Wiskunde · Book 3 · Bachelor jaar 1

University Mathematics — Year 1

University Mathematics — Year 1 · Bachelor jaar 1

11Sequences

Sequences were manipulated in the High School volume with the limit concept taken half on faith. Here the theory is rebuilt on the completeness of R\R (Chapter 10): every classical theorem — monotone convergence, adjacent sequences, Bolzano–Weierstrass, the Cauchy criterion — is a face of that single axiom. The chapter ends with the practical study of sequences defined by un+1=f(un)u_{n+1} = f(u_n).

11.1 Convergence

Definition 11.1 (Limit of a sequence)

A sequence (un)(u_n) of reals converges to ℓ∈R\ell \in \R when

∀ε>0, ∃N∈N, ∀n≥N,∣un−ℓ∣≤ε.\forall \varepsilon > 0,\ \exists N \in \N,\ \forall n \geq N, \qquad \abs{u_n - \ell} \leq \varepsilon .

One writes un→ℓu_n \to \ell or lim⁡un=ℓ\lim u_n = \ell. A sequence that does not converge (to any real) diverges. Divergence to +∞+\infty: ∀M, ∃N, ∀n≥N, un≥M\forall M,\ \exists N,\ \forall n \geq N,\ u_n \geq M (similarly −∞-\infty).

Example 11.2 (An ε\varepsilon–NN proof, written out once)

Claim: un=n2+12n2−3→12u_n = \dfrac{n^2 + 1}{2n^2 - 3} \to \dfrac12. First isolate the error:

∣un−12∣=∣2(n2+1)−(2n2−3)2(2n2−3)∣=52 ∣2n2−3∣=52 (2n2−3)(n≥2).\Bigl| u_n - \frac12 \Bigr| = \Bigl| \frac{2(n^2 + 1) - (2n^2 - 3)}{2(2n^2 - 3)} \Bigr| = \frac{5}{2\,\abs{2n^2 - 3}} = \frac{5}{2\,(2n^2 - 3)} \quad (n \geq 2).

Then dominate it by something simple: for n≥2n \geq 2, 2n2−3≥n22n^2 - 3 \geq n^2, so the error is ≤52n2≤52n\leq \frac{5}{2n^2} \leq \frac 5{2n}. Given ε>0\varepsilon > 0, the Archimedean property provides N≥max⁡(2,52ε)N \geq \max\bigl(2, \frac{5}{2\varepsilon}\bigr); for n≥Nn \geq N the error is ≤ε\leq \varepsilon. Done. The closing insight: an ε\varepsilon–NN proof has exactly three moves — compute the error, bound it by a decreasing elementary expression, solve for the threshold — and after this chapter’s theorems (operations, squeeze) one almost never writes such a proof again: the theorems package the three moves once and for all.

Example 11.3 (Divergence to infinity, certified)

Claim: un=n2−100n→+∞u_n = n^2 - 100n \to +\infty. Factor the dominant term: un=n2(1−100n)≥n22u_n = n^2\bigl(1 - \frac{100}{n}\bigr) \geq \frac{n^2}{2} for n≥200n \geq 200. Given MM, take N=max⁡(200,⌈2M⌉)N = \max\bigl(200, \lceil\sqrt{2M}\rceil\bigr): for n≥Nn \geq N, un≥n22≥Mu_n \geq \frac{n^2}{2} \geq M. Two habits are on display: dominant-term factoring converts a competition (n2n^2 against −100n-100n) into a single scale times a factor tending to 11; and the threshold may be huge (u100=0u_{100} = 0, the sequence is even negative before n=100n = 100) — divergence to +∞+\infty is a statement about the tail, indifferent to any finite amount of misbehavior.

Proposition 11.4 (First properties)

  1. The limit, if it exists, is unique.
  2. A convergent sequence is bounded.
  3. If un→ℓu_n \to \ell, every modification of finitely many terms leaves the convergence and the limit unchanged.

Proof. (1) If un→ℓu_n \to \ell and un→ℓ′u_n \to \ell' with ℓ≠ℓ′\ell \neq \ell', take ε=∣ℓ−ℓ′∣3\varepsilon = \frac{\abs{\ell - \ell'}}{3}: beyond the two thresholds, ∣ℓ−ℓ′∣≤∣ℓ−un∣+∣un−ℓ′∣≤2ε=23∣ℓ−ℓ′∣\abs{\ell - \ell'} \leq \abs{\ell - u_n} + \abs{u_n - \ell'} \leq 2\varepsilon = \frac23 \abs{\ell - \ell'}, absurd.

(2) With ε=1\varepsilon = 1: beyond NN, ∣un∣≤∣ℓ∣+1\abs{u_n} \leq \abs\ell + 1; the finitely many earlier terms are bounded too, so ∣un∣≤max⁡(∣u0∣,…,∣uN−1∣,∣ℓ∣+1)\abs{u_n} \leq \max(\abs{u_0}, \dots, \abs{u_{N-1}}, \abs\ell + 1).

(3) In detail: suppose vn=unv_n = u_n for n≥n0n \geq n_0 and un→ℓu_n \to \ell. Given ε>0\varepsilon > 0, take the threshold NN for (un)(u_n): for n≥max⁡(N,n0)n \geq \max(N, n_0), ∣vn−ℓ∣=∣un−ℓ∣≤ε\abs{v_n - \ell} = \abs{u_n - \ell} \leq \varepsilon. So vn→ℓv_n \to \ell: the definition quantifies only over n≥Nn \geq N, and any finite prefix can be overwritten at the cost of enlarging the threshold. (This is why hypotheses “for all large nn” suffice everywhere in this chapter.) ∎

Theorem 11.5 (Operations on limits)

If un→ℓu_n \to \ell and vn→mv_n \to m, then

un+vn→ℓ+m,unvn→ℓm,unvn→ℓm (if m≠0),∣un∣→∣ℓ∣.u_n + v_n \to \ell + m, \qquad u_n v_n \to \ell m, \qquad \frac{u_n}{v_n} \to \frac{\ell}{m} \ (\text{if } m \neq 0), \qquad \abs{u_n} \to \abs\ell .

Proof. Sum: ∣(un+vn)−(ℓ+m)∣≤∣un−ℓ∣+∣vn−m∣≤2ε\abs{(u_n + v_n) - (\ell + m)} \leq \abs{u_n - \ell} + \abs{v_n - m} \leq 2\varepsilon beyond the larger threshold. Product: write

unvn−ℓm=(un−ℓ) vn+ℓ (vn−m);u_n v_n - \ell m = (u_n - \ell)\,v_n + \ell\,(v_n - m);

(vn)(v_n) is bounded by some BB (Proposition 11.4), so the right side is ≤B∣un−ℓ∣+∣ℓ∣ ∣vn−m∣\leq B\abs{u_n - \ell} + \abs{\ell}\,\abs{v_n - m}, arbitrarily small. Quotient: it suffices to treat 1vn\frac 1{v_n}. With ε=∣m∣2\varepsilon = \frac{\abs m}{2}: beyond some N0N_0, ∣vn∣≥∣m∣2\abs{v_n} \geq \frac{\abs m}{2}, so

∣1vn−1m∣=∣m−vn∣∣vnm∣≤2m2 ∣vn−m∣⟶0.\Bigl| \frac{1}{v_n} - \frac 1m \Bigr| = \frac{\abs{m - v_n}}{\abs{v_n m}} \leq \frac{2}{m^2}\,\abs{v_n - m} \longrightarrow 0 .

Absolute value: ∣∣un∣−∣ℓ∣∣≤∣un−ℓ∣\bigl|\abs{u_n} - \abs\ell\bigr| \leq \abs{u_n - \ell} (reverse triangle inequality, Proposition 3.2). ∎

Example 11.6 (Operations plus one algebraic trick)

Compute lim⁡ (n2+n−n)\lim\,\bigl(\sqrt{n^2 + n} - n\bigr). The two pieces separately tend to +∞+\infty: the operations theorem says nothing about their difference (an indeterminate form). Multiply by the conjugate:

n2+n−n=(n2+n)−n2n2+n+n=nn2+n+n=11+1n+1.\sqrt{n^2 + n} - n = \frac{(n^2 + n) - n^2}{\sqrt{n^2 + n} + n} = \frac{n}{\sqrt{n^2+n} + n} = \frac{1}{\sqrt{1 + \frac1n} + 1} .

Now everything converges: 1+1n→1\sqrt{1 + \frac1n} \to 1, because 0≤1+h−1=h1+h+1≤h0 \leq \sqrt{1 + h} - 1 = \frac{h}{\sqrt{1+h} + 1} \leq h (conjugate again, then squeeze with h=1nh = \frac1n); then the operations theorem gives the limit 11+1=12\frac{1}{1 + 1} = \frac12. The closing insight: the operations theorem is not a calculator for all limits — indeterminate forms (∞−∞\infty - \infty, 00\frac00, 0×∞0 \times \infty, 1∞1^\infty) must first be transformed by algebra (conjugates, factoring the dominant term) until every piece converges; the systematic machine for resistant cases is the asymptotic expansion of Chapter 16.

Theorem 11.7 (Limits and order)

  1. If un≤vnu_n \leq v_n for all large nn, and both converge, then lim⁡un≤lim⁡vn\lim u_n \leq \lim v_n. (Strict inequalities do not pass to the limit: 1n>0\frac 1n > 0 but lim⁡=0\lim = 0.)
  2. (Squeeze theorem) If un≤wn≤vnu_n \leq w_n \leq v_n for all large nn and un,vn→ℓu_n, v_n \to \ell, then wn→ℓw_n \to \ell.
  3. If un→ℓ>0u_n \to \ell > 0, then un>ℓ2>0u_n > \frac\ell2 > 0 for all large nn.

Proof. (1) Suppose ℓ=lim⁡un>m=lim⁡vn\ell = \lim u_n > m = \lim v_n; with ε=ℓ−m3\varepsilon = \frac{\ell - m}{3}, large terms satisfy vn≤m+ε<ℓ−ε≤unv_n \leq m + \varepsilon < \ell - \varepsilon \leq u_n, contradicting un≤vnu_n \leq v_n.

(2) Beyond the thresholds: ℓ−ε≤un≤wn≤vn≤ℓ+ε\ell - \varepsilon \leq u_n \leq w_n \leq v_n \leq \ell + \varepsilon.

(3) is Definition 11.1 with ε=ℓ2\varepsilon = \frac\ell2. ∎

Example 11.8 (Two squeezes)

(i) sin⁡nn→0\dfrac{\sin n}{n} \to 0: from −1n≤sin⁡nn≤1n-\frac1n \leq \frac{\sin n}{n} \leq \frac1n, both walls collapsing on 00 — no need to understand the erratic numerator at all. (ii) (2n+3n)1/n→3(2^n + 3^n)^{1/n} \to 3: frame the inside,

3n≤2n+3n≤2⋅3n⟹3≤(2n+3n)1/n≤3⋅21/n,3^n \leq 2^n + 3^n \leq 2\cdot3^n \quad\Longrightarrow\quad 3 \leq (2^n + 3^n)^{1/n} \leq 3\cdot 2^{1/n} ,

and 21/n=eln⁡2n→12^{1/n} = \eu^{\frac{\ln 2}{n}} \to 1 (as for 51/n5^{1/n} in Exercise 11.2): the squeeze delivers 33. The closing insight: a sum of competing exponentials behaves like its largest term — the smaller ones are absorbed by a harmless constant factor, which the nn-th root then erases.

