Mathematics · Book 4 · Bachelor Year 2

University Mathematics — Year 2

University Mathematics — Year 2 · Bachelor Year 2

7Sequences and Series

The theory of numerical series (Year 1 volume) matures here in three directions: series with values in Banach spaces, where absolute convergence does the work; the finer tests for real series (Abel summation); and summable families — summation freed from the order of the terms — with the Fubini theorem for double sums and the Cauchy product. These tools carry all the function-series chapters ahead.

7.1 Series in normed spaces

Definition 7.1

For a sequence (un)(u_n) in a normed space EE, the series un\sum u_n converges when its partial sums do; it converges absolutely when un<\sum \norm{u_n} < \infty. In a Banach space, absolute convergence implies convergence (Theorem 5.21); in a non-complete space this may fail (Exercise 7.9).

Example 7.2

In Mn(K)\mathcal{M}_n(K) (or Lc(E)\mathcal{L}_c(E), EE Banach): for A<1\vertiii A < 1, the Neumann series Ak\sum A^k converges absolutely to (IA)1(I - A)^{-1} (proved in Exercise 5.5); Akk!\sum \frac{A^k}{k!} converges absolutely to eA\eu^A for every AA (Example 5.22). Operator-valued geometric and exponential series behave like their scalar models — the whole point of the Banach framework.

7.2 Abel summation

Theorem 7.3 (Abel’s summation and test)

(Summation by parts) For scalars ana_n and vectors bnb_n, with Bn=k=0nbkB_n = \sum_{k=0}^{n} b_k:

n=0Nanbn=aNBNn=0N1(an+1an)Bn.\sum_{n=0}^{N} a_n b_n = a_N B_N - \sum_{n=0}^{N-1} (a_{n+1} - a_n) B_n .

(Abel’s test) If (an)(a_n) is a real sequence, decreasing to 00, and the partial sums BnB_n are bounded (in a Banach space), then anbn\sum a_n b_n converges.

Proof. The identity, step by step: with B1=0B_{-1} = 0, write bn=BnBn1b_n = B_n - B_{n-1} and split,

n=0Nanbn=n=0NanBnn=0NanBn1=n=0NanBnn=0N1an+1Bn,\sum_{n=0}^{N} a_nb_n = \sum_{n=0}^{N} a_nB_n - \sum_{n=0}^{N} a_nB_{n-1} = \sum_{n=0}^{N} a_nB_n - \sum_{n=0}^{N-1} a_{n+1}B_{n} ,

reindexing the second sum by nn+1n \mapsto n + 1 (the B1B_{-1} term vanishes); collecting the common range 0nN10 \leq n \leq N-1 leaves aNBNa_NB_N plus nN1(anan+1)Bn\sum_{n\leq N-1}(a_n - a_{n+1})B_n: the stated formula. It is the discrete integration by parts, with (Bn)(B_n) as antiderivative of (bn)(b_n) and the difference an+1ana_{n+1} - a_n as derivative of (an)(a_n). For the test, with BnM\norm{B_n} \leq M: the boundary term aNBN0a_N B_N \to 0; the series (anan+1)Bn\sum (a_n - a_{n+1})B_n converges absolutely, since

n(an+1an)BnMn(anan+1)=Ma0<\sum_n \norm{(a_{n+1} - a_n)B_n} \leq M \sum_n (a_n - a_{n+1}) = M a_0 < \infty

(telescoping, an0a_n \downarrow 0). Both pieces of the identity converge, hence so does anbn\sum a_n b_n.

Example 7.4

sinnn\sum \frac{\sin n}{n} converges: an=1n0a_n = \frac1n \downarrow 0 and Bn=k=1nsinkB_n = \sum_{k=1}^{n} \sin k is bounded — indeed Bn=kneik=ei(ein1)ei1B_n = \Im\sum_{k \leq n} \eu^{\iu k} = \Im\,\frac{\eu^{\iu}(\eu^{\iu n} - 1)}{\eu^{\iu} - 1}, of modulus 2ei1\leq \frac{2}{\abs{\eu^{\iu} - 1}}. It does not converge absolutely (sinnsin2n=1cos2n2\abs{\sin n} \geq \sin^2 n = \frac{1 - \cos 2n}{2}, and 1cos2n2n\sum \frac{1 - \cos 2n}{2n} diverges since cos2nn\sum \frac{\cos 2n}{n} converges by the same Abel test while 12n\sum \frac{1}{2n} diverges). The alternating series test is the special case bn=(1)nb_n = (-1)^n.

Example 7.5 (Abel on the circle of convergence)

For which complex zz with z=1\abs z = 1 does n1znn\sum_{n \geq 1} \frac{z^n}{n} converge? At z=1z = 1 it is the harmonic series: divergent. For z1z \neq 1 on the circle, Abel’s test applies with an=1n0a_n = \frac1n \downarrow 0 and bn=znb_n = z^n, whose partial sums are bounded independently of NN:

n=1Nzn=z(zN1)z12z1.\Bigl|\sum_{n=1}^{N} z^n\Bigr| = \Bigl|\frac{z(z^N - 1)}{z - 1}\Bigr| \leq \frac{2}{\abs{z - 1}} .

Convergent — though never absolutely (1n\sum\frac1n). One series, a circle of behaviours: divergence at a single point, semi-convergence everywhere else. This is the standard boundary behaviour of power series (Chapter 11), met here with bare hands; at z=1z = -1 it recovers the alternating harmonic series, and at z=eiθz = \eu^{\iu\theta} its real and imaginary parts are the series cosnθn\sum\frac{\cos n\theta}{n} and sinnθn\sum\frac{\sin n\theta}{n} of Exercise 7.4.

Example 7.6 (A booby-trapped alternating series)

Does n2(1)nn+(1)n\sum_{n\geq2} \dfrac{(-1)^n}{\sqrt n + (-1)^n} converge? The signs alternate and the terms tend to 00 — yet the alternating test does not apply: the moduli 1n+(1)n\frac{1}{\sqrt n + (-1)^n} are not decreasing (they jump up at each odd nn). Expand instead:

(1)nn+(1)n=(1)nn11+(1)nn=(1)nn1n+O(1n3/2).\frac{(-1)^n}{\sqrt n + (-1)^n} = \frac{(-1)^n}{\sqrt n}\cdot \frac{1}{1 + \frac{(-1)^n}{\sqrt n}} = \frac{(-1)^n}{\sqrt n} - \frac{1}{n} + O\Bigl(\frac{1}{n^{3/2}}\Bigr).

The first piece converges (alternating test, honestly applied to 1n0\frac1{\sqrt n}\downarrow0), the third converges absolutely — but the middle piece is the divergent harmonic series: the sum diverges to -\infty. The closing insight: when monotonicity fails, expand until every piece is either absolutely convergent or a clean test case; the hidden 1n-\frac1n is invisible to sign-counting.

Remark 7.7 (Common pitfalls)

(i) “Terms tend to 00” proves nothing: the harmonic series diverges. (ii) The alternating test requires decreasing moduli — Example 7.6 is the canonical counterexample, and Exercise 7.1’s third series the drill. (iii) Conditionally convergent series may not be rearranged (Example 7.12), and their Cauchy products may diverge: for (1)nn+1\sum\frac{(-1)^n}{\sqrt{n+1}} squared, the diagonal terms satisfy

ck=m=0k1(m+1)(km+1)(k+1)2k+220\abs{c_k} = \sum_{m=0}^{k} \frac{1}{\sqrt{(m+1)(k-m+1)}} \geq (k+1)\cdot\frac{2}{k+2} \longrightarrow 2 \neq 0

(each factor is at most k+22\frac{k+2}2 by AM–GM), so ck\sum c_k diverges — absolute convergence of at least one factor (Exercise 7.8) is not a luxury. (iv) Summability is about absolute bounds by definition: there is no such thing as a conditionally summable family.

7.3 Summable families

Definition 7.8

Let II be a countable index set. A family (ui)iI(u_i)_{i \in I} of nonnegative reals is summable when the finite partial sums are bounded; its sum is

iIui=supFI finiteiFui[0,+].\sum_{i \in I} u_i = \sup_{F \subseteq I \text{ finite}} \sum_{i \in F} u_i \in \intcc{0}{+\infty} .

A family of reals or complexes (or Banach vectors) is summable when (ui)(\norm{u_i}) is; its sum is then defined by splitting into positive/negative (or real/imaginary) parts — equivalently, as the common value of nuσ(n)\sum_{n} u_{\sigma(n)} over all enumerations σ\sigma of II (see below).

