The Selberg zeta-function was introduced by Atle Selberg (1956). It is analogous to the famous Riemann zeta function
where P {\displaystyle \mathbb {P} } is the set of prime numbers. The Selberg zeta-function uses the lengths of simple closed geodesics instead of the prime numbers. If Γ {\displaystyle \Gamma } is a subgroup of SL(2,R), the associated Selberg zeta function is defined as follows,
or
where p runs over conjugacy classes of prime geodesics (equivalently, conjugacy classes of primitive hyperbolic elements of Γ {\displaystyle \Gamma } ), and N(p) denotes exp ( length of p ) {\displaystyle \exp({\text{length of }}p)} (equivalently, the 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:
The zeta-function also has poles at 1 / 2 − N {\displaystyle 1/2-\mathbb {N} } , and can have zeros or poles at the points − N {\displaystyle -\mathbb {N} } .
The Ihara zeta function is considered a p-adic (and a graph-theoretic) analogue of the Selberg zeta function.