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Dirichlet series

 
Sci-Tech Dictionary: Dirichlet series
(′dē·rē′klā ′sir·ēz)

(mathematics) A series whose nth term is a complex number divided by n to the zth power.


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In mathematics, a Dirichlet series is any series of the form

\sum_{n=1}^{\infty} \frac{a_n}{n^s},

where s and an, n = 1, 2, 3, ... are complex numbers. It is a special case of general Dirichlet series.

Dirichlet series play a variety of important roles in analytic number theory. The most usually seen definition of the Riemann zeta function is a Dirichlet series, as are the Dirichlet L-functions. It is conjectured that the Selberg class of series obeys the generalized Riemann hypothesis. The series is named in honor of Johann Peter Gustav Lejeune Dirichlet.

Contents

Examples

The most famous of Dirichlet series is

\zeta(s)=\sum_{n=1}^{\infty} \frac{1}{n^s},

which is the Riemann zeta function. Another is:

\frac{1}{\zeta(s)}=\sum_{n=1}^{\infty} \frac{\mu(n)}{n^s}

where μ(n) is the Möbius function. This and many of the following series may be obtained by applying Möbius inversion and Dirichlet convolution to known series. For example, given a Dirichlet character \scriptstyle\chi(n) one has

\frac{1}{L(\chi,s)}=\sum_{n=1}^{\infty} \frac{\mu(n)\chi(n)}{n^s}

where L(χ,s) is a Dirichlet L-function.

Other identities include

\frac{\zeta(s-1)}{\zeta(s)}=\sum_{n=1}^{\infty} 
\frac{\varphi(n)}{n^s}

where φ(n) is the totient function, and

\zeta(s) \zeta(s-a)=\sum_{n=1}^{\infty} \frac{\sigma_{a}(n)}{n^s}
\frac{\zeta(s)\zeta(s-a)\zeta(s-b)\zeta(s-a-b)}{\zeta(2s-a-b)}
=\sum_{n=1}^{\infty} \frac{\sigma_a(n)\sigma_b(n)}{n^s}

where σa(n) is the divisor function. Other identities involving the divisor function d0 are

 \frac{\zeta^3(s)}{\zeta(2s)}=\sum_{n=1}^{\infty}\frac{d(n^2)}{n^s}
 \frac{\zeta^4(s)}{\zeta(2s)}=\sum_{n=1}^{\infty}\frac{d(n)^2}{n^s}.

The logarithm of the zeta function is given by

\log \zeta(s)=\sum_{n=2}^\infty \frac{\Lambda(n)}{\log(n)}\,\frac{1}{n^s}

for Re(s) > 1. Here, \scriptstyle \Lambda(n) is the von Mangoldt function. The logarithmic derivative is then

\frac {\zeta^\prime(s)}{\zeta(s)} = -\sum_{n=1}^\infty \frac{\Lambda(n)}{n^s}.

These last two are special cases of a more general relationship for derivatives of Dirichlet series, given below.

Given the Liouville function \scriptstyle\lambda(n), one has

\frac {\zeta(2s)}{\zeta(s)} = \sum_{n=1}^\infty \frac{\lambda(n)}{n^s}.

Yet another example involves Ramanujan's sum:

\frac{\sigma_{1-s}(m)}{\zeta(s)}=\sum_{n=1}^\infty\frac{c_n(m)}{n^s}.

Analytic properties of Dirichlet series: the abscissa of convergence

Given a sequence {an}nN of complex numbers we try to consider the value of

 f(s) = \sum_{n=1}^\infty \frac{a_n}{n^s}

as a function of the complex variable s. In order for this to make sense, we need to consider the convergence properties of the above infinite series:

If {an}nN is a bounded sequence of complex numbers, then the corresponding Dirichlet series f converges absolutely on the open half-plane of s such that Re(s) > 1. In general, if an = O(nk), the series converges absolutely in the half plane Re(s) > k + 1.

If the set of sums an + an + 1 + ... + an + k is bounded for n and k ≥ 0, then the above infinite series converges on the open half-plane of s such that Re(s) > 0.

In both cases f is an analytic function on the corresponding open half plane.

In general the abscissa of convergence of a Dirichlet series is the intercept on the real axis of the vertical line in the complex plane, such that there is convergence to the right of it, and divergence to the left. This is the analogue for Dirichlet series of the radius of convergence for power series. The Dirichlet series case is more complicated, though: absolute convergence and uniform convergence may occur in distinct half-planes.

In many cases, the analytic function associated with a Dirichlet series has an analytic extension to a larger domain.

Derivatives

Given

F(s) =\sum_{n=1}^\infty \frac{f(n)}{n^s}

it is possible to show that

F'(s) =\sum_{n=1}^\infty \frac{f(n)\log(n)}{n^s}

assuming the right hand side converges. For a completely multiplicative function ƒ(n), and assuming the series converges for Re(s) > σ0, then one has that

\frac {F^\prime(s)}{F(s)} = - \sum_{n=1}^\infty \frac{f(n)\Lambda(n)}{n^s}

converges for Re(s) > σ0. Here, \scriptstyle\Lambda(n) is the von Mangoldt function.

Products

Suppose

 F(s)= \sum_{n=1}^{\infty} f(n)n^{-s}

and

 G(s)= \sum_{n=1}^{\infty} g(n)n^{-s}.

If both F(s) and G(s) are absolutely convergent for s > a and s > b then we have

 \frac{1}{2T}\int_{-T}^{T}\,F(a+it)G(b-it)\,dt= \sum_{n=1}^{\infty} f(n)g(n)n^{-a-b} \text{ as }T \sim \infty.

If a = b and ƒ(n) = g(n) we have

 \frac{1}{2T}\int_{-T}^{T}|F(a+it)|^{2} dt= \sum_{n=1}^{\infty} [f(n)]^{2}n^{-2a} \text{ as } T \sim \infty.

Integral transforms

The Mellin transform of a Dirichlet series is given by Perron's formula.

See also

References


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