Bourbaki

Corollary 2

Tag 08IE, permanent. Cite it as [Bourbaki, Tag 08IE].

Functions of a Real Variable, chapter VI, § 2. EULERIAN EXPANSIONS OF THE TRIGONOMETRIC FUNCTIONS AND BERNOULLI NUMBERS

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:

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

Cited by

Nothing.

Cites

Nothing.

Transcribed from the printed volume. Not translated.