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 (a_n)_{n=0}^\infty be a sequence of real or complex numbers. Define the partial sum function A by

:A(t) = \sum_{0 \le n \le t} a_n

for any real number t. Fix real numbers x < y, and let \phi be a continuously differentiable function on [x, y]. Then:

:\sum_{x < n \le y} a_n\phi(n) = A(y)\phi(y) - A(x)\phi(x) - \int_x^y A(u)\phi'(u)\,du.

The formula is derived by applying integration by parts for a Riemann–Stieltjes integral to the functions A and \phi.

=Variations=

Taking the left endpoint to be -1 gives the formula

:\sum_{0 \le n \le x} a_n\phi(n) = A(x)\phi(x) - \int_0^x A(u)\phi'(u)\,du.

If the sequence (a_n) is indexed starting at n = 1, then we may formally define a_0 = 0. The previous formula becomes

:\sum_{1 \le n \le x} a_n\phi(n) = A(x)\phi(x) - \int_1^x A(u)\phi'(u)\,du.

A common way to apply Abel's summation formula is to take the limit of one of these formulas as x \to \infty. The resulting formulas are

:\begin{align}

\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 a_n = 1 for all n \ge 0. In this case, A(x) = \lfloor x + 1 \rfloor. For this sequence, Abel's summation formula simplifies to

:\sum_{0 \le n \le x} \phi(n) = \lfloor x + 1 \rfloor\phi(x) - \int_0^x \lfloor u + 1\rfloor \phi'(u)\,du.

Similarly, for the sequence a_0 = 0 and a_n = 1 for all n \ge 1, the formula becomes

:\sum_{1 \le n \le x} \phi(n) = \lfloor x \rfloor\phi(x) - \int_1^x \lfloor u \rfloor \phi'(u)\,du.

Upon taking the limit as x \to \infty, we find

:\begin{align}

\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 \phi is only assumed to be continuous if the integral is interpreted as a Riemann–Stieltjes integral:

:\sum_{x < n \le y} a_n\phi(n) = A(y)\phi(y) - A(x)\phi(x) - \int_x^y A(u)\,d\phi(u).

By taking \phi to be the partial sum function associated to some sequence, this leads to the summation by parts formula.

Examples

=Harmonic numbers=

If a_n = 1 for n \ge 1 and \phi(x) = 1/x, then A(x) = \lfloor x \rfloor and the formula yields

:\sum_{n=1}^{\lfloor x \rfloor} \frac{1}{n} = \frac{\lfloor x \rfloor}{x} + \int_1^x \frac{\lfloor u \rfloor}{u^2} \,du.

The left-hand side is the harmonic number H_{\lfloor x \rfloor}.

=Representation of Riemann's zeta function=

Fix a complex number s. If a_n = 1 for n \ge 1 and \phi(x) = x^{-s}, then A(x) = \lfloor x \rfloor and the formula becomes

:\sum_{n=1}^{\lfloor x \rfloor} \frac{1}{n^s} = \frac{\lfloor x \rfloor}{x^s} + s\int_1^x \frac{\lfloor u\rfloor}{u^{1+s}}\,du.

If \Re(s) > 1, then the limit as x \to \infty exists and yields the formula

:\zeta(s) = s\int_1^\infty \frac{\lfloor u\rfloor}{u^{1+s}}\,du.

where \zeta(s) is the Riemann zeta function.

This may be used to derive Dirichlet's theorem that \zeta(s) 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 a_n = \mu(n) is the Möbius function and \phi(x) = x^{-s}, then A(x) = M(x) = \sum_{n \le x} \mu(n) is Mertens function and

:\frac{1}{\zeta(s)} = \sum_{n=1}^\infty \frac{\mu(n)}{n^s} = s\int_1^\infty \frac{M(u)}{u^{1+s}}\,du.

This formula holds for \Re(s) > 1.

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}}.

Category:Number theory

Category:Summability methods