11.2 Monotone sequences

Theorem 11.9 (Monotone limit theorem)

An increasing sequence bounded above converges, to sup⁡{un:n∈N}\sup\{u_n : n \in \N\}; an increasing sequence not bounded above diverges to +∞+\infty. (Mirror statements for decreasing sequences.)

Proof. Let s=sup⁡{un}s = \sup\{u_n\} (Theorem 10.2). Given ε>0\varepsilon > 0, the ε\varepsilon-characterization (Proposition 10.4) yields NN with uN>s−εu_N > s - \varepsilon; by monotonicity, s−ε<uN≤un≤ss - \varepsilon < u_N \leq u_n \leq s for all n≥Nn \geq N: convergence to ss. If unbounded: for every MM some uN>Mu_N > M, and monotonicity keeps all later terms above MM. ∎

Example 11.10 (The monotone theorem as an existence machine)

Let un=∏k=1n(1+12k)u_n = \prod_{k=1}^{n} \bigl(1 + \frac{1}{2^k}\bigr). Each factor exceeds 11, so (un)(u_n) is increasing. Bounded above? Take logarithms and use ln⁡(1+x)≤x\ln(1 + x) \leq x (Example 14.20 anticipates it; or the crude 1+x≤ex1 + x \leq \eu^x from the High School volume):

ln⁡un=∑k=1nln⁡(1+12k)≤∑k=1n12k<1,\ln u_n = \sum_{k=1}^{n} \ln\Bigl(1 + \frac{1}{2^k}\Bigr) \leq \sum_{k=1}^{n} \frac{1}{2^k} < 1 ,

so un<eu_n < \eu. Increasing and bounded: (un)(u_n) converges to some ℓ∈(u1, e]\ell \in \intoc{u_1}{\eu} — a perfectly well-defined real number with no closed form in sight (ℓ=2.384…\ell = 2.384\dots). The closing insight: the monotone limit theorem is the cheapest existence machine in analysis; it named e\eu itself (Example 11.12 below), and in Chapter 17 it will decide the convergence of every positive series by mere boundedness.

Theorem 11.11 (Adjacent sequences)

Let (an)(a_n) be increasing, (bn)(b_n) decreasing, with bn−an→0b_n - a_n \to 0. Then both converge, to a common limit ℓ\ell, and an≤ℓ≤bna_n \leq \ell \leq b_n for all nn.

Proof. First, an≤bna_n \leq b_n for all nn: the sequence (bn−an)(b_n - a_n) is decreasing and tends to 00, so it is ≥0\geq 0 (a negative term would freeze it below 00). Then (an)(a_n) is increasing and bounded above by b0b_0: it converges to some ℓ\ell (Theorem 11.9); likewise (bn)→ℓ′(b_n) \to \ell'; and ℓ′−ℓ=lim⁡(bn−an)=0\ell' - \ell = \lim (b_n - a_n) = 0. The inequalities an≤ℓ≤bna_n \leq \ell \leq b_n follow from monotonicity (ℓ=sup⁡ak≥an\ell = \sup a_k \geq a_n, etc.). ∎

Adjacent sequences: (a_n) climbs, (b_n) descends, and the gap between them shrinks to 0. Each interval [a_n, b_n] contains all later ones, and the common limit  is the unique point left in every interval — the picture behind the dichotomy proofs of Bolzano–Weierstrass below and of the intermediate value theorem in .
Adjacent sequences: (an)(a_n) climbs, (bn)(b_n) descends, and the gap between them shrinks to 00. Each interval [an, bn]\intcc{a_n}{b_n} contains all later ones, and the common limit ℓ\ell is the unique point left in every interval — the picture behind the dichotomy proofs of Bolzano–Weierstrass below and of the intermediate value theorem in Chapter 13.

Example 11.12 (The number e\eu)

Set an=∑k=0n1k!a_n = \sum_{k=0}^{n} \frac{1}{k!} and bn=an+1n⋅n!b_n = a_n + \frac{1}{n \cdot n!} (n≥1n \geq 1). Then (an)(a_n) increases; and

bn+1−bn=1(n+1)!+1(n+1)(n+1)!−1n n!=n(n+1)+n−(n+1)2n(n+1)(n+1)!=−1n(n+1)(n+1)!<0,b_{n+1} - b_n = \frac{1}{(n+1)!} + \frac{1}{(n+1)(n+1)!} - \frac{1}{n\,n!} = \frac{n(n+1) + n - (n+1)^2}{n(n+1)(n+1)!} = \frac{-1}{n(n+1)(n+1)!} < 0 ,

so (bn)(b_n) decreases, and bn−an→0b_n - a_n \to 0: adjacent. Their common limit is (by definition here) the number e≈2.71828\eu \approx 2.71828; the inequalities an<e<bna_n < \eu < b_n are sharp enough to prove e∉Q\eu \notin \Q (Exercise 11.9).

11.3 Subsequences and Bolzano–Weierstrass

Definition 11.13 (Subsequence)

A subsequence of (un)(u_n) is a sequence (uφ(n))(u_{\varphi(n)}) where φ ⁣:N→N\varphi \colon \N \to \N is strictly increasing (note φ(n)≥n\varphi(n) \geq n, by induction).

Proposition 11.14

If un→ℓu_n \to \ell (ℓ∈R\ell \in \R or ±∞\pm\infty), every subsequence tends to ℓ\ell. Consequently, a sequence with two subsequences of different limits diverges. Conversely, if (u2n)(u_{2n}) and (u2n+1)(u_{2n+1}) both converge to the same ℓ\ell, then un→ℓu_n \to \ell.

Proof. Beyond the threshold NN for (un)(u_n), all indices φ(n)≥n≥N\varphi(n) \geq n \geq N qualify (the inequality φ(n)≥n\varphi(n) \geq n is the induction noted in Definition 11.13: φ(0)≥0\varphi(0) \geq 0, and φ(n+1)>φ(n)≥n\varphi(n+1) > \varphi(n) \geq n forces φ(n+1)≥n+1\varphi(n+1) \geq n + 1). For the converse: given ε\varepsilon, take the two thresholds N0N_0 (evens) and N1N_1 (odds); an arbitrary index n≥max⁡(2N0,2N1+1)n \geq \max(2N_0, 2N_1 + 1) is either even, n=2kn = 2k with k≥N0k \geq N_0, or odd, n=2k+1n = 2k+1 with k≥N1k \geq N_1 — in both cases ∣un−ℓ∣≤ε\abs{u_n - \ell} \leq \varepsilon: every index is covered by one of the two subsequences, and that is the whole point. ∎

Example 11.15 (Subsequential limits)

For un=(−1)nnn+1u_n = (-1)^n \frac{n}{n+1}: the even subsequence tends to 11, the odd one to −1-1, so the sequence diverges — but it does so in an organized way, clustering around the two values ±1\pm 1. For un=cos⁡2πn3u_n = \cos\frac{2\pi n}{3}: the three subsequences of indices 3k3k, 3k+13k + 1, 3k+23k + 2 are constant, equal to 11, −12-\frac12, −12-\frac12; the set of subsequential limits is {1,−12}\{1, -\frac12\}. The closing insight: a bounded sequence converges exactly when it has a single subsequential limit (Exercise 11.8); divergence of a bounded sequence always means at least two clusters, and Bolzano–Weierstrass below guarantees there is at least one.

Theorem 11.16 (Bolzano–Weierstrass)

Every bounded sequence of reals has a convergent subsequence.

Proof. Let un∈[a, b]u_n \in \intcc{a}{b} for all nn. Build nested segments by dichotomy: set [a0, b0]=[a, b]\intcc{a_0}{b_0} = \intcc{a}{b}; given [ak, bk]\intcc{a_k}{b_k} containing unu_n for infinitely many nn, one of its two halves still contains unu_n for infinitely many nn — call it [ak+1, bk+1]\intcc{a_{k+1}}{b_{k+1}}. The sequences (ak)(a_k), (bk)(b_k) are adjacent (bk−ak=b−a2k→0b_k - a_k = \frac{b-a}{2^k} \to 0), with common limit ℓ\ell (Theorem 11.11).

Extract: choose φ(0)\varphi(0) with uφ(0)∈[a0, b0]u_{\varphi(0)} \in \intcc{a_0}{b_0}, then, inductively, φ(k+1)>φ(k)\varphi(k+1) > \varphi(k) with uφ(k+1)∈[ak+1, bk+1]u_{\varphi(k+1)} \in \intcc{a_{k+1}}{b_{k+1}} — possible since that segment contains infinitely many terms. Then ak≤uφ(k)≤bka_k \leq u_{\varphi(k)} \leq b_k, and the squeeze theorem gives uφ(k)→ℓu_{\varphi(k)} \to \ell. ∎

Remark 11.17 (What Bolzano–Weierstrass does, and does not, say)

It does say: from boundedness alone, some subsequence converges — existence with no formula, as the dichotomy proof makes clear (nothing tells us which indices survive). It does not say the limit is unique: ((−1)n)((-1)^n) has subsequences converging to 11 and to −1-1, and the set of subsequential limits can even be infinite (Example 11.15, and all of the Cantor set in Problem 12.1). It does not survive unboundedness: (n)(n) has no convergent subsequence at all — though one can always extract a subsequence tending to +∞+\infty or −∞-\infty from any unbounded sequence (choose φ(k)\varphi(k) with uφ(k)≥ku_{\varphi(k)} \geq k, say). Used correctly, the theorem is an existence pump: it appears at the crux of the Cauchy criterion below, of Heine’s theorem, and of the extreme value theorem — always to produce a point that no explicit construction offers.

11.4 Cauchy sequences and completeness

Definition 11.18

A sequence (un)(u_n) is a Cauchy sequence when its terms become arbitrarily close to each other:

∀ε>0, ∃N, ∀p,q≥N,∣up−uq∣≤ε.\forall \varepsilon > 0,\ \exists N,\ \forall p, q \geq N, \qquad \abs{u_p - u_q} \leq \varepsilon .

Example 11.19 (Verifying the Cauchy property by hand)

Let un=∑k=0ncos⁡k2ku_n = \sum_{k=0}^{n} \frac{\cos k}{2^k} — no monotonicity, no guessable limit. For p>qp > q:

∣up−uq∣=∣∑k=q+1pcos⁡k2k∣≤∑k=q+1p12k<12q,\abs{u_p - u_q} = \Bigl| \sum_{k=q+1}^{p} \frac{\cos k}{2^k} \Bigr| \leq \sum_{k=q+1}^{p} \frac{1}{2^k} < \frac{1}{2^{q}} ,

by the triangle inequality, ∣cos⁡k∣≤1\abs{\cos k} \leq 1 and a finite geometric sum. Given ε>0\varepsilon > 0, choose NN with 2−N≤ε2^{-N} \leq \varepsilon: all gaps beyond NN are ≤ε\leq \varepsilon, the sequence is Cauchy, hence converges — to a limit nobody can name in closed form, which is exactly the point. The closing insight: geometric domination of the increments is the standard way to earn the Cauchy property, and Chapter 17 will bottle the argument as “absolute convergence implies convergence”.

