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Ruelle zeta function for cofinite hyperbolic Riemann surfaces with ramification points

Number Theory 2019-10-23 v2 Mathematical Physics Complex Variables math.MP

Abstract

We consider the Ruelle zeta function R(s)R(s) of a genus gg hyperbolic Riemann surface with nn punctures and vv ramification points. R(s)R(s) is equal to Z(s)/Z(s+1)Z(s)/Z(s+1), where Z(s)Z(s) is the Selberg zeta function. The main result of this work is the leading behavior of R(s)R(s) at s=0s=0. If n0n_0 is the order of the determinant of the scattering matrix φ(s)\varphi(s) at s=0s=0, we find that \begin{align*} \lim_{s\rightarrow 0}\frac{R(s)}{s^{2g-2+n-n_0}}=(-1)^{\frac{A}{2}+1}(2\pi)^{2g-2+n }\tilde{\varphi}(0)^{-1} \prod_{j=1}^v m_j, \end{align*}which says that R(s)R(s) has order 2g2+nn02g-2+n-n_0 at s=0s=0, and its leading coefficient can be expressed in terms of m1m_1, m2m_2, \ldots, mvm_v, the ramification indices at the ramification points, and φ~(0)\tilde{\varphi}(0), the leading coefficient of φ(s)\varphi(s) at s=0s=0. The constant AA is an even integer, equal to twice the multiplicity of the eigenvalue 1-1 in the scattering matrix Φ(s)\Phi(s) at s=1/2s=1/2, and (1)A2=φ(12)(-1)^{\frac{A}{2}}=\varphi\left(\frac{1}{2}\right). We also consider the order of the Ruelle zeta function at other integers.

Keywords

Cite

@article{arxiv.1901.07898,
  title  = {Ruelle zeta function for cofinite hyperbolic Riemann surfaces with ramification points},
  author = {Lee-Peng Teo},
  journal= {arXiv preprint arXiv:1901.07898},
  year   = {2019}
}

Comments

18 pages

R2 v1 2026-06-23T07:19:46.525Z