Abstract:In this paper we prove that the generalization to RP n of the pentagram map defined in [3] is invariant under certain scalings for any n. This property allows