Theorem 11.20 (Completeness of R\R)

A sequence of reals converges if and only if it is a Cauchy sequence.

Proof. (⇒\Rightarrow) If un→ℓu_n \to \ell: beyond the threshold for ε2\frac\varepsilon2, ∣up−uq∣≤∣up−ℓ∣+∣ℓ−uq∣≤ε\abs{u_p - u_q} \leq \abs{u_p - \ell} + \abs{\ell - u_q} \leq \varepsilon.

(⇐\Leftarrow) Let (un)(u_n) be Cauchy. It is bounded: with ε=1\varepsilon = 1, beyond NN all terms lie within 11 of uNu_N, and the head is finite. Extract: by Theorem 11.16, some subsequence uφ(n)→ℓu_{\varphi(n)} \to \ell. Conclude: given ε>0\varepsilon > 0, take NN (Cauchy, for ε2\frac\varepsilon2) and n≥Nn \geq N with ∣uφ(n)−ℓ∣≤ε2\abs{u_{\varphi(n)} - \ell} \leq \frac\varepsilon2 and φ(n)≥N\varphi(n) \geq N; then for every p≥Np \geq N:

∣up−ℓ∣≤∣up−uφ(n)∣+∣uφ(n)−ℓ∣≤ε.\abs{u_p - \ell} \leq \abs{u_p - u_{\varphi(n)}} + \abs{u_{\varphi(n)} - \ell} \leq \varepsilon . \qedhere

∎

Remark 11.21

The value of the criterion: it certifies convergence without naming the limit. It fails over Q\Q (the decimal truncations of 2\sqrt 2 form a Cauchy sequence of rationals with no rational limit): completeness is a property of R\R, equivalent to the upper bound axiom. It is also the workhorse behind the convergence of series (Chapter 17).

Example 11.22 (A Cauchy sequence with an invisible limit)

Let Sn=∑k=1n1k2S_n = \sum_{k=1}^{n} \frac{1}{k^2}. For p>q≥1p > q \geq 1:

Sp−Sq=∑k=q+1p1k2≤∑k=q+1p1k(k−1)=∑k=q+1p(1k−1−1k)=1q−1p<1q,S_p - S_q = \sum_{k=q+1}^{p} \frac{1}{k^2} \leq \sum_{k=q+1}^{p} \frac{1}{k(k-1)} = \sum_{k=q+1}^{p} \Bigl(\frac{1}{k-1} - \frac 1k\Bigr) = \frac 1q - \frac 1p < \frac 1q ,

so beyond N>1εN > \frac1\varepsilon all gaps are ≤ε\leq \varepsilon: (Sn)(S_n) is Cauchy, hence converges. Notice what just happened: we proved that a specific real number exists without having any name for it. (It is π26\frac{\pi^2}{6} — a celebrated identity of Euler, proved in the Year 2 volume; nothing in this chapter could tell us that.) This division of labor — existence now, identification later, if ever — is the Cauchy criterion’s whole point, and the engine of the theory of series in Chapter 17.

11.5 Recurrent sequences

Method 11.23 (Studying un+1=f(un)u_{n+1} = f(u_n))

Given ff and a starting point u0u_0:

  1. Stable interval: find an interval II with f(I)⊆If(I) \subseteq I containing u0u_0: then all un∈Iu_n \in I (by induction).
  2. Candidate limits: if un→ℓ∈Iu_n \to \ell \in I and ff is continuous at ℓ\ell (Chapter 13), then ℓ\ell is a fixed point: f(ℓ)=ℓf(\ell) = \ell. Solve f(x)=xf(x) = x.
  3. Monotonicity: if ff is increasing on II, then (un)(u_n) is monotonic (increasing if u1≥u0u_1 \geq u_0, decreasing otherwise); combined with boundedness, Theorem 11.9 concludes. If ff is decreasing, study the two subsequences (u2n)(u_{2n}) and (u2n+1)(u_{2n+1}), which are monotonic for f∘ff \circ f.
  4. Error control: an inequality ∣f(x)−ℓ∣≤k∣x−ℓ∣\abs{f(x) - \ell} \leq k\abs{x - \ell} with k<1k < 1 gives ∣un−ℓ∣≤kn∣u0−ℓ∣→0\abs{u_n - \ell} \leq k^n \abs{u_0 - \ell} \to 0 directly.

Example 11.24 (Heron’s method)

Let u0=2u_0 = 2 and un+1=12(un+2un)u_{n+1} = \dfrac12\Bigl(u_n + \dfrac{2}{u_n}\Bigr): the ancient algorithm for 2\sqrt 2.

  • Stability: for x>0x > 0, the arithmetic–geometric mean inequality gives 12(x+2x)≥x⋅2x=2\frac12(x + \frac2x) \geq \sqrt{x \cdot \frac 2x} = \sqrt 2; so I=[2, +∞)I = \intco{\sqrt 2}{+\infty} is stable and contains u1u_1 (indeed u1=32≥2u_1 = \frac32 \geq \sqrt 2).
  • Monotonicity: for x≥2x \geq \sqrt 2,   x−f(x)=x2−22x≥0\;x - f(x) = \frac{x^2 - 2}{2x} \geq 0: the sequence decreases from u1u_1 on, and is bounded below by 2\sqrt 2: it converges.
  • Limit: the fixed points solve x=12(x+2x)x = \frac12(x + \frac2x), i.e. x2=2x^2 = 2: on II, ℓ=2\ell = \sqrt 2.
  • Speed: un+1−2=(un−2)22un≤(un−2)222u_{n+1} - \sqrt 2 = \frac{(u_n - \sqrt2)^2}{2u_n} \leq \frac{(u_n - \sqrt 2)^2}{2\sqrt 2}: the number of correct digits roughly doubles at each step (quadratic convergence).
Heron’s iteration u_n+1 = 1/2 (u_n + 2/u_n ), drawn as a staircase between the graph of f and the diagonal y = x: from u_0 = 2, the iterates slide down to the fixed point √ 2.
Heron’s iteration un+1=12(un+2un)u_{n+1} = \frac12\bigl(u_n + \frac{2}{u_n}\bigr), drawn as a staircase between the graph of ff and the diagonal y=xy = x: from u0=2u_0 = 2, the iterates slide down to the fixed point 2\sqrt 2.

Remark 11.25 (Common pitfalls with limits)

Four classics. (i) Small steps do not imply convergence: un+1−un→0u_{n+1} - u_n \to 0 is far weaker than the Cauchy property — the harmonic sums HnH_n have steps 1n+1→0\frac{1}{n+1} \to 0 yet diverge to +∞+\infty (Exercise 11.5); the Cauchy condition controls ∣up−uq∣\abs{u_p - u_q} for all large pairs, not consecutive ones. (ii) Strict inequalities die in the limit: from un<vnu_n < v_n for all nn one gets only lim⁡un≤lim⁡vn\lim u_n \leq \lim v_n (Theorem 11.7); 1n>0\frac1n > 0 and yet lim⁡=0\lim = 0. (iii) Bounded is not convergent: ((−1)n)((-1)^n) is bounded and diverges; boundedness plus monotonicity converges, boundedness alone only guarantees a convergent subsequence (Theorem 11.16). (iv) The fixed-point equation comes second, not first: for un+1=f(un)u_{n+1} = f(u_n), solving f(ℓ)=ℓf(\ell) = \ell identifies the limit only after convergence is proved. The recurrence un+1=2unu_{n+1} = 2u_n has the unique fixed point ℓ=0\ell = 0, yet from u0=1u_0 = 1 the sequence runs to +∞+\infty: the equation ℓ=2ℓ\ell = 2\ell was never entitled to a limit. Order of operations, always: existence first (Method 11.23, steps 1–3), identification second.

Example 11.26 (A decreasing ff: the golden recurrence)

Let u0=1u_0 = 1 and un+1=11+unu_{n+1} = \dfrac{1}{1 + u_n}. Here f(x)=11+xf(x) = \frac{1}{1+x} is decreasing, so the sequence is not monotonic (it alternates around its limit); the contraction step of Method 11.23 is the right tool. Stability: if x∈[12, 1]x \in \intcc{\frac12}{1} then 1+x∈[32, 2]1 + x \in \intcc{\frac32}{2}, so f(x)∈[12, 23]⊆[12, 1]f(x) \in \intcc{\frac12}{\frac23} \subseteq \intcc{\frac12}{1}, and u1=12u_1 = \frac12 puts the whole sequence there. Fixed point: ℓ=11+ℓ\ell = \frac{1}{1+\ell} with ℓ>0\ell > 0 gives ℓ2+ℓ−1=0\ell^2 + \ell - 1 = 0, i.e.

ℓ=5−12=0.6180…\ell = \frac{\sqrt5 - 1}{2} = 0.6180\dots

(the golden ratio’s inverse). Contraction: for x,y∈[12, 1]x, y \in \intcc{\frac12}{1},

∣f(x)−f(y)∣=∣x−y∣(1+x)(1+y)≤∣x−y∣(3/2)2=49 ∣x−y∣,\abs{f(x) - f(y)} = \frac{\abs{x - y}}{(1+x)(1+y)} \leq \frac{\abs{x-y}}{(3/2)^2} = \frac49\,\abs{x - y} ,

so ∣un−ℓ∣≤(49)n−1∣u1−ℓ∣→0\abs{u_n - \ell} \leq \bigl(\frac49\bigr)^{n-1}\abs{u_1 - \ell} \to 0: convergence, with geometric speed, no monotonicity needed. The closing insight: monotone methods and contraction methods split the recurrent world between them — increasing ff gives monotone orbits, decreasing ff gives alternating orbits tamed by a Lipschitz constant <1< 1 (the systematic theory is Exercise 14.11).

Remark 11.27 (Perspectives inside this volume)

Sequences are the measuring instrument the rest of the volume holds up to every object. In Chapter 12 they characterize closedness and compactness; in Chapter 13 they transport limits of functions; in Chapter 15 Riemann sums are sequences converging to the integral; Chapter 17 is the theory of one special class of sequences, the partial sums. Even the algebra chapters consume them: the iterates of a matrix in Chapter 21 form sequences whose behavior (convergence of AnA^n) is a linear-algebra question with this chapter’s vocabulary. The two theorems to carry everywhere: monotone limit (existence from order) and Bolzano–Weierstrass (existence from boundedness) — between them, nearly every limit in this book is born.

Remark 11.28 (Complex sequences)

A sequence (zn)(z_n) of complex numbers converges to ℓ\ell when ∣zn−ℓ∣→0\abs{z_n - \ell} \to 0; equivalently, when ℜ(zn)→ℜ(ℓ)\Re(z_n) \to \Re(\ell) and ℑ(zn)→ℑ(ℓ)\Im(z_n) \to \Im(\ell) (compare ∣z∣\abs{z} with ∣ℜz∣+∣ℑz∣\abs{\Re z} + \abs{\Im z}). The theorems not involving order — operations, Bolzano–Weierstrass (extract twice), Cauchy criterion — carry over verbatim.

