In mathematics, the Bolza surface, alternatively, complex algebraic Bolza curve (introduced by Oskar Bolza (1887)), is a compact Riemann surface of genus ${\displaystyle 2}$ with the highest possible order of the conformal automorphism group in this genus, namely ${\displaystyle GL_{2}(3)}$ of order 48 (the general linear group of ${\displaystyle 2\times 2}$ matrices over the finite field ${\displaystyle \mathbb {F} _{3}}$). The full automorphism group (including reflections) is the semi-direct product ${\displaystyle GL_{2}(3)\rtimes \mathbb {Z} _{2}}$ of order 96. An affine model for the Bolza surface can be obtained as the locus of the equation

${\displaystyle y^{2}=x^{5}-x}$

in ${\displaystyle \mathbb {C} ^{2}}$. The Bolza surface is the smooth completion of the affine curve. Of all genus ${\displaystyle 2}$ hyperbolic surfaces, the Bolza surface maximizes the length of the systole (Schmutz 1993). As a hyperelliptic Riemann surface, it arises as the ramified double cover of the Riemann sphere, with ramification locus at the six vertices of a regular octahedron inscribed in the sphere, as can be readily seen from the equation above.

The Bolza surface has attracted the attention of physicists, as it provides a relatively simple model for quantum chaos; in this context, it is usually referred to as the Hadamard–Gutzwiller model.^[1] The spectral theory of the Laplace–Beltrami operator acting on functions on the Bolza surface is of interest to both mathematicians and physicists, since the surface is conjectured to maximize the first positive eigenvalue of the Laplacian among all compact, closed Riemann surfaces of genus ${\displaystyle 2}$ with constant negative curvature.

The Bolza surface is conformally equivalent to a ${\displaystyle (2,3,8)}$ triangle surface – see Schwarz triangle. More specifically, the Fuchsian group defining the Bolza surface is a subgroup of the group generated by reflections in the sides of a hyperbolic triangle with angles ${\displaystyle {\tfrac {\pi }{2}},{\tfrac {\pi }{3}},{\tfrac {\pi }{8}}}$. The group of orientation preserving isometries is a subgroup of the index-two subgroup of the group of reflections, which consists of products of an even number of reflections, which has an abstract presentation in terms of generators ${\displaystyle s_{2},s_{3},s_{8}}$ and relations ${\displaystyle s_{2}{}^{2}=s_{3}{}^{3}=s_{8}{}^{8}=1}$ as well as ${\displaystyle s_{2}s_{3}=s_{8}}$. The Fuchsian group ${\displaystyle \Gamma }$ defining the Bolza surface is also a subgroup of the (3,3,4) triangle group, which is a subgroup of index 2 in the ${\displaystyle (2,3,8)}$ triangle group. The ${\displaystyle (2,3,8)}$ group does not have a realization in terms of a quaternion algebra, but the ${\displaystyle (3,3,4)}$ group does.

Under the action of ${\displaystyle \Gamma }$ on the Poincare disk, the fundamental domain of the Bolza surface is a regular octagon with angles ${\displaystyle {\tfrac {\pi }{4}}}$ and corners at

${\displaystyle p_{k}=2^{-1/4}e^{i\left({\tfrac {\pi }{8}}+{\tfrac {k\pi }{4}}\right)},}$

where ${\displaystyle k=0,\ldots ,7}$. Opposite sides of the octagon are identified under the action of the Fuchsian group. Its generators are the matrices

${\displaystyle g_{k}={\begin{pmatrix}1+{\sqrt {2}}&(2+{\sqrt {2}})\alpha e^{\tfrac {ik\pi }{4}}\\(2+{\sqrt {2}})\alpha e^{-{\tfrac {ik\pi }{4}}}&1+{\sqrt {2}}\end{pmatrix}},}$

where ${\displaystyle \alpha ={\sqrt {{\sqrt {2}}-1}}}$ and ${\displaystyle k=0,\ldots ,3}$, along with their inverses. The generators satisfy the relation

${\displaystyle g_{0}g_{1}^{-1}g_{2}g_{3}^{-1}g_{0}^{-1}g_{1}g_{2}^{-1}g_{3}=1.}$