Method 7.9 (Choosing a test)

Facing un\sum u_n, in order: (1) if un↛0u_n \not\to 0, divergence, stop. (2) If the terms have constant sign, compare: find an equivalent (Chapter 6) and place it on the Riemann–Bertrand map. (3) If signs alternate with decreasing moduli, the alternating test; if the moduli are not monotone, expand the term until each piece is absolutely convergent or a clean test case (Example 7.6). (4) If the sign pattern is oscillatory but structured (sinnθ\sin n\theta, einθ\eu^{\iu n\theta}, matrix powers), Abel’s test with bounded partial sums. (5) Absolute convergence is always worth checking first: it is stronger, order-proof, and unlocks Cauchy products and Fubini.

Example 7.10 (Summability by diagonal counting)

For which s>0s > 0 is the family ((m+n)s)m,n1\bigl((m + n)^{-s}\bigr)_{m, n \geq 1} summable? Group the finite partial sums by diagonals m+n=km + n = k: the diagonal kk carries k1k - 1 pairs, each contributing ksk^{-s}, so the finite sums are exactly bounded by (and exhaust)

k2k1ks,\sum_{k \geq 2} \frac{k - 1}{k^{s}} ,

a series with positive terms equivalent to k1sk^{1-s}: summable iff s1>1s - 1 > 1, i.e. s>2s > 2. The two-dimensional index eats one full power: a plane of terms is “one dimension more divergent” than a line — the counting geometry of the index set, not the size of individual terms, decides summability. (The same census shows ((m2+n2)1)\bigl((m^2 + n^2)^{-1}\bigr) is not summable: on the diagonal m+n=km + n = k, each term is at least k2k^{-2}, and (k1)k2(k-1)\cdot k^{-2} sums like the harmonic series.)

Theorem 7.11 (Summability and order)

  1. For nonnegative families, the sum is invariant under any enumeration: iui=n=0uσ(n)\sum_{i} u_i = \sum_{n=0}^{\infty} u_{\sigma(n)} for every bijection σ ⁣:NI\sigma \colon \N \to I.
  2. A real or complex series un\sum u_n is commutatively convergent (every rearrangement converges, with the same sum) if and only if it is absolutely convergent.

Proof. (1) Every partial sum nNuσ(n)\sum_{n \leq N} u_{\sigma(n)} is a finite partial sum of the family (so \leq the sup); every finite FF is contained in some {σ(0),,σ(N)}\{\sigma(0), \dots, \sigma(N)\} (so the sup \leq the series’ limit). The two bounds match.

(2) If un<\sum\abs{u_n} < \infty: for any rearrangement σ\sigma and ε>0\varepsilon > 0, choose NN with n>Nunε\sum_{n > N}\abs{u_n} \leq \varepsilon; beyond the rank where σ\sigma has exhausted [ ⁣[0,N] ⁣]\intint{0}{N}, the rearranged partial sums differ from the original limit by at most ε\varepsilon: same sum. If un=\sum \abs{u_n} = \infty but un\sum u_n converges (real case; complex follows coordinatewise): the positive and negative parts both diverge, and one can rearrange to reach any prescribed limit — Riemann’s theorem, carried out in Exercise 7.5 — so commutative convergence fails.

Example 7.12 (A rearrangement caught red-handed)

The alternating harmonic series sums to n1(1)n1n=ln2\sum_{n\geq1}\frac{(-1)^{n-1}}{n} = \ln 2 (Year 1 volume). Rearrange it as “one positive, two negatives”:

11214+131618+151 - \frac12 - \frac14 + \frac13 - \frac16 - \frac18 + \frac15 - \cdots

Grouping each block of three,

12k114k214k=14k214k=12(12k112k),\frac{1}{2k-1} - \frac{1}{4k-2} - \frac1{4k} = \frac{1}{4k-2} - \frac{1}{4k} = \frac12\Bigl(\frac{1}{2k-1} - \frac1{2k}\Bigr),

so the rearranged series converges to 12ln2\frac12\ln 2 — half the original sum, with exactly the same terms. Non-absolutely convergent series remember the order of their terms; summable families are precisely the ones that do not.

Example 7.13 (Grouping is safe, ungrouping is not)

Grouping consecutive terms of a convergent series never changes the sum: the grouped partial sums form a subsequence of the original ones. The converse operation is forbidden:

(11)+(11)+(11)+=0+0+=0,(1 - 1) + (1 - 1) + (1 - 1) + \cdots = 0 + 0 + \cdots = 0,

yet the ungrouped 11+11+1 - 1 + 1 - 1 + \cdots diverges (partial sums oscillate between 11 and 00). Ungrouping is legitimate only with a compensating hypothesis — for instance, terms tending to 00 with bounded group lengths: then between two grouped partial sums the original ones drift by at most a sum of o(1)o(1) terms of bounded number, and convergence transfers back. That is exactly the clause under which the block computation of Example 7.12 is a proof and not a sleight of hand.

Theorem 7.14 (Fubini for families; Cauchy products)

Let (um,n)(m,n)N2(u_{m,n})_{(m,n) \in \N^2} be a summable double family (i.e. supFFum,n<\sup_F \sum_F \abs{u_{m,n}} < \infty). Then

(m,n)um,n=m=0(n=0um,n)=n=0(m=0um,n)=k=0(m+n=kum,n),\sum_{(m,n)} u_{m,n} = \sum_{m=0}^{\infty}\Bigl(\sum_{n=0}^{\infty} u_{m,n}\Bigr) = \sum_{n=0}^{\infty}\Bigl(\sum_{m=0}^{\infty} u_{m,n}\Bigr) = \sum_{k=0}^{\infty}\Bigl(\sum_{m+n=k} u_{m,n}\Bigr),

all inner series converging (absolutely). In particular, if am\sum a_m and bn\sum b_n converge absolutely, their Cauchy product converges absolutely with

(mam)(nbn)=k=0ck,ck=m=0kambkm.\Bigl(\sum_m a_m\Bigr)\Bigl(\sum_n b_n\Bigr) = \sum_{k=0}^{\infty} c_k, \qquad c_k = \sum_{m=0}^{k} a_m b_{k-m} .

Proof. Nonnegative case. Each grouping (by rows, columns, or diagonals) computes the same supremum: any finite set of pairs is contained in a finite block of rows (bounding each grouped sum below by finite partial sums and above by the total), and monotone convergence of partial sums does the rest — concretely, for rows: mMnNum,nS\sum_{m \leq M}\sum_{n \leq N} u_{m,n} \leq S gives, letting NN \to \infty then MM \to \infty, mnum,nS\sum_m \sum_n u_{m,n} \leq S; conversely every finite FF sits in such a rectangle, so Smnum,nS \leq \sum_m\sum_n u_{m,n}. Diagonals: same two bounds with triangles instead of rectangles.

General case. Split into positive and negative (real and imaginary) parts, each a summable nonnegative family; the four groupings agree on each part, hence on the difference; absolute convergence of the inner series comes from the nonnegative case applied to um,n\abs{u_{m,n}}.

Cauchy product. The family um,n=ambnu_{m,n} = a_m b_n is summable: finite partial sums of ambn\abs{a_mb_n} are bounded by (am)(bn)\bigl(\sum\abs{a_m}\bigr)\bigl(\sum\abs{b_n}\bigr). Rows give (am)(bn)\bigl(\sum a_m\bigr)\bigl(\sum b_n\bigr); diagonals give kck\sum_k c_k.

Example 7.15 (The exponential identity, honestly)

For a,bCa, b \in \C (or commuting matrices):

(mamm!)(nbnn!)=km+n=kambnm!n!=k(a+b)kk!,\Bigl(\sum_m \frac{a^m}{m!}\Bigr)\Bigl(\sum_n \frac{b^n}{n!}\Bigr) = \sum_k \sum_{m+n=k} \frac{a^m b^n}{m!\,n!} = \sum_k \frac{(a + b)^k}{k!},

by the binomial theorem on each diagonal: eaeb=ea+b\eu^a \eu^b = \eu^{a+b} — the functional equation of exp\exp derived from the series alone. (Commutation is used in the binomial step; for non-commuting matrices the identity genuinely fails, Chapter 16.)

Example 7.16 (Cauchy products as a computing device)

From the geometric series and Exercise 7.2’s n1nzn=z(1z)2\sum_{n \geq 1} nz^n = \frac{z}{(1-z)^2} (z<1\abs z < 1), one more Cauchy product finishes the second moment. Multiply mmzm\sum_m mz^m by nzn\sum_n z^n: the diagonal coefficient is m=0km=k(k+1)2\sum_{m=0}^k m = \frac{k(k+1)}2, so

z(1z)3=k0k(k+1)2zk,\frac{z}{(1-z)^3} = \sum_{k\geq0}\frac{k(k+1)}{2}\,z^k ,

and the identity n2=2n(n+1)2nn^2 = 2\cdot\frac{n(n+1)}2 - n assembles

n1n2zn=2z(1z)3z(1z)2=z(1+z)(1z)3.\sum_{n\geq1} n^2z^n = \frac{2z}{(1-z)^3} - \frac{z}{(1-z)^2} = \frac{z(1+z)}{(1-z)^3} .