11.6 Exercises

Exercise 11.1 ★

Directly from Definition 11.1, prove that 2n+1n+3→2\dfrac{2n+1}{n+3} \to 2, and that (un)=((−1)n)(u_n) = ((-1)^n) diverges.

Solution

Solution of Exercise 11.1.

∣2n+1n+3−2∣=5n+3\Bigl|\dfrac{2n+1}{n+3} - 2\Bigr| = \dfrac{5}{n+3}. Given ε>0\varepsilon > 0, take N>5ε−3N > \frac 5\varepsilon - 3 (Archimedes): for n≥Nn \geq N, 5n+3≤ε\frac{5}{n+3} \leq \varepsilon. Hence the limit is 22.

((−1)n)((-1)^n): its subsequences (u2n)=(1)(u_{2n}) = (1) and (u2n+1)=(−1)(u_{2n+1}) = (-1) converge to different limits, so the sequence diverges (Proposition 11.14). (Directly: any candidate ℓ\ell fails for ε=12\varepsilon = \frac12, since consecutive terms are at distance 22.)

Exercise 11.2 ★

Compute the limits:

n2−3n+12n2+5,n+1−n,2n+n33n−n2,5n (=51/n).\frac{n^2 - 3n + 1}{2n^2 + 5}, \qquad \sqrt{n+1} - \sqrt n, \qquad \frac{2^n + n^3}{3^n - n^2}, \qquad \sqrt[n]{5}\ \Bigl(= 5^{1/n}\Bigr).
Solution

Solution of Exercise 11.2.

Dividing by n2n^2: 1−3/n+1/n22+5/n2→12\dfrac{1 - 3/n + 1/n^2}{2 + 5/n^2} \to \dfrac12.

n+1−n=1n+1+n→0\sqrt{n+1} - \sqrt n = \dfrac{1}{\sqrt{n+1} + \sqrt n} \to 0 (conjugate).

2n+n33n−n2=(2/3)n+n3/3n1−n2/3n→0+01−0=0\dfrac{2^n + n^3}{3^n - n^2} = \dfrac{(2/3)^n + n^3/3^n}{1 - n^2/3^n} \to \dfrac{0 + 0}{1 - 0} = 0, using qn→0q^n \to 0 for ∣q∣<1\abs q < 1 and the polynomial-vs-geometric comparison (Proposition 4.6).

51/n=eln⁡5n→e0=15^{1/n} = \eu^{\frac{\ln 5}{n}} \to \eu^0 = 1.

Exercise 11.3 ★

Prove the standard comparison: if ∣q∣<1\abs{q} < 1 then qn→0q^n \to 0 (write 1∣q∣=1+h\frac{1}{\abs q} = 1 + h, h>0h > 0, and use the Bernoulli inequality (1+h)n≥1+nh(1+h)^n \geq 1 + nh, to be proved by induction). What are the behaviors for q=1q = 1, q=−1q = -1, ∣q∣>1\abs q > 1?

Solution

Solution of Exercise 11.3.

Bernoulli: (1+h)n≥1+nh(1+h)^n \geq 1 + nh for h≥−1h \geq -1, by induction — (1+h)n+1=(1+h)n(1+h)≥(1+nh)(1+h)=1+(n+1)h+nh2≥1+(n+1)h(1+h)^{n+1} = (1+h)^n(1+h) \geq (1+nh)(1+h) = 1 + (n+1)h + nh^2 \geq 1 + (n+1)h.

For 0<∣q∣<10 < \abs q < 1: write 1∣q∣=1+h\frac{1}{\abs q} = 1 + h, h>0h > 0; then ∣q∣n=1(1+h)n≤11+nh→0\abs{q}^n = \frac{1}{(1+h)^n} \leq \frac{1}{1 + nh} \to 0, and the squeeze gives qn→0q^n \to 0 (the case q=0q = 0 is trivial). For q=1q = 1: constant sequence, limit 11. For q=−1q = -1: diverges (Exercise 11.1). For ∣q∣>1\abs q > 1: ∣q∣n=(1+h)n≥1+nh→+∞\abs q^n = (1 + h)^n \geq 1 + nh \to +\infty, so (qn)(q^n) is unbounded, hence divergent (to +∞+\infty if q>1q > 1; with alternating signs, no limit, if q<−1q < -1).

Exercise 11.4 ★

Let un+1=un+32u_{n+1} = \frac{u_n + 3}{2}, u0=0u_0 = 0. Find the fixed point ℓ\ell, prove that vn=un−ℓv_n = u_n - \ell is geometric, and give an explicit formula and the limit of (un)(u_n).

Solution

Solution of Exercise 11.4.

Fixed point: ℓ=ℓ+32\ell = \frac{\ell + 3}{2} gives ℓ=3\ell = 3. Then

vn+1=un+1−3=un+32−3=un−32=vn2:v_{n+1} = u_{n+1} - 3 = \frac{u_n + 3}{2} - 3 = \frac{u_n - 3}{2} = \frac{v_n}{2}:

(vn)(v_n) is geometric with ratio 12\frac12, v0=−3v_0 = -3. So un=3−32n→3u_n = 3 - \frac{3}{2^n} \to 3.

Exercise 11.5 ★★

(Harmonic series) Let Hn=∑k=1n1kH_n = \sum_{k=1}^{n} \frac 1k. Prove that H2n−Hn≥12H_{2n} - H_n \geq \frac12 for all n≥1n \geq 1, and conclude that (Hn)(H_n) is not a Cauchy sequence, hence diverges (to +∞+\infty, being increasing).

Solution

Solution of Exercise 11.5.

H2n−Hn=∑k=n+12n1k≥n⋅12n=12H_{2n} - H_n = \sum_{k=n+1}^{2n} \frac 1k \geq n \cdot \frac{1}{2n} = \frac12 (each of the nn terms is ≥12n\geq \frac{1}{2n}). If (Hn)(H_n) were Cauchy, taking ε=13\varepsilon = \frac13 would force ∣H2n−Hn∣≤13\abs{H_{2n} - H_n} \leq \frac13 for large nn: contradiction. An increasing non-convergent sequence diverges to +∞+\infty (Theorem 11.9): Hn→+∞H_n \to +\infty.

Exercise 11.6 ★★

Suppose (u2n)(u_{2n}), (u2n+1)(u_{2n+1}) and (u3n)(u_{3n}) all converge. Prove that (un)(u_n) converges. (Find common subsequences to equate the limits.)

Solution

Solution of Exercise 11.6.

Let a=lim⁡u2na = \lim u_{2n}, b=lim⁡u2n+1b = \lim u_{2n+1}, c=lim⁡u3nc = \lim u_{3n}. The sequence (u6n)(u_{6n}) is a subsequence both of (u2n)(u_{2n}) and of (u3n)(u_{3n}): its limit equals aa and cc, so a=ca = c. The sequence (u6n+3)(u_{6n+3}) is a subsequence of (u2n+1)(u_{2n+1}) (odd indices) and of (u3n)(u_{3n}) (indices 6n+3=3(2n+1)6n + 3 = 3(2n+1)): so b=cb = c. Hence a=ba = b, and Proposition 11.14 (evens and odds with equal limits) gives the convergence of (un)(u_n).

Exercise 11.7 ★★

Study the sequence u0=0u_0 = 0, un+1=2+unu_{n+1} = \sqrt{2 + u_n}: stability, monotonicity, limit. Then prove the error bound ∣un−2∣≤23 n\abs{u_n - 2} \leq \dfrac{2}{3^{\,n}} (show 2−un+1=2−un2+2+un2 - u_{n+1} = \dfrac{2 - u_n}{2 + \sqrt{2 + u_n}} and bound the denominator below by 33).

Solution

Solution of Exercise 11.7.

Stability and bounds: I=[0, 2]I = \intcc{0}{2} is stable: for x∈Ix \in I, 2+x∈[2, 2]⊆I\sqrt{2 + x} \in \intcc{\sqrt 2}{2} \subseteq I; and u0=0∈Iu_0 = 0 \in I.

Monotonicity: f(x)=2+xf(x) = \sqrt{2+x} is increasing and u1=2>u0u_1 = \sqrt 2 > u_0: by induction (un)(u_n) is increasing. Increasing and bounded above by 22: it converges (Theorem 11.9).

Limit: ℓ=2+ℓ\ell = \sqrt{2 + \ell} with ℓ≥0\ell \geq 0 gives ℓ2−ℓ−2=0\ell^2 - \ell - 2 = 0, so ℓ=2\ell = 2.

Error bound: multiplying by the conjugate,

2−un+1=2−2+un=4−(2+un)2+2+un=2−un2+2+un≤2−un3,2 - u_{n+1} = 2 - \sqrt{2 + u_n} = \frac{4 - (2 + u_n)}{2 + \sqrt{2+u_n}} = \frac{2 - u_n}{2 + \sqrt{2 + u_n}} \leq \frac{2 - u_n}{3},

since 2+un≥2>1\sqrt{2 + u_n} \geq \sqrt 2 > 1. By induction from 2−u0=22 - u_0 = 2:   0≤2−un≤23n\;0 \leq 2 - u_n \leq \frac{2}{3^n}.

Exercise 11.8 ★★

Let (un)(u_n) be bounded, such that every convergent subsequence of (un)(u_n) has the same limit ℓ\ell. Prove un→ℓu_n \to \ell. (Contradiction plus Bolzano–Weierstrass.)

Solution

Solution of Exercise 11.8.

Suppose (un)(u_n) does not converge to ℓ\ell: for some ε0>0\varepsilon_0 > 0, infinitely many indices satisfy ∣un−ℓ∣>ε0\abs{u_n - \ell} > \varepsilon_0; they form a subsequence (uφ(n))(u_{\varphi(n)}). This subsequence is bounded, so by Bolzano–Weierstrass (Theorem 11.16) it has a convergent sub-subsequence, whose limit ℓ′\ell' satisfies ∣ℓ′−ℓ∣≥ε0\abs{\ell' - \ell} \geq \varepsilon_0 (pass the inequality to the limit, Theorem 11.7). But a sub-subsequence of (un)(u_n) is a convergent subsequence of (un)(u_n), so by hypothesis ℓ′=ℓ\ell' = \ell: contradiction.

Exercise 11.9 ★★★

With the notation of Example 11.12, suppose e=pq\eu = \frac pq with p,q∈N∗p, q \in \N^*. Using aq<e<bq=aq+1q q!a_q < \eu < b_q = a_q + \frac{1}{q\, q!}, multiply by q!q! and derive a contradiction between two integers. Conclude: e\eu is irrational.

Solution

Solution of Exercise 11.9.

Suppose e=pq\eu = \frac pq, q≥1q \geq 1. The strict inequalities aq<e<aq+1q q!a_q < \eu < a_q + \frac{1}{q\,q!} (strict since (an)(a_n) is strictly increasing and (bn)(b_n) strictly decreasing) multiplied by q!q! give

q! aq  <  q! pq  <  q! aq+1q≤q! aq+1.q!\,a_q \;<\; q!\,\frac pq \;<\; q!\,a_q + \frac 1q \leq q!\,a_q + 1.

