Solitons for the inverse curve shortening flow on the hyperbolic plane
Abstract
We study the solitons of the inverse curve shortening flow in the hyperbolic plane with respect to Killing fields: all parabolic fields, and the hyperbolic and elliptic fields with unit translation length and unit angular speed. The three cases reduce to one planar system. Except for a family of horocycles, every soliton has an endpoint at finite distance where the curvature blows up and the curve is a branch of a cusp. In the parabolic and elliptic cases there is a critical value H of the parameter of the family: below H the other end meets the ideal boundary orthogonally, above H it is a second singular endpoint, and at H the curvature tends to $1$. In the hyperbolic case H=π/2 and the critical solitons are horocycles. These horocycles are the only complete solitons and the only solitons of constant curvature.
Related
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BibTeX
@misc{krznaric2026solitons,
title = {{Solitons for the inverse curve shortening flow on the hyperbolic plane}},
author = {Ivan Krznarić and Rafael López},
howpublished = {arXiv},
year = {2026},
month = nov,
doi = {10.48550/arxiv.2605.14385},
eprint = {2605.14385},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2605.14385},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Solitons for the inverse curve shortening flow on the hyperbolic plane
AU - Ivan Krznarić
AU - Rafael López
PY - 2026
DA - 2026/11/04
PB - arXiv
DO - 10.48550/arxiv.2605.14385
UR - https://arxiv.org/abs/2605.14385
AB - We study the solitons of the inverse curve shortening flow in the hyperbolic plane with respect to Killing fields: all parabolic fields, and the hyperbolic and elliptic fields with unit translation length and unit angular speed. The three cases reduce to one planar system. Except for a family of horocycles, every soliton has an endpoint at finite distance where the curvature blows up and the curve is a branch of a cusp. In the parabolic and elliptic cases there is a critical value H of the parameter of the family: below H the other end meets the ideal boundary orthogonally, above H it is a second singular endpoint, and at H the curvature tends to $1$. In the hyperbolic case H=π/2 and the critical solitons are horocycles. These horocycles are the only complete solitons and the only solitons of constant curvature.
ER -