Bourbaki

§ 2. Eulerian expansions of the trigonometric functions and Bernoulli numbers

1. Eulerian expansion of cot⁡z\cot z

By formula (20) of VI, p. 275, the numbers bn/n!b_n / n! are the coefficients in the expansion of S/(eS−1)S/(e^S - 1) as a formal series; we shall show in this section that the function z/(ez−1)z/(e^z - 1) is equal to the sum of an absolutely convergent entire series on a neighbourhood of 0 in C\mathbf{C}; it will follow from the lemma of VI, p. 280, that the coefficients of this series are the numbers bn/n!b_n / n!, from which we shall deduce estimates for the Bernoulli numbers bnb_n.

In the first place we note that

zez−1=−z2+z2ez+1ez−1=−z2+iz2cot⁡iz2. \frac{z}{e^z - 1} = - \frac{z}{2} + \frac{z}{2} \frac{e^z + 1}{e^z - 1} = - \frac{z}{2} + \frac{iz}{2} \cot \frac{iz}{2}.
(1)

We shall obtain below a series expansion for cot⁡z\cot z, valid for every zz not an integer multiple of π\pi.

Proposition 1

For every complex number* zz and every integer nn *one has

sin⁡nz=2n−1sin⁡zsin⁡(z+πn)sin⁡(z+2πn)…sin⁡(z+(n−1)πn). \sin nz = 2^{n-1} \sin z \sin \left(z + \frac{\pi}{n}\right) \sin \left(z + \frac{2\pi}{n}\right) \ldots \sin \left(z + \frac{(n-1)\pi}{n}\right).
(2)

Indeed, one can write

sin⁡nz=eniz−e−niz2i=e−niz(e2niz−1)2i=e−niz(e2iz−1)(e2iz−e−2iπ/n)…(e2iz−e−2(n−1)iπ/n)2i=Asin⁡zsin⁡(z+πn)sin⁡(z+2πn)…sin⁡(z+(n−1)πn) \sin nz = \frac{e^{niz} - e^{-niz}}{2i} = \frac{e^{-niz}(e^{2niz} - 1)}{2i} = \frac{e^{-niz}(e^{2iz} - 1)(e^{2iz} - e^{-2i\pi/n}) \ldots (e^{2iz} - e^{-2(n-1)i\pi/n})}{2i} = A \sin z \sin \left( z + \frac{\pi}{n} \right) \sin \left( z + \frac{2\pi}{n} \right) \ldots \sin \left( z + \frac{(n-1)\pi}{n} \right)

where

A=(2i)n−1e−iπn(1+2+…+(n−1))=(2i)n−1e−i(n−1)π2=2n−1. A = (2i)^{n-1} e^{-\frac{i\pi}{n}(1+2+\ldots+(n-1))} = (2i)^{n-1} e^{-i(n-1)\frac{\pi}{2}} = 2^{n-1}.

Corollary 1

For every integer n one has*

sin⁡πnsin⁡2πn…sin⁡(n−1)πn=n2n−1. \sin \frac{\pi}{n} \sin \frac{2\pi}{n} \ldots \sin \frac{(n-1)\pi}{n} = \frac{n}{2^{n-1}}.
(3)

It suffices to divide both sides of (2) by sin⁡z\sin z and let zz tend to 0.

Corollary 2

For every odd integer n=2m+1n = 2m + 1, and every complex number zz such that nznz is not an integral multiple of π\pi, one has*

cot⁡nz=(−1)mcot⁡zcot⁡(z+πn)…cot⁡(z+(n−1)πn). \cot nz = (-1)^m \cot z \cot \left( z + \frac{\pi}{n} \right) \ldots \cot \left( z + \frac{(n-1)\pi}{n} \right).
(4)

Indeed, sin⁡n(z+π2)=sin⁡(nz+π2+mπ)=(−1)mcos⁡nz\sin n \left( z + \frac{\pi}{2} \right) = \sin \left( nz + \frac{\pi}{2} + m\pi \right) = (-1)^m \cos nz, whence, replacing zz by z+π2z + \frac{\pi}{2} in (2),

cos⁡nz=(−1)m2n−1cos⁡zcos⁡(z+πn)…cos⁡(z+(n−1)πn) \cos nz = (-1)^m 2^{n-1} \cos z \cos \left( z + \frac{\pi}{n} \right) \ldots \cos \left( z + \frac{(n-1)\pi}{n} \right)
(5)

and the formulae (2) and (5) give (4) on division term-by-term when sin⁡nz≠0\sin nz \neq 0.

