3)\sum_{n\geq0}\frac{(-1)^n}{3n+1} = \int_0^1\frac{\dd x}{1+x^3} = \frac13\Bigl(\ln 2 + \frac{\pi}{\sqrt3}\Bigr)

    (the series converges by Leibniz; integrate the geometric series (1)nx3n\sum(-1)^nx^{3n} with question 16; then partial fractions: 11+x3=1/31+x+(2x)/3x2x+1\frac{1}{1+x^3} = \frac{1/3}{1+x} + \frac{(2-x)/3}{x^2-x+1}).

  4. From the binomial series for (1t)1/2(1-t)^{-1/2} (Exercise 11.12) derive

    arcsinx=n0(2nn)4n(2n+1)x2n+1(x<1),thenn0(2nn)4n(2n+1)=π2,\arcsin x = \sum_{n\geq0} \frac{\binom{2n}{n}}{4^n(2n+1)}\,x^{2n+1} \quad(\abs x < 1), \qquad\text{then}\qquad \sum_{n\geq0}\frac{\binom{2n}{n}}{4^n(2n+1)} = \frac\pi2 ,

    justifying the boundary value by normal convergence on [1,1]\intcc{-1}{1} (use (2nn)4n1πn\binom{2n}n4^{-n} \sim \frac{1}{\sqrt{\pi n}}, Example 6.14) — here not even Abel is needed.

  5. (Catalan at the boundary) Show that Cn4n=2\sum C_n 4^{-n} = 2: the Catalan series of Example 11.21 converges at its radius 14\frac14 (asymptotics of Exercise 11.8), its sum is continuous on [0,14]\intcc{0}{\frac14}, and the closed form has limit 22 there.

Part V — Rigidity: the identity theorem.

  1. (Isolated zeros) Let f=anxnf = \sum a_nx^n have radius R>0R > 0 and not all an=0a_n = 0; let mm be the smallest index with am0a_m \neq 0. Show f(x)=xmg(x)f(x) = x^m g(x) with gg a power series of radius RR, g(0)=am0g(0) = a_m \neq 0, and deduce that ff has no zero in some punctured neighborhood of 00.
  2. (Identity theorem) Let f,hf, h be sums of power series near 00 and (xk)(x_k) a sequence of nonzero points with xk0x_k \to 0 and f(xk)=h(xk)f(x_k) = h(x_k). Prove that ff and hh have the same coefficients, hence coincide near 00.
  3. Find all functions ff analytic near 00 with

    f(1k)=k2k2+1for all large integers k.f\Bigl(\frac1k\Bigr) = \frac{k^2}{k^2+1} \qquad\text{for all large integers } k .
  4. Show that a function analytic on an open interval II which vanishes on a subinterval vanishes identically on II (the set of points around which ff vanishes identically is open and, by the identity theorem applied at accumulation points, closed in II). Conclude that no nonzero analytic function on R\R has compact support — whereas CC^\infty bump functions exist (Exercise 11.7 supplies the building block): analyticity is rigid, smoothness is flabby.
  5. Synthesis. In one sentence each: (i) what Abel’s theorem adds to the normal-convergence package of Lemma 11.1; (ii) the exact hypotheses under which the converse holds (Tauber) and the intermediate rung (Frobenius); (iii) one boundary constant from Part IV you could now derive for a friend in two lines; (iv) where Cesàro means will reappear in this book, for series of a very different kind.
Solution

Solution of Problem 11.1.

1. With an=rnrn+1a_n = r_n - r_{n+1}, summation by parts:

n=NManxn=rNxN+n=N+1Mrn(xnxn1)rM+1xM.\sum_{n=N}^{M} a_nx^n = r_Nx^N + \sum_{n=N+1}^{M} r_n\bigl(x^n - x^{n-1}\bigr) - r_{M+1}x^M .

For 0x10 \leq x \leq 1 the increments xn1xnx^{n-1} - x^n are nonnegative and telescope to xNxMx^N - x^M; with s=supnNrns = \sup_{n\geq N}\abs{r_n}:

n=NManxns(xN+(xNxM)+xM)=2sxN2s.\Bigl|\sum_{n=N}^{M}a_nx^n\Bigr| \leq s\bigl(x^N + (x^N - x^M) + x^M\bigr) = 2s\,x^N \leq 2s .