Now N=q! aq=∑k=0qq!k!N = q!\,a_q = \sum_{k=0}^{q} \frac{q!}{k!} is an integer (each q!k!\frac{q!}{k!} is a product of integers for k≤qk \leq q), and so is q! pq=(q−1)! pq!\,\frac pq = (q-1)!\,p. The display thus places the integer (q−1)! p(q-1)!\,p strictly between NN and N+1q≤N+1N + \frac 1q \leq N + 1: an integer strictly inside (N, N+1)\intoo{N}{N+1}, which is impossible. Hence e∉Q\eu \notin \Q.

Exercise 11.10 ★★★

(Cesàro means) For a sequence (un)n≥1(u_n)_{n \geq 1}, set cn=u1+⋯+unnc_n = \frac{u_1 + \dots + u_n}{n}.

  1. Prove that un→ℓu_n \to \ell implies cn→ℓc_n \to \ell (cut the sum at a threshold NN; bound the head by a fixed quantity over nn, the tail by ε\varepsilon).
  2. Show by example that the converse fails.
  3. Deduce that if un+1−un→ℓu_{n+1} - u_n \to \ell, then unn→ℓ\frac{u_n}{n} \to \ell.
Solution

Solution of Exercise 11.10.

  1. Let ε>0\varepsilon > 0 and NN with ∣uk−ℓ∣≤ε2\abs{u_k - \ell} \leq \frac{\varepsilon}{2} for k>Nk > N. For n>Nn > N:

    ∣cn−ℓ∣=∣∑k=1n(uk−ℓ)n∣≤∑k=1N∣uk−ℓ∣n+n−Nn⋅ε2≤Cn+ε2,\abs{c_n - \ell} = \Bigl|\frac{\sum_{k=1}^{n}(u_k - \ell)}{n}\Bigr| \leq \frac{\sum_{k=1}^{N} \abs{u_k - \ell}}{n} + \frac{n - N}{n}\cdot\frac{\varepsilon}{2} \leq \frac{C}{n} + \frac{\varepsilon}{2},

    where C=∑k=1N∣uk−ℓ∣C = \sum_{k=1}^N \abs{u_k - \ell} is fixed. For nn large, Cn≤ε2\frac Cn \leq \frac\varepsilon2: then ∣cn−ℓ∣≤ε\abs{c_n - \ell} \leq \varepsilon.

  2. un=(−1)nu_n = (-1)^n: diverges, yet cn→0c_n \to 0 (partial sums bounded by 11, divided by nn).
  3. Apply (1) to the sequence vn=un+1−un→ℓv_n = u_{n+1} - u_n \to \ell: its Cesàro mean is un+1−u1n→ℓ\frac{u_{n+1} - u_1}{n} \to \ell (telescoping), and un+1n=un+1−u1n+u1n→ℓ\frac{u_{n+1}}{n} = \frac{u_{n+1} - u_1}{n} + \frac{u_1}{n} \to \ell; renormalizing indices (unn=unn−1⋅n−1n\frac{u_n}{n} = \frac{u_n}{n-1}\cdot\frac{n-1}{n}) gives unn→ℓ\frac{u_n}{n} \to \ell.

Exercise 11.11 ★★★

Let (un)(u_n) satisfy 0≤um+n≤um+un0 \leq u_{m+n} \leq u_m + u_n for all m,nm, n (subadditivity). Prove that (unn)\bigl(\frac{u_n}{n}\bigr) converges to inf⁡n≥1unn\inf_{n \geq 1} \frac{u_n}{n}. (For fixed mm, write n=qm+rn = qm + r and bound unn\frac{u_n}{n} using un≤q um+uru_n \leq q\,u_m + u_r.)

Solution

Solution of Exercise 11.11.

Let L=inf⁡n≥1unn≥0L = \inf_{n \geq 1} \frac{u_n}{n} \geq 0, and ε>0\varepsilon > 0. Choose mm with umm≤L+ε\frac{u_m}{m} \leq L + \varepsilon. Every nn writes n=qm+rn = qm + r, 0≤r<m0 \leq r < m; subadditivity (iterated) gives un≤q um+uru_n \leq q\,u_m + u_r, so

unn≤qmn⋅umm+urn≤umm+max⁡(u0,…,um−1)n≤L+ε+Cmn,\frac{u_n}{n} \leq \frac{q m}{n}\cdot\frac{u_m}{m} + \frac{u_r}{n} \leq \frac{u_m}{m} + \frac{\max(u_0, \dots, u_{m-1})}{n} \leq L + \varepsilon + \frac{C_m}{n},

using qm≤nqm \leq n. For nn large, Cmn≤ε\frac{C_m}{n} \leq \varepsilon: thus L≤unn≤L+2εL \leq \frac{u_n}{n} \leq L + 2\varepsilon for all large nn, which is the convergence to LL.

Exercise 11.12 ★★★

Using the density of the subgroup Z+2πZ\Z + 2\pi\Z of (R,+)(\R, +) (Exercise 10.9), prove that the sequence (sin⁡n)n∈N(\sin n)_{n \in \N} is dense in [−1, 1]\intcc{-1}{1} — in particular it diverges.

Solution

Solution of Exercise 11.12.

The subgroup G=Z+2πZG = \Z + 2\pi\Z of (R,+)(\R, +) is dense: it is not αZ\alpha\Z, since 1=pα1 = p\alpha, 2π=qα2\pi = q\alpha would make 2π=qp2\pi = \frac qp rational — and π∉Q\pi \notin \Q (admitted here; a proof is sketched in Chapter 15). By Exercise 10.9, GG is dense in R\R.

Let now y∈[−1, 1]y \in \intcc{-1}{1} and θ=arcsin⁡y\theta = \arcsin y. By density, for every ε>0\varepsilon > 0 there are n∈Zn \in \Z, k∈Zk \in \Z with ∣(n+2πk)−θ∣≤ε\abs{(n + 2\pi k) - \theta} \leq \varepsilon, i.e. nn is within ε\varepsilon of θ−2πk\theta - 2\pi k; then, sin⁡\sin being 2π2\pi-periodic and 11-Lipschitz (∣sin⁡a−sin⁡b∣≤∣a−b∣\abs{\sin a - \sin b} \leq \abs{a - b}, from the mean value inequality of Chapter 14),

∣sin⁡n−y∣=∣sin⁡(n+2πk)−sin⁡θ∣≤∣n+2πk−θ∣≤ε.\abs{\sin n - y} = \abs{\sin(n + 2\pi k) - \sin\theta} \leq \abs{n + 2\pi k - \theta} \leq \varepsilon .

One detail: nn ranges over Z\Z, but sin⁡(−n)=−sin⁡n\sin(-n) = -\sin n and yy was arbitrary in [−1, 1]\intcc{-1}{1}, so nonnegative indices suffice (replace (n,y)(n, y) by (−n,−y)(-n, -y) if needed). Hence {sin⁡n:n∈N}\{\sin n : n \in \N\} is dense in [−1, 1]\intcc{-1}{1}; a dense-in-a-segment sequence has subsequences approaching distinct values, so it diverges.

11.7 Problem: Cesàro, Stolz, and the slow fall of the sine

Problem 11.1

Weekend problem — the Cesàro–Stolz theorem and the asymptotics un∼3/nu_n \sim \sqrt{3/n} for un+1=sin⁡unu_{n+1} = \sin u_n

The Cesàro–Stolz theorem is the discrete l’Hospital rule: to find the limit of a quotient an/bna_n/b_n, it suffices to find the limit of the quotient of increments (an+1−an)/(bn+1−bn)(a_{n+1} - a_n)/(b_{n+1} - b_n). This problem proves the theorem, harvests classical limits with it, and then aims it at a famous target: the sequence un+1=sin⁡unu_{n+1} = \sin u_n, which creeps to 00 at the exactly computable speed un∼3/nu_n \sim \sqrt{3/n}. Two facts from the High School volume are granted here and re-proved honestly later in this volume: the tangent-line inequality

eu≥1+u(u∈R),(G1)\tag{G1} \eu^{u} \geq 1 + u \quad (u \in \R),

re-proved by convexity in Chapter 14, and the sine bracketing

x−x36  ≤  sin⁡x  ≤  x−x36+x5120(0≤x≤1),∣sin⁡x∣≤∣x∣(x∈R),(G2)\tag{G2} x - \frac{x^3}{6} \;\leq\; \sin x \;\leq\; x - \frac{x^3}{6} + \frac{x^5}{120} \quad (0 \leq x \leq 1), \qquad \abs{\sin x} \leq \abs{x} \quad (x \in \R),

re-proved by Taylor’s formula in Chapter 16.

Part I — Sums without closed formulas.

  1. Using 1+2+⋯+n=n(n+1)21 + 2 + \dots + n = \frac{n(n+1)}{2} and 12+⋯+n2=n(n+1)(2n+1)61^2 + \dots + n^2 = \frac{n(n+1)(2n+1)}{6}, compute lim⁡1+2+⋯+nn2\lim \frac{1 + 2 + \dots + n}{n^2} and lim⁡12+⋯+n2n3\lim \frac{1^2 + \dots + n^2}{n^3}.
  2. Let Tn=∑k=1nkT_n = \sum_{k=1}^n \sqrt k, for which no closed formula exists. Prove the bracketing

    122 n3/2  ≤  Tn  ≤  n3/2\frac{1}{2\sqrt 2}\,n^{3/2} \;\leq\; T_n \;\leq\; n^{3/2}

    (keep only the terms k>n2k > \frac n2 for the lower bound). So TnT_n has the order n3/2n^{3/2} — but which constant? Hold the question until question 8.

  3. (Telescoping lemma) Let (bn)(b_n) be strictly increasing and suppose that for all k≥Nk \geq N,

    m  ≤  ak+1−akbk+1−bk  ≤  M.m \;\leq\; \frac{a_{k+1} - a_k}{b_{k+1} - b_k} \;\leq\; M .

    Prove that m≤an−aNbn−bN≤Mm \leq \dfrac{a_n - a_N}{b_n - b_N} \leq M for every n>Nn > N.

Part II — The Cesàro–Stolz theorem. Let (bn)(b_n) be strictly increasing with bn→+∞b_n \to +\infty, and suppose an+1−anbn+1−bn→ℓ∈R\dfrac{a_{n+1} - a_n}{b_{n+1} - b_n} \to \ell \in \R.

  1. Fix ε>0\varepsilon > 0. Show there is NN such that ℓ−ε≤an−aNbn−bN≤ℓ+ε\ell - \varepsilon \leq \dfrac{a_n - a_N}{b_n - b_N} \leq \ell + \varepsilon for all n>Nn > N.
  2. Establish, for n>Nn > N, the identity

    anbn−ℓ=aN−ℓ bNbn+(1−bNbn)(an−aNbn−bN−ℓ),\frac{a_n}{b_n} - \ell = \frac{a_N - \ell\,b_N}{b_n} + \Bigl(1 - \frac{b_N}{b_n}\Bigr) \Bigl(\frac{a_n - a_N}{b_n - b_N} - \ell\Bigr),

    and conclude the theorem: anbn→ℓ\dfrac{a_n}{b_n} \to \ell.