In all that follows we shall always assume that n=2m+1n = 2m + 1 is an odd integer; the formula (4) can also be written

cot⁡nz=(−1)m∏k=−mmcot⁡(z−kπn). \cot nz = (-1)^m \prod_{k=-m}^{m} \cot \left( z - \frac{k\pi}{n} \right).

or, one has

cot⁡(z−kπn)=1+tan⁡ztan⁡kπntan⁡z−tan⁡kπn \cot \left( z - \frac{k\pi}{n} \right) = \frac{1 + \tan z \tan \frac{k\pi}{n}}{\tan z - \tan \frac{k\pi}{n}}

for tan z finite; cot nznz is thus a rational function in u=tan⁡zu = \tan z, whose numerator is of degree n−1n - 1, and whose denominator, of degree nn, has the nn simple roots tan⁡kπ/n\tan k\pi / n; decomposing this into simple fractions yields

cot⁡nz=∑k=−mmAku−tan⁡kπn \cot nz = \sum_{k=-m}^{m} \frac{A_k}{u - \tan \frac{k\pi}{n}}

where

Ak=lim⁡z→kπ/ncot⁡nz(tan⁡z−tan⁡kπn)=lim⁡z→kπ/ncos⁡nzsin⁡nzsin⁡(z−kπn)cos⁡zcos⁡kπn A_k = \lim_{z \to k\pi/n} \cot nz \left( \tan z - \tan \frac{k\pi}{n} \right) = \lim_{z \to k\pi/n} \frac{\cos nz}{\sin nz} \frac{\sin \left( z - \frac{k\pi}{n} \right)}{\cos z \cos \frac{k\pi}{n}}
=lim⁡h→0cos⁡nhcos⁡kπncos⁡(h+kπn)sin⁡hsin⁡nh=1ncos⁡2kπn = \lim_{h \to 0} \frac{\cos nh}{\cos \frac{k\pi}{n} \cos \left( h + \frac{k\pi}{n} \right)} \frac{\sin h}{\sin nh} = \frac{1}{n \cos^2 \frac{k\pi}{n}}

whence, on isolating the term in (6) corresponding to k=0k = 0 and combining the terms corresponding to opposite values of kk, and replacing zz by z/nz/n,

cot⁡z=1ntan⁡zn+∑k=1m2ntan⁡zncos⁡2kπn(ntan⁡zn)2−(nsin⁡kπn)2 \cot z = \frac{1}{n \tan \frac{z}{n}} + \sum_{k=1}^{m} \frac{2n \tan \frac{z}{n}}{\cos^2 \frac{k\pi}{n} \left( n \tan \frac{z}{n} \right)^2 - \left( n \sin \frac{k\pi}{n} \right)^2}

valid for every complex number zz not an integral multiple of π/2\pi/2. One can write this formula in the form

cot⁡z=1ntan⁡zn+∑k=1∞vk(n,z) \cot z = \frac{1}{n \tan \frac{z}{n}} + \sum_{k=1}^{\infty} v_k(n, z)

with vk(n,z)=0v_k(n, z) = 0 for k>mk > m and

vk(n,z)=2ntan⁡zncos⁡2kπn(ntan⁡zn)2−(nsin⁡kπn)2 v_k(n, z) = \frac{2n \tan \frac{z}{n}}{\cos^2 \frac{k\pi}{n} \left( n \tan \frac{z}{n} \right)^2 - \left( n \sin \frac{k\pi}{n} \right)^2}

for 1≤k≤m1 \leq k \leq m. We shall see that for every zz contained in a compact subset K of C\mathbf{C}, not containing any integral multiple of π\pi, and for every sufficiently large odd nn, the series with general term vk(n,z)v_k(n, z) is normally convergent. Indeed, as nn tends to +∞+\infty, tan⁡zn\tan \frac{z}{n} tends to zn\frac{z}{n} uniformly on K, so there exists a number M>0M > 0 such that ∣ntan⁡zn∣≤M\left| n \tan \frac{z}{n} \right| \leq M for every sufficiently large mm and every z∈Kz \in K. On the other hand, for 0≤x≤π/20 \leq x \leq \pi/2 one has sin⁡x/x≥1−x26≥12\sin x / x \geq 1 - \frac{x^2}{6} \geq \frac{1}{2}, so for 1≤k≤m1 \leq k \leq m one has nsin⁡kπn≥kπ/2n \sin \frac{k\pi}{n} \geq k\pi/2; consequently, when mm is sufficiently large, for every integer kk such that kπ/2>Mk\pi /2 > M one has ∣vk(n,z)∣≤8Mk2π2−4M2|v_k(n, z)| \leq \frac{8M}{k^2 \pi^2 - 4M^2}, which proves our assertion. For kk odd, vk(n,z)v_k(n, z) tends (uniformly on K) to 2zz2−k2π2\frac{2z}{z^2 - k^2 \pi^2} as nn tends to +∞+\infty. Consequently:

Theorem 1

For every complex number zz not an integral multiple of π\pi one has

Cited by 1

Cited by § 2. Eulerian expansions of the trigonometric functions and Bernoulli numbers

cot⁡z=1z+∑n=1∞2zz2−n2π2 \cot z = \frac{1}{z} + \sum_{n=1}^{\infty} \frac{2z}{z^2 - n^2 \pi^2}

(the series on the right being normally convergent on every compact subset K⊂CK \subset \mathbf{C} not containing any integer multiple of π\pi (Eulerian expansion of cot⁡z\cot z).)

2. Eulerian expansion of sin⁡z\sin z

For every odd integer n=2m+1n = 2m + 1 and complex zz the formula (2) of VI, p. 283, can be written

sin⁡nz=(−1)m2n−1∏k=−mmsin⁡(z−kπn) \sin nz = (-1)^m 2^{n-1} \prod_{k=-m}^{m} \sin \left( z - \frac{k\pi}{n} \right)
=(−1)m2n−1sin⁡z∏k=1msin⁡(z−kπn)sin⁡(z+kπn). = (-1)^m 2^{n-1} \sin z \prod_{k=1}^{m} \sin \left( z - \frac{k\pi}{n} \right) \sin \left( z + \frac{k\pi}{n} \right).

Now, one has sin⁡(z−kπn)sin⁡(z+kπn)=sin⁡2z−sin⁡2kπn\sin \left( z - \frac{k\pi}{n} \right) \sin \left( z + \frac{k\pi}{n} \right) = \sin^2 z - \sin^2 \frac{k\pi}{n}, and, by (3) (VI, 284), ∏k=1msin⁡2kπn=n2n−1\prod_{k=1}^{m} \sin^2 \frac{k\pi}{n} = \frac{n}{2^{n-1}}, whence, on replacing zz by z/nz/n,

sin⁡z=nsin⁡zn∏k=1m(1−sin⁡2znsin⁡2kπn). \sin z = n \sin \frac{z}{n} \prod_{k=1}^{m} \left( 1 - \frac{\sin^2 \frac{z}{n}}{\sin^2 \frac{k\pi}{n}} \right).

We can write this formula as sin⁡z=nsin⁡zn∏k=1m(1−wk(n,z))\sin z = n \sin \frac{z}{n} \prod_{k=1}^{m} (1 - w_k(n, z)), with wk(n,z)=0w_k(n, z) = 0 if k>mk > m and wk(n,z)=sin⁡2znsin⁡2kπnw_k(n, z) = \frac{\sin^2 \frac{z}{n}}{\sin^2 \frac{k\pi}{n}} for 1≤k≤m1 \leq k \leq m. We shall see that for every zz contained in a compact subset KK of C\mathbf{C}, and for nn odd, the series with general term wk(n,z)w_k(n, z) is normally convergent. Indeed, as nn tends to +∞+\infty, nsin⁡znn \sin \frac{z}{n} tends uniformly to zz on KK, so there exists a number M>0M > 0 such that ∣nsin⁡zn∣≤M\left| n \sin \frac{z}{n} \right| \leq M for every integer nn and every z∈Kz \in K. We saw, moreover, in the proof of th. 1 of VI, p. 286, that for 1≤k≤m1 \leq k \leq m one has nsin⁡kπn≥kπ2n \sin \frac{k \pi}{n} \geq \frac{k \pi}{2}; thus for every integer kk such that kπ/2≥Mk \pi / 2 \geq M one has ∣wk(n,z)∣≤4M2/k2π2|w_k(n, z)| \leq 4M^2 / k^2 \pi^2, which proves our assertion. Since, for every fixed kk, wk(n,z)w_k(n, z) tends (uniformly on K) to z2/k2π2z^2 / k^2 \pi^2 as nn tends to +∞+\infty, one sees that:

Theorem 2

For every complex number zz one has

sin⁡z=z∏n=1∞(1−z2n2π2) \sin z = z \prod_{n=1}^{\infty} \left( 1 - \frac{z^2}{n^2 \pi^2} \right)

the infinite product on the right being absolutely and uniformly convergent on every compact subset of C\mathbf{C} (Eulerian expansion of sin⁡z\sin z).