2. Since rn0r_n \to 0, supnNrn0\sup_{n\geq N}\abs{r_n} \to 0: question 1 is exactly the uniform Cauchy criterion on [0,1]\intcc{0}{1}, so anxn\sum a_nx^n converges uniformly there and its sum is continuous (Theorem 10.11). The value at 11 being an\sum a_n, continuity at 11 is the radial limit of Exercise 11.9.

3. For x<1\abs x < 1 all three power series converge absolutely and (anxn)(bnxn)=cnxn\bigl(\sum a_nx^n\bigr)\bigl(\sum b_nx^n\bigr) = \sum c_nx^n (Proposition 11.4). By question 2 each factor and the product side are continuous on [0,1]\intcc{0}{1} (their coefficient series converge by hypothesis); letting x1x \to 1^- in the identity: AB=CAB = C.

4. Here

cn=k=0n1(k+1)(nk+1)k=0n2n+2=2(n+1)n+21,\abs{c_n} = \sum_{k=0}^{n} \frac{1}{\sqrt{(k+1)(n-k+1)}} \geq \sum_{k=0}^{n}\frac{2}{n+2} = \frac{2(n+1)}{n+2} \geq 1,

by AM–GM: (k+1)(nk+1)(k+1)+(nk+1)2=n+22\sqrt{(k+1)(n-k+1)} \leq \frac{(k+1) + (n-k+1)}{2} = \frac{n+2}{2}. The general term of cn\sum c_n does not tend to 00: the Cauchy product diverges, although both factors converge (alternating series).

5. Exercise 11.5 gives ln(1x)1x=Hnxn\frac{-\ln(1-x)}{1-x} = \sum H_nx^n (x<1\abs x < 1). Term-by-term primitives (Theorem 11.7 (2)), both sides vanishing at 00:

(ln(1x))22=n1Hnn+1xn+1.\frac{\bigl(\ln(1-x)\bigr)^2}{2} = \sum_{n\geq1}\frac{H_n}{n+1}\,x^{n+1} .

Decrease: (n+2)Hn(n+1)Hn+1(n+2)H_n \geq (n+1)H_{n+1} amounts to Hn1H_n \geq 1, true for n1n \geq 1; and Hnn+1lnnn0\frac{H_n}{n+1} \sim \frac{\ln n}{n} \to 0: at x=1x = -1 the series converges by the alternating test. Substituting xxx \mapsto -x and applying question 2 at x=1x = 1:

(ln2)22=n1Hnn+1(1)n+1,\frac{(\ln 2)^2}{2} = \sum_{n\geq1}\frac{H_n}{n+1}(-1)^{n+1},

the announced value.

6. f(x)=(1)nxn=11+x12f(x) = \sum(-1)^nx^n = \frac{1}{1+x} \to \frac12 as x1x \to 1^-: Abel-summable to 12\frac12. But the partial sums are 1,0,1,0,1, 0, 1, 0, \dots: divergent.

7. Given ε>0\varepsilon > 0 choose mm with unε\abs{u_n} \leq \varepsilon for n>mn > m; for NmN \geq m:

u1++uNNu1++umN+εNmNCmN+ε,\Bigl|\frac{u_1 + \dots + u_N}{N}\Bigr| \leq \frac{\abs{u_1} + \dots + \abs{u_m}}{N} + \varepsilon\,\frac{N - m}{N} \leq \frac{C_m}{N} + \varepsilon,

so lim supε\limsup \leq \varepsilon for every ε\varepsilon: the means tend to 00.

8. For 0x10 \leq x \leq 1: 1xn=(1x)(1+x++xn1)n(1x)1 - x^n = (1-x)(1 + x + \dots + x^{n-1}) \leq n(1-x), so

n=0Nan(1xNn)(1xN)n=1Nnan=1Nn=1Nnan.\Bigl|\sum_{n=0}^N a_n(1 - x_N^n)\Bigr| \leq (1 - x_N)\sum_{n=1}^N n\abs{a_n} = \frac1N\sum_{n=1}^{N}n\abs{a_n} .

