Let K {\displaystyle K} be the real subfield of Q [ ρ ] {\displaystyle \mathbb {Q} [\rho ]} where ρ {\displaystyle \rho } is a 7th-primitive root of unity. The ring of integers of K is Z [ η ] {\displaystyle \mathbb {Z} [\eta ]} , where η = 2 cos ( 2 π 7 ) {\displaystyle \eta =2\cos({\tfrac {2\pi }{7}})} . Let D {\displaystyle D} be the quaternion algebra, or symbol algebra ( η , η ) K {\displaystyle (\eta ,\eta )_{K}} . Also Let τ = 1 + η + η 2 {\displaystyle \tau =1+\eta +\eta ^{2}} and j ′ = 1 2 ( 1 + η i + τ j ) {\displaystyle j'={\tfrac {1}{2}}(1+\eta i+\tau j)} . Let Q H u r = Z [ η ] [ i , j , j ′ ] {\displaystyle {\mathcal {Q}}_{\mathrm {Hur} }=\mathbb {Z} [\eta ][i,j,j']} . Then Q H u r {\displaystyle {\mathcal {Q}}_{\mathrm {Hur} }} is a maximal order of D {\displaystyle D} (see Hurwitz quaternion order), described explicitly by Noam Elkies [1].
In order to construct the first Hurwitz triplet, consider the prime decomposition of 13 in Z [ η ] {\displaystyle \mathbb {Z} [\eta ]} , namely
where η ( η + 2 ) {\displaystyle \eta (\eta +2)} is invertible. Also consider the prime ideals generated by the non-invertible factors. The principal congruence subgroup defined by such a prime ideal I is by definition the group
namely, the group of elements of reduced norm 1 in Q H u r {\displaystyle {\mathcal {Q}}_{\mathrm {Hur} }} equivalent to 1 modulo the ideal I Q H u r {\displaystyle I{\mathcal {Q}}_{\mathrm {H} ur}} . The corresponding Fuchsian group is obtained as the image of the principal congruence subgroup under a representation to PSL(2,R).
Each of the three Riemann surfaces in the first Hurwitz triplet can be formed as a Fuchsian model, the quotient of the hyperbolic plane by one of these three Fuchsian groups.
The Gauss–Bonnet theorem states that
where χ ( Σ ) {\displaystyle \chi (\Sigma )} is the Euler characteristic of the surface and K ( u ) {\displaystyle K(u)} is the Gaussian curvature . In the case g = 14 {\displaystyle g=14} we have
thus we obtain that the area of these surfaces is
The lower bound on the systole as specified in [2], namely
is 3.5187.
Some specific details about each of the surfaces are presented in the following tables (the number of systolic loops is taken from [3]). The term Systolic Trace refers to the least reduced trace of an element in the corresponding subgroup Q H u r 1 ( I ) {\displaystyle {\mathcal {Q}}_{Hur}^{1}(I)} . The systolic ratio is the ratio of the square of the systole to the area.