  3. Prove the +∞+\infty variant: if an+1−anbn+1−bn→+∞\dfrac{a_{n+1} - a_n}{b_{n+1} - b_n} \to +\infty (same hypotheses on (bn)(b_n)), then anbn→+∞\dfrac{a_n}{b_n} \to +\infty.
  4. Take bn=nb_n = n: recover the Cesàro mean theorem of Exercise 11.10. Then show the converse of Cesàro–Stolz fails: for an=(−1)na_n = (-1)^n, bn=nb_n = n, the quotient an/bna_n/b_n converges while the quotient of increments does not. Stolz is a one-way street.

Part III — First dividends.

  1. Prove (1+h)3/2−1=3h+3h2+h3(1+h)3/2+1(1+h)^{3/2} - 1 = \dfrac{3h + 3h^2 + h^3}{(1+h)^{3/2} + 1} by conjugation, deduce n((1+1n)3/2−1)→32n\bigl((1 + \tfrac1n)^{3/2} - 1\bigr) \to \tfrac32, and conclude with Cesàro–Stolz:

    Tn=∑k=1nk  ∼  23 n3/2,T_n = \sum_{k=1}^{n} \sqrt k \;\sim\; \tfrac23\, n^{3/2} ,

    resolving the cliffhanger of question 2.

  2. From (G1) alone, derive the logarithm bracketing

    t1+t  ≤  ln⁡(1+t)  ≤  t(t>−1)\frac{t}{1 + t} \;\leq\; \ln(1 + t) \;\leq\; t \qquad (t > -1)

    (apply (G1) at u=ln⁡(1+t)u = \ln(1+t) and at u=−t/(1+t)u = -t/(1+t)).

  3. Show that bn=ln⁡nb_n = \ln n is strictly increasing with ln⁡n→+∞\ln n \to +\infty, and prove with Cesàro–Stolz and question 9 that

    Hn=∑k=1n1k  ∼  ln⁡n.H_n = \sum_{k=1}^{n} \frac 1k \;\sim\; \ln n .

    (The finer structure Hn=ln⁡n+γ+o(1)H_n = \ln n + \gamma + o(1) is the weekend problem of Chapter 17.)

  4. (From ratios to roots) Let un>0u_n > 0 with un+1un→L>0\frac{u_{n+1}}{u_n} \to L > 0. Using question 9, show ln⁡un+1un→ln⁡L\ln\frac{u_{n+1}}{u_n} \to \ln L; apply Cesàro to conclude ln⁡unn→ln⁡L\frac{\ln u_n}{n} \to \ln L, then, with (G1), that un1/n→Lu_n^{1/n} \to L. Application: compute lim⁡ (2nn)1/n\lim\,\binom{2n}{n}^{1/n}.

Part IV — The slow fall of the sine. Let u0∈Ru_0 \in \R and un+1=sin⁡unu_{n+1} = \sin u_n.

  1. From (G2), show 0<sin⁡x<x0 < \sin x < x for 0<x≤10 < x \leq 1. Deduce: u1∈[−1, 1]u_1 \in \intcc{-1}{1}; if u1=0u_1 = 0 the sequence is zero from rank 11; and if u1>0u_1 > 0 (the case u1<0u_1 < 0 being symmetric, sin⁡\sin odd), then (un)n≥1(u_n)_{n \geq 1} is strictly decreasing, positive, and converges to 00 (identify the limit via ℓ=sin⁡ℓ\ell = \sin \ell, using ∣sin⁡a−sin⁡b∣≤∣a−b∣\abs{\sin a - \sin b} \leq \abs{a - b}, itself a consequence of (G2) and the product-to-sum formula).
  2. Assume from now on u1∈(0, 1]u_1 \in \intoc{0}{1}. Show by squeezing, using (G2):

    sin⁡unun→1andun−sin⁡unun3→16.\frac{\sin u_n}{u_n} \to 1 \qquad\text{and}\qquad \frac{u_n - \sin u_n}{u_n^{3}} \to \frac16 .
  3. Prove the factorization

    wn:=1un+12−1un2=un−sin⁡unun3⋅un+sin⁡unun⋅(unsin⁡un)2,w_n := \frac{1}{u_{n+1}^{2}} - \frac{1}{u_n^{2}} = \frac{u_n - \sin u_n}{u_n^{3}} \cdot \frac{u_n + \sin u_n}{u_n} \cdot \Bigl(\frac{u_n}{\sin u_n}\Bigr)^{2},

    and deduce wn→13w_n \to \frac13.

  4. Conclude with Exercise 11.10 (increments version) that 1n un2→13\frac{1}{n\,u_n^{2}} \to \frac13, then, by a conjugation argument for the square root, the headline:

    n  un⟶3,i.e.un∼3n.\sqrt n\;u_n \longrightarrow \sqrt 3 , \qquad\text{i.e.}\qquad u_n \sim \sqrt{\frac 3n} .
  5. Quantify the slowness: show that eventually 2/n≤un≤2/n\sqrt{2/n} \leq u_n \leq 2/\sqrt n, so that reaching un≤10−2u_n \leq 10^{-2} requires more than 20 00020\,000 iterations (about 30 00030\,000, by the asymptotics). Contrast with Heron’s method (Example 11.24) and explain the structural reason: at the fixed point 00, the slope of sin⁡\sin is 11 (a neutral fixed point), while error-halving iterations need a slope of modulus <1< 1.
  6. Show that for every starting point u0∈Ru_0 \in \R, either un=0u_n = 0 from rank 11 on, or ∣un∣∼3/n\abs{u_n} \sim \sqrt{3/n} — the fall is universal, only the sign remembers u0u_0.

Part V — The general principle. The sine is one instance of a machine.

  1. Let un>0u_n > 0, un→0u_n \to 0, and un−un+1un2→a>0\dfrac{u_n - u_{n+1}}{u_n^{2}} \to a > 0. Prove successively: un+1un→1\frac{u_{n+1}}{u_n} \to 1; then 1un+1−1un→a\frac{1}{u_{n+1}} - \frac{1}{u_n} \to a; then n un→1an\,u_n \to \frac1a.
  2. (Exact model) For un+1=un1+unu_{n+1} = \dfrac{u_n}{1 + u_n}, u0>0u_0 > 0: show 1un\frac{1}{u_n} is arithmetic, solve exactly, and check question 18’s conclusion against the exact formula.
  3. For un+1=une−unu_{n+1} = u_n \eu^{-u_n}, u0>0u_0 > 0: show un→0u_n \to 0, use (G1) to squeeze 1−e−tt\frac{1 - \eu^{-t}}{t} between 11+t\frac{1}{1+t} and 11 for t>0t > 0, and conclude un∼1nu_n \sim \frac 1n.
  4. (Cubic contact, squared telescope) Let un>0u_n > 0, un→0u_n \to 0, un−un+1un3→a>0\dfrac{u_n - u_{n+1}}{u_n^{3}} \to a > 0. Adapt question 14’s factorization to show 1un+12−1un2→2a\frac{1}{u_{n+1}^2} - \frac{1}{u_n^2} \to 2a, and conclude n un2→12an\,u_n^{2} \to \frac{1}{2a}. Check that a=16a = \frac16 recovers Part IV.

Part VI — Limits of the method, and morals.

  1. Show that the hypothesis bn→+∞b_n \to +\infty cannot be dropped: for an=2−2−na_n = 2 - 2^{-n} and bn=1−2−nb_n = 1 - 2^{-n}, the increment quotient tends to 11 while anbn→2\frac{a_n} {b_n} \to 2. Point to the exact line of question 5’s proof that breaks.
  2. (Stolz twice) Prove ∑k=1nHk∼nln⁡n\sum_{k=1}^{n} H_k \sim n \ln n (one application of Cesàro–Stolz, then question 10; bound (n+1)ln⁡(n+1)−nln⁡n(n+1)\ln(n+1) - n\ln n using question 9).
  3. (Geometric means) If un>0u_n > 0 and un→ℓ>0u_n \to \ell > 0, show (u1u2⋯un)1/n→ℓ(u_1 u_2 \cdots u_n)^{1/n} \to \ell; if un→+∞u_n \to +\infty, show (u1⋯un)1/n→+∞(u_1 \cdots u_n)^{1/n} \to +\infty. Deduce (n!)1/n→+∞(n!)^{1/n} \to +\infty.
  4. Synthesis, one sentence each: (i) where exactly did completeness enter this problem; (ii) in what sense is Cesàro–Stolz a discrete l’Hospital rule (its differential twin rests on the mean value theorem of Chapter 14); (iii) state the heuristic linking the contact order of ff at a neutral fixed point to the decay exponent of un+1=f(un)u_{n+1} = f(u_n); (iv) trace the constant 33 of 3/n\sqrt{3/n} back through the pipeline 16→13→3\frac16 \to \frac13 \to 3.
Solution

Solution of Problem 11.1.

1. n(n+1)/2n2=1+1/n2→12\dfrac{n(n+1)/2}{n^2} = \dfrac{1 + 1/n}{2} \to \dfrac12, and n(n+1)(2n+1)/6n3=(1+1/n)(2+1/n)6→13\dfrac{n(n+1)(2n+1)/6}{n^3} = \dfrac{(1 + 1/n)(2 + 1/n)}{6} \to \dfrac13.

2. Upper: each of the nn terms is ≤n\leq \sqrt n, so Tn≤nnT_n \leq n\sqrt n. Lower: the terms with k>n2k > \frac n2 number at least n2\frac n2, and each is ≥n/2\geq \sqrt{n/2}:

Tn≥n2n2=n3/222.T_n \geq \frac n2 \sqrt{\frac n2} = \frac{n^{3/2}}{2\sqrt 2} .

3. For k≥Nk \geq N, since bk+1−bk>0b_{k+1} - b_k > 0: m(bk+1−bk)≤ak+1−ak≤M(bk+1−bk)m(b_{k+1} - b_k) \leq a_{k+1} - a_k \leq M(b_{k+1} - b_k). Summing for k=N,…,n−1k = N, \dots, n - 1, both sides telescope:

m (bn−bN)≤an−aN≤M (bn−bN),m\,(b_n - b_N) \leq a_n - a_N \leq M\,(b_n - b_N),

and dividing by bn−bN>0b_n - b_N > 0 gives the claim.

4. By definition of the limit there is NN with ℓ−ε≤ak+1−akbk+1−bk≤ℓ+ε\ell - \varepsilon \leq \frac{a_{k+1} - a_k}{b_{k+1} - b_k} \leq \ell + \varepsilon for all k≥Nk \geq N; question 3 with m=ℓ−εm = \ell - \varepsilon, M=ℓ+εM = \ell + \varepsilon transfers the bracketing to an−aNbn−bN\frac{a_n - a_N}{b_n - b_N}.

5. Expanding the right side of the identity:

aN−ℓbNbn+an−aNbn−ℓ bn−bNbn=an−ℓbnbn=anbn−ℓ.\frac{a_N - \ell b_N}{b_n} + \frac{a_n - a_N}{b_n} - \ell\,\frac{b_n - b_N}{b_n} = \frac{a_n - \ell b_n}{b_n} = \frac{a_n}{b_n} - \ell .

