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) in a normed space E, the series ∑un converges when its partial sums do; it converges absolutely when ∑∥un∥<∞. 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) (or Lc(E), E Banach): for ∣∣∣A∣∣∣<1, the Neumann series∑Ak converges absolutely to (I−A)−1 (proved in Exercise 5.5); ∑k!Ak converges absolutely to eA for every A (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 an and vectors bn, with Bn=∑k=0nbk:
n=0∑Nanbn=aNBN−n=0∑N−1(an+1−an)Bn.
(Abel’s test) If (an) is a real sequence, decreasing to 0, and the partial sums Bn are bounded (in a Banach space), then ∑anbn converges.
Proof. The identity, step by step: with B−1=0, write bn=Bn−Bn−1 and split,
reindexing the second sum by n↦n+1 (the B−1 term vanishes); collecting the common range 0≤n≤N−1 leaves aNBN plus ∑n≤N−1(an−an+1)Bn: the stated formula. It is the discrete integration by parts, with (Bn) as antiderivative of (bn) and the difference an+1−an as derivative of (an). For the test, with ∥Bn∥≤M: the boundary term aNBN→0; the series ∑(an−an+1)Bn converges absolutely, since
n∑∥(an+1−an)Bn∥≤Mn∑(an−an+1)=Ma0<∞
(telescoping, an↓0). Both pieces of the identity converge, hence so does ∑anbn. ∎
Example 7.4
∑nsinn converges: an=n1↓0 and Bn=∑k=1nsink is bounded — indeed Bn=ℑ∑k≤neik=ℑei−1ei(ein−1), of modulus ≤∣ei−1∣2. It does not converge absolutely (∣sinn∣≥sin2n=21−cos2n, and ∑2n1−cos2n diverges since ∑ncos2n converges by the same Abel test while ∑2n1 diverges). The alternating series test is the special case bn=(−1)n.
Example 7.5(Abel on the circle of convergence)
For which complex z with ∣z∣=1 does ∑n≥1nzn converge? At z=1 it is the harmonic series: divergent. For z=1 on the circle, Abel’s test applies with an=n1↓0 and bn=zn, whose partial sums are bounded independently of N:
n=1∑Nzn=z−1z(zN−1)≤∣z−1∣2.
Convergent — though never absolutely (∑n1). 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=−1 it recovers the alternating harmonic series, and at z=eiθ its real and imaginary parts are the series ∑ncosnθ and ∑nsinnθ of Exercise 7.4.
Example 7.6(A booby-trapped alternating series)
Does ∑n≥2n+(−1)n(−1)n converge? The signs alternate and the terms tend to 0 — yet the alternating test does not apply: the moduli n+(−1)n1 are not decreasing (they jump up at each odd n). Expand instead:
The first piece converges (alternating test, honestly applied to n1↓0), the third converges absolutely — but the middle piece is the divergent harmonic series: the sum diverges to −∞. The closing insight: when monotonicity fails, expand until every piece is either absolutely convergent or a clean test case; the hidden −n1 is invisible to sign-counting.
Remark 7.7(Common pitfalls)
(i) “Terms tend to 0” 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 ∑n+1(−1)n squared, the diagonal terms satisfy
∣ck∣=m=0∑k(m+1)(k−m+1)1≥(k+1)⋅k+22⟶2=0
(each factor is at most 2k+2 by AM–GM), so ∑ck 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 I be a countable index set. A family (ui)i∈I of nonnegative reals is summable when the finite partial sums are bounded; its sum is
i∈I∑ui=F⊆I finitesupi∈F∑ui∈[0,+∞].
A family of reals or complexes (or Banach vectors) is summable when (∥ui∥) is; its sum is then defined by splitting into positive/negative (or real/imaginary) parts — equivalently, as the common value of ∑nuσ(n) over all enumerations σ of I (see below).
Method 7.9(Choosing a test)
Facing ∑un, in order: (1) if un→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, einθ, 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>0 is the family ((m+n)−s)m,n≥1summable? Group the finite partial sums by diagonals m+n=k: the diagonal k carries k−1 pairs, each contributing k−s, so the finite sums are exactly bounded by (and exhaust)
k≥2∑ksk−1,
a series with positive terms equivalent to k1−s: summable iff s−1>1, i.e. s>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) is not summable: on the diagonal m+n=k, each term is at least k−2, and (k−1)⋅k−2 sums like the harmonic series.)
