Singular barriers and quartic integrability breaking in the TTW system

Abstract

We study a symmetric quartic deformation of the classical ($k=1$) Tempesta-Turbiner-Winternitz system, $H=\frac{1}{2}\left(P_X^2+P_Y^2\right)+X^2+Y^2 +\fracγ{X^2}+\fracγ{Y^2} +κ\,X^2Y^2 $, which interpolates between the maximally superintegrable Smorodinsky-Winternitz oscillator and the quartically coupled Contopoulos oscillator. For $γ>0$, the inverse-square terms generate impenetrable walls at ($X=0$) and ($Y=0$), splitting configuration space into invariant sectors. We show that, for sufficiently small nonzero $κ$, resonant averaging produces a phase-locked periodic orbit whose fixed-energy reduced Poincaré map has no unit characteristic multiplier. The Poincaré's nonintegrability criterion then excludes a second independent $C^1$ first integral in any invariant neighbourhood of this orbit. The result is local in phase space and perturbative in $κ$. At finite coupling, Poincaré sections and finite-time Lyapunov maps show the breakup of invariant curves and the growth of chaotic layers with increasing energy and quartic coupling. Comparison with the barrier-free Contopoulos limit shows that the singular TTW walls suppress phase-space transport without restoring integrability.