Commuting integrable maps from a deformed D$_4$ cluster algebra
A. N. W. Hone, W. Kim, T. Mase
TL;DR
This work analyzes a two-parameter deformation of the D$_4$ cluster map, showing that while Zamolodchikov periodicity and the Laurent property fail in the original coordinates, the system preserves a presymplectic form and admits a planar Liouville-integrable reduction $\hat{\varphi}$. By lifting to an extended cluster algebra, the authors construct a second commuting map $\hat{\chi}$ and develop tau-function dynamics on a $\mathbb{Z}^2$ lattice, revealing quadratic degree growth with distinct leading coefficients and independence. The geometry of the first integral's elliptic fibration yields a rational elliptic surface of rank $2$ (Mordell–Weil group), enabling a Laurentification that preserves integrability and allows a QRT-type reformulation in a suitable chart. The results connect cluster mutation dynamics, elliptic surface arithmetic, and integrable mappings, and point to deep links with q-Painlevé equations and higher-rank deformations, with several open directions for general Dynkin types. $
Abstract
In this paper we revisit an integrable map of the plane which we obtained recently as a two-parameter family of deformed mutations in the cluster algebra of type D$_4$. The rational first integral for this map defines an invariant foliation of the plane by level curves, and we explain how this corresponds to a rational elliptic surface of rank 2. This leads us to construct another (independent) integrable map, commuting with the first, such that both maps lift to compositions of mutations in an enlarged cluster algebra, whose underlying quiver is equivalent to the one found by Okubo for the $q$-Painlevé VI equation. The degree growth of the two commuting maps is calculated in two different ways: firstly, from the tropical (max-plus) equations for the d-vectors of the cluster variables; and secondly, by constructing the minimal space of initial conditions for the two maps, via blowing up $\mathbb{P}^1 \times \mathbb{P}^1$.