Theorem 7.11(Summability and order)
For nonnegative families, the sum is invariant under any enumeration: ∑iui=∑n=0∞uσ(n) for every bijection σ:N→I.
A real or complex series ∑un is commutatively convergent (every rearrangement converges, with the same sum) if and only if it is absolutely convergent.
Proof. (1) Every partial sum ∑n≤Nuσ(n) is a finite partial sum of the family (so ≤ the sup); every finite F is contained in some {σ(0),…,σ(N)} (so the sup ≤ the series’ limit). The two bounds match.
(2) If ∑∣un∣<∞: for any rearrangement σ and ε>0, choose N with ∑n>N∣un∣≤ε; beyond the rank where σ has exhausted [[0,N]], the rearranged partial sums differ from the original limit by at most ε: same sum. If ∑∣un∣=∞ but ∑un 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 ∑n≥1n(−1)n−1=ln2 (Year 1 volume). Rearrange it as “one positive, two negatives”:
1−21−41+31−61−81+51−⋯
Grouping each block of three,
2k−11−4k−21−4k1=4k−21−4k1=21(2k−11−2k1),
so the rearranged series converges to 21ln2 — 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:
(1−1)+(1−1)+(1−1)+⋯=0+0+⋯=0,
yet the ungrouped 1−1+1−1+⋯ diverges (partial sums oscillate between 1 and 0). Ungrouping is legitimate only with a compensating hypothesis — for instance, terms tending to 0 with bounded group lengths: then between two grouped partial sums the original ones drift by at most a sum of 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 be a summable double family (i.e. supF∑F∣um,n∣<∞). Then
all inner series converging (absolutely). In particular, if ∑am and ∑bn converge absolutely, their Cauchy product converges absolutely with
(m∑am)(n∑bn)=k=0∑∞ck,ck=m=0∑kambk−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: ∑m≤M∑n≤Num,n≤S gives, letting N→∞ then M→∞, ∑m∑num,n≤S; conversely every finite F sits in such a rectangle, so S≤∑m∑num,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∣.
Cauchy product. The family um,n=ambn is summable: finite partial sums of ∣ambn∣ are bounded by (∑∣am∣)(∑∣bn∣). Rows give (∑am)(∑bn); diagonals give ∑kck. ∎
by the binomial theorem on each diagonal: eaeb=ea+b — the functional equation of 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 ∑n≥1nzn=(1−z)2z (∣z∣<1), one more Cauchy product finishes the second moment. Multiply ∑mmzm by ∑nzn: the diagonal coefficient is ∑m=0km=2k(k+1), so
(1−z)3z=k≥0∑2k(k+1)zk,
and the identity n2=2⋅2n(n+1)−n assembles
n≥1∑n2zn=(1−z)32z−(1−z)2z=(1−z)3z(1+z).
At z=21: ∑n≥12nn2=8121⋅23=6 — a closed value with no differentiation anywhere, just absolutely convergent series multiplied like polynomials. The same telescoping of identities computes every ∑ndzn, and probabilists will recognize the second factorial moment of the geometric law (Chapter 23).
Example 7.17(A double-sum evaluation)
For s>1 real, let ζ(s)=∑n≥1n−s. Counting divisors by double summation — the family (m−sn−s) over (m,n)∈(N∗)2 is summable (product of convergent positive series) — and grouping by the product q=mn:
ζ(s)2=m,n∑(mn)s1=q=1∑∞qsd(q),
where d(q) is the number of divisors of q. Summable families turn combinatorics into analysis.
Example 7.18(A Fubini evaluation: ∑n(ζ(n)−1)=1)
For integer n≥2, ζ(n)−1=∑k≥2k−n. The double family (k−n)k,n≥2 is summable: summing the geometric columns first,
k≥2∑n≥2∑kn1=k≥2∑1−1/k1/k2=k≥2∑k(k−1)1=1
(telescoping), and all terms are positive, so Theorem 7.14 authorizes summing by rows instead:
n≥2∑(ζ(n)−1)=1.
The infinitely many ζ-values, each transcendental-looking, have tails that add up to exactly 1. 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]),∥⋅∥∞), solve x−K(x)=y where K(f) is the constant function 21∫01f. The operator norm is ∣∣∣K∣∣∣≤21<1, so the Neumann series applies (Example 7.2): x=∑n≥0Kn(y). Compute the iterates: K(y)=21∫01y (a constant), and applying K to a constant c gives 2c, so Kn(y)=2n−11⋅21∫01y for n≥1. Summing the geometric constants:
x=y+(∫01y)n≥1∑2n1=y+∫01y.
