24 Bernoulli and Euler PolynomialsProperties

§24.7 Integral Representations

Contents
  1. §24.7(i) Bernoulli and Euler Numbers
  2. §24.7(ii) Bernoulli and Euler Polynomials
  3. §24.7(iii) Compendia

§24.7(i) Bernoulli and Euler Numbers

The identities in this subsection hold for n=1,2,…. (24.7.6) also holds for n=0.

24.7.1 B2⁢n =(−1)n+1⁢4⁢n1−21−2⁢n⁢∫0∞t2⁢n−1e2⁢π⁢t+1⁢dt=(−1)n+1⁢2⁢n1−21−2⁢n⁢∫0∞t2⁢n−1⁢e−π⁢t⁢sech⁡(π⁢t)⁢dt,
24.7.2 B2⁢n =(−1)n+1⁢4⁢n⁢∫0∞t2⁢n−1e2⁢π⁢t−1⁢dt=(−1)n+1⁢2⁢n⁢∫0∞t2⁢n−1⁢e−π⁢t⁢csch⁡(π⁢t)⁢dt,
24.7.3 B2⁢n =(−1)n+1⁢π1−21−2⁢n⁢∫0∞t2⁢n⁢sech2⁡(π⁢t)⁢dt,
24.7.4 B2⁢n =(−1)n+1⁢π⁢∫0∞t2⁢n⁢csch2⁡(π⁢t)⁢dt,
24.7.5 B2⁢n =(−1)n⁢2⁢n⁢(2⁢n−1)π⁢∫0∞t2⁢n−2⁢ln⁡(1−e−2⁢π⁢t)⁢dt.
24.7.6 E2⁢n =(−1)n⁢22⁢n+1⁢∫0∞t2⁢n⁢sech⁡(π⁢t)⁢dt.

§24.7(ii) Bernoulli and Euler Polynomials

The following four equations hold for 0<ℜ⁡x<1.

24.7.7 B2⁢n⁡(x) =(−1)n+1⁢2⁢n⁢∫0∞cos⁡(2⁢π⁢x)−e−2⁢π⁢tcosh⁡(2⁢π⁢t)−cos⁡(2⁢π⁢x)⁢t2⁢n−1⁢dt,
n=1,2,…,
24.7.8 B2⁢n+1⁡(x) =(−1)n+1⁢(2⁢n+1)⁢∫0∞sin⁡(2⁢π⁢x)cosh⁡(2⁢π⁢t)−cos⁡(2⁢π⁢x)⁢t2⁢n⁢dt.
24.7.9 E2⁢n⁡(x) =(−1)n⁢4⁢∫0∞sin⁡(π⁢x)⁢cosh⁡(π⁢t)cosh⁡(2⁢π⁢t)−cos⁡(2⁢π⁢x)⁢t2⁢n⁢dt,
24.7.10 E2⁢n+1⁡(x) =(−1)n+1⁢4⁢∫0∞cos⁡(π⁢x)⁢sinh⁡(π⁢t)cosh⁡(2⁢π⁢t)−cos⁡(2⁢π⁢x)⁢t2⁢n+1⁢dt.

Mellin–Barnes Integral

24.7.11 Bn⁡(x)=12⁢π⁢i⁢∫−c−i⁢∞−c+i⁢∞(x+t)n⁢(πsin⁡(π⁢t))2⁢dt,
0<c<1.

§24.7(iii) Compendia

For further integral representations see Prudnikov et al. (1986a, §§2.3–2.6) and Gradshteyn and Ryzhik (2015, Chapters 3 and 4).