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Abstract:A Zoll magnetic system on an oriented closed surface $M$ is a Riemannian metric $g$ together with a function $\lambda\colon M\to \mathbb{R}$, such that every unit speed solution of the ODE $\ddot \gamma(t)=\lambda(\gamma(t))\gamma(t)^\perp$ is periodic and the minimal period depends continuously on $\gamma$. The trivial example is given by $g$ with constant curvature $K$ and $\lambda\equiv {\rm const.}$ such that $\lambda^2+K>0$. This article exhibits non-trivial Zoll magnetic systems for every genus-for genus $\ge 2$ these are the first such examples.
The approach is twistor theoretic: To a general magnetic system $(g,\lambda)$ one associates its transport twistor space $Z(g,\lambda)$, which is the unit disk bundle $DM$, equipped with a degenerate complex structure that encodes the magnetic flow. For the trivial Zoll magnetic systems explicit holomorphic blow-down maps $\beta\colon Z(g,\lambda)\to W$ into certain ruled surfaces $W\to M$ are constructed, mapping $\partial Z(g,\lambda)$ onto a Lagrangian $P\subset W$. For small Lagrangian perturbations $P'\approx P$ the procedure can be reversed and this results in a large class of (non-trivial) nearby Zoll magnetic systems.

Submission history

From: Jan Bohr [view email]
[v1] Tue, 23 Jun 2026 21:05:42 UTC (71 KB)