These generators are connected to the length spectrum, which gives all of the possible lengths of geodesic loops.  The shortest such length is called the systole of the surface. The systole of the Bolza surface is

${\displaystyle \ell _{1}=2\operatorname {\rm {arcosh}} (1+{\sqrt {2}})\approx 3.05714.}$

The ${\displaystyle n^{\text{th}}}$ element ${\displaystyle \ell _{n}}$ of the length spectrum for the Bolza surface is given by

${\displaystyle \ell _{n}=2\operatorname {\rm {arcosh}} (m+n{\sqrt {2}}),}$

where ${\displaystyle n}$ runs through the positive integers (but omitting 4, 24, 48, 72, 140, and various higher values) (Aurich, Bogomolny & Steiner 1991) and where ${\displaystyle m}$ is the unique odd integer that minimizes

${\displaystyle \vert m-n{\sqrt {2}}\vert .}$

It is possible to obtain an equivalent closed form of the systole directly from the triangle group. Formulae exist to calculate the side lengths of a (2,3,8) triangles explicitly. The systole is equal to four times the length of the side of medial length in a (2,3,8) triangle, that is,

${\displaystyle \ell _{1}=4\operatorname {\rm {arcosh}} \left({\tfrac {\csc \left({\tfrac {\pi }{8}}\right)}{2}}\right)\approx 3.05714.}$

The geodesic lengths ${\displaystyle \ell _{n}}$ also appear in the Fenchel–Nielsen coordinates of the surface. A set of Fenchel-Nielsen coordinates for a surface of genus 2 consists of three pairs, each pair being a length and twist.  Perhaps the simplest such set of coordinates for the Bolza surface is ${\displaystyle (\ell _{2},{\tfrac {1}{2}};\;\ell _{1},0;\;\ell _{1},0)}$, where ${\displaystyle \ell _{2}=2\operatorname {\rm {arcosh}} (3+2{\sqrt {2}})\approx 4.8969}$.

There is also a "symmetric" set of coordinates ${\displaystyle (\ell _{1},t;\;\ell _{1},t;\;\ell _{1},t)}$, where all three of the lengths are the systole ${\displaystyle \ell _{1}}$ and all three of the twists are given by^[2]

${\displaystyle t={\frac {\operatorname {\rm {arcosh}} \left({\sqrt {{\tfrac {2}{7}}(3+{\sqrt {2}})}}\right)}{\operatorname {\rm {arcosh}} (1+{\sqrt {2}})}}\approx 0.321281.}$

The fundamental domain of the Bolza surface is a regular octagon in the Poincaré disk; the four symmetric actions that generate the (full) symmetry group are:

• R – rotation of order 8 about the centre of the octagon;
• S – reflection in the real line;
• T – reflection in the side of one of the 16 (4,4,4) triangles that tessellate the octagon;
• U – rotation of order 3 about the centre of a (4,4,4) triangle.

These are shown by the bold lines in the adjacent figure. They satisfy the following set of relations:

${\displaystyle \langle R,\,S,\,T,\,U\mid R^{8}=S^{2}=T^{2}=U^{3}=RSRS=STST=RTR^{3}T=e,\,UR=R^{7}U^{2},\,U^{2}R=STU,\,US=SU^{2},\,UT=RSU\rangle ,}$

where ${\displaystyle e}$ is the trivial (identity) action. One may use this set of relations in GAP to retrieve information about the representation theory of the group. In particular, there are four 1-dimensional, two 2-dimensional, four 3-dimensional, and three 4-dimensional irreducible representations, and

${\displaystyle 4(1^{2})+2(2^{2})+4(3^{2})+3(4^{2})=96}$

as expected.

Here, spectral theory refers to the spectrum of the Laplacian, ${\displaystyle \Delta }$. The first eigenspace (that is, the eigenspace corresponding to the first positive eigenvalue) of the Bolza surface is three-dimensional, and the second, four-dimensional (Cook 2018), (Jenni 1981). It is thought that investigating perturbations of the nodal lines of functions in the first eigenspace in Teichmüller space will yield the conjectured result in the introduction. This conjecture is based on extensive numerical computations of eigenvalues of the surface and other surfaces of genus 2. In particular, the spectrum of the Bolza surface is known to a very high accuracy (Strohmaier & Uski 2013). The following table gives the first ten positive eigenvalues of the Bolza surface.

