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) is bounded for some z0=0, then ∑anzn converges absolutely for every ∣z∣<∣z0∣, and normally on every disk ∣z∣≤r<∣z0∣.
Proof. With ∣anz0n∣≤M and ∣z∣≤r:
∣anzn∣=∣anz0n∣z0zn≤M(∣z0∣r)n,
a convergent geometric bound, uniform on the disk. ∎
Definition 11.2(Radius of convergence)
The radius of convergence of ∑anzn is
R=sup{r≥0:(anrn) bounded}∈[0,+∞].
By Lemma 11.1: absolute convergence for ∣z∣<R (normal on compact subdisks), divergence — indeed unbounded terms — for ∣z∣>R. On the boundary circle, anything can happen (Exercise 11.2). In practice R is computed by d’Alembert’s ratio test on ∣an∣∣z∣n or by comparison.
Example 11.3(A radius with no ratio test)
What is the radius of ∑sin(n)zn? The ratio ∣sin(n+1)/sinn∣ has no limit, but the definition works directly. R≥1:∣sinn∣≤1, so (sinn⋅rn) is bounded for every r<1 — indeed for r=1. R≤1: it suffices that sinn→0. Suppose sinn→0; the addition formula
sin(n+1)=sinncos1+cosnsin1
would force cosn→0 (solve for cosn: sin1=0), contradicting sin2n+cos2n=1. So the terms sin(n)1n do not tend to 0: the series diverges at z=1, and R≤1. Conclusion: R=1. Closing insight: the radius is a statement about ∣an∣rn 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, ∑bnzn have radii Ra,Rb. Then, for ∣z∣<min(Ra,Rb):
both series having radius ≥min(Ra,Rb). (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 is bounded whenever both anrn and bnrn are: radius ≥min(Ra,Rb). For the product, fix ∣z∣<min(Ra,Rb): both series converge absolutely there (Lemma 11.1), so the doubly indexed family (akzkblzl)k,l is summable, and Theorem 7.14 allows any grouping. Grouping by k+l=n:
absolutely convergent for every such z: the product series has radius ≥min(Ra,Rb) as well. ∎
Example 11.5(A Cauchy square, cross-checked)
Square the geometric series: for ∣x∣<1, the coefficient of xn in (∑xk)2 is cn=∑k+l=n1⋅1=n+1, so
(1−x)21=n≥0∑(n+1)xn.
Cross-check by term-by-term differentiation (Theorem 11.7 below): differentiating 1−x1=∑xn gives (1−x)21=∑nxn−1=∑(n+1)xn — 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 ∑(k2k)(n−k2n−2k)=4n runs the convolution engine at full power.
Example 11.6(Multiplying by 1−x1 sums the coefficients)
A Cauchy product against the geometric series has a memorable meaning: for any ∑anxn of radius R>0 and ∣x∣<min(R,1),
1−x1n≥0∑anxn=n≥0∑(k=0∑nak)xn:
multiplication by 1−x1 replaces coefficients by their partial sums (convolve with the all-ones sequence). Instance: 1−xex=∑nsnxn with sn=∑k≤nk!1, the partial sums of e — compare Exercise 11.11, where the same product with e−x encodes the derangement counts. Closing insight: operations on power series are operations on coefficient sequences in disguise (multiply by 1−x1: sum; multiply by x: shift; differentiate: multiply by n 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)=∑n≥0anxn have radius R>0 (real variable x∈(−R,R)).
The derived series ∑nanxn−1 has the same radius R, and f is C1 with f′(x)=∑n≥1nanxn−1. Iterating, f is C∞ and
an=n!f(n)(0):
the coefficients of a power series are unique (two series with the same sum near 0 have equal coefficients).
Term-by-term primitive: ∑n+1anxn+1 has radius R and derivative f.
Proof.Same radius: if (anrn) is bounded and r′<r, then n∣an∣r′n−1=r′n∣anrn∣(rr′)n is bounded (indeed →0: geometric beats n), so R′≥R; conversely ∣anxn∣≤∣x∣⋅n∣an∣∣x∣n−1 gives R≥R′.