At z=12z = \frac12: n1n22n=123218=6\sum_{n\geq1}\frac{n^2}{2^n} = \frac{\frac12\cdot\frac32}{\frac18} = 6 — a closed value with no differentiation anywhere, just absolutely convergent series multiplied like polynomials. The same telescoping of identities computes every ndzn\sum n^dz^n, and probabilists will recognize the second factorial moment of the geometric law (Chapter 23).

Example 7.17 (A double-sum evaluation)

For s>1s > 1 real, let ζ(s)=n1ns\zeta(s) = \sum_{n\geq1} n^{-s}. Counting divisors by double summation — the family (msns)(m^{-s}n^{-s}) over (m,n)(N)2(m,n) \in (\N^*)^2 is summable (product of convergent positive series) — and grouping by the product q=mnq = mn:

ζ(s)2=m,n1(mn)s=q=1d(q)qs,\zeta(s)^2 = \sum_{m,n} \frac{1}{(mn)^s} = \sum_{q=1}^{\infty} \frac{d(q)}{q^s},

where d(q)d(q) is the number of divisors of qq. Summable families turn combinatorics into analysis.

Example 7.18 (A Fubini evaluation: n(ζ(n)1)=1\sum_n (\zeta(n) - 1) = 1)

For integer n2n \geq 2, ζ(n)1=k2kn\zeta(n) - 1 = \sum_{k \geq 2} k^{-n}. The double family (kn)k,n2(k^{-n})_{k, n \geq 2} is summable: summing the geometric columns first,

k2n21kn=k21/k211/k=k21k(k1)=1\sum_{k\geq2}\sum_{n\geq2} \frac{1}{k^n} = \sum_{k\geq2} \frac{1/k^2}{1 - 1/k} = \sum_{k\geq2} \frac{1}{k(k-1)} = 1

(telescoping), and all terms are positive, so Theorem 7.14 authorizes summing by rows instead:

n2(ζ(n)1)=1.\sum_{n\geq2}\bigl(\zeta(n) - 1\bigr) = 1 .

The infinitely many ζ\zeta-values, each transcendental-looking, have tails that add up to exactly 11. Closing insight: when a double sum has positive terms, compute it in whichever order collapses — here columns are geometric, rows are mysterious, and Fubini transfers the collapse.

Example 7.19 (The geometric series solves an equation)

In the Banach space (C([0,1]),)\bigl(C(\intcc01), \norm\cdot_\infty\bigr), solve xK(x)=yx - K(x) = y where K(f)K(f) is the constant function 1201f\frac12\int_0^1 f. The operator norm is K12<1\vertiii K \leq \frac12 < 1, so the Neumann series applies (Example 7.2): x=n0Kn(y)x = \sum_{n\geq0} K^n(y). Compute the iterates: K(y)=1201yK(y) = \frac12\int_0^1 y (a constant), and applying KK to a constant cc gives c2\frac c2, so Kn(y)=12n11201yK^n(y) = \frac{1}{2^{n-1}}\cdot\frac12\int_0^1 y for n1n \geq 1. Summing the geometric constants:

x=y+(01y)n112n=y+01y.x = y + \Bigl(\int_0^1 y\Bigr) \sum_{n\geq1}\frac{1}{2^n} = y + \int_0^1 y .

Check: xK(x)=y+y12(y+y)=yx - K(x) = y + \int y - \frac12\bigl(\int y + \int y\bigr) = y. An infinite series, a finite answer, and a one-line verification — the geometric series is an inversion algorithm, not just a convergence statement.

Example 7.20 (Telescoping by partial fractions)

Exact summation is rare; telescoping is its main supplier. Decompose

1n(n+1)(n+2)=12(1n(n+1)1(n+1)(n+2)),\frac{1}{n(n+1)(n+2)} = \frac{1}{2}\Bigl(\frac{1}{n(n+1)} - \frac{1}{(n+1)(n+2)}\Bigr),

(check by reduction to the common denominator), so the partial sums collapse:

n=1N1n(n+1)(n+2)=12(1121(N+1)(N+2))14.\sum_{n=1}^{N}\frac{1}{n(n+1)(n+2)} = \frac12\Bigl(\frac{1}{1\cdot2} - \frac{1}{(N+1)(N+2)}\Bigr) \longrightarrow \frac14 .

The same pattern — write the term as c(unun+1)c(u_n - u_{n+1}) for an explicit (un)(u_n) — solved Exercise 7.10 (arctangents) and computes every 1n(n+1)(n+k)=1kk!\sum\frac{1}{n(n+1)\cdots(n + k)} = \frac{1}{k\cdot k!}. When an exact sum exists at this level, a telescope is usually hiding in the term.

Remark 7.21 (Perspectives within this volume)

Three chapters ahead are direct clients. For Chapter 10: normal convergence of fn\sum f_n is absolute convergence of fn\sum\norm{f_n}_\infty in the Banach space (C,)\bigl(C, \norm\cdot_\infty\bigr) — this chapter’s Theorem 5.21 in costume. For Chapter 11: inside the disk of convergence everything is absolute and summable, so Cauchy products and rearrangements run free (that is why power series multiply like polynomials); on the boundary, Abel’s test takes over (Example 7.5). For Chapter 23: probability generating functions are power series whose manipulations — products for sums of independent variables, double sums for compound laws — are all licensed by Theorem 7.14. Summable families are the legal department of the analysis to come.

Remark 7.22 (Where this chapter is used)

Everything with an infinite sum passes through here: power series (Chapter 11) are summable families in disguise, Fourier coefficients get multiplied by Cauchy products and rearranged by Parseval (Chapter 14), and probability generating functions (Chapter 23) are Fubini’s theorem applied to expectations. The Year 3 volume absorbs summable families into Lebesgue integration over the counting measure — where Theorem 7.14 becomes a special case of the Fubini–Tonelli theorem.

7.4 Exercises

Exercise 7.1

Nature of: cosnn\sum \dfrac{\cos n}{n};   (1)nlnn\;\sum \dfrac{(-1)^n}{\ln n};   (1)nn3/4+cosn\;\sum \dfrac{(-1)^n}{n^{3/4} + \cos n} (expand as in the Year 1 trap: the alternating test needs monotonicity).

Solution

Solution of Exercise 7.1.

cosnn\sum\frac{\cos n}{n}: Abel’s test with an=1na_n = \frac1n and bn=cosnb_n = \cos n, whose partial sums are bounded (real part of a geometric sum, as in Example 7.4): convergent (not absolutely, by the same cos2\cos^2 trick).

(1)nlnn\sum \frac{(-1)^n}{\ln n} (n2n \geq 2): alternating test, 1lnn0\frac{1}{\ln n} \downarrow 0: convergent; not absolutely (lnnn\ln n \leq n).

(1)nn3/4+cosn\sum \frac{(-1)^n}{n^{3/4} + \cos n}: expand,

(1)nn3/4+cosn=(1)nn3/411+cosnn3/4=(1)nn3/4(1)ncosnn3/2+O(1n9/4).\frac{(-1)^n}{n^{3/4} + \cos n} = \frac{(-1)^n}{n^{3/4}}\cdot \frac{1}{1 + \frac{\cos n}{n^{3/4}}} = \frac{(-1)^n}{n^{3/4}} - \frac{(-1)^n\cos n}{n^{3/2}} + O\Bigl(\frac{1}{n^{9/4}}\Bigr).

First series: alternating, convergent. Second: absolutely convergent (1n3/2\frac{1}{n^{3/2}} scale). Third: absolutely convergent. Total: convergent.

Exercise 7.2

Prove that for z<1\abs z < 1: n1nzn=z(1z)2\sum_{n\geq1} n z^{n} = \dfrac{z}{(1-z)^2}, via the Cauchy product of zn\sum z^n with itself.

Solution

Solution of Exercise 7.2.

Cauchy product of m0zm\sum_{m\geq0} z^m with itself (both absolutely convergent for z<1\abs z < 1): the diagonal coefficient is ck=m=0k1=k+1c_k = \sum_{m=0}^{k} 1 = k + 1, so

1(1z)2=k0(k+1)zk.\frac{1}{(1-z)^2} = \sum_{k\geq0} (k+1)z^k .

Multiplying by zz and reindexing: n1nzn=z(1z)2\sum_{n \geq 1} n z^n = \frac{z}{(1-z)^2}.

Exercise 7.3 ★★

(Kronecker-type lemma) Let bn\sum b_n be a convergent real series. Prove, by Abel summation, that 1nk=1nkbk0\dfrac{1}{n}\sum_{k=1}^{n} k\,b_k \to 0.

Solution

Solution of Exercise 7.3.

