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Tevelev degrees and Hurwitz moduli spaces

Published online by Cambridge University Press:  03 December 2021

A. CELA
Affiliation:
Department of Mathematics, ETH Zurich Office: HG J 14.4 Rämistrasse 101 8092 Zurich Switzerland e-mails: alessio.cela@math.ethz.ch
R. PANDHARIPANDE
Affiliation:
Department of Mathematics, ETH Zurich Office: HG G 55 Rämistrasse 101 8092 Zurich Switzerland e-mails: rahul@math.ethz.ch
J. SCHMITT
Affiliation:
Institute for Mathematics, University of Zurich Office: Y27K42 Winterthurerstrasse 190 8057 Zürich Switzerland e-mail: johannes.schmitt@math.uzh.ch
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Abstract

We interpret the degrees which arise in Tevelev’s study of scattering amplitudes in terms of moduli spaces of Hurwitz covers. Via excess intersection theory, the boundary geometry of the Hurwitz moduli space yields a simple recursion for the Tevelev degrees (together with their natural two parameter generalisation). We find exact solutions which specialise to Tevelev’s formula in his cases and connect to the projective geometry of lines and Castelnuovo’s classical count of $g^1_d$’s in other cases. For almost all values, the calculation of the two parameter generalisation of the Tevelev degree is new. A related count of refined Dyck paths is solved along the way.

Information

Type
Research Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
Copyright
© The Author(s), 2021. Published by Cambridge University Press on behalf of Cambridge Philosophical Society
Figure 0

Fig. 1. A curve $C \to \mathbb{P}^1$ in $\overline{\mathcal{H}}_{1,d,4,2}$ with $n=4$ markings in C of which $r=2$ lie in the fibre over the same point of $\mathbb{P}^1$.

Figure 1

Fig. 2. Possible paths from (0,1) to $(-3,1)$. There are exactly $C_3 = 5$ possible paths, where $C_3$ is the third Catalan number. Our paths are equivalent to Dyck paths [27].

Figure 2

Table 1. Values of $\mathsf{T}_{\ell,r}$ for $\ell<0$