Differentiation: on [−r,r], r<R, the derived series converges normally (n∣an∣rn−1summable by the radius computation); the original converges at x=0: the differentiation theorem for series (Theorem 10.11) applies on every such segment, hence on (−R,R). Iterating k times and evaluating at 0: explicitly, the k-th derived series is
f(k)(x)=n≥k∑n(n−1)⋯(n−k+1)anxn−k,
and at x=0 every term with n>k vanishes, leaving only the constant term k(k−1)⋯1⋅ak: f(k)(0)=k!ak. Uniqueness of coefficients follows: two power series with the same sum near 0 have the same derivatives at 0, hence the same ak. Primitives: same radius by the same computation, and differentiate term by term back. ∎
Example 11.8(Evaluating a series at a point)
What is ∑n≥12nn2? It is the sum ∑n2xn of Exercise 11.3 evaluated inside the disk, at x=21<1=R, where every manipulation used to derive the closed form was legitimate:
Same engine, other dials: x=31 gives ∑3nn2=(2/3)331⋅34=23. Closing insight: a power-series identity is a machine, not a single formula — one derivation prices every numerical series ∑n2qn at once, for all ∣q∣<1; this is how the generating-functions chapter will compute expectations and variances wholesale.
Example 11.9(The classics, this time honestly)
1−x1=∑xn (R=1); integrating term by term (Theorem 11.7 (2)):
the second in two steps: substitute −x2 in the geometric series to get 1+x21=∑(−1)nx2n (radius 1, since x2<1⟺∣x∣<1), then take the term-by-term primitive vanishing at 0; both sides are primitives of the same function with the same value at 0, hence equal on (−1,1). And exp: the series E(x)=∑n!xn (R=∞) satisfies E′=E, E(0)=1 by termwise differentiation, so E=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(1−x)=∑nxn at the interior point x=21:
n≥1∑n2n1=ln2,
a fast-converging representation of ln2 (ten terms already give 0.69306… against ln2=0.69314…), far better than the alternating series 1−21+31−… 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 ∑n≥1n2xn has radius 1 and converges at both endpoints (∑n21 and its alternating twin). Its derived series,
n≥1∑nxn−1,
has the same radius 1 — as Theorem 11.7 guarantees — but now diverges at x=1 (harmonic series) while still converging at x=−1 (alternating). One more differentiation yields ∑n≥2nn−1xn−2, divergent at both ends (terms do not tend to 0). Closing insight: each differentiation multiplies the coefficients by n, 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)=∑n≥0(4n)!x4n in closed form. Both coshx=∑(2m)!x2m and cosx=∑(2m)!(−1)mx2m have radius ∞, so their average may be computed term by term:
The filter 21+(−1)m keeps exactly the even m: this is the real avatar of the roots-of-unity filter (the complex version, with in, extracts residues modulo 4 in one stroke). Closing check: f solves f′′′′=f with f(0)=1, f′(0)=f′′(0)=f′′′(0)=0 — differentiate the series four times (Theorem 11.7) and watch it reproduce itself; 2cosh+cos satisfies the same data.
Definition 11.13(Analytic functions)
f is analytic at x0 when it is the sum of a power series in (x−x0) 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=0 being Theorem 11.7). Analytic implies C∞; the converse fails: the flat function e−1/x2 (Exercise 11.7).
Example 11.14(Re-centering, and the radius as a distance)
Expand f(x)=1−x1 around x0=21: writing x=21+h,
valid for ∣2h∣<1, i.e. x−21<21. The new radius is exactly the distance from the new center to the singularity x=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∣ has no limit (Example 11.3, Exercise 11.1), go back to the definition: R=sup{r:(anrn) bounded}. (ii) Nothing crosses the boundary for free: term-by-term differentiation and integration are theorems inside the open disk; at ∣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) is only a lower bound — cancellations can enlarge it (an=1,bn=−1: sum identically 0, radius ∞). (iv) C∞ is not analytic: a convergent Taylor series may converge to the wrong function (Exercise 11.7); before writing f(x)=∑n!f(n)(0)xn, 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 (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 itself.