Check: x−K(x)=y+∫y−21(∫y+∫y)=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
n(n+1)(n+2)1=21(n(n+1)1−(n+1)(n+2)1),
(check by reduction to the common denominator), so the partial sums collapse:
n=1∑Nn(n+1)(n+2)1=21(1⋅21−(N+1)(N+2)1)⟶41.
The same pattern — write the term as c(un−un+1) for an explicit (un) — solved Exercise 7.10 (arctangents) and computes every ∑n(n+1)⋯(n+k)1=k⋅k!1. 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 is absolute convergence of ∑∥fn∥∞ in the Banach space(C,∥⋅∥∞) — 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: ∑ncosn; ∑lnn(−1)n; ∑n3/4+cosn(−1)n(expand as in the Year 1 trap: the alternating test needs monotonicity).
Solution
Solution of Exercise 7.1.
∑ncosn: Abel’s test with an=n1 and bn=cosn, whose partial sums are bounded (real part of a geometric sum, as in Example 7.4): convergent (not absolutely, by the same cos2 trick).
∑lnn(−1)n (n≥2): alternating test, lnn1↓0: convergent; not absolutely (lnn≤n).
0<α≤1: Abel’s test applies (an=n−α↓0; partial sums of sinnθ bounded by ∣sin(θ/2)∣1, geometric sum): convergent. Not absolutely: ∣sinnθ∣≥sin2nθ=21−cos2nθ, and ∑2nα1−cos2nθ diverges (∑n−α diverges; ∑nαcos2nθ converges by Abel when 2θ∈/2πZ; the excluded case 2θ∈2πZ means θ∈πZ, already handled). Semi-convergent.
Exercise 7.5★★★
(Riemann rearrangement) Let ∑un be a convergent but not absolutely convergent real series, and ℓ∈R. Prove that some rearrangement of ∑un converges to ℓ. (Show both subseries of positive and negative terms diverge; then greedily alternate: take positive terms until exceeding ℓ, then negative until dropping below, and so on; the terms tend to 0, forcing convergence to ℓ.)
Solution
Solution of Exercise 7.5.
Let p1,p2,… be the nonnegative terms of (un) in order, q1,q2,… the negative ones. Both ∑pk and ∑qk diverge: if one of them converged, the other would equal the convergent ∑un minus it, hence converge too — and then ∑∣un∣=∑pk−∑qk would converge, contradicting the hypothesis. Also un→0 (∑un converges).
Greedy rearrangement: take positive terms p1,p2,… until the running total first exceeds ℓ (possible: ∑pk=+∞); then negative terms until the total first drops below ℓ (possible: ∑qk=−∞); 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 ℓ is at most the last term used; since the terms used at the m-th switch have index →∞, and un→0, the running totals converge to ℓ.
Exercise 7.6★★
Prove that the family (m!n!xm+n)(m,n)∈N2 is summable for every x∈R, and re-derive the identity (ex)2=e2x by grouping the double sum along the diagonals m+n=k.
Solution
Solution of Exercise 7.6.
Summability: the finite partial sums of m!n!∣x∣m+n are bounded by (∑mm!∣x∣m)2=e2∣x∣. Diagonal grouping (Theorem 7.14):
Prove that the family (m2n21)m,n≥1 is summable, and that grouping by gcd: with q=gcd(m,n),
ζ(2)2=q≥1∑q41a,b≥1gcd(a,b)=1∑a2b21=ζ(4)⋅S,
where S=∑gcd(a,b)=1a2b21: deduce S=ζ(2)2/ζ(4). (Every pair (m,n) writes uniquely (qa,qb) with gcd(a,b)=1.)
Solution
Solution of Exercise 7.7.
Summability: bounded by ζ(2)2 as a product family (Theorem 7.14’s Cauchy-product argument). The map (q,a,b)↦(qa,qb), from triples with gcd(a,b)=1 to pairs (m,n), is a bijection (set 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):
(With the values ζ(2)=6π2, ζ(4)=90π4 from Chapter 14: S=25.)
Exercise 7.8★★★
(Abel’s theorem on products, light version) Suppose ∑an converges absolutely and ∑bn converges. Prove that their Cauchy product∑cn converges, with ∑cn=(∑an)(∑bn). (Write CN=∑k≤Nck=∑nanBN−n with B the partial sums of b; split according to n≤N/2 or not, using boundedness of (Bm) and the absolute tail of (an).)