Let Bn=knbkBB_n = \sum_{k \leq n} b_k \to B. Abel summation with ak=ka_k = k:

k=1nkbk=nBnk=1n1Bk1nk=1nkbk=Bn1nk=1n1Bk.\sum_{k=1}^{n} k\,b_k = n B_n - \sum_{k=1}^{n-1} B_k \quad\Longrightarrow\quad \frac1n \sum_{k=1}^{n} k b_k = B_n - \frac{1}{n}\sum_{k=1}^{n-1} B_k .

The Cesàro means of the convergent (Bk)(B_k) tend to its limit BB (Year 1 volume), so the right side tends to BB=0B - B = 0.

Exercise 7.4 ★★

Study the convergence of sin(nθ)nα\sum \dfrac{\sin(n\theta)}{n^\alpha} (θR\theta \in \R, α>0\alpha > 0) — for which (θ,α)(\theta, \alpha) is it absolutely convergent, semi-convergent, divergent?

Solution

Solution of Exercise 7.4.

If θπZ\theta \in \pi\Z: all terms vanish — convergent trivially. Assume θπZ\theta \notin \pi\Z.

α>1\alpha > 1: absolutely convergent (domination by nαn^{-\alpha}).

0<α10 < \alpha \leq 1: Abel’s test applies (an=nα0a_n = n^{-\alpha} \downarrow 0; partial sums of sinnθ\sin n\theta bounded by 1sin(θ/2)\frac{1}{\abs{\sin(\theta/2)}}, geometric sum): convergent. Not absolutely: sinnθsin2nθ=1cos2nθ2\abs{\sin n\theta} \geq \sin^2 n\theta = \frac{1 - \cos 2n\theta}{2}, and 1cos2nθ2nα\sum \frac{1 - \cos 2n\theta}{2n^\alpha} diverges (nα\sum n^{-\alpha} diverges; cos2nθnα\sum \frac{\cos 2n\theta}{n^\alpha} converges by Abel when 2θ2πZ2\theta \notin 2\pi\Z; the excluded case 2θ2πZ2\theta \in 2\pi\Z means θπZ\theta \in \pi\Z, already handled). Semi-convergent.

Exercise 7.5 ★★★

(Riemann rearrangement) Let un\sum u_n be a convergent but not absolutely convergent real series, and R\ell \in \R. Prove that some rearrangement of un\sum u_n converges to \ell. (Show both subseries of positive and negative terms diverge; then greedily alternate: take positive terms until exceeding \ell, then negative until dropping below, and so on; the terms tend to 00, forcing convergence to \ell.)

Solution

Solution of Exercise 7.5.

Let p1,p2,p_1, p_2, \dots be the nonnegative terms of (un)(u_n) in order, q1,q2,q_1, q_2, \dots the negative ones. Both pk\sum p_k and qk\sum q_k diverge: if one of them converged, the other would equal the convergent un\sum u_n minus it, hence converge too — and then un=pkqk\sum \abs{u_n} = \sum p_k - \sum q_k would converge, contradicting the hypothesis. Also un0u_n \to 0 (un\sum u_n converges).

Greedy rearrangement: take positive terms p1,p2,p_1, p_2, \dots until the running total first exceeds \ell (possible: pk=+\sum p_k = +\infty); then negative terms until the total first drops below \ell (possible: qk=\sum q_k = -\infty); repeat forever (each phase is finite, and every term is used exactly once: a genuine rearrangement). After each switch, the distance from the running total to \ell is at most the last term used; since the terms used at the mm-th switch have index \to \infty, and un0u_n \to 0, the running totals converge to \ell.

Exercise 7.6 ★★

Prove that the family (xm+nm!n!)(m,n)N2\Bigl(\dfrac{x^{m+n}}{m!\,n!}\Bigr)_{(m,n)\in\N^2} is summable for every xRx \in \R, and re-derive the identity (ex)2=e2x(\eu^x)^2 = \eu^{2x} by grouping the double sum along the diagonals m+n=km + n = k.

Solution

Solution of Exercise 7.6.

Summability: the finite partial sums of xm+nm!n!\frac{\abs x^{m+n}}{m!n!} are bounded by (mxmm!)2=e2x\bigl(\sum_m \frac{\abs x^m}{m!}\bigr)^2 = \eu^{2\abs x}. Diagonal grouping (Theorem 7.14):

(ex)2=m,nxm+nm!n!=k=0xkm+n=k1m!n!=kxkk!m=0k(km)=k(2x)kk!=e2x.(\eu^{x})^2 = \sum_{m,n} \frac{x^{m+n}}{m!\,n!} = \sum_{k=0}^{\infty} x^k \sum_{m+n=k} \frac{1}{m!\,n!} = \sum_k \frac{x^k}{k!}\sum_{m=0}^{k}\binom km = \sum_k \frac{(2x)^k}{k!} = \eu^{2x} .

Exercise 7.7 ★★

Prove that the family (1m2n2)m,n1\bigl(\frac{1}{m^2 n^2}\bigr)_{m,n \geq 1} is summable, and that grouping by gcd\gcd: with q=gcd(m,n)q = \gcd(m,n),

ζ(2)2=q11q4a,b1gcd(a,b)=11a2b2=ζ(4)S,\zeta(2)^2 = \sum_{q\geq1} \frac{1}{q^4} \sum_{\substack{a,b \geq 1\\ \gcd(a,b)=1}} \frac{1}{a^2b^2} = \zeta(4) \cdot S,

where S=gcd(a,b)=11a2b2S = \sum_{\gcd(a,b)=1} \frac{1}{a^2b^2}: deduce S=ζ(2)2/ζ(4)S = \zeta(2)^2/\zeta(4). (Every pair (m,n)(m,n) writes uniquely (qa,qb)(qa, qb) with gcd(a,b)=1\gcd(a,b) = 1.)

Solution

Solution of Exercise 7.7.

Summability: bounded by ζ(2)2\zeta(2)^2 as a product family (Theorem 7.14’s Cauchy-product argument). The map (q,a,b)(qa,qb)(q, a, b) \mapsto (qa, qb), from triples with gcd(a,b)=1\gcd(a, b) = 1 to pairs (m,n)(m, n), is a bijection (set q=gcd(m,n)q = \gcd(m,n)). Grouping the summable family accordingly (a partition of the index set — legitimate for summable families by Theorem 7.11/Theorem 7.14 applied to the partition into countably many classes):

ζ(2)2=qgcd(a,b)=11q4a2b2=ζ(4)S,soS=ζ(2)2ζ(4).\zeta(2)^2 = \sum_{q} \sum_{\gcd(a,b)=1} \frac{1}{q^4 a^2 b^2} = \zeta(4)\, S, \qquad\text{so}\qquad S = \frac{\zeta(2)^2}{\zeta(4)} .

(With the values ζ(2)=π26\zeta(2) = \frac{\pi^2}{6}, ζ(4)=π490\zeta(4) = \frac{\pi^4}{90} from Chapter 14: S=52S = \frac{5}{2}.)

Exercise 7.8 ★★★

(Abel’s theorem on products, light version) Suppose an\sum a_n converges absolutely and bn\sum b_n converges. Prove that their Cauchy product cn\sum c_n converges, with cn=(an)(bn)\sum c_n = (\sum a_n)(\sum b_n). (Write CN=kNck=nanBNnC_N = \sum_{k\leq N} c_k = \sum_n a_n B_{N-n} with BB the partial sums of bb; split according to nN/2n \leq N/2 or not, using boundedness of (Bm)(B_m) and the absolute tail of (an)(a_n).)

Solution

Solution of Exercise 7.8.

Let A=anA = \sum a_n (absolute), Bm=kmbkBB_m = \sum_{k\leq m} b_k \to B, bounded by MM. Then

CN=k=0Nck=n=0NanBNnC_N = \sum_{k=0}^{N} c_k = \sum_{n=0}^{N} a_n B_{N-n}

(collect by the index of aa). Write

CNAB=n=0Nan(BNnB)Bn>Nan.C_N - AB = \sum_{n=0}^{N} a_n (B_{N-n} - B) - B\sum_{n > N} a_n .

The last term tends to 00. Split the sum at n=N/2n = \lfloor N/2 \rfloor: for nN/2n \leq N/2, NnN/2N - n \geq N/2, so BNnBεN:=supmN/2BmB0\abs{B_{N-n} - B} \leq \varepsilon_N := \sup_{m \geq N/2}\abs{B_m - B} \to 0, and this part is εNan\leq \varepsilon_N \sum\abs{a_n}; for n>N/2n > N/2, BNnB2M\abs{B_{N-n} - B} \leq 2M, and this part is 2Mn>N/2an0\leq 2M \sum_{n > N/2} \abs{a_n} \to 0. Hence CNABC_N \to AB.

Exercise 7.9 ★★★

In the (non-complete) space EE of eventually-zero real sequences with the sup norm, exhibit an absolutely convergent series that does not converge in EE. (Try un=2nenu_n = 2^{-n} e_n with (en)(e_n) the canonical sequences.)