Method 11.17(Expanding via a differential equation)
To expand a function f in a power series: find a linear ODE with polynomial coefficients satisfied by f; inject ∑anxn; identify coefficients to get a recurrence for (an); solve, and check radius and initial conditions. Example — the binomial series: f(x)=(1+x)α satisfies (1+x)f′=αf, f(0)=1; injecting gives (n+1)an+1=(α−n)an, so an=(nα), radius 1 (ratio test), and the sum, satisfying the same ODE with the same initial value, equals (1+x)α by the uniqueness theorem for linear ODEs (Year 1 volume).
Example 11.18(The method on a forced equation)
Solve y′=y+x, y(0)=0, by power series. Injecting y=∑anxn:
n≥0∑(n+1)an+1xn=n≥0∑anxn+x,
and identifying coefficients: a1=a0=0, 2a2=a1+1=1, and (n+1)an+1=an for n≥2. So a2=2!1 and, by induction, an=n!1 for every n≥2: radius ∞, and
y(x)=n≥2∑n!xn=ex−1−x.
Check: y′=ex−1=y+x and y(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)=∑n≥0Fnxn (Fibonacci numbers, F0=0, F1=1). The recurrence Fn+2=Fn+1+Fn translates, multiplying by xn+2 and summing, into
F(x)−x=xF(x)+x2F(x)⟹F(x)=1−x−x2x,
valid where the series converges. The radius is φ1: from Fn∼5φn (Binet, next example — or the crude induction Fn≤2n plus the recurrence), the ratio test gives
Partial fractions on 1−x−x2x and the geometric series re-derive Binet’s formula — generating functions industrialize linear recurrences.
Example 11.20(Binet’s formula, carried out)
Let φ=21+5 and ψ=21−5, the roots of X2=X+1; since φ+ψ=1 and φψ=−1,
1−x−x2=(1−φx)(1−ψx).
Partial fractions: seeking (1−φx)(1−ψx)x=1−φxA+1−ψxB, the constant term gives A+B=0 and the x-coefficient −Aψ−Bφ=1, so A(φ−ψ)=1: A=51=−B. Two geometric series later,
F(x)=51n≥0∑(φn−ψn)xn⟹Fn=5φn−ψn
by uniqueness of coefficients (Theorem 11.7). Since ∣ψ∣<1, the term 5ψn has absolute value <21: Fn is the nearest integer to 5φn. Closing insight: the radius φ1 of F is the reciprocal of the dominant root — growth of coefficients and radius of convergence are the same information read in opposite directions.
choosing the root with C(0)=1: solving the quadratic xC2−C+1=0 gives the two candidates 2x1±1−4x, and as x→0 the “+” root blows up like x1 while the “−” root tends to 1 (expand 1−4x=1−2x+O(x2)) — only the minus sign can carry a power series with C0=1. Expanding 1−4x by the binomial series gives the closed form
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” Fn or Cn, one must know R>0. A crude a priori bound suffices — Fn≤2n (immediate induction) gives R≥21 for Fibonacci; Cn≤4n (each Catalan number counts subsets of paths) gives R≥41. Beware the degenerate end of the scale: ∑n!xn has radius 0, 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!), 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, 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: ∑2nn2zn; ∑(n2n)zn; ∑zn!; ∑(2+(−1)n)nzn.
Solution
Solution of Exercise 11.1.
∑2nn2zn: ratio 2n+1(n+1)2⋅n22n→21: R=2.
∑(n2n)zn: (n2n)∼πn4n (Example 6.14), so ∣an∣−1≈4n up to polynomial factors: R=4 (ratio test: (n+12n+2)(n2n)=(2n+1)(2n+2)(n+1)2→41).
∑zn!: coefficients ak=1 if k=n!, else 0. For ∣z∣<1, ∑∣z∣n! converges (dominated by geometric); for ∣z∣≥1 the terms do not tend to 0: R=1.
∑(2+(−1)n)nzn: coefficients 3n (even n) and 1 (odd n). Boundedness of anrn requires 3r≤1; and r<31 works: R=31.
Exercise 11.2★
Show that ∑zn, ∑nzn, ∑n2zn all have radius 1 but behave differently at z=1 and z=−1: divergence/divergence, divergence/convergence, convergence/convergence.
Solution
Solution of Exercise 11.2.
