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Selberg zeta function : ウィキペディア英語版
Selberg zeta function
The Selberg zeta-function was introduced by . It is analogous to the famous Riemann zeta function
: \zeta(s) = \prod_ is the set of prime numbers. The Selberg zeta-function uses the lengths of simple closed geodesics instead of the primes numbers. If \Gamma is a subgroup of SL(2,R) Selberg zeta function is defined as follows,
:\zeta_\Gamma(s)=\prod_p(1-N(p)^)^,
or
:Z_\Gamma(s)=\prod_p\prod^\infty_(1-N(p)^),
where p run all over the prime congruent class and N(p) is the norm of congruent class p, which is square of the bigger eigenvalue of p.
For any hyperbolic surface of finite area there is an associated Selberg zeta-function; this function is a meromorphic function defined in the complex plane. The zeta function is defined in terms of the closed geodesics of the surface.
The zeros and poles of the Selberg zeta-function, ''Z''(''s''), can be described in terms of spectral data of the surface.
The zeros are at the following points:
# For every cusp form with eigenvalue s_0(1-s_0) there exists a zero at the point s_0. The order of the zero equals the dimension of the corresponding eigenspace. (A cusp form is an eigenfunction to the Laplace–Beltrami operator which has Fourier expansion with zero constant term.)
# The zeta-function also has a zero at every pole of the determinant of the scattering matrix, \phi(s) . The order of the zero equals the order of the corresponding pole of the scattering matrix.
The zeta-function also has poles at 1/2 - \mathbb , and can have zeros or poles at the points - \mathbb .
The Ihara zeta function is considered a p-adic (and a graph-theoretic) analogue of the Selberg zeta function.
== Selberg zeta-function for the modular group ==
For the case where the surface is \Gamma \backslash \mathbb^2 , where \Gamma is the modular group, the Selberg zeta-function is of special interest. For this special case the Selberg zeta-function is intimately connected to the Riemann zeta-function.
In this case the determinant of the scattering matrix is given by:
: \varphi(s) = \pi^ \frac.
In particular, we see that if the Riemann zeta-function has a zero at s_0, then the determinant of the scattering matrix has a pole at s_0/2, and hence the Selberg zeta-function has a zero at s_0/2.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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