By question 4 the second factor of the product is bounded by ε\varepsilon in absolute value, and 0<1−bNbn≤10 < 1 - \frac{b_N}{b_n} \leq 1 for large nn, so

∣anbn−ℓ∣≤∣aN−ℓbN∣bn+ε≤2ε\Bigl|\frac{a_n}{b_n} - \ell\Bigr| \leq \frac{\abs{a_N - \ell b_N}}{b_n} + \varepsilon \leq 2\varepsilon

as soon as bn≥∣aN−ℓbN∣εb_n \geq \frac{\abs{a_N - \ell b_N}}{\varepsilon}, which happens eventually since bn→+∞b_n \to +\infty. Hence anbn→ℓ\frac{a_n}{b_n} \to \ell: the Cesàro–Stolz theorem.

6. Given MM, choose NN with ak+1−akbk+1−bk≥M\frac{a_{k+1} - a_k}{b_{k+1} - b_k} \geq M for k≥Nk \geq N; the lower half of question 3 gives an−aN≥M(bn−bN)a_n - a_N \geq M(b_n - b_N), so

anbn≥aNbn+M(1−bNbn)⟶M.\frac{a_n}{b_n} \geq \frac{a_N}{b_n} + M\Bigl(1 - \frac{b_N}{b_n}\Bigr) \longrightarrow M .

Beyond some rank, anbn≥M−1\frac{a_n}{b_n} \geq M - 1; as MM was arbitrary, anbn→+∞\frac{a_n}{b_n} \to +\infty.

7. With bn=nb_n = n and an=u1+⋯+una_n = u_1 + \dots + u_n: the increment quotient is un+1→ℓu_{n+1} \to \ell, so the Cesàro mean ann\frac{a_n}{n} tends to ℓ\ell: part (1) of Exercise 11.10. With an=una_n = u_n: the increment quotient is un+1−unu_{n+1} - u_n, giving part (3). Converse: an=(−1)na_n = (-1)^n, bn=nb_n = n has anbn→0\frac{a_n}{b_n} \to 0, yet an+1−an=±2a_{n+1} - a_n = \pm 2 alternates: the increment quotient has no limit.

8. Conjugation:

((1+h)3/2−1)((1+h)3/2+1)=(1+h)3−1=3h+3h2+h3.\bigl((1+h)^{3/2} - 1\bigr)\bigl((1+h)^{3/2} + 1\bigr) = (1+h)^3 - 1 = 3h + 3h^2 + h^3 .

For h=1nh = \frac1n: n((1+1n)3/2−1)=3+3/n+1/n2(1+1/n)3/2+1n\bigl((1 + \frac1n)^{3/2} - 1\bigr) = \frac{3 + 3/n + 1/n^2}{(1 + 1/n)^{3/2} + 1}, and 1≤(1+1n)3/2≤(1+1n)2→11 \leq (1 + \frac1n)^{3/2} \leq (1 + \frac1n)^2 \to 1 (squeeze), so the denominator tends to 22 and the expression to 32\frac32. Now Stolz with an=Tna_n = T_n, bn=n3/2b_n = n^{3/2} (strictly increasing, →+∞\to +\infty):

n+1(n+1)3/2−n3/2=n+1n⋅1n((1+1n)3/2−1)⟶1⋅23,\frac{\sqrt{n+1}}{(n+1)^{3/2} - n^{3/2}} = \frac{\sqrt{n+1}}{\sqrt n} \cdot \frac{1}{n\bigl((1 + \frac1n)^{3/2} - 1\bigr)} \longrightarrow 1 \cdot \frac{2}{3},

hence Tn∼23 n3/2T_n \sim \frac23\,n^{3/2}. (The bracketing of question 2 had trapped the constant in [0.35, 1]\intcc{0.35}{1}; Stolz pins it.)

9. (G1) at u=ln⁡(1+t)u = \ln(1+t): 1+t=eln⁡(1+t)≥1+ln⁡(1+t)1 + t = \eu^{\ln(1+t)} \geq 1 + \ln(1+t), so ln⁡(1+t)≤t\ln(1+t) \leq t. (G1) at u=−t1+tu = -\frac{t}{1+t}: e−t/(1+t)≥1−t1+t=11+t>0\eu^{-t/(1+t)} \geq 1 - \frac{t}{1+t} = \frac{1}{1+t} > 0; taking ln⁡\ln (increasing): −t1+t≥−ln⁡(1+t)-\frac{t}{1+t} \geq -\ln(1+t), i.e. ln⁡(1+t)≥t1+t\ln(1+t) \geq \frac{t}{1+t}.

10. ln⁡\ln is strictly increasing (Proposition 4.1), and ln⁡(2k)=kln⁡2\ln(2^k) = k\ln 2 is unbounded, so ln⁡n→+∞\ln n \to +\infty. Increments: with t=1nt = \frac1n in question 9,

1n+1=1/n1+1/n≤ln⁡(1+1n)≤1n⟹nn+1≤1/(n+1)ln⁡(1+1/n)≤1,\frac 1{n+1} = \frac{1/n}{1 + 1/n} \leq \ln\Bigl(1 + \frac1n\Bigr) \leq \frac1n \quad\Longrightarrow\quad \frac{n}{n+1} \leq \frac{1/(n+1)}{\ln(1 + 1/n)} \leq 1 ,

so the increment quotient Hn+1−Hnln⁡(n+1)−ln⁡n\frac{H_{n+1} - H_n}{\ln(n+1) - \ln n} tends to 11; Stolz gives Hn∼ln⁡nH_n \sim \ln n.

11. Set xn=un+1un→Lx_n = \frac{u_{n+1}}{u_n} \to L and tn=xnL−1→0t_n = \frac{x_n}{L} - 1 \to 0. Question 9: tn1+tn≤ln⁡(1+tn)≤tn\frac{t_n}{1 + t_n} \leq \ln(1 + t_n) \leq t_n, so ln⁡xn−ln⁡L=ln⁡(1+tn)→0\ln x_n - \ln L = \ln(1 + t_n) \to 0 by squeezing. Cesàro (question 7) applied to (ln⁡xk)(\ln x_k):

1n∑k=0n−1ln⁡xk=ln⁡un−ln⁡u0n⟶ln⁡L,\frac1n \sum_{k=0}^{n-1} \ln x_k = \frac{\ln u_n - \ln u_0}{n} \longrightarrow \ln L ,

so ln⁡unn→ln⁡L\frac{\ln u_n}{n} \to \ln L. With hn=ln⁡unn−ln⁡L→0h_n = \frac{\ln u_n}{n} - \ln L \to 0: un1/n=L ehnu_n^{1/n} = L\,\eu^{h_n}, and (G1) squeezes 1+hn≤ehn≤11−hn1 + h_n \leq \eu^{h_n} \leq \frac{1}{1 - h_n} (for hn<1h_n < 1), so ehn→1\eu^{h_n} \to 1 and un1/n→Lu_n^{1/n} \to L. Application: un=(2nn)u_n = \binom{2n}{n} gives

un+1un=(2n+1)(2n+2)(n+1)2=2(2n+1)n+1⟶4,so(2nn)1/n→4.\frac{u_{n+1}}{u_n} = \frac{(2n+1)(2n+2)}{(n+1)^2} = \frac{2(2n+1)}{n+1} \longrightarrow 4 , \qquad\text{so}\qquad \binom{2n}{n}^{1/n} \to 4 .

12. For 0<x≤10 < x \leq 1, (G2) gives sin⁡x≥x(1−x26)≥5x6>0\sin x \geq x(1 - \frac{x^2}{6}) \geq \frac{5x}{6} > 0 and

x−sin⁡x≥x36−x5120=x3(16−x2120)≥19120 x3>0:x - \sin x \geq \frac{x^3}{6} - \frac{x^5}{120} = x^3\Bigl(\frac16 - \frac{x^2}{120}\Bigr) \geq \frac{19}{120}\,x^3 > 0 :

thus 0<sin⁡x<x0 < \sin x < x on (0, 1]\intoc{0}{1}. Always u1=sin⁡u0∈[−1, 1]u_1 = \sin u_0 \in \intcc{-1}{1}. If u1=0u_1 = 0, then un=0u_n = 0 for n≥1n \geq 1. If u1∈(0, 1]u_1 \in \intoc{0}{1}: by induction 0<un+1=sin⁡un<un≤10 < u_{n+1} = \sin u_n < u_n \leq 1, so (un)n≥1(u_n)_{n\geq1} is strictly decreasing and bounded below by 00: it converges to some ℓ∈[0, 1)\ell \in \intco{0}{1} (Theorem 11.9). The product-to-sum formula and (G2) give ∣sin⁡a−sin⁡b∣=2∣cos⁡a+b2∣ ∣sin⁡a−b2∣≤∣a−b∣\abs{\sin a - \sin b} = 2\abs{\cos \frac{a+b}{2}}\,\abs{\sin\frac{a-b}{2}} \leq \abs{a - b}, so un+1=sin⁡un→sin⁡ℓu_{n+1} = \sin u_n \to \sin \ell: ℓ=sin⁡ℓ\ell = \sin\ell. If ℓ>0\ell > 0 then sin⁡ℓ<ℓ\sin\ell < \ell: impossible. So un→0u_n \to 0.

13. Dividing (G2) by un>0u_n > 0:

1−un26≤sin⁡unun≤1−un26+un4120≤1,1 - \frac{u_n^2}{6} \leq \frac{\sin u_n}{u_n} \leq 1 - \frac{u_n^2}{6} + \frac{u_n^4}{120} \leq 1 ,

and un→0u_n \to 0 squeezes sin⁡unun→1\frac{\sin u_n}{u_n} \to 1. Dividing x−sin⁡xx - \sin x by x3x^3:

16−un2120≤un−sin⁡unun3≤16⟶16.\frac16 - \frac{u_n^2}{120} \leq \frac{u_n - \sin u_n}{u_n^3} \leq \frac16 \longrightarrow \frac16 .

14. Since un+1=sin⁡unu_{n+1} = \sin u_n:

wn=un2−sin⁡2unun2sin⁡2un=(un−sin⁡un)(un+sin⁡un)un2sin⁡2un=un−sin⁡unun3⋅un+sin⁡unun⋅(unsin⁡un)2w_n = \frac{u_n^2 - \sin^2 u_n}{u_n^2 \sin^2 u_n} = \frac{(u_n - \sin u_n)(u_n + \sin u_n)}{u_n^2 \sin^2 u_n} = \frac{u_n - \sin u_n}{u_n^3}\cdot \frac{u_n + \sin u_n}{u_n}\cdot \Bigl(\frac{u_n}{\sin u_n}\Bigr)^{2}

(check the powers of unu_n: 3+1+(−4)3 + 1 + (-4) against the un2u_n^2 downstairs and un4u_n^4 upstairs). By question 13 the three factors tend to 16\frac16, 22, 11: wn→13w_n \to \frac13.