All three have radius 1 (ratio test). At z=1: ∑1 diverges; ∑n1 diverges; ∑n21 converges. At z=−1: ∑(−1)n diverges; ∑n(−1)n converges (alternating); ∑n2(−1)n converges (absolutely). Boundary behavior is invisible to the radius.
Exercise 11.3★
Compute the sums, for ∣x∣<1:
n≥0∑nxn,n≥0∑n2xn,n≥0∑2n+1x2n+1.
Solution
Solution of Exercise 11.3.
From 1−x1=∑xn, differentiate and multiply by x (Theorem 11.7):
ln(1+x+x2)=ln1−x1−x3=ln(1−x3)−ln(1−x)=∑n≥1nxn−∑m≥1mx3m: the coefficient of xn is n1 if 3∤n, and n1−n3=−n2 if 3∣n. Radius 1 (the nearest obstruction: the series for ln(1−x3)).
Exercise 11.5★★
Prove that f(x)=∑n≥1Hnxn=−1−xln(1−x) for ∣x∣<1, where Hn is the harmonic number (Cauchy product of ∑xn and ∑nxn).
Solution
Solution of Exercise 11.5.
Cauchy product of ∑m≥0xm (coefficients 1) and ∑k≥1kxk (coefficients k1, k≥1), both absolutely convergent for ∣x∣<1: the coefficient of xn in the product is ∑k=1nk1⋅1=Hn. Hence
(∑xm)(∑kxk)=1−x1⋅(−ln(1−x))=n≥1∑Hnxn.
Exercise 11.6★★
Solve by generating function the recurrence u0=1, un+1=2un+n: compute U(x)=∑unxn in closed form, decompose, and read off un=2n+1−n−1.
Solution
Solution of Exercise 11.6.
Multiply the recurrence by xn+1 and sum (∣x∣<21):
Partial fractions (cover-up at x=21 gives coefficient 2; at the double pole x=1, coefficient −1; the middle coefficient vanishes by evaluating at x=0):
U(x)=1−2x2−(1−x)21.
Expanding both:
un=2⋅2n−(n+1)=2n+1−n−1.
(Check: u0=1, u1=2u0+0=2=4−2.)
Exercise 11.7★★
Let f(x)=e−1/x2 for x=0, f(0)=0. Prove that f is C∞ on R with f(n)(0)=0 for all n(show by induction that f(n)(x)=Pn(x1)e−1/x2 for polynomials Pn, and use the growth comparison). Conclude that f is not analytic at 0: its Taylor series at 0 converges — to the wrong function.
Solution
Solution of Exercise 11.7.
Induction: f′(x)=x32e−1/x2, and if f(n)(x)=Pn(x1)e−1/x2 then
f(n+1)(x)=(−x21Pn′(x1)+x32Pn(x1))e−1/x2:
again of the stated form. At 0: difference quotients hf(n)(h)=h1Pn(h1)e−1/h2→0 as h→0, since Q(u)e−u2→0 as u→±∞ for any polynomial Q (exponential beats powers): by induction all f(n)(0) exist and vanish, and each f(n) is continuous at 0 by the same limit. So f∈C∞ with zero Taylor series at 0; the Taylor series sums to 0=f: not analytic at 0.
Exercise 11.8★★★
Complete Example 11.21: expand 1−4x with the binomial series, showing
(n+11/2)(−4)n+1=−n+12(n2n),
and deduce Cn=n+11(n2n); determine the radius of convergence of C(x) and the asymptotics of Cn via Stirling.
Solution
Solution of Exercise 11.8.
Binomial series: 1−4x=∑k≥0(k1/2)(−4x)k. For k=n+1≥1:
Cn=n+11(n2n). Radius: 41 (the binomial series in 4x). Asymptotics via Example 6.14:
Cn∼πn3/24n.
Exercise 11.9★★★
(Abel’s radial limit theorem, special case) Suppose ∑an converges. Prove that limx→1−∑nanxn=∑nan. (Abel summation: with An the partial sums and A=limAn, write ∑anxn=(1−x)∑Anxn; then ∑anxn−A=(1−x)∑(An−A)xn, split the sum at a large N.) Application: ∑n(−1)n−1=ln2 and ∑2n+1(−1)n=4π, re-proved from the power series.
and letting x→1−: limsup ≤ε for all ε. Hence the radial limit is A.
