On the generalization of classical Zernike system

Abstract

We generalize the results obtained recently (Nonlinearity \underline{36} (2023), 1143) by providing a very simple proof of the superintegrability of the Hamiltonian H=\vec{p}\,^{2}+F(\vec{q}\cdot\vec{p}), qβƒ—,pβƒ—βˆˆR2\vec{q}, \vec{p}\in\mathbb{R}^{2}, for any analytic function FF. The additional integral of motion is constructed explicitly and shown to reduce to a polynomial in canonical variables for polynomial FF. The generalization to the case qβƒ—,pβƒ—βˆˆRn\vec{q}, \vec{p}\in \mathbb{R}^{n} is sketched.Comment: 9 pages, no figures; pasections reorganized, references updated, some misprints correcte

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