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Algebraic interaction strength for translation surfaces with multiple singularities

Published online by Cambridge University Press:  27 July 2026

Julien Boulanger*
Affiliation:
Centro de Modelamiento matemático, Universidad de Chile & IRL 2807 - CNRS , Chile
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Abstract

Given two closed curves on a surface consider their algebraic intersection divided by their length product. In this article, we compute the maximum of this ratio. This ratio, called the interaction strength, is difficult to compute for translation surfaces with several singularities as geodesics can change direction at singularities. The main contribution of this paper is to deal with this type of surfaces. Namely, we study the interaction strength of the regular $n$-gons for $n \equiv 2 \pmod 4$ and the Bouw–Möller surfaces $S_{m,n}$ with $1 \lt \gcd (m,n) \lt n$. This answers a conjecture of the author, and it completes the study of the algebraic interaction strength KVol on the regular polygon Veech surfaces. Our results on Bouw–Möller surfaces extends results of the author with Pasquinelli. This is also the first exact computation of KVol on translation surfaces with several singularities, and the pairs of curves that achieve the best ratio are singular geodesics made of two saddle connections with different directions.

Information

Type
Research Article
Copyright
© The Author(s), 2026. Published by Cambridge University Press on behalf of Glasgow Mathematical Journal Trust
Figure 0

Figure 1. A triple cover of the double regular pentagon with three singularities (of angle 6π$6\pi$) and for which the algebraic interaction strength can be computed from [6] and is 154tan⁡(π5)$\frac {15}{4\tan (\frac {\pi }{5})}$. The same picture can be extended to any number of singularities.

Figure 1

Figure 2. The decomposition into three horizontal cylinders on the 14$14$-gon. On the right, the unfolding of the smallest cylinder C1$C_1$. The closed geodesic α$\alpha$ is homologous to the union of two saddle connections.

Figure 2

Figure 3. The sign of a transverse intersection.

Figure 3

Figure 4. The cyclic order of the sides at the singularities. The segments γ=1∪3$\gamma = 1 \cup 3$ and δ=2∪5$\delta = 2 \cup 5$ intersect twice.

Figure 4

Figure 5. The permutation σ0$\sigma _0$ associated with the transition diagram in sector Σ0$\Sigma _0$ for n=10$n=10$.

Figure 5

Figure 6. On the left, a saddle connection of type (2). Any saddle connection of type (2) can be obtained from Δ$\Delta$ by a symmetry or a rotation. On the right, a saddle connection of type (3), that is staying strictly inside the big cylinder associated with its diagram. Its endpoints A$A$ and A′$A'$ are opposite vertices of the decagon, hence representing different singularities.

Figure 6

Figure 7. The unfolding of the saddle connections staying inside the big cylinder with nα≤3$n_{\alpha } \leq 3$ (and for n=10$n = 10$). Here, L10=5+1=22+ε1$L_{10} = \sqrt {5} +1 = 2\sqrt {2} + \varepsilon _1$ is the length of the longest diagonal of the unit-sided regular decagon.

Figure 7

Figure 8. On the left, a segment whose endpoints on sides of label σ0(i)$\sigma _0(i)$ for i≥3$i \geq 3$. This segment is longer than the short dashed diagonals. On the right, a maximal trip through the short horizontal cylinder. Here, the first segment αi0$\alpha _{i_0}$ is a long segment, whereas the last segment αi0+p−1$\alpha _{i_0+p-1}$ (p=5$p=5$) is the terminal segment and goes to the vertex A′$A'$.

Figure 8

Figure 9. Example of unfolding of a maximal trip in the shortest horizontal cylinder (here the saddle connection α$\alpha$ starts at A$A$ and ends at A′$A'$ and is completely contained in the short horizontal cylinder). Each segment (sandwiched or non-sandwiched) accounts for a horizontal length at least 1+cos⁡(π5)$1 + \cos (\frac {\pi }{5})$, except the last one which may account for only 1$1$. Further, the vertical length is at least sin⁡(π5)$\sin (\frac {\pi }{5})$, and each sandwiched segment accounts for an additional vertical length of sin⁡(π5)$\sin (\frac {\pi }{5})$.

Figure 9

Figure 10. The short horizontal cylinder and the two possible combinatorics for the first segment αi0$\alpha _{i_0}$ of a maximal trip through the short horizontal cylinder for a saddle connection α$\alpha$ in sector Σ0$\Sigma _0$: αi0$\alpha _{i_0}$ can either start at A$A$, or on the segment BC$BC$ – possibly at B$B$).

Figure 10

Figure 11. Virtual length of segments intersecting the short horizontal cylinder. Top-left: the two cases for the first segment of a maximal trip through the horizontal cylinder; top-right: a sandwiched segment; bottom-left: an intermediate non-sandwiched segment; bottom-right: the last segment of a maximal trip.

Figure 11

Figure 12. The two pairs of curves γ1∪γ2$\gamma _1 \cup \gamma _2$ and δ1∪δ2$\delta _1 \cup \delta _2$ intersect at both singularities z1$z_1$ and z2$z_2$ with the same sign, for Bouw–Möller surfaces with 1$1 \lt \gcd (m,n) \lt n$.

Figure 12

Figure 13. A segment αi$\alpha _i$ of type (e). The segment αi+1$\alpha _{i+1}$ can have an endpoint αi+1+$\alpha _{i+1}^+$ on either side s1,s2$s_1,s_2$ or s3$s_3$.

Figure 13

Figure 14. The segment paired with a pair of adjacent segments of type (g) is a long segment contained in P(1)$P(1)$ which has one endpoint on s1$s_1$ and one endpoint on either of the sides s0,s2$s_0, s_2$ or s3$s_3$. This is similar for the segment paired with a non-adjacent segment of type (f) whose supporting side is s0$s_0$. The main reason this holds is because the vertices A,B$A, B$ and C$C$ are aligned (the segments AB$AB$ and BC$BC$ both make an angle πn$\frac {\pi }{n}$ with the horizontal).