Applications: ∑n(−1)n−1 converges (alternating), and for x<1 its power series sums to ln(1+x): by Abel, the sum is ln2. Likewise ∑2n+1(−1)nx2n+1=arctanx gives 4π at x=1 — the Year 1 integral proofs, now structural.
Exercise 11.10★
Show that n≥1∑n(n+1)xn=1+x1−xln(1−x) for 0<∣x∣<1, determine the radius, and check that the convergence is normal on [−1,1]; verify that the value at x=1 predicted by continuity agrees with the telescoping sum ∑n(n+1)1=1.
Solution
Solution of Exercise 11.10.
Both ∑nxn and ∑n+1xn have radius 1, and n(n+1)1=n1−n+11, so for 0<∣x∣<1:
Radius 1; and ∥xn/(n(n+1))∥∞,[−1,1]=n(n+1)1 is summable: normal convergence on [−1,1], so the sum is continuous there. As x→1−, (1−x)ln(1−x)→0 and the closed form tends to 1 — in agreement with the telescoping value ∑n(n+1)1=limN(1−N+11)=1 at x=1.
Exercise 11.11★★
(Derangements) Let Dn be the number of permutations of n objects without fixed point (D0=1). Sorting the permutations of {1,…,n} by their fixed-point set gives n!=∑k=0n(kn)Dn−k. Multiply by n!xn, sum, and recognize a Cauchy product to obtain the exponential generating function
n≥0∑Dnn!xn=1−xe−x(∣x∣<1),
then read off the closed form n!Dn=∑k=0nk!(−1)k and the limit n!Dn→e−1.
Solution
Solution of Exercise 11.11.
Sorting the n! permutations by their fixed-point set: choosing the k fixed points ((kn) ways) and deranging the other n−k objects gives n!=∑k=0n(kn)Dn−k. Dividing by n!:
1=k=0∑nk!1⋅(n−k)!Dn−k,
which says exactly that the Cauchy product of ex=∑k!xk and D(x)=∑Dnn!xn is ∑xn=1−x1. Both factors converge absolutely for ∣x∣<1 (Dn≤n!, so D is dominated by the geometric series): the product identity is legitimate (Proposition 11.4), and
D(x)=1−xe−x.
Cauchy product of e−x=∑k!(−1)kxk and ∑xm: the coefficient of xn is ∑k=0nk!(−1)k, and by uniqueness of power series coefficients (Theorem 11.7):
n!Dn=k=0∑nk!(−1)kn→∞e−1:
about 37% of all permutations are derangements, whatever n.
Exercise 11.12★★★
Prove, with the binomial series of Method 11.17, that
1−4x1=n≥0∑(n2n)xn(∣x∣<41),
and deduce, by squaring (Cauchy product against 1−4x1=∑4nxn), the convolution identity
using 1⋅3⋯(2n−1)=2nn!(2n)!. Hence (1−4x)−1/2=∑(n2n)xn for ∣4x∣<1. Squaring (Cauchy product, legitimate by absolute convergence) and comparing with 1−4x1=∑4nxn: the coefficient of xn in the square is ∑k=0n(k2k)(n−k2n−2k), and uniqueness of coefficients gives
k=0∑n(k2k)(n−k2n−2k)=4n.
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) is a real sequence, f(x)=∑n≥0anxn, and An=a0+⋯+an.
Part I — Abel’s theorem, uniformly. Assume in this part that ∑an converges, and set rn=∑k≥nak (so rn→0 and an=rn−rn+1).
Prove, by summation by parts, that for all 0≤x≤1 and N≤M:
n=N∑Manxn≤2n≥Nsup∣rn∣.
Deduce that ∑anxn converges uniformly on [0,1], that its sum is continuous there, and recover the radial limit of Exercise 11.9: f(x)→∑an as x→1−.
(Abel’s theorem for Cauchy products) Let ∑an=A, ∑bn=B and suppose the Cauchy product∑cn, cn=∑kakbn−k, converges, with sum C. Prove C=AB(inside the disk the product identity holds by Proposition 11.4; let x→1−).
