Indent Continuation of Sum in Equation

In mathematics, the Abel–Plana formula is a summation formula discovered independently by Niels Henrik Abel (1823) and Giovanni Antonio Amedeo Plana (1820). It states that

n = 0 f ( n ) = 1 2 f ( 0 ) + 0 f ( x ) d x + i 0 f ( i t ) f ( i t ) e 2 π t 1 d t . {\displaystyle \sum _{n=0}^{\infty }f(n)={\frac {1}{2}}f(0)+\int _{0}^{\infty }f(x)\,dx+i\int _{0}^{\infty }{\frac {f(it)-f(-it)}{e^{2\pi t}-1}}\,dt.}

It holds for functions f that are holomorphic in the region Re(z) ≥ 0, and satisfy a suitable growth condition in this region; for example it is enough to assume that |f| is bounded by C/|z|1+ε in this region for some constants C, ε > 0, though the formula also holds under much weaker bounds. (Olver 1997, p.290).

An example is provided by the Hurwitz zeta function,

ζ ( s , α ) = n = 0 1 ( n + α ) s = α 1 s s 1 + 1 2 α s + 2 0 sin ( s arctan t α ) ( α 2 + t 2 ) s 2 d t e 2 π t 1 , {\displaystyle \zeta (s,\alpha )=\sum _{n=0}^{\infty }{\frac {1}{(n+\alpha )^{s}}}={\frac {\alpha ^{1-s}}{s-1}}+{\frac {1}{2\alpha ^{s}}}+2\int _{0}^{\infty }{\frac {\sin \left(s\arctan {\frac {t}{\alpha }}\right)}{(\alpha ^{2}+t^{2})^{\frac {s}{2}}}}{\frac {dt}{e^{2\pi t}-1}},}

which holds for all s C {\displaystyle s\in \mathbb {C} } , s ≠ 1.

Abel also gave the following variation for alternating sums:

n = 0 ( 1 ) n f ( n ) = 1 2 f ( 0 ) + i 0 f ( i t ) f ( i t ) 2 sinh ( π t ) d t . {\displaystyle \sum _{n=0}^{\infty }(-1)^{n}f(n)={\frac {1}{2}}f(0)+i\int _{0}^{\infty }{\frac {f(it)-f(-it)}{2\sinh(\pi t)}}\,dt.}

Proof [edit]

Let f {\displaystyle f} be holomorphic on ( z ) 0 {\displaystyle \Re (z)\geq 0} , such that f ( 0 ) = 0 {\displaystyle f(0)=0} , f ( z ) = O ( | z | k ) {\displaystyle f(z)=O(|z|^{k})} and for arg ( z ) ( β , β ) {\displaystyle {\text{arg}}(z)\in (-\beta ,\beta )} , f ( z ) = O ( | z | 1 δ ) {\displaystyle f(z)=O(|z|^{-1-\delta })} . Taking a = e i β / 2 {\displaystyle a=e^{i\beta /2}} with the residue theorem

a 1 0 + 0 a f ( z ) e 2 i π z 1 d z = 2 i π n = 0 R e s ( f ( z ) e 2 i π z 1 ) = n = 0 f ( n ) . {\displaystyle \int _{a^{-1}\infty }^{0}+\int _{0}^{a\infty }{\frac {f(z)}{e^{-2i\pi z}-1}}dz=-2i\pi \sum _{n=0}^{\infty }\mathrm {Res} \left({\frac {f(z)}{e^{-2i\pi z}-1}}\right)=\sum _{n=0}^{\infty }f(n).}

Then

a 1 0 f ( z ) e 2 i π z 1 d z = 0 a 1 f ( z ) e 2 i π z 1 d z = 0 a 1 f ( z ) e 2 i π z 1 d z + 0 a 1 f ( z ) d z = 0 f ( a 1 t ) e 2 i π a 1 t 1 d ( a 1 t ) + 0 f ( t ) d t . {\displaystyle {\begin{aligned}\int _{a^{-1}\infty }^{0}{\frac {f(z)}{e^{-2i\pi z}-1}}dz&=-\int _{0}^{a^{-1}\infty }{\frac {f(z)}{e^{-2i\pi z}-1}}dz\\&=\int _{0}^{a^{-1}\infty }{\frac {f(z)}{e^{2i\pi z}-1}}dz+\int _{0}^{a^{-1}\infty }f(z)dz\\&=\int _{0}^{\infty }{\frac {f(a^{-1}t)}{e^{2i\pi a^{-1}t}-1}}d(a^{-1}t)+\int _{0}^{\infty }f(t)dt.\end{aligned}}}

Using the Cauchy integral theorem for the last one.

0 a f ( z ) e 2 i π z 1 d z = 0 f ( a t ) e 2 i π a t 1 d ( a t ) , {\displaystyle \int _{0}^{a\infty }{\frac {f(z)}{e^{-2i\pi z}-1}}dz=\int _{0}^{\infty }{\frac {f(at)}{e^{-2i\pi at}-1}}d(at),}

thus obtaining

n = 0 f ( n ) = 0 ( f ( t ) + a f ( a t ) e 2 i π a t 1 + a 1 f ( a 1 t ) e 2 i π a 1 t 1 ) d t . {\displaystyle \sum _{n=0}^{\infty }f(n)=\int _{0}^{\infty }\left(f(t)+{\frac {a\,f(at)}{e^{-2i\pi at}-1}}+{\frac {a^{-1}f(a^{-1}t)}{e^{2i\pi a^{-1}t}-1}}\right)dt.}

This identity stays true by analytic continuation everywhere the integral converges, letting a i {\displaystyle a\to i} we obtain Abel-Plana's formula

n = 0 f ( n ) = 0 ( f ( t ) + i f ( i t ) i f ( i t ) e 2 π t 1 ) d t . {\displaystyle \sum _{n=0}^{\infty }f(n)=\int _{0}^{\infty }\left(f(t)+{\frac {i\,f(it)-i\,f(-it)}{e^{2\pi t}-1}}\right)dt.}

The case f(0) ≠ 0 is obtained similarly, replacing a 1 a f ( z ) e 2 i π z 1 d z {\textstyle \int _{a^{-1}\infty }^{a\infty }{\frac {f(z)}{e^{-2i\pi z}-1}}dz} by two integrals following the same curves with a small indentation on the left and right of 0.

See also [edit]

  • Euler–Maclaurin summation formula
  • Euler–Boole summation

References [edit]

  • Abel, N.H. (1823), Solution de quelques problèmes à l'aide d'intégrales définies
  • Butzer, P. L.; Ferreira, P. J. S. G.; Schmeisser, G.; Stens, R. L. (2011), "The summation formulae of Euler–Maclaurin, Abel–Plana, Poisson, and their interconnections with the approximate sampling formula of signal analysis", Results in Mathematics, 59 (3): 359–400, doi:10.1007/s00025-010-0083-8, ISSN 1422-6383, MR 2793463, S2CID 54634413
  • Olver, Frank William John (1997) [1974], Asymptotics and special functions, AKP Classics, Wellesley, MA: A K Peters Ltd., ISBN978-1-56881-069-0, MR 1429619
  • Plana, G.A.A. (1820), "Sur une nouvelle expression analytique des nombres Bernoulliens, propre à exprimer en termes finis la formule générale pour la sommation des suites", Mem. Accad. Sci. Torino, 25: 403–418

External links [edit]

  • Anderson, David. "Abel-Plana Formula". MathWorld.

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Source: https://en.wikipedia.org/wiki/Abel%E2%80%93Plana_formula

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