Solution
Solution of Exercise 7.8.
Let A=∑an (absolute), Bm=∑k≤mbk→B, bounded by M. Then
CN=k=0∑Nck=n=0∑NanBN−n
(collect by the index of a). Write
CN−AB=n=0∑Nan(BN−n−B)−Bn>N∑an.
The last term tends to 0. Split the sum at n=⌊N/2⌋: for n≤N/2, N−n≥N/2, so ∣BN−n−B∣≤εN:=supm≥N/2∣Bm−B∣→0, and this part is ≤εN∑∣an∣; for n>N/2, ∣BN−n−B∣≤2M, and this part is ≤2M∑n>N/2∣an∣→0. Hence CN→AB.
Exercise 7.9★★★
In the (non-complete) space E of eventually-zero real sequences with the sup norm, exhibit an absolutely convergent series that does not converge in E. (Try un=2−nen with (en) the canonical sequences.)
Solution
Solution of Exercise 7.9.
Take un=2−nen (en the sequence with a single 1 in position n). Then ∑∥un∥∞=∑2−n<∞: absolutely convergent. But the partial sums SN=(1,21,…,2−N,0,…) would have to converge to the sequence (2−n)n, which is not eventually zero: outside E. Inside E, (SN) is Cauchy without limit (∥SN−x∥∞≥2−N−1 fails to help any eventually-zero x: for any x∈E vanishing beyond rank K, ∥SN−x∥≥2−K−1 for N>K): the series does not converge in E. Completeness is exactly what Theorem 5.21 needs.
Exercise 7.10★★
Verify the identity arctan(n+1)−arctan(n)=arctann2+n+11, and deduce the exact value of
n=1∑∞arctann2+n+11.
Solution
Solution of Exercise 7.10.
Both arctan(n+1)−arctann and arctann2+n+11 lie in (0,2π), and the tangent addition formula gives
First: n+1−n=n+1+n1∼2n1, so the terms are ∼2−αn−α/2: convergence iff 2α>1, i.e. α>2. Second: 1−cosn1∼2n21: converges. Third: (1+n1)n=enln(1+1/n)=e1−2n1+O(n−2)=e(1−2n1+O(n−2)), so
e−(1+n1)n∼2ne:
positive terms equivalent to a harmonic multiple: diverges.
Exercise 7.12★★★
Let (an) be positive and decreasing with ∑an convergent. Prove that nan→0(bound na2n by a tail). Show that the converse fails, and that monotonicity is essential, with explicit counterexamples.
Solution
Solution of Exercise 7.12.
By monotonicity, na2n≤an+1+an+2+⋯+a2n=S2n−Sn→0 (Cauchy criterion for the convergent series). Hence 2na2n→0, and (2n+1)a2n+1≤(2n+1)a2n=2n2n+1(2na2n)→0: both subsequences of (nan) tend to 0, so nan→0.
Converse fails:an=nlnn1 is positive decreasing with nan=lnn1→0, yet ∑an diverges (Bertrand frontier, Problem 7.1, question 18). Monotonicity essential: let an=n1 when n is a power of 2 and an=2−n otherwise: ∑an≤∑k2−k+∑n2−n<∞, but nan=1 along the powers of 2: nan→0.
7.5 Problem: Euler’s ζ(2)=π2/6, by Cauchy’s Cotangent Sum
Euler’s most famous identity, 1+41+91+⋯=6π2, admits a completely elementary proof, due to Cauchy: de Moivre’s formula produces a polynomial whose roots are the numbers cot22n+1kπ, Vieta sums those roots exactly, and the squeeze cot2θ<θ21<1+cot2θ crushes the partial sums of ∑k21 between two explicit rational bounds. We run the proof in full, extract ζ(4)=90π4 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 and the Bertrand panorama
Throughout, n≥1 and θk=2n+1kπ for k=1,…,n; note 0<θk<2π.
Part I — The cotangent identity.
Prove de Moivre’s formula (cosθ+isinθ)m=cosmθ+isinmθ (m∈N), and deduce, for m=2n+1,
and squeeze with cot4<θ−4<(1+cot2)2 to obtain ζ(4)=90π4.
Part III — Dividends.
Deduce from ζ(2)=6π2:
k≥0∑(2k+1)21=8π2,k≥1∑k2(−1)k−1=12π2.