Solution

Solution of Exercise 7.9.

Take un=2nenu_n = 2^{-n} e_n (ene_n the sequence with a single 11 in position nn). Then un=2n<\sum \norm{u_n}_\infty = \sum 2^{-n} < \infty: absolutely convergent. But the partial sums SN=(1,12,,2N,0,)S_N = (1, \tfrac12, \dots, 2^{-N}, 0, \dots) would have to converge to the sequence (2n)n(2^{-n})_n, which is not eventually zero: outside EE. Inside EE, (SN)(S_N) is Cauchy without limit (SNx2N1\norm{S_N - x}_\infty \geq 2^{-N-1} fails to help any eventually-zero xx: for any xEx \in E vanishing beyond rank KK, SNx2K1\norm{S_N - x} \geq 2^{-K-1} for N>KN > K): the series does not converge in EE. Completeness is exactly what Theorem 5.21 needs.

Exercise 7.10 ★★

Verify the identity arctan(n+1)arctan(n)=arctan1n2+n+1\arctan(n+1) - \arctan(n) = \arctan\dfrac{1}{n^2 + n + 1}, and deduce the exact value of

n=1arctan1n2+n+1.\sum_{n=1}^{\infty} \arctan\frac{1}{n^2 + n + 1} .
Solution

Solution of Exercise 7.10.

Both arctan(n+1)arctann\arctan(n+1) - \arctan n and arctan1n2+n+1\arctan\frac{1}{n^2+n+1} lie in (0,π2)\intoo{0}{\frac\pi2}, and the tangent addition formula gives

tan(arctan(n+1)arctann)=(n+1)n1+n(n+1)=1n2+n+1:\tan\bigl(\arctan(n{+}1) - \arctan n\bigr) = \frac{(n+1) - n}{1 + n(n+1)} = \frac{1}{n^2 + n + 1} :

equal tangents in an interval where tan\tan is injective, so the identity holds. Telescoping,

n=1Narctan1n2+n+1=arctan(N+1)arctan1Nπ2π4=π4.\sum_{n=1}^{N}\arctan\frac{1}{n^2+n+1} = \arctan(N{+}1) - \arctan 1 \xrightarrow[N\to\infty]{} \frac\pi2 - \frac\pi4 = \frac\pi4 .

Exercise 7.11 ★★

Determine the nature (with equivalents) of

n(n+1n)α (α>0),n(1cos1n),n(e(1+1n) ⁣n).\sum_n \bigl(\sqrt{n+1} - \sqrt n\bigr)^{\alpha} \ (\alpha > 0), \qquad \sum_n \Bigl(1 - \cos\frac1n\Bigr), \qquad \sum_n \Bigl(\eu - \Bigl(1 + \frac1n\Bigr)^{\!n}\Bigr).
Solution

Solution of Exercise 7.11.

First: n+1n=1n+1+n12n\sqrt{n+1} - \sqrt n = \frac{1}{\sqrt{n+1} + \sqrt n} \sim \frac{1}{2\sqrt n}, so the terms are 2αnα/2\sim 2^{-\alpha}n^{-\alpha/2}: convergence iff α2>1\frac\alpha2 > 1, i.e. α>2\alpha > 2. Second: 1cos1n12n21 - \cos\frac1n \sim \frac{1}{2n^2}: converges. Third: (1+1n)n=enln(1+1/n)=e112n+O(n2)=e(112n+O(n2))\bigl(1 + \frac1n\bigr)^n = \eu^{\,n\ln(1 + 1/n)} = \eu^{\,1 - \frac1{2n} + O(n^{-2})} = \eu\bigl(1 - \frac{1}{2n} + O(n^{-2})\bigr), so

e(1+1n) ⁣ne2n:\eu - \Bigl(1 + \frac1n\Bigr)^{\!n} \sim \frac{\eu}{2n} :

positive terms equivalent to a harmonic multiple: diverges.

Exercise 7.12 ★★★

Let (an)(a_n) be positive and decreasing with an\sum a_n convergent. Prove that nan0n\,a_n \to 0 (bound na2nn a_{2n} by a tail). Show that the converse fails, and that monotonicity is essential, with explicit counterexamples.

Solution

Solution of Exercise 7.12.

By monotonicity, na2nan+1+an+2++a2n=S2nSn0n\,a_{2n} \leq a_{n+1} + a_{n+2} + \dots + a_{2n} = S_{2n} - S_n \to 0 (Cauchy criterion for the convergent series). Hence 2na2n02n\,a_{2n} \to 0, and (2n+1)a2n+1(2n+1)a2n=2n+12n(2na2n)0(2n{+}1)\, a_{2n+1} \leq (2n{+}1)a_{2n} = \frac{2n+1}{2n}\,(2n\,a_{2n}) \to 0: both subsequences of (nan)(na_n) tend to 00, so nan0na_n \to 0.

Converse fails: an=1nlnna_n = \frac1{n\ln n} is positive decreasing with nan=1lnn0na_n = \frac1{\ln n} \to 0, yet an\sum a_n diverges (Bertrand frontier, Problem 7.1, question 18). Monotonicity essential: let an=1na_n = \frac1n when nn is a power of 22 and an=2na_n = 2^{-n} otherwise: ank2k+n2n<\sum a_n \leq \sum_k 2^{-k} + \sum_n 2^{-n} < \infty, but nan=1na_n = 1 along the powers of 22: nan↛0na_n \not\to 0.

7.5 Problem: Euler’s ζ(2)=π2/6\zeta(2) = \pi^2/6, by Cauchy’s Cotangent Sum

Euler’s most famous identity, 1+14+19+=π261 + \frac14 + \frac19 + \cdots = \frac{\pi^2}6, admits a completely elementary proof, due to Cauchy: de Moivre’s formula produces a polynomial whose roots are the numbers cot2kπ2n+1\cot^2\frac{k\pi}{2n+1}, Vieta sums those roots exactly, and the squeeze cot2θ<1θ2<1+cot2θ\cot^2\theta < \frac{1}{\theta^2} < 1 + \cot^2\theta crushes the partial sums of 1k2\sum\frac1{k^2} between two explicit rational bounds. We run the proof in full, extract ζ(4)=π490\zeta(4) = \frac{\pi^4}{90} by the same method, then map the entire frontier between convergence and divergence with the Bertrand series — and prove that the frontier carries no slowest convergent series at all.

Problem 7.1

Weekend problem — ζ(2)=π2/6\zeta(2) = \pi^2/6 and the Bertrand panorama

Throughout, n1n \geq 1 and θk=kπ2n+1\theta_k = \dfrac{k\pi}{2n+1} for k=1,,nk = 1, \dots, n; note 0<θk<π20 < \theta_k < \frac\pi2.

Part I — The cotangent identity.

  1. Prove de Moivre’s formula (cosθ+isinθ)m=cosmθ+isinmθ(\cos\theta + \iu\sin\theta)^m = \cos m\theta + \iu\sin m\theta (mNm \in \N), and deduce, for m=2n+1m = 2n + 1,

    sin((2n+1)θ)=j=0n(1)j(2n+12j+1)cos2(nj)θsin2j+1θ.\sin\bigl((2n{+}1)\theta\bigr) = \sum_{j=0}^{n} (-1)^j\binom{2n+1}{2j+1}\cos^{2(n-j)}\theta\, \sin^{2j+1}\theta .
  2. Deduce that for θ(0,π2)\theta \in \intoo{0}{\frac\pi2},

    sin((2n+1)θ)=sin2n+1θ  Pn(cot2θ),Pn(x)=j=0n(1)j(2n+12j+1)xnj,\sin\bigl((2n{+}1)\theta\bigr) = \sin^{2n+1}\theta\; P_n(\cot^2\theta), \qquad P_n(x) = \sum_{j=0}^{n} (-1)^j\binom{2n+1}{2j+1}x^{\,n-j},

    a polynomial of degree nn with leading coefficient 2n+12n + 1.

  3. Show that xk=cot2θkx_k = \cot^2\theta_k, k=1,,nk = 1, \dots, n, are nn distinct roots of PnP_n — hence all of them.
  4. By Vieta, prove the exact identity

    k=1ncot2kπ2n+1=n(2n1)3.\sum_{k=1}^{n} \cot^2\frac{k\pi}{2n+1} = \frac{n(2n-1)}{3}.
  5. Deduce also k=1n1sin2θk=2n(n+1)3\displaystyle\sum_{k=1}^{n} \frac{1}{\sin^2\theta_k} = \frac{2n(n+1)}{3}.
  6. Prove the squeeze: cot2θ<1θ2<1sin2θ\cot^2\theta < \dfrac1{\theta^2} < \dfrac{1}{\sin^2\theta} for θ(0,π2)\theta \in \intoo{0}{\frac\pi2} (from sinθ<θ<tanθ\sin\theta < \theta < \tan\theta).

