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PreprintCC BY 4.0arXiv

Irrational Seshadri constants from dihedral orbits

Abstract

We construct an irrational one-point Seshadri constant on the blow-up X9 of ℙ2 at nine very general points. The divisor L=9H−3(E1+⋯+E5)−2(E6+⋯+E9) is ample and satisfies ε(L;x)=2√5 at a very general point x∈ X9. To prove this, we establish that the Seshadri constant of 𝒪ℙ1×ℙ1(1,1) at ten very general points is 1/√5, completing the reflection approach proposed by Dionne and Roth for the ten-point case. We also prove that the same equality holds at a very general free orbit of a fixed dihedral group of order ten. This yields an irrational one-point Seshadri constant on the singular quotient surface. A plane model of its minimal resolution and a deformation of the blow-up centers then give the result on X9.

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BibTeX
@misc{laface2026irrational,
  title = {{Irrational Seshadri constants from dihedral orbits}},
  author = {Antonio Laface and Luca Ugaglia},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.26521},
  eprint = {2609.26521},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.26521},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Irrational Seshadri constants from dihedral orbits
AU  - Antonio Laface
AU  - Luca Ugaglia
PY  - 2026
DA  - 2026/09/25
PB  - arXiv
DO  - 10.48550/arxiv.2609.26521
UR  - https://arxiv.org/abs/2609.26521
AB  - We construct an irrational one-point Seshadri constant on the blow-up X_9 of ℙ^2 at nine very general points. The divisor L=9H−3(E_1+⋯+E_5)−2(E_6+⋯+E_9) is ample and satisfies ε(L;x)=2√5 at a very general point x∈ X_9. To prove this, we establish that the Seshadri constant of 𝒪_ℙ^1×ℙ^1(1,1) at ten very general points is 1/√5, completing the reflection approach proposed by Dionne and Roth for the ten-point case. We also prove that the same equality holds at a very general free orbit of a fixed dihedral group of order ten. This yields an irrational one-point Seshadri constant on the singular quotient surface. A plane model of its minimal resolution and a deformation of the blow-up centers then give the result on X_9.
ER  -