For n>Nn > N: an=nann1Nsupm>Nmam\abs{a_n} = \frac{n\abs{a_n}}{n} \leq \frac{1}{N}\sup_{m>N}m\abs{a_m}, and n>NxNn11xN=N\sum_{n>N}x_N^n \leq \frac{1}{1 - x_N} = N:

n>NanxNnsupm>NmamNN=supm>Nmam.\Bigl|\sum_{n>N}a_nx_N^n\Bigr| \leq \frac{\sup_{m>N}m\abs{a_m}}{N}\cdot N = \sup_{m>N}\,m\abs{a_m} .

9. Decompose

ANL=n=0Nan(1xNn)n>NanxNn+(f(xN)L).A_N - L = \sum_{n=0}^{N}a_n\bigl(1 - x_N^n\bigr) - \sum_{n>N}a_nx_N^n + \bigl(f(x_N) - L\bigr) .

The first term tends to 00 by question 7 (the means of nan0n\abs{a_n} \to 0), the second by question 8 (the sup tends to 00), the third because xN1x_N \to 1^- and f(x)Lf(x) \to L. Hence ANLA_N \to L: Tauber’s theorem.

10. For x[0,1)x \in \intco{0}{1} and any NN: nNanxnf(x)M\sum_{n\leq N}a_nx^n \leq f(x) \leq M (nonnegative terms). Let x1x \to 1^- in the finite sum: nNanM\sum_{n\leq N}a_n \leq M. The partial sums are increasing and bounded: an\sum a_n converges, and then question 2 gives limx1f(x)=an\lim_{x\to1^-}f(x) = \sum a_n.

11. σNL\sigma_N - L is the mean of the NN numbers AnLA_n - L (0n<N0 \leq n < N), which tend to 00: question 7.

12. An=1A_n = 1 for even nn, 00 for odd: A0++AN1=N/2A_0 + \dots + A_{N-1} = \lceil N/2\rceil, so σN=N/2N12\sigma_N = \frac{\lceil N/2\rceil}{N} \to \frac12, the Abel value of question 6.

13. Under σNL\sigma_N \to L one has Sn=O(n)S_n = O(n), hence An=SnSn1=O(n)A_n = S_n - S_{n-1} = O(n) and an=O(n)a_n = O(n): all the series below have radius 1\geq 1. For x<1\abs x < 1, from an=AnAn1a_n = A_n - A_{n-1} and Anxn0A_nx^n \to 0:

(1x)nAnxn=nAnxnnAnxn+1=nanxn=f(x),(1-x)\sum_n A_nx^n = \sum_n A_nx^n - \sum_n A_nx^{n+1} = \sum_n a_nx^n = f(x),

and identically (1x)Snxn=Anxn(1-x)\sum S_nx^n = \sum A_nx^n, so f(x)=(1x)2nSnxn=(1x)2n(n+1)σn+1xnf(x) = (1-x)^2\sum_n S_nx^n = (1-x)^2\sum_n(n+1)\sigma_{n+1}x^n. Finally (n+1)xn=1(1x)2\sum(n+1)x^n = \frac{1}{(1-x)^2} (Exercise 11.3), which is the second identity.

14. Subtracting LL times the second identity from the first:

f(x)L=(1x)2n0(n+1)(σn+1L)xn.f(x) - L = (1-x)^2\sum_{n\geq0}(n+1) \bigl(\sigma_{n+1} - L\bigr)x^n .

Given ε\varepsilon, choose NN with σn+1Lε\abs{\sigma_{n+1} - L} \leq \varepsilon for nNn \geq N; then

f(x)L(1x)2CN+ε(1x)2n(n+1)xn=(1x)2CN+ε,\abs{f(x) - L} \leq (1-x)^2 C_N + \varepsilon(1-x)^2\sum_{n}(n+1)x^n = (1-x)^2C_N + \varepsilon ,

and letting x1x \to 1^-: lim supε\limsup \leq \varepsilon. Hence f(x)Lf(x) \to L: Frobenius’ theorem.

15. f(x)=(1)n(n+1)xn=1(1+x)2f(x) = \sum(-1)^n(n+1)x^n = \frac{1}{(1+x)^2} (differentiate the geometric series at x-x): Abel value 14\frac14. Partial sums: A2k=k+1A_{2k} = k+1, A2k+1=(k+1)A_{2k+1} = -(k+1) (immediate induction). Then S2m1=0S_{2m-1} = 0 (consecutive pairs cancel) and S2m=m+1S_{2m} = m + 1, so

σ2m=S2m12m=0,σ2m+1=m+12m+112:\sigma_{2m} = \frac{S_{2m-1}}{2m} = 0, \qquad \sigma_{2m+1} = \frac{m+1}{2m+1} \to \frac12 :

(σN)(\sigma_N) has two distinct cluster values: not Cesàro-summable. With questions 6 and 11–14, the hierarchy convergent \Rightarrow Cesàro \Rightarrow Abel is strict at both arrows.