Numerical computations of the first ten positive eigenvalues of the Bolza surface

Eigenvalue	Numerical value	Multiplicity
${\displaystyle \lambda _{0}}$	0	1
${\displaystyle \lambda _{1}}$	3.8388872588421995185866224504354645970819150157	3
${\displaystyle \lambda _{2}}$	5.353601341189050410918048311031446376357372198	4
${\displaystyle \lambda _{3}}$	8.249554815200658121890106450682456568390578132	2
${\displaystyle \lambda _{4}}$	14.72621678778883204128931844218483598373384446932	4
${\displaystyle \lambda _{5}}$	15.04891613326704874618158434025881127570452711372	3
${\displaystyle \lambda _{6}}$	18.65881962726019380629623466134099363131475471461	3
${\displaystyle \lambda _{7}}$	20.5198597341420020011497712606420998241440266544635	4
${\displaystyle \lambda _{8}}$	23.0785584813816351550752062995745529967807846993874	1
${\displaystyle \lambda _{9}}$	28.079605737677729081562207945001124964945310994142	3
${\displaystyle \lambda _{10}}$	30.833042737932549674243957560470189329562655076386	4

The spectral determinant and Casimir energy ${\displaystyle \zeta (-1/2)}$ of the Bolza surface are

${\displaystyle \det {}_{\zeta }(\Delta )\approx 4.72273280444557}$

and

${\displaystyle \zeta _{\Delta }(-1/2)\approx -0.65000636917383}$

respectively, where all decimal places are believed to be correct. It is conjectured that the spectral determinant is maximized in genus 2 for the Bolza surface.

Following MacLachlan and Reid, the quaternion algebra can be taken to be the algebra over ${\displaystyle \mathbb {Q} ({\sqrt {2}})}$ generated as an associative algebra by generators i,j and relations

${\displaystyle i^{2}=-3,\;j^{2}={\sqrt {2}},\;ij=-ji,}$

with an appropriate choice of an order.

• Hyperelliptic curve
• Klein quartic
• Bring's curve
• Macbeath surface
• First Hurwitz triplet

• Bolza, Oskar (1887), "On Binary Sextics with Linear Transformations into Themselves", American Journal of Mathematics, 10 (1): 47–70, doi:10.2307/2369402, JSTOR 2369402
• Katz, M.; Sabourau, S. (2006). "An optimal systolic inequality for CAT(0) metrics in genus two". Pacific J. Math. 227 (1): 95–107. arXiv:math.DG/0501017. doi:10.2140/pjm.2006.227.95. S2CID 16510851.
• Schmutz, P. (1993). "Riemann surfaces with shortest geodesic of maximal length". GAFA. 3 (6): 564–631. doi:10.1007/BF01896258. S2CID 120508826.
• Aurich, R.; Bogomolny, E.B.; Steiner, F. (1991). "Periodic orbits on the regular hyperbolic octagon". Physica D: Nonlinear Phenomena. 48 (1): 91–101. Bibcode:1991PhyD...48...91A. doi:10.1016/0167-2789(91)90053-C.
• Cook, J. (2018). Properties of Eigenvalues on Riemann Surfaces with Large Symmetry Groups (PhD thesis, unpublished). Loughborough University.
• Jenni, F. (1981). Über das Spektrum des Laplace-Operators auf einer Schar kompakter Riemannscher Flächen (PhD thesis). University of Basel. OCLC 45934169.
• Strohmaier, A.; Uski, V. (2013). "An Algorithm for the Computation of Eigenvalues, Spectral Zeta Functions and Zeta-Determinants on Hyperbolic Surfaces". Communications in Mathematical Physics. 317 (3): 827–869. arXiv:1110.2150. Bibcode:2013CMaPh.317..827S. doi:10.1007/s00220-012-1557-1. S2CID 14305255.
• Maclachlan, C.; Reid, A. (2003). The Arithmetic of Hyperbolic 3-Manifolds. Graduate Texts in Math. Vol. 219. New York: Springer. ISBN 0-387-98386-4.

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