Combine with Exercise 7.7: compute S=∑gcd(a,b)=1a2b21=ζ(4)ζ(2)2=25, and interpret ζ(2)1=π26≈0.608 as the density of coprime pairs (state the heuristic honestly: the rigorous count is a Year 3 volume matter).
(Certified acceleration) The tail formula of question 9 gives ∑k≤nk−2+n1−2n21=6π2+O(n−3). Compare the work needed for six digits of ζ(2): direct summation versus the corrected sum at n=100 (where the error is 1.7⋅10−7).
Check question 4 by hand at n=1 and n=2 (the values cot23π=31 and cot25π+cot252π=2), using cos5π=41+5 or a numerical evaluation.
Prove the companion identity
k=1∑ntan22n+1kπ=n(2n+1)
(the numbers tan2θk are the roots of the reversed polynomial xnPn(1/x)), and verify it at n=1.
Part IV — The Bertrand panorama. For α,β∈R, consider the Bertrand series
n≥3∑nα(lnn)β1.
Show that for α>1 the series converges, whatever β(compare with n−(1+α)/2).
Show that for α<1 it diverges, whatever β.
For α=1: using the series–integral comparison (Theorem 6.6) with f(t)=t(lnt)β1, prove convergence iff β>1.
Iterate the frontier: show ∑nlnnlnlnn1 diverges while ∑nlnn(lnlnn)21 converges.
Two traps: determine the nature of
n∑n1+1/lnn1andn∑n1+1/lnlnn1
(compute n1/lnn exactly; compare n1/lnlnn with every power of lnn).
(No slowest convergent series) Let ∑an be any convergent series with an>0, and Rn=∑k≥nak its tails. Prove that ∑Rnan still converges(compare with the telescoping 2(Rn−Rn+1)), although anan/Rn→∞: 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.
(Cauchy condensation) Prove: for (an) positive decreasing, ∑an converges iff ∑2ka2k converges. Re-derive question 18’s frontier from it.
(The cost of slowness) For ∑n(lnn)21, bound the tail by an integral and show that summing up to N=106 still leaves an error larger than 0.07: convergence certified by theory can be useless for numerics — contrast with question 13.
(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)=6π2 (and its floor above, ζ(4)=90π4), and the Bertrand classification. Note where ζ(2) will be proved again: by Parseval in Chapter 14 — one theorem, two civilizations.
Solution
Solution of Problem 7.1.
1. Induction on m: for m=0 both sides are 1; the step multiplies by cosθ+isinθ and uses the addition formulas cos(mθ+θ)=cosmθcosθ−sinmθsinθ, sin(mθ+θ)=sinmθcosθ+cosmθsinθ. Expanding instead by the binomial theorem with m=2n+1 and collecting the imaginary part (the odd powers of isinθ, with i2j+1=(−1)ji):
2. On (0,2π), sinθ=0: factor sin2n+1θ from each term, leaving (sin2θcos2θ)n−j=(cot2θ)n−j: the displayed identity with Pn(x)=∑j(−1)j(2j+12n+1)xn−j. Its degree-n coefficient is j=0’s (12n+1)=2n+1=0.
3. At θk=2n+1kπ: sin((2n+1)θk)=sinkπ=0 while sin2n+1θk=0, so Pn(cot2θk)=0. The θk increase strictly in (0,2π), where cot2 is strictly decreasing: the values xk=cot2θk are pairwise distinct — n distinct roots of a degree-n polynomial, hence all of them.
4. Vieta: the sum of the roots is minus the ratio of the xn−1- and xn-coefficients:
Both bounds tend to 3π2⋅21=6π2 (the rational fractions tend to 21). The partial sums increase, so they converge, and the squeeze gives ζ(2)=6π2: Euler’s theorem, by Cauchy’s proof.
9. The partial sums increase to ζ(2)=6π2, so 0≤6π2−∑k≤nk−2; and the lower bound of question 8 gives
Squeezing cot4θ<θ−4<(1+cot2θ)2=1+2cot2θ+cot4θ and summing: both outer sums are 458n4(1+o(1)) (the added n+2σ1=O(n2) is negligible), while the middle is π4(2n+1)4∑k≤nk−4. Hence
k≤n∑k41⟶π4⋅168/45=90π4.