Part II — The squeeze closes: Euler’s theorem.

  1. Summing question 6 over k=1,,nk = 1, \dots, n with θ=θk\theta = \theta_k, establish

    n(2n1)3  <  (2n+1)2π2k=1n1k2  <  2n(n+1)3.\frac{n(2n-1)}{3} \;<\; \frac{(2n+1)^2}{\pi^2}\sum_{k=1}^{n}\frac1{k^2} \;<\; \frac{2n(n+1)}{3}.
  2. Conclude (Euler’s theorem, by Cauchy’s proof):

    ζ(2)=k=11k2=π26.\zeta(2) = \sum_{k=1}^{\infty}\frac{1}{k^2} = \frac{\pi^2}{6}.
  3. Extract a rate from the sandwich: show

    k=1n1k2π26=O(1n),\Bigl|\sum_{k=1}^{n}\frac1{k^2} - \frac{\pi^2}6\Bigr| = O\Bigl(\frac1n\Bigr),

    consistent with the exact tail k>nk2=1n12n2+O(n3)\sum_{k>n}k^{-2} = \frac1n - \frac{1}{2n^2} + O(n^{-3}) of Exercise 6.11.

  4. Run the machine one floor higher: using the second Vieta function of PnP_n, show

    k=1ncot4θk=(n(2n1)3) ⁣22n(2n1)(2n2)(2n3)60    8n445,\sum_{k=1}^{n}\cot^4\theta_k = \Bigl(\frac{n(2n-1)}3\Bigr)^{\!2} - \frac{2n(2n-1)(2n-2)(2n-3)}{60} \;\sim\; \frac{8n^4}{45},

    and squeeze with cot4<θ4<(1+cot2)2\cot^4 < \theta^{-4} < (1 + \cot^2)^2 to obtain ζ(4)=π490\zeta(4) = \dfrac{\pi^4}{90}.

Part III — Dividends.

  1. Deduce from ζ(2)=π26\zeta(2) = \frac{\pi^2}6:

    k01(2k+1)2=π28,k1(1)k1k2=π212.\sum_{k\geq0}\frac{1}{(2k+1)^2} = \frac{\pi^2}{8}, \qquad \sum_{k\geq1}\frac{(-1)^{k-1}}{k^2} = \frac{\pi^2}{12}.
  2. Combine with Exercise 7.7: compute S=gcd(a,b)=11a2b2=ζ(2)2ζ(4)=52S = \sum_{\gcd(a,b)=1}\frac{1}{a^2b^2} = \frac{\zeta(2)^2}{\zeta(4)} = \frac52, and interpret 1ζ(2)=6π20.608\frac{1}{\zeta(2)} = \frac{6}{\pi^2} \approx 0.608 as the density of coprime pairs (state the heuristic honestly: the rigorous count is a Year 3 volume matter).
  3. (Certified acceleration) The tail formula of question 9 gives knk2+1n12n2=π26+O(n3)\sum_{k\leq n}k^{-2} + \frac1n - \frac1{2n^2} = \frac{\pi^2}6 + O(n^{-3}). Compare the work needed for six digits of ζ(2)\zeta(2): direct summation versus the corrected sum at n=100n = 100 (where the error is 1.71071.7\cdot10^{-7}).
  4. Check question 4 by hand at n=1n = 1 and n=2n = 2 (the values cot2π3=13\cot^2\frac\pi3 = \frac13 and cot2π5+cot22π5=2\cot^2\frac\pi5 + \cot^2\frac{2\pi}5 = 2), using cosπ5=1+54\cos\frac\pi5 = \frac{1+\sqrt5}4 or a numerical evaluation.
  5. Prove the companion identity

    k=1ntan2kπ2n+1=n(2n+1)\sum_{k=1}^{n}\tan^2\frac{k\pi}{2n+1} = n(2n+1)

    (the numbers tan2θk\tan^2\theta_k are the roots of the reversed polynomial xnPn(1/x)x^nP_n(1/x)), and verify it at n=1n = 1.

Part IV — The Bertrand panorama. For α,βR\alpha, \beta \in \R, consider the Bertrand series

n31nα(lnn)β.\sum_{n \geq 3} \frac{1}{n^{\alpha}(\ln n)^{\beta}} .
  1. Show that for α>1\alpha > 1 the series converges, whatever β\beta (compare with n(1+α)/2n^{-(1+\alpha)/2}).
  2. Show that for α<1\alpha < 1 it diverges, whatever β\beta.
  3. For α=1\alpha = 1: using the series–integral comparison (Theorem 6.6) with f(t)=1t(lnt)βf(t) = \frac{1}{t(\ln t)^\beta}, prove convergence iff β>1\beta > 1.
  4. Iterate the frontier: show 1nlnnlnlnn\sum\frac{1}{n\ln n\,\ln\ln n} diverges while 1nlnn(lnlnn)2\sum\frac{1}{n\ln n\,(\ln\ln n)^2} converges.
  5. Two traps: determine the nature of

    n1n1+1/lnnandn1n1+1/lnlnn\sum_n \frac{1}{n^{1 + 1/\ln n}} \qquad\text{and}\qquad \sum_n \frac{1}{n^{1 + 1/\ln\ln n}}

    (compute n1/lnnn^{1/\ln n} exactly; compare n1/lnlnnn^{1/\ln\ln n} with every power of lnn\ln n).

  6. (No slowest convergent series) Let an\sum a_n be any convergent series with an>0a_n > 0, and Rn=knakR_n = \sum_{k \geq n}a_k its tails. Prove that anRn\sum \frac{a_n}{\sqrt{R_n}} still converges (compare with the telescoping 2(RnRn+1)2(\sqrt{R_n} - \sqrt{R_{n+1}})), although an/Rnan\frac{a_n/\sqrt{R_n}}{a_n} \to \infty: every convergent series is strictly dominated by another convergent series. The frontier of convergence is not a curve but a fog.

Part V — Cross-checks and synthesis.

  1. (Cauchy condensation) Prove: for (an)(a_n) positive decreasing, an\sum a_n converges iff 2ka2k\sum 2^k a_{2^k} converges. Re-derive question 18’s frontier from it.
  2. (The cost of slowness) For 1n(lnn)2\sum\frac1{n(\ln n)^2}, bound the tail by an integral and show that summing up to N=106N = 10^6 still leaves an error larger than 0.070.07: convergence certified by theory can be useless for numerics — contrast with question 13.
  3. Classify (with one-line justifications): 1nlnn\sum\frac1{n\ln n}, 1n1.01\sum\frac1{n^{1.01}}, (lnn)100n1.001\sum\frac{(\ln n)^{100}}{n^{1.001}}, 1n(lnn)(lnlnn)3\sum\frac1{n(\ln n)(\ln\ln n)^{3}}.
  4. (Synthesis) One sentence each: how de Moivre turned a trigonometric identity into a polynomial with computable root sums; where the squeeze needed exact endpoint identities rather than equivalents; which tool of Chapter 6 powered Part IV; and what question 21 says about the dream of a “universal comparison test”. Name the two summits: Euler’s ζ(2)=π26\zeta(2) = \frac{\pi^2}6 (and its floor above, ζ(4)=π490\zeta(4) = \frac{\pi^4}{90}), and the Bertrand classification. Note where ζ(2)\zeta(2) will be proved again: by Parseval in Chapter 14 — one theorem, two civilizations.
Solution

Solution of Problem 7.1.

1. Induction on mm: for m=0m = 0 both sides are 11; the step multiplies by cosθ+isinθ\cos\theta + \iu\sin\theta and uses the addition formulas cos(mθ+θ)=cosmθcosθsinmθsinθ\cos(m\theta + \theta) = \cos m\theta\cos\theta - \sin m\theta\sin\theta, sin(mθ+θ)=sinmθcosθ+cosmθsinθ\sin(m\theta + \theta) = \sin m\theta\cos\theta + \cos m\theta\sin\theta. Expanding instead by the binomial theorem with m=2n+1m = 2n+1 and collecting the imaginary part (the odd powers of isinθ\iu\sin\theta, with i2j+1=(1)ji\iu^{2j+1} = (-1)^j\iu):

sin((2n+1)θ)=j=0n(1)j(2n+12j+1)cos2(nj)θsin2j+1θ.\sin\bigl((2n{+}1)\theta\bigr) = \sum_{j=0}^{n}(-1)^j \binom{2n+1}{2j+1}\cos^{2(n-j)}\theta\,\sin^{2j+1}\theta .