3. Application to the Bernoulli numbers

Theorem 1 of VI, p. 286, shows that, for 0≤x<π0 \leq x < \pi, the series with general term

2xn2π2−x2≥0 \frac{2x}{n^2 \pi^2 - x^2} \geq 0

converges. On the other hand, one can write, for every complex number zz such that ∣z∣<π|z| < \pi,

2zn2π2−z2=2zn2π2∑k=0∞z2kn2kπ2k \frac{2z}{n^2 \pi^2 - z^2} = \frac{2z}{n^2 \pi^2} \sum_{k=0}^{\infty} \frac{z^{2k}}{n^{2k} \pi^{2k}}

the series on the right being absolutely convergent. We shall deduce from this that the "double" series

∑n=1∞∑k=1∞−2z2k−1n2kπ2k \sum_{n=1}^{\infty} \sum_{k=1}^{\infty} \frac{-2z^{2k-1}}{n^{2k} \pi^{2k}}

is absolutely convergent in the open disc ∣z∣<π|z| < \pi, normally convergent on every compact set contained in this disc, and has sum cot⁡z−1z\cot z - \frac{1}{z}. Indeed, for ∣z∣≤a<π|z| \leq a < \pi the absolute value of the general term of (11) is at most equal to 2a2k−1/n2kπ2k2a^{2k-1} / n^{2k} \pi^{2k}, and the sum of any finite number of the terms 2a2k−1/n2kπ2k2a^{2k-1} / n^{2k} \pi^{2k} is less than the finite number ∑n=1∞2an2π2−a2\sum_{n=1}^{\infty} \frac{2a}{n^2 \pi^2 - a^2}; on summing first over kk, then over nn, one sees that the sum of the series (11) is equal to ∑n=1∞2zz2−n2π2\sum_{n=1}^{\infty} \frac{2z}{z^2 - n^2 \pi^2}, which proves our statement.

If now one sums the series (11) first over nn and then over kk one obtains the identity (for ∣z∣<π|z| < \pi)

cot⁡z−1z=−2∑k=1∞S2kπ2kz2k−1 \cot z - \frac{1}{z} = -2 \sum_{k=1}^{\infty} \frac{S_{2k}}{\pi^{2k}} z^{2k-1}

where we have put Sk=∑n=1∞1nkS_k = \sum_{n=1}^{\infty} \frac{1}{n^k}. By (1) (VI, p. 283) one thus has, for ∣z∣<2π|z| < 2\pi whence we obtain the formula

b2n=(−1)n−1(2n)!2S2n(2π)2nfor n≥1, b_{2n} = (-1)^{n-1} (2n)! \frac{2 S_{2n}}{(2\pi)^{2n}} \quad \text{for } n \geq 1,

a formula which shows in particular that the numbers S2n/π2nS_{2n}/\pi^{2n} are rational. Clearly Sk+1≤SkS_{k+1} \leq S_k so, for every integer k≥2k \geq 2, we have Sk≤S2=π2/6≤2S_k \leq S_2 = \pi^2/6 \leq 2; from (14) one deduces the following inequalities for the Bernoulli numbers

2(2n)!(2π)2n≤∣b2n∣≤4(2n)!(2π)2nfor n≥1. \frac{2 (2n)!}{(2\pi)^{2n}} \leq |b_{2n}| \leq 4 \frac{(2n)!}{(2\pi)^{2n}} \quad \text{for } n \geq 1.

From these inequalities one can deduce an estimate for the Bernoulli polynomial

Bn(x)=∑k=0n(nk)bkxn−k; in particular, for 0≤x≤1 one has B_n(x) = \sum_{k=0}^n \binom{n}{k} b_k x^{n-k}; \text{ in particular, for } 0 \leq x \leq 1 \text{ one has}
∣Bn(x)∣≤4∑k=0n(nk)k!(2π)k=4n!(2π)n∑k=0n(2π)kk!≤4e2πn!(2π)n. |B_n(x)| \leq 4 \sum_{k=0}^n \binom{n}{k} \frac{k!}{(2\pi)^k} = 4 \frac{n!}{(2\pi)^n} \sum_{k=0}^n \frac{(2\pi)^k}{k!} \leq 4 e^{2\pi} \frac{n!}{(2\pi)^n}.

Exercises

See the exercises for § 2.

Transcribed from the printed volume. Not translated.