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In mathematics, the Bernoulli numbers Bn were first discovered in connection with the closed forms of the sums
for various fixed values of n. The closed forms are always polynomials in m of degree n+1 and are called Bernoulli polynomials. The coefficients of the Bernoulli polynomials are closely related to the Bernoulli numbers, as follows:
For example, taking n to be 1, we have 0 + 1 + 2 + ... + (m−1) = 1/2 (B0 m2 + 2 B1 m1) = 1/2 (m2 − m).
The Bernoulli numbers were first studied by Jakob Bernoulli, after whom they were named by Abraham de Moivre.
Bernoulli numbers may be calculated by using the following recursive formula:
plus the initial condition that B0 = 1.
The Bernoulli numbers may also be defined using the technique of generating functions. Their exponential generating function is x/(ex − 1), so that:
\frac{x}{e^x-1} = \sum_{n=0}^{\infin} B_n \frac{x^n}{n!} <math> for all values of x of absolute value less than 2π (the radius of convergence of this power series).
Sometimes the lower-case bn is used in order to distinguish these from the Bell numbers.
The first few Bernoulli numbers (sequences and in OEIS) are listed below.
| n | Bn |
|---|---|
| 0 | 1 |
| 1 | −1/2 |
| 2 | 1/6 |
| 3 | 0 |
| 4 | −1/30 |
| 5 | 0 |
| 6 | 1/42 |
| 7 | 0 |
| 8 | −1/30 |
| 9 | 0 |
| 10 | 5/66 |
| 11 | 0 |
| 12 | −691/2730 |
| 13 | 0 |
| 14 | 7/6 |
It can be shown that Bn = 0 for all odd n other than 1. The appearance of the peculiar value B12 = −691/2730 appears to rule out the possibility of a simple closed form for Bernoulli numbers.
The Bernoulli numbers also appear in the Taylor series expansion of the tangent and hyperbolic tangent functions, in the Euler-Maclaurin formula, and in expressions of certain values of the Riemann zeta function.
In note G of Ada Byron's notes on the analytical engine from 1842 an algorithm for computer generated Bernoulli numbers was described for the first time.