Show the hypothesis matters: for an=bn=n+1(−1)n, both series converge, yet ∣cn∣≥n+22(n+1)≥1(bound each factor (k+1)(n−k+1) by AM–GM): the Cauchy product of two convergent series may diverge.
(A dividend of Exercise 11.5) Show that (ln(1−x))2=2∑n≥1n+1Hnxn+1 on (−1,1), check that (n+1Hn)n≥1 decreases to 0, and conclude with Abel:
n≥1∑(−1)n+1n+1Hn=2(ln2)2.
Part II — Tauber’s converse. Call ∑anAbel-summable to L when f(x)→L as x→1−.
Show that ∑(−1)n is Abel-summable to 21 yet divergent: Abel’s theorem has no unconditional converse.
(Cesàro lemma) If un→0 then Nu1+⋯+uN→0(split the sum at a fixed m).
Assume now nan→0 and f(x)→L. With xN=1−N1, prove the two estimates
(for the first, 1−xn≤n(1−x); for the second, ∣an∣≤N1supm>Nm∣am∣ and ∑xNn≤N).
Conclude Tauber’s theorem: if nan→0 and ∑an is Abel-summable to L, then ∑an converges to L.
(The easy Tauberian for positive coefficients) If an≥0 and f is bounded on [0,1), show that ∑an converges and ∑an=limx→1−f(x)(bound ∑n≤Nanxn≤f(x) and let x→1−, then use Abel).
Part III — Cesàro means and Frobenius’ theorem. Call ∑anCesàro-summable to L when σN=NA0+⋯+AN−1→L.
Show that a convergent series is Cesàro-summable to its sum (question 7 applied to An−L).
Compute the Cesàro value of ∑(−1)n and check it agrees with the Abel value 21 of question 6.
With Sn=A0+⋯+An=(n+1)σn+1, prove the two identities, for 0≤x<1:
(Frobenius) Deduce: if σN→L then f(x)→L as x→1− — Cesàro-summable implies Abel-summable, to the same value (subtract the two identities and split the sum at a large N, as in Exercise 11.9).
Show that the hierarchy
convergent⟹Cesaˋro-summable⟹Abel-summable
is strict at both arrows: question 6 for the first; for the second, show that ∑(−1)n(n+1) is Abel-summable to 41 (compute f) but not Cesàro-summable (compute σN separately for even and odd N).
Part IV — Integrating to the boundary.
Suppose ∑anxn converges on [0,1) and ∑n+1an converges. Prove that the improper integral∫01f exists and
∫01(n≥0∑anxn)dx=n≥0∑n+1an
(the primitive F(x)=∑n+1anxn+1 is continuous at 1 by Part I).
Let η=∑n≥1n2(−1)n−1. Show ∫01xln(1+x)dx=η and, by splitting even and odd indices in the absolutely convergent ∑n21, that η=21∑n≥1n21. (The Fourier chapter’s weekend problem evaluates ∑n21=6π2.)
Prove
n≥0∑3n+1(−1)n=∫011+x3dx=31(ln2+3π)
(the series converges by Leibniz; integrate the geometric series ∑(−1)nx3n with question 16; then partial fractions: 1+x31=1+x1/3+x2−x+1(2−x)/3).
From the binomial series for (1−t)−1/2 (Exercise 11.12) derive
justifying the boundary value by normal convergence on [−1,1] (use (n2n)4−n∼πn1, Example 6.14) — here not even Abel is needed.
(Catalan at the boundary) Show that ∑Cn4−n=2: the Catalan series of Example 11.21 converges at its radius 41 (asymptotics of Exercise 11.8), its sum is continuous on [0,41], and the closed form has limit 2 there.
Part V — Rigidity: the identity theorem.
(Isolated zeros) Let f=∑anxn have radius R>0 and not all an=0; let m be the smallest index with am=0. Show f(x)=xmg(x) with g a power series of radius R, g(0)=am=0, and deduce that f has no zero in some punctured neighborhood of 0.
(Identity theorem) Let f,h be sums of power series near 0 and (xk) a sequence of nonzero points with xk→0 and f(xk)=h(xk). Prove that f and h have the same coefficients, hence coincide near 0.