2. On (0,π2)\intoo0{\frac\pi2}, sinθ0\sin\theta \neq 0: factor sin2n+1θ\sin^{2n+1}\theta from each term, leaving (cos2θsin2θ)nj=(cot2θ)nj\bigl(\frac{\cos^2\theta}{\sin^2\theta}\bigr)^{n-j} = (\cot^2\theta)^{n-j}: the displayed identity with Pn(x)=j(1)j(2n+12j+1)xnjP_n(x) = \sum_j(-1)^j\binom{2n+1}{2j+1}x^{n-j}. Its degree-nn coefficient is j=0j = 0’s (2n+11)=2n+10\binom{2n+1}{1} = 2n + 1 \neq 0.

3. At θk=kπ2n+1\theta_k = \frac{k\pi}{2n+1}: sin((2n+1)θk)=sinkπ=0\sin\bigl((2n{+}1)\theta_k\bigr) = \sin k\pi = 0 while sin2n+1θk0\sin^{2n+1}\theta_k \neq 0, so Pn(cot2θk)=0P_n(\cot^2\theta_k) = 0. The θk\theta_k increase strictly in (0,π2)\intoo0{\frac\pi2}, where cot2\cot^2 is strictly decreasing: the values xk=cot2θkx_k = \cot^2\theta_k are pairwise distinct — nn distinct roots of a degree-nn polynomial, hence all of them.

4. Vieta: the sum of the roots is minus the ratio of the xn1x^{n-1}- and xnx^n-coefficients:

k=1ncot2θk=(2n+13)(2n+11)=(2n+1)(2n)(2n1)/62n+1=n(2n1)3.\sum_{k=1}^{n}\cot^2\theta_k = \frac{\binom{2n+1}{3}}{\binom{2n+1}{1}} = \frac{(2n+1)(2n)(2n-1)/6}{2n+1} = \frac{n(2n-1)}{3}.

5. 1sin2θ=1+cot2θ\frac{1}{\sin^2\theta} = 1 + \cot^2\theta: summing, n+n(2n1)3=3n+2n2n3=2n(n+1)3n + \frac{n(2n-1)}3 = \frac{3n + 2n^2 - n}{3} = \frac{2n(n+1)}{3}.

6. On (0,π2)\intoo{0}{\frac\pi2}: sinθ<θ<tanθ\sin\theta < \theta < \tan\theta (Year 1 volume). Taking reciprocals reverses: cotθ<1θ<1sinθ\cot\theta < \frac1\theta < \frac1{\sin\theta}, and squaring (all positive) gives cot2θ<1θ2<1sin2θ\cot^2\theta < \frac1{\theta^2} < \frac1{\sin^2\theta}.

7. Sum question 6 at θ=θk\theta = \theta_k over knk \leq n, using questions 4 and 5, and 1θk2=(2n+1)2k2π2\frac1{\theta_k^2} = \frac{(2n+1)^2}{k^2\pi^2}:

n(2n1)3<(2n+1)2π2k=1n1k2<2n(n+1)3.\frac{n(2n-1)}3 < \frac{(2n+1)^2}{\pi^2}\sum_{k=1}^n\frac1{k^2} < \frac{2n(n+1)}3 .

8. Multiply by π2(2n+1)2\frac{\pi^2}{(2n+1)^2}:

π23n(2n1)(2n+1)2<k=1n1k2<π232n(n+1)(2n+1)2.\frac{\pi^2}{3}\cdot\frac{n(2n-1)}{(2n+1)^2} < \sum_{k=1}^{n}\frac1{k^2} < \frac{\pi^2}{3}\cdot\frac{2n(n+1)}{(2n+1)^2}.

Both bounds tend to π2312=π26\frac{\pi^2}3\cdot\frac12 = \frac{\pi^2}6 (the rational fractions tend to 12\frac12). The partial sums increase, so they converge, and the squeeze gives ζ(2)=π26\zeta(2) = \frac{\pi^2}6: Euler’s theorem, by Cauchy’s proof.

9. The partial sums increase to ζ(2)=π26\zeta(2) = \frac{\pi^2}6, so 0π26knk20 \leq \frac{\pi^2}6 - \sum_{k\leq n}k^{-2}; and the lower bound of question 8 gives

π26kn1k2π26π23n(2n1)(2n+1)2=π26(2n+1)2(4n22n)(2n+1)2=π266n+1(2n+1)2=O(1n),\frac{\pi^2}6 - \sum_{k\leq n}\frac1{k^2} \leq \frac{\pi^2}6 - \frac{\pi^2}3\cdot\frac{n(2n-1)}{(2n+1)^2} = \frac{\pi^2}6\cdot\frac{(2n+1)^2 - (4n^2 - 2n)}{(2n+1)^2} = \frac{\pi^2}6\cdot\frac{6n + 1}{(2n+1)^2} = O\Bigl(\frac1n\Bigr),

matching the exact tail 1n12n2+O(n3)\frac1n - \frac1{2n^2} + O(n^{-3}) of Exercise 6.11.

10. The second elementary symmetric function of the roots is σ2=(2n+15)(2n+11)=(2n)(2n1)(2n2)(2n3)120\sigma_2 = \frac{\binom{2n+1}5}{\binom{2n+1}1} = \frac{(2n)(2n-1)(2n-2)(2n-3)}{120}, so

kcot4θk=σ122σ2=(n(2n1)3)22n(2n1)(2n2)(2n3)604n494n415=8n445.\sum_k\cot^4\theta_k = \sigma_1^2 - 2\sigma_2 = \Bigl(\frac{n(2n-1)}3\Bigr)^2 - \frac{2n(2n-1)(2n-2)(2n-3)}{60} \sim \frac{4n^4}9 - \frac{4n^4}{15} = \frac{8n^4}{45}.

Squeezing cot4θ<θ4<(1+cot2θ)2=1+2cot2θ+cot4θ\cot^4\theta < \theta^{-4} < (1 + \cot^2\theta)^2 = 1 + 2\cot^2\theta + \cot^4\theta and summing: both outer sums are 8n445(1+o(1))\frac{8n^4}{45}(1 + o(1)) (the added n+2σ1=O(n2)n + 2\sigma_1 = O(n^2) is negligible), while the middle is (2n+1)4π4knk4\frac{(2n+1)^4}{\pi^4}\sum_{k\leq n}k^{-4}. Hence

kn1k4π48/4516=π490.\sum_{k\leq n}\frac1{k^4} \longrightarrow \pi^4\cdot\frac{8/45}{16} = \frac{\pi^4}{90}.

11. Splitting ζ(2)\zeta(2) over parities: even=j1(2j)2=14ζ(2)=π224\sum_{\text{even}} = \sum_j\frac{1}{(2j)^2} = \frac14\zeta(2) = \frac{\pi^2}{24}, so odd=ζ(2)π224=π28\sum_{\text{odd}} = \zeta(2) - \frac{\pi^2}{24} = \frac{\pi^2}8. Alternating: k(1)k1k2=oddeven=π28π224=π212\sum_k\frac{(-1)^{k-1}}{k^2} = \sum_{\text{odd}} - \sum_{\text{even}} = \frac{\pi^2}8 - \frac{\pi^2}{24} = \frac{\pi^2}{12} (absolute convergence justifies the regrouping, Theorem 7.11).

12. S=ζ(2)2ζ(4)=(π2/6)2π4/90=9036=52S = \frac{\zeta(2)^2}{\zeta(4)} = \frac{(\pi^2/6)^2}{\pi^4/90} = \frac{90}{36} = \frac52. Heuristic: the identity ζ(2)2=ζ(4)S\zeta(2)^2 = \zeta(4)S of Exercise 7.7 says that pulling out the gcd\gcd renormalizes pairs into coprime pairs; the reciprocal 1ζ(2)=6π20.608\frac1{\zeta(2)} = \frac6{\pi^2} \approx 0.608 is the natural candidate for the density of coprime pairs among all pairs — a statement about limN1N2#{(m,n)N:gcd=1}\lim_N \frac{1}{N^2}\#\{(m,n) \leq N : \gcd = 1\} whose honest proof (with error terms) belongs to the Year 3 volume.

13. Direct summation has error 1n\sim \frac1n: six digits require about 10610^6 terms. The corrected sum knk2+1n12n2\sum_{k\leq n}k^{-2} + \frac1n - \frac1{2n^2} has error O(n3)O(n^{-3}): at n=100n = 100 it equals 1.64493391.6449339\dots against π26=1.6449341\frac{\pi^2}6 = 1.6449341\dots — error 1.71071.7\cdot10^{-7}, seven digits from a hundred terms. Asymptotic corrections beat raw patience by four orders of magnitude.

14. n=1n = 1: P1(x)=3x1P_1(x) = 3x - 1, root 13\frac13, and indeed cot2π3=(13)2=13=113\cot^2\frac\pi3 = \bigl(\frac1{\sqrt3}\bigr)^2 = \frac13 = \frac{1\cdot1}3. n=2n = 2: the formula predicts 233=2\frac{2\cdot3}3 = 2; with cosπ5=1+54\cos\frac\pi5 = \frac{1 + \sqrt5}{4}, one computes cot2361.894\cot^2 36^\circ \approx 1.894 and cot2720.106\cot^2 72^\circ \approx 0.106: sum 2.0002.000.