16. The primitive series F(x)=ann+1xn+1F(x) = \sum\frac{a_n}{n+1}x^{n+1} has the same radius and F=fF' = f on [0,1)\intco{0}{1} (Theorem 11.7); since ann+1\sum\frac{a_n}{n+1} converges, Part I (question 2) makes FF continuous on [0,1]\intcc{0}{1}. As 0xf=F(x)\int_0^x f = F(x) (equal derivatives, equal value 00 at 00),

0xfx1F(1)=n0ann+1:\int_0^x f \xrightarrow[x\to1^-]{} F(1) = \sum_{n\geq0}\frac{a_n}{n+1} :

the improper integral exists with the stated value.

17. ln(1+x)x=n1(1)n1nxn1\frac{\ln(1+x)}{x} = \sum_{n\geq1}\frac{(-1)^{n-1}}{n}x^{n-1} (radius 11; continuous at 00). The series of amm+1\frac{a_m}{m+1} is n1(1)n1n2\sum_{n\geq1}\frac{(-1)^{n-1}}{n^2}, absolutely convergent: question 16 gives 01ln(1+x)x ⁣dx=η\int_0^1\frac{\ln(1+x)}{x}\dd x = \eta. In the absolutely convergent 1n2\sum\frac1{n^2}, regroup even and odd:

η=odd1n2even1n2=n1n22k1(2k)2=(112)n1n2=12n11n2.\eta = \sum_{\text{odd}}\frac1{n^2} - \sum_{\text{even}}\frac1{n^2} = \sum_{n}\frac1{n^2} - 2\sum_{k}\frac1{(2k)^2} = \Bigl(1 - \frac12\Bigr)\sum_n\frac1{n^2} = \frac12\sum_{n\geq1}\frac1{n^2} .

18. Leibniz: 13n+10\frac{1}{3n+1}\downarrow0, the series converges. On [0,1)\intco{0}{1}, (1)nx3n=11+x3\sum(-1)^nx^{3n} = \frac{1}{1+x^3}, and (1)n3n+1\sum\frac{(-1)^n}{3n+1} converges: question 16 gives (1)n3n+1=01 ⁣dx1+x3\sum\frac{(-1)^n}{3n+1} = \int_0^1\frac{\dd x}{1+x^3}. Partial fractions (check: 13(x2x+1)+2x3(1+x)=1\frac13(x^2-x+1) + \frac{2-x}{3}(1+x) = 1):

01 ⁣dx1+x3=13ln2+13012xx2x+1 ⁣dx.\int_0^1\frac{\dd x}{1+x^3} = \frac13\ln2 + \frac13\int_0^1\frac{2-x}{x^2-x+1}\dd x .

Writing 2x=12(2x1)+322 - x = -\frac12(2x-1) + \frac32: the ln(x2x+1)\ln(x^2-x+1) part vanishes at both ends, and

3201 ⁣dx(x12)2+34=3223[arctan2x13]01=3π3=π3.\frac32\int_0^1\frac{\dd x}{(x-\frac12)^2 + \frac34} = \frac32\cdot\frac{2}{\sqrt3} \Bigl[\arctan\frac{2x-1}{\sqrt3}\Bigr]_0^1 = \sqrt3\cdot\frac{\pi}{3} = \frac{\pi}{\sqrt3} .

Total: 13(ln2+π3)\frac13\bigl(\ln2 + \frac{\pi}{\sqrt3}\bigr).

19. Substituting t=x2t = x^2 in the series of Exercise 11.12 and integrating term by term (the primitive of (1x2)1/2(1-x^2)^{-1/2} vanishing at 00 is arcsin\arcsin):

arcsinx=n0(2nn)4n(2n+1)x2n+1(x<1).\arcsin x = \sum_{n\geq0} \frac{\binom{2n}n}{4^n(2n+1)}x^{2n+1} \qquad(\abs x < 1) .

