Abel's summation formula
{{Short description|Integration by parts version of Abel's method for summation by parts}}
{{dablink|Other concepts sometimes known by this name are summation by parts and Abel–Plana formula.}}
In mathematics, Abel's summation formula, introduced by Niels Henrik Abel, is intensively used in analytic number theory and the study of special functions to compute series.
Formula
{{wikibooks|Analytic Number Theory/Useful summation formulas}}
Let be a sequence of real or complex numbers. Define the partial sum function by
:
for any real number . Fix real numbers , and let be a continuously differentiable function on . Then:
:
The formula is derived by applying integration by parts for a Riemann–Stieltjes integral to the functions and .
=Variations=
Taking the left endpoint to be gives the formula
:
If the sequence is indexed starting at , then we may formally define . The previous formula becomes
:
A common way to apply Abel's summation formula is to take the limit of one of these formulas as . The resulting formulas are
:
\sum_{n=0}^\infty a_n\phi(n) &= \lim_{x \to \infty}\bigl(A(x)\phi(x)\bigr) - \int_0^\infty A(u)\phi'(u)\,du, \\
\sum_{n=1}^\infty a_n\phi(n) &= \lim_{x \to \infty}\bigl(A(x)\phi(x)\bigr) - \int_1^\infty A(u)\phi'(u)\,du.
\end{align}
These equations hold whenever both limits on the right-hand side exist and are finite.
A particularly useful case is the sequence for all . In this case, . For this sequence, Abel's summation formula simplifies to
:
Similarly, for the sequence and for all , the formula becomes
:
Upon taking the limit as , we find
:
\sum_{n=0}^\infty \phi(n) &= \lim_{x \to \infty}\bigl(\lfloor x + 1 \rfloor\phi(x)\bigr) - \int_0^\infty \lfloor u + 1\rfloor \phi'(u)\,du, \\
\sum_{n=1}^\infty \phi(n) &= \lim_{x \to \infty}\bigl(\lfloor x \rfloor\phi(x)\bigr) - \int_1^\infty \lfloor u\rfloor \phi'(u)\,du,
\end{align}
assuming that both terms on the right-hand side exist and are finite.
Abel's summation formula can be generalized to the case where is only assumed to be continuous if the integral is interpreted as a Riemann–Stieltjes integral:
:
By taking to be the partial sum function associated to some sequence, this leads to the summation by parts formula.
Examples
=Harmonic numbers=
=Representation of Riemann's zeta function=
Fix a complex number . If for and then and the formula becomes
:
If , then the limit as exists and yields the formula
:
where is the Riemann zeta function.
This may be used to derive Dirichlet's theorem that has a simple pole with residue 1 at {{math|s {{=}} 1}}.
=Reciprocal of Riemann zeta function=
The technique of the previous example may also be applied to other Dirichlet series. If is the Möbius function and , then is Mertens function and
:
This formula holds for .
See also
References
- {{citation|first=Tom|last=Apostol|authorlink=Tom Apostol|title=Introduction to Analytic Number Theory|publisher=Springer-Verlag|series=Undergraduate Texts in Mathematics|year=1976}}.