15. vn=1un2v_n = \frac{1}{u_n^2} has increments vn+1−vn=wn→13v_{n+1} - v_n = w_n \to \frac13, so vnn→13\frac{v_n}{n} \to \frac13 by Exercise 11.10 (3): nun2→3n u_n^2 \to 3. Then

∣n un−3∣=∣nun2−3∣n un+3≤∣nun2−3∣3⟶0:\abs{\sqrt n\,u_n - \sqrt 3} = \frac{\abs{n u_n^2 - 3}}{\sqrt n\,u_n + \sqrt 3} \leq \frac{\abs{n u_n^2 - 3}}{\sqrt 3} \longrightarrow 0 :

n un→3\sqrt n\,u_n \to \sqrt 3, i.e. un∼3/nu_n \sim \sqrt{3/n}.

16. Since nun2→3n u_n^2 \to 3, eventually 2≤nun2≤42 \leq n u_n^2 \leq 4, i.e. 2/n≤un≤2/n\sqrt{2/n} \leq u_n \leq 2/\sqrt n. If un≤10−2u_n \leq 10^{-2} with nn in that range, then 2/n≤10−42/n \leq 10^{-4}: n≥20 000n \geq 20\,000; and 3/n=10−2\sqrt{3/n} = 10^{-2} at n=30 000n = 30\,000. Heron’s method squares the error at each step — the digit count doubles — because at its fixed point the relevant slope is <1< 1 in modulus (indeed the iteration is contracting). Here sin⁡′0=cos⁡0=1\sin' 0 = \cos 0 = 1: the fixed point is neutral, no geometric contraction exists, and the decay is governed by the first nonlinear term −x36-\frac{x^3}{6}, hence polynomial. One step of Heron gains more accuracy than ten thousand steps of the sine.

17. For arbitrary u0u_0: u1=sin⁡u0∈[−1, 1]u_1 = \sin u_0 \in \intcc{-1}{1}. If u1=0u_1 = 0 the sequence vanishes from rank 11. If u1>0u_1 > 0, Part IV applies verbatim. If u1<0u_1 < 0, set vn=−unv_n = -u_n: oddness of sin⁡\sin gives vn+1=−sin⁡un=sin⁡(−un)=sin⁡vnv_{n+1} = -\sin u_n = \sin(-u_n) = \sin v_n with v1∈(0, 1]v_1 \in \intoc{0}{1}, so vn∼3/nv_n \sim \sqrt{3/n}, i.e. un∼−3/nu_n \sim -\sqrt{3/n}. In all cases ∣un∣∼3/n\abs{u_n} \sim \sqrt{3/n} (or the sequence is eventually 00): the fall is universal, only the sign remembers the start.

18. First un+1un=1−un−un+1un2 un→1−a⋅0=1\frac{u_{n+1}}{u_n} = 1 - \frac{u_n - u_{n+1}}{u_n^2}\,u_n \to 1 - a \cdot 0 = 1. Then

1un+1−1un=un−un+1unun+1=un−un+1un2⋅unun+1⟶a⋅1=a,\frac{1}{u_{n+1}} - \frac{1}{u_n} = \frac{u_n - u_{n+1}}{u_n u_{n+1}} = \frac{u_n - u_{n+1}}{u_n^2}\cdot\frac{u_n}{u_{n+1}} \longrightarrow a \cdot 1 = a ,

and Exercise 11.10 (3) gives 1nun→a\frac{1}{n u_n} \to a, i.e. nun→1an u_n \to \frac1a.

19. vn=1unv_n = \frac{1}{u_n}: vn+1=1+unun=vn+1v_{n+1} = \frac{1 + u_n}{u_n} = v_n + 1, so vn=v0+nv_n = v_0 + n and

un=u01+nu0,nun=nu01+nu0⟶1.u_n = \frac{u_0}{1 + n u_0} , \qquad n u_n = \frac{n u_0}{1 + n u_0} \longrightarrow 1 .

Lemma check: un−un+1=un21+unu_n - u_{n+1} = \frac{u_n^2}{1 + u_n}, so un−un+1un2=11+un→1=a\frac{u_n - u_{n+1}}{u_n^2} = \frac{1}{1 + u_n} \to 1 = a, and question 18 predicts nun→1n u_n \to 1: exact agreement.

20. Positivity by induction (e−u>0\eu^{-u} > 0); decreasing since e−un<1\eu^{-u_n} < 1 for un>0u_n > 0; hence un→ℓ≥0u_n \to \ell \geq 0 (Theorem 11.9). Continuity bridge: with hn=ℓ−un→0h_n = \ell - u_n \to 0, e−un=e−ℓehn→e−ℓ\eu^{-u_n} = \eu^{-\ell} \eu^{h_n} \to \eu^{-\ell} by the (G1) squeeze 1+hn≤ehn≤11−hn1 + h_n \leq \eu^{h_n} \leq \frac{1}{1 - h_n}; so ℓ=ℓ e−ℓ\ell = \ell\, \eu^{-\ell}, and ℓ>0\ell > 0 would force e−ℓ=1\eu^{-\ell} = 1, false: ℓ=0\ell = 0. For t>0t > 0, (G1) gives e−t≥1−t\eu^{-t} \geq 1 - t and e−t≤11+t\eu^{-t} \leq \frac{1}{1 + t}, so

11+t≤1−e−tt≤1.\frac{1}{1 + t} \leq \frac{1 - \eu^{-t}}{t} \leq 1 .

With t=unt = u_n: un−un+1un2=1−e−unun→1\frac{u_n - u_{n+1}}{u_n^2} = \frac{1 - \eu^{-u_n}}{u_n} \to 1. Question 18 with a=1a = 1: nun→1n u_n \to 1, so un∼1nu_n \sim \frac1n.

21. As in question 18, un+1un=1−un−un+1un3 un2→1\frac{u_{n+1}}{u_n} = 1 - \frac{u_n - u_{n+1}}{u_n^3}\,u_n^2 \to 1. Then

1un+12−1un2=(un−un+1)(un+un+1)un2un+12=un−un+1un3⋅un+un+1un⋅(unun+1)2⟶a⋅2⋅1=2a,\frac{1}{u_{n+1}^2} - \frac{1}{u_n^2} = \frac{(u_n - u_{n+1})(u_n + u_{n+1})}{u_n^2 u_{n+1}^2} = \frac{u_n - u_{n+1}}{u_n^3}\cdot \frac{u_n + u_{n+1}}{u_n}\cdot \Bigl(\frac{u_n}{u_{n+1}}\Bigr)^2 \longrightarrow a \cdot 2 \cdot 1 = 2a ,

and Exercise 11.10 (3) gives 1nun2→2a\frac{1}{n u_n^2} \to 2a: nun2→12an u_n^2 \to \frac{1}{2a}. For the sine, a=16a = \frac16 (question 13): nun2→3n u_n^2 \to 3, exactly Part IV.

22. Increments: an+1−an=2−n−2−n−1=2−n−1=bn+1−bna_{n+1} - a_n = 2^{-n} - 2^{-n-1} = 2^{-n-1} = b_{n+1} - b_n, so the increment quotient is constantly 11. Yet anbn=2−2−n1−2−n→2≠1\frac{a_n}{b_n} = \frac{2 - 2^{-n}}{1 - 2^{-n}} \to 2 \neq 1. The proof of question 5 breaks at the boundary term: aN−ℓbNbn→0\frac{a_N - \ell b_N}{b_n} \to 0 needed bn→+∞b_n \to +\infty; here (with ℓ=1\ell = 1) aN−bN=1a_N - b_N = 1 and bn→1b_n \to 1, so the term tends to 11 — precisely the residual gap 2−12 - 1.

23. Stolz with An=∑k=1nHkA_n = \sum_{k=1}^n H_k and Bn=nln⁡nB_n = n\ln n: Bn+1−Bn=ln⁡(n+1)+nln⁡(1+1n)>0B_{n+1} - B_n = \ln(n+1) + n\ln(1 + \frac1n) > 0 and Bn→+∞B_n \to +\infty. By question 9, nn+1≤nln⁡(1+1n)≤1\frac{n}{n+1} \leq n\ln(1 + \frac1n) \leq 1, so Bn+1−Bn=ln⁡(n+1)+θnB_{n+1} - B_n = \ln(n+1) + \theta_n with 12≤θn≤1\frac12 \leq \theta_n \leq 1. Hence

An+1−AnBn+1−Bn=Hn+1ln⁡(n+1)⋅11+θn/ln⁡(n+1)⟶1⋅1=1\frac{A_{n+1} - A_n}{B_{n+1} - B_n} = \frac{H_{n+1}}{\ln(n+1)}\cdot \frac{1}{1 + \theta_n/\ln(n+1)} \longrightarrow 1 \cdot 1 = 1

(question 10 for the first factor; θn\theta_n bounded and ln⁡(n+1)→∞\ln(n+1) \to \infty for the second). Stolz concludes: ∑k=1nHk∼nln⁡n\sum_{k=1}^n H_k \sim n\ln n.

24. If un→ℓ>0u_n \to \ell > 0: as in question 11, ln⁡un→ln⁡ℓ\ln u_n \to \ln\ell (question 9 squeeze on ln⁡unℓ\ln\frac{u_n}{\ell}), so the Cesàro means 1n∑k=1nln⁡uk→ln⁡ℓ\frac1n\sum_{k=1}^n \ln u_k \to \ln\ell, and the exponential bridge of question 11 gives (u1⋯un)1/n=exp⁡(1n∑ln⁡uk)→ℓ(u_1\cdots u_n)^{1/n} = \exp\bigl(\frac1n\sum\ln u_k\bigr) \to \ell. If un→+∞u_n \to +\infty: for any MM, eventually un≥eMu_n \geq \eu^M, so ln⁡un≥M\ln u_n \geq M: ln⁡un→+∞\ln u_n \to +\infty; the +∞+\infty Cesàro (question 6, bn=nb_n = n) gives 1n∑ln⁡uk→+∞\frac1n\sum \ln u_k \to +\infty, and (G1) (es≥1+s\eu^s \geq 1 + s) sends the geometric mean to +∞+\infty. With un=nu_n = n: (n!)1/n→+∞(n!)^{1/n} \to +\infty.

25. (i) Completeness entered only through the monotone limit theorem, to produce the limits in questions 12 and 20; the Cesàro–Stolz theorem itself is pure ε\varepsilon-management, valid over Q\Q. (ii) Stolz replaces lim⁡anbn\lim \frac{a_n}{b_n} by lim⁡\lim of the quotient of increments, exactly as l’Hospital replaces lim⁡fg\lim\frac fg by lim⁡f′g′\lim\frac{f'}{g'} — the differential twin rests on the mean value theorem of Chapter 14. (iii) Heuristic: if f(x)=x−a xp+1+o(xp+1)f(x) = x - a\,x^{p+1} + o(x^{p+1}) at the neutral fixed point 00, then 1un+1p−1unp→pa\frac{1}{u_{n+1}^p} - \frac{1}{u_n^p} \to pa and un∼(pan)−1/pu_n \sim (pan)^{-1/p}: contact of order p+1p + 1 yields decay n−1/pn^{-1/p} — the flatter the graph against the diagonal, the slower the fall. (iv) The constant: (G2) supplies the cubic coefficient 16\frac16; the factorization of question 14 doubles it into the telescope increment 13\frac13; Cesàro turns 1un2\frac{1}{u_n^2} into n3\frac n3; inverting and taking roots delivers 3/n\sqrt{3/n}.

Terms defined in this chapter

See all 395 terms in the glossary