15. The numbers tan2θk=1xk\tan^2\theta_k = \frac1{x_k} are the roots of Q(x)=xnPn(1x)=j=0n(1)j(2n+12j+1)xjQ(x) = x^nP_n\bigl(\frac1x\bigr) = \sum_{j=0}^n(-1)^j\binom{2n+1}{2j+1}x^j (the xkx_k are nonzero). Vieta on QQ: the leading coefficient is (1)n(-1)^n (term j=nj = n), the next is (1)n1(2n+12n1)=(1)n1(2n+12)(-1)^{n-1}\binom{2n+1}{2n-1} = (-1)^{n-1}\binom{2n+1}{2}, so

k=1ntan2θk=(1)n1(2n+12)(1)n=(2n+12)22n+12n+12=n(2n+1).\sum_{k=1}^n\tan^2\theta_k = -\frac{(-1)^{n-1}\binom{2n+1}2}{(-1)^n} = \binom{2n+1}2\cdot \frac{2}{2n+1}\cdot\frac{2n+1}{2} = n(2n+1).

Check n=1n = 1: tan2π3=3=13\tan^2\frac\pi3 = 3 = 1\cdot3.

16. Let γ=1+α2(1,α)\gamma = \frac{1+\alpha}2 \in \intoo{1}{\alpha}. Then nα(lnn)βnγ=nγα(lnn)β0\frac{n^{-\alpha}(\ln n)^{-\beta}}{n^{-\gamma}} = n^{\gamma - \alpha}(\ln n)^{-\beta} \to 0 (a negative power of nn beats any power of lnn\ln n), so eventually the terms are nγ\leq n^{-\gamma} with γ>1\gamma > 1: convergence by comparison with a Riemann series.

17. Let γ=1+α2(α,1)\gamma = \frac{1+\alpha}2 \in \intoo{\alpha}{1}: now nγnα(lnn)β=nαγ(lnn)β0\frac{n^{-\gamma}}{n^{-\alpha}(\ln n)^{-\beta}} = n^{\alpha-\gamma}(\ln n)^{\beta} \to 0, so eventually the terms are nγ\geq n^{-\gamma} with γ<1\gamma < 1: divergence.

18. f(t)=1t(lnt)βf(t) = \frac1{t(\ln t)^\beta} is positive, continuous, and decreasing for large tt (its logarithm has derivative 1t(1+βlnt)<0-\frac1t\bigl(1 + \frac{\beta}{\ln t}\bigr) < 0 eventually). Antiderivatives: for β1\beta \neq 1, xf=(lnx)1β1β+const\int^x f = \frac{(\ln x)^{1-\beta}}{1-\beta} + \text{const}, which has a finite limit iff β>1\beta > 1; for β=1\beta = 1, xf=lnlnx\int^x f = \ln\ln x \to \infty. By Theorem 6.6, the series and the integral share their nature: convergence iff β>1\beta > 1.

19. Same test:  ⁣d ⁣dtlnlnlnt=1tlntlnlnt\frac{\dd}{\dd t}\ln\ln\ln t = \frac{1}{t\ln t\,\ln\ln t}, and lnlnlnt\ln\ln\ln t \to \infty: divergence. And  ⁣d ⁣dt(1lnlnt)=1tlnt(lnlnt)2\frac{\dd}{\dd t}\Bigl(-\frac1{\ln\ln t}\Bigr) = \frac{1}{t\ln t\,(\ln\ln t)^2} with 1lnlnt0-\frac1{\ln\ln t} \to 0: convergence.

20. First: n1/lnn=elnn/lnn=en^{1/\ln n} = \eu^{\ln n/\ln n} = \eu, so the terms are exactly 1en\frac{1}{\eu\,n}: a multiple of the harmonic series, divergent — the exponent 1+1lnn1 + \frac1{\ln n} crawls to 11 too fast. Second: n1/lnlnn=elnn/lnlnnn^{1/\ln\ln n} = \eu^{\ln n/\ln\ln n}, and lnnlnlnn2lnlnn\frac{\ln n}{\ln\ln n} \geq 2\ln\ln n eventually, so n1/lnlnn(lnn)2n^{1/\ln\ln n} \geq (\ln n)^2: the terms are 1n(lnn)2\leq \frac1{n(\ln n)^2}, a convergent Bertrand series (question 18): convergent. The frontier passes strictly between these two exponents.

21. Rn0R_n \downarrow 0 and

RnRn+1=RnRn+1Rn+Rn+1=anRn+Rn+1an2Rn,\sqrt{R_n} - \sqrt{R_{n+1}} = \frac{R_n - R_{n+1}}{\sqrt{R_n} + \sqrt{R_{n+1}}} = \frac{a_n}{\sqrt{R_n} + \sqrt{R_{n+1}}} \geq \frac{a_n}{2\sqrt{R_n}},

so nanRn2n(RnRn+1)=2R1<\sum_n \frac{a_n}{\sqrt{R_n}} \leq 2\sum_n(\sqrt{R_n} - \sqrt{R_{n+1}}) = 2\sqrt{R_1} < \infty (telescoping). Yet an/Rnan=1Rn\frac{a_n/\sqrt{R_n}}{a_n} = \frac1{\sqrt{R_n}} \to \infty: the new series converges while being infinitely larger. No convergent series is slowest; comparison tests against any fixed family can never be complete.

22. For decreasing positive (an)(a_n), group the terms between consecutive powers of 22:

2ka2k+1n=2k2k+11an2ka2k.2^{k}a_{2^{k+1}} \leq \sum_{n=2^k}^{2^{k+1}-1} a_n \leq 2^ka_{2^k} .

Summing over kk: if 2ka2k\sum 2^ka_{2^k} converges, the partial sums of an\sum a_n are bounded (converges); if an\sum a_n converges, then k2k+1a2k+12nan<\sum_k 2^{k+1}a_{2^{k+1}} \leq 2\sum_n a_n < \infty. For an=1n(lnn)βa_n = \frac1{n(\ln n)^\beta}: 2ka2k=1(kln2)β2^ka_{2^k} = \frac{1}{(k\ln 2)^\beta}, and kβ\sum k^{-\beta} converges iff β>1\beta > 1: the frontier of question 18 again, without integrals.

23. By the integral comparison,

n>N1n(lnn)2N+1 ⁣dtt(lnt)2=1ln(N+1),\sum_{n > N}\frac{1}{n(\ln n)^2} \geq \int_{N+1}^{\infty}\frac{\dd t}{t(\ln t)^2} = \frac{1}{\ln(N+1)},

which at N=106N = 10^6 is 0.0724\approx 0.0724: after a million terms the tail still exceeds 0.070.07 — the series converges, but no direct summation will ever exhibit its sum. Contrast with question 13, where one asymptotic correction bought seven digits from a hundred terms: knowing how a series converges is worth more than knowing that it does.

24. 1nlnn\sum\frac1{n\ln n}: diverges (α=1\alpha = 1, β=1\beta = 1, question 18). 1n1.01\sum\frac1{n^{1.01}}: converges (Riemann, α>1\alpha > 1). (lnn)100n1.001\sum\frac{(\ln n)^{100}}{n^{1.001}}: converges (α=1.001>1\alpha = 1.001 > 1, β=100\beta = -100, question 16). 1nlnn(lnlnn)3\sum\frac1{n\ln n(\ln\ln n)^3}: converges (question 19’s pattern: antiderivative 12(lnlnt)2-\frac12(\ln\ln t)^{-2}, finite limit).

25. De Moivre converts the vanishing of sin(2n+1)θk\sin(2n{+}1) \theta_k into the vanishing of a polynomial at cot2θk\cot^2\theta_k, and Vieta reads off the exact root sums that analysis alone could only estimate (questions 1–5). The squeeze needed the exact values n(2n1)3\frac{n(2n-1)}3 and 2n(n+1)3\frac{2n(n+1)}3 on both sides — equivalents would have begged the question, since the whole point is the constant π26\frac{\pi^2}6 (questions 7–8). Part IV ran entirely on Chapter 6’s series–integral comparison, the logarithmic antiderivatives doing the classifying (questions 18–19). Question 21 destroys the dream of a universal comparison test: below every convergent series lies another, infinitely slower — scales like Bertrand’s map the frontier ever more finely but never reach it. Summits: Euler’s ζ(2)=π26\zeta(2) = \frac{\pi^2}6 with its upper floor ζ(4)=π490\zeta(4) = \frac{\pi^4}{90} (questions 8, 10), and the Bertrand classification (questions 16–18); ζ(2)\zeta(2) returns in Chapter 14, where Parseval’s identity re-proves it in one line from the Fourier series of the sawtooth — one constant, two civilizations.