11. Splitting ζ(2) over parities: ∑even=∑j(2j)21=41ζ(2)=24π2, so ∑odd=ζ(2)−24π2=8π2. Alternating: ∑kk2(−1)k−1=∑odd−∑even=8π2−24π2=12π2 (absolute convergence justifies the regrouping, Theorem 7.11).
12.S=ζ(4)ζ(2)2=π4/90(π2/6)2=3690=25. Heuristic: the identity ζ(2)2=ζ(4)S of Exercise 7.7 says that pulling out the gcd renormalizes pairs into coprime pairs; the reciprocal ζ(2)1=π26≈0.608 is the natural candidate for the density of coprime pairs among all pairs — a statement about limNN21#{(m,n)≤N:gcd=1} whose honest proof (with error terms) belongs to the Year 3 volume.
13. Direct summation has error ∼n1: six digits require about 106 terms. The corrected sum ∑k≤nk−2+n1−2n21 has error O(n−3): at n=100 it equals 1.6449339… against 6π2=1.6449341… — error 1.7⋅10−7, seven digits from a hundred terms. Asymptotic corrections beat raw patience by four orders of magnitude.
14.n=1: P1(x)=3x−1, root 31, and indeed cot23π=(31)2=31=31⋅1. n=2: the formula predicts 32⋅3=2; with cos5π=41+5, one computes cot236∘≈1.894 and cot272∘≈0.106: sum 2.000.
15. The numbers tan2θk=xk1 are the roots of Q(x)=xnPn(x1)=∑j=0n(−1)j(2j+12n+1)xj (the xk are nonzero). Vieta on Q: the leading coefficient is (−1)n (term j=n), the next is (−1)n−1(2n−12n+1)=(−1)n−1(22n+1), so
16. Let γ=21+α∈(1,α). Then n−γn−α(lnn)−β=nγ−α(lnn)−β→0 (a negative power of n beats any power of lnn), so eventually the terms are ≤n−γ with γ>1: convergence by comparison with a Riemann series.
17. Let γ=21+α∈(α,1): now n−α(lnn)−βn−γ=nα−γ(lnn)β→0, so eventually the terms are ≥n−γ with γ<1: divergence.
18.f(t)=t(lnt)β1 is positive, continuous, and decreasing for large t (its logarithm has derivative −t1(1+lntβ)<0 eventually). Antiderivatives: for β=1, ∫xf=1−β(lnx)1−β+const, which has a finite limit iff β>1; for β=1, ∫xf=lnlnx→∞. By Theorem 6.6, the series and the integral share their nature: convergence iff β>1.
19. Same test: dtdlnlnlnt=tlntlnlnt1, and lnlnlnt→∞: divergence. And dtd(−lnlnt1)=tlnt(lnlnt)21 with −lnlnt1→0: convergence.
20. First: n1/lnn=elnn/lnn=e, so the terms are exactly en1: a multiple of the harmonic series, divergent — the exponent 1+lnn1 crawls to 1 too fast. Second: n1/lnlnn=elnn/lnlnn, and lnlnnlnn≥2lnlnn eventually, so n1/lnlnn≥(lnn)2: the terms are ≤n(lnn)21, a convergent Bertrand series (question 18): convergent. The frontier passes strictly between these two exponents.
so ∑nRnan≤2∑n(Rn−Rn+1)=2R1<∞ (telescoping). Yet anan/Rn=Rn1→∞: 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), group the terms between consecutive powers of 2:
2ka2k+1≤n=2k∑2k+1−1an≤2ka2k.
Summing over k: if ∑2ka2k converges, the partial sums of ∑an are bounded (converges); if ∑an converges, then ∑k2k+1a2k+1≤2∑nan<∞. For an=n(lnn)β1: 2ka2k=(kln2)β1, and ∑k−β converges iff β>1: the frontier of question 18 again, without integrals.
23. By the integral comparison,
n>N∑n(lnn)21≥∫N+1∞t(lnt)2dt=ln(N+1)1,
which at N=106 is ≈0.0724: after a million terms the tail still exceeds 0.07 — 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.
25. De Moivre converts the vanishing of sin(2n+1)θk into the vanishing of a polynomial at cot2θk, and Vieta reads off the exact root sums that analysis alone could only estimate (questions 1–5). The squeeze needed the exact values 3n(2n−1) and 32n(n+1) on both sides — equivalents would have begged the question, since the whole point is the constant 6π2 (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)=6π2 with its upper floor ζ(4)=90π4 (questions 8, 10), and the Bertrand classification (questions 16–18); ζ(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.