Show that a function analytic on an open interval I which vanishes on a subinterval vanishes identically on I(the set of points around which f vanishes identically is open and, by the identity theorem applied at accumulation points, closed in I). Conclude that no nonzero analytic function on R has compact support — whereas C∞ bump functions exist (Exercise 11.7 supplies the building block): analyticity is rigid, smoothness is flabby.
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=rn−rn+1, summation by parts:
n=N∑Manxn=rNxN+n=N+1∑Mrn(xn−xn−1)−rM+1xM.
For 0≤x≤1 the increments xn−1−xn are nonnegative and telescope to xN−xM; with s=supn≥N∣rn∣:
n=N∑Manxn≤s(xN+(xN−xM)+xM)=2sxN≤2s.
2. Since rn→0, supn≥N∣rn∣→0: question 1 is exactly the uniform Cauchy criterion on [0,1], so ∑anxn converges uniformly there and its sum is continuous (Theorem 10.11). The value at 1 being ∑an, continuity at 1 is the radial limit of Exercise 11.9.
3. For ∣x∣<1 all three power series converge absolutely and (∑anxn)(∑bnxn)=∑cnxn (Proposition 11.4). By question 2 each factor and the product side are continuous on [0,1] (their coefficient series converge by hypothesis); letting x→1− in the identity: AB=C.
by AM–GM: (k+1)(n−k+1)≤2(k+1)+(n−k+1)=2n+2. The general term of ∑cn does not tend to 0: the Cauchy product diverges, although both factors converge (alternating series).
5.Exercise 11.5 gives 1−x−ln(1−x)=∑Hnxn (∣x∣<1). Term-by-term primitives (Theorem 11.7 (2)), both sides vanishing at 0:
2(ln(1−x))2=n≥1∑n+1Hnxn+1.
Decrease: (n+2)Hn≥(n+1)Hn+1 amounts to Hn≥1, true for n≥1; and n+1Hn∼nlnn→0: at x=−1 the series converges by the alternating test. Substituting x↦−x and applying question 2 at x=1:
2(ln2)2=n≥1∑n+1Hn(−1)n+1,
the announced value.
6.f(x)=∑(−1)nxn=1+x1→21 as x→1−: Abel-summable to 21. But the partial sums are 1,0,1,0,…: divergent.
7. Given ε>0 choose m with ∣un∣≤ε for n>m; for N≥m:
For n>N: ∣an∣=nn∣an∣≤N1supm>Nm∣am∣, and ∑n>NxNn≤1−xN1=N:
n>N∑anxNn≤Nsupm>Nm∣am∣⋅N=m>Nsupm∣am∣.
9. Decompose
AN−L=n=0∑Nan(1−xNn)−n>N∑anxNn+(f(xN)−L).
The first term tends to 0 by question 7 (the means of n∣an∣→0), the second by question 8 (the sup tends to 0), the third because xN→1− and f(x)→L. Hence AN→L: Tauber’s theorem.
10. For x∈[0,1) and any N: ∑n≤Nanxn≤f(x)≤M (nonnegative terms). Let x→1− in the finite sum: ∑n≤Nan≤M. The partial sums are increasing and bounded: ∑an converges, and then question 2 gives limx→1−f(x)=∑an.
11.σN−L is the mean of the N numbers An−L (0≤n<N), which tend to 0: question 7.
12.An=1 for even n, 0 for odd: A0+⋯+AN−1=⌈N/2⌉, so σN=N⌈N/2⌉→21, the Abel value of question 6.
13. Under σN→L one has Sn=O(n), hence An=Sn−Sn−1=O(n) and an=O(n): all the series below have radius ≥1. For ∣x∣<1, from an=An−An−1 and Anxn→0:
(1−x)n∑Anxn=n∑Anxn−n∑Anxn+1=n∑anxn=f(x),
and identically (1−x)∑Snxn=∑Anxn, so f(x)=(1−x)2∑nSnxn=(1−x)2∑n(n+1)σn+1xn. Finally ∑(n+1)xn=(1−x)21 (Exercise 11.3), which is the second identity.
14. Subtracting L times the second identity from the first:
f(x)−L=(1−x)2n≥0∑(n+1)(σn+1−L)xn.