The coefficients are 12πn3/2\sim \frac{1}{2\sqrt\pi\,n^{3/2}} (Example 6.14), summable: the series converges normally on [1,1]\intcc{-1}{1}, its sum is continuous there, and coincides with the continuous arcsin\arcsin on (1,1)\intoo{-1}{1}, hence at x=1x = 1 too:

n0(2nn)4n(2n+1)=arcsin1=π2.\sum_{n\geq0}\frac{\binom{2n}n}{4^n(2n+1)} = \arcsin 1 = \frac\pi2 .

20. Cn4n1πn3/2C_n4^{-n} \sim \frac{1}{\sqrt\pi\,n^{3/2}} (Exercise 11.8): normal convergence of Cnxn\sum C_nx^n on [0,14]\intcc{0}{\frac14}, so its sum is continuous there; on (0,14)\intoo{0}{\frac14} it equals 114x2x\frac{1-\sqrt{1-4x}}{2x} (Example 11.21), whose limit at 14\frac14^- is 101/2=2\frac{1-0}{1/2} = 2. Hence n0Cn4n=2\sum_{n\geq0} C_n4^{-n} = 2.

21. f(x)=nmanxn=xmg(x)f(x) = \sum_{n\geq m}a_nx^n = x^m g(x) with g(x)=k0am+kxkg(x) = \sum_{k\geq0}a_{m+k}x^k; if (anrn)(a_nr^n) is bounded then (am+krk)(a_{m+k}r^k) is too (divide by rmr^m): gg has radius R\geq R. gg is continuous with g(0)=am0g(0) = a_m \neq 0, so g0g \neq 0 on some [δ,δ]\intcc{-\delta}{\delta}, and f(x)=xmg(x)0f(x) = x^mg(x) \neq 0 for 0<xδ0 < \abs x \leq \delta.

22. d=fhd = f - h is the sum of a power series near 00 vanishing at the nonzero points xk0x_k \to 0. If some coefficient of dd were nonzero, question 21 would give a punctured neighborhood of 00 free of zeros of dd — contradicting d(xk)=0d(x_k) = 0. So all coefficients of dd vanish: ff and hh have equal coefficients and coincide near 00.

23. The function h(x)=11+x2=(1)nx2nh(x) = \frac{1}{1+x^2} = \sum(-1)^nx^{2n} (radius 11) satisfies h(1k)=11+1/k2=k2k2+1h(\frac1k) = \frac{1}{1 + 1/k^2} = \frac{k^2}{k^2+1}. Any analytic ff with the same values agrees with hh at the points 1k0\frac1k \to 0: by the identity theorem (question 22), f=11+x2f = \frac{1}{1+x^2} near 00 — the unique solution.

24. Let ZZ be the set of points of II having a neighborhood on which ff vanishes identically: open by definition, nonempty (the subinterval). Closed in II: if yIy \in I is a limit of points of ZZ, then yy is an accumulation point of zeros of ff; expanding ff in a power series at yy (analyticity) and applying questions 21–22 re-centered at yy, all coefficients at yy vanish, so f0f \equiv 0 near yy: yZy \in Z. An interval is connected, so Z=IZ = I: f0f \equiv 0 on II. In particular an analytic function on R\R vanishing outside a compact set vanishes on an interval, hence everywhere: no nonzero analytic bump. The CC^\infty world is different: gluing the flat function of Exercise 11.7 (e.g. xe1/x21x>0x \mapsto \eu^{-1/x^2}\mathbf 1_{x>0} and its mirror) produces smooth bumps with compact support.

25. (i) Normal convergence lives on compact subdisks strictly inside the disk; Abel’s theorem extends continuity to a boundary point, under the sole hypothesis that the coefficient series converges there. (ii) The converse holds under Tauber’s condition nan0na_n \to 0 (question 9), and Cesàro summability sits strictly between convergence and Abel summability (Frobenius, questions 14–15). (iii) For a friend: (1)n3n+1=01 ⁣dx1+x3\sum\frac{(-1)^n}{3n+1} = \int_0^1\frac{\dd x}{1+x^3} by integrating the geometric series to the boundary, then partial fractions. (iv) Cesàro means return in the Fourier chapter as Fejér’s theorem, where averaging the partial sums repairs the failure of pointwise convergence — same medicine, new patient.