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Bernoulli polynomials
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==Another explicit formula== An explicit formula for the Bernoulli polynomials is given by <math display="block"> B_n(x) = \sum_{k=0}^n \biggl[ \frac{1}{k + 1} \sum_{\ell=0}^k (-1)^\ell { k \choose \ell } (x + \ell)^n \biggr].</math> That is similar to the series expression for the [[Hurwitz zeta function]] in the complex plane. Indeed, there is the relationship <math display="block">B_n(x) = -n \zeta(1 - n,\,x)</math> where <math>\zeta(s,\,q)</math> is the [[Hurwitz zeta function]]. The latter generalizes the Bernoulli polynomials, allowing for non-integer values {{nobr|of {{mvar|n}}.}} The inner sum may be understood to be the {{mvar|n}}th [[forward difference]] of <math>x^m,</math> that is, <math display="block">\Delta^n x^m = \sum_{k=0}^n (-1)^{n - k}{n \choose k}(x + k)^m</math> where <math>\Delta</math> is the [[forward difference operator]]. Thus, one may write <math display="block">B_n(x) = \sum_{k=0}^n \frac{(-1)^k}{k + 1}\Delta^k x^n.</math> This formula may be derived from an identity appearing above as follows. Since the forward difference operator {{math|Δ}} equals <math display="block">\Delta = e^D - 1</math> where {{mvar|D}} is differentiation with respect to {{mvar|x}}, we have, from the [[Mercator series]], <math display="block">\frac{ D }{e^D - 1} = \frac{\log(\Delta + 1)}{\Delta} = \sum_{n=0}^\infty \frac{(-\Delta)^n }{n + 1}.</math> As long as this operates on an {{mvar|m}}th-degree polynomial such as <math>x^m,</math> one may let {{mvar|n}} go from {{math|0}} only up {{nobr|to {{mvar|m}}.}} An integral representation for the Bernoulli polynomials is given by the [[Nörlund–Rice integral]], which follows from the expression as a finite difference. An explicit formula for the Euler polynomials is given by <math display="block">E_n(x) = \sum_{k=0}^n \left[ \frac{1}{2^k}\sum_{\ell=0}^n (-1)^\ell {k \choose \ell}(x + \ell)^n \right] .</math> The above follows analogously, using the fact that <math display="block">\frac{2}{e^D + 1} = \frac{1}{1 + \tfrac12 \Delta} = \sum_{n = 0}^\infty \bigl( {-\tfrac{1}{2}} \Delta \bigr)^n .</math>
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