Given ε, choose N with ∣σn+1−L∣≤ε for n≥N; then
∣f(x)−L∣≤(1−x)2CN+ε(1−x)2n∑(n+1)xn=(1−x)2CN+ε,
and letting x→1−: limsup≤ε. Hence f(x)→L: Frobenius’ theorem.
15.f(x)=∑(−1)n(n+1)xn=(1+x)21 (differentiate the geometric series at −x): Abel value 41. Partial sums: A2k=k+1, A2k+1=−(k+1) (immediate induction). Then S2m−1=0 (consecutive pairs cancel) and S2m=m+1, so
σ2m=2mS2m−1=0,σ2m+1=2m+1m+1→21:
(σN) has two distinct cluster values: not Cesàro-summable. With questions 6 and 11–14, the hierarchy convergent ⇒ Cesàro ⇒ Abel is strict at both arrows.
16. The primitive series F(x)=∑n+1anxn+1 has the same radius and F′=f on [0,1) (Theorem 11.7); since ∑n+1an converges, Part I (question 2) makes Fcontinuous on [0,1]. As ∫0xf=F(x) (equal derivatives, equal value 0 at 0),
17.xln(1+x)=∑n≥1n(−1)n−1xn−1 (radius 1; continuous at 0). The series of m+1am is ∑n≥1n2(−1)n−1, absolutely convergent: question 16 gives ∫01xln(1+x)dx=η. In the absolutely convergent ∑n21, regroup even and odd:
18. Leibniz: 3n+11↓0, the series converges. On [0,1), ∑(−1)nx3n=1+x31, and ∑3n+1(−1)n converges: question 16 gives ∑3n+1(−1)n=∫011+x3dx. Partial fractions (check: 31(x2−x+1)+32−x(1+x)=1):
∫011+x3dx=31ln2+31∫01x2−x+12−xdx.
Writing 2−x=−21(2x−1)+23: the ln(x2−x+1) part vanishes at both ends, and
19. Substituting t=x2 in the series of Exercise 11.12 and integrating term by term (the primitive of (1−x2)−1/2 vanishing at 0 is arcsin):
arcsinx=n≥0∑4n(2n+1)(n2n)x2n+1(∣x∣<1).
The coefficients are ∼2πn3/21 (Example 6.14), summable: the series converges normally on [−1,1], its sum is continuous there, and coincides with the continuousarcsin on (−1,1), hence at x=1 too:
21.f(x)=∑n≥manxn=xmg(x) with g(x)=∑k≥0am+kxk; if (anrn) is bounded then (am+krk) is too (divide by rm): g has radius ≥R. g is continuous with g(0)=am=0, so g=0 on some [−δ,δ], and f(x)=xmg(x)=0 for 0<∣x∣≤δ.
22.d=f−h is the sum of a power series near 0 vanishing at the nonzero points xk→0. If some coefficient of d were nonzero, question 21 would give a punctured neighborhood of 0 free of zeros of d — contradicting d(xk)=0. So all coefficients of d vanish: f and h have equal coefficients and coincide near 0.
23. The function h(x)=1+x21=∑(−1)nx2n (radius 1) satisfies h(k1)=1+1/k21=k2+1k2. Any analyticf with the same values agrees with h at the points k1→0: by the identity theorem (question 22), f=1+x21 near 0 — the unique solution.
24. Let Z be the set of points of I having a neighborhood on which f vanishes identically: open by definition, nonempty (the subinterval). Closed in I: if y∈I is a limit of points of Z, then y is an accumulation point of zeros of f; expanding f in a power series at y (analyticity) and applying questions 21–22 re-centered at y, all coefficients at y vanish, so f≡0 near y: y∈Z. An interval is connected, so Z=I: f≡0 on I. In particular an analytic function on R vanishing outside a compact set vanishes on an interval, hence everywhere: no nonzero analytic bump. The C∞ world is different: gluing the flat function of Exercise 11.7 (e.g. x↦e−1/x21x>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 nan→0 (question 9), and Cesàro summability sits strictly between convergence and Abel summability (Frobenius, questions 14–15). (iii) For a friend: ∑3n+1(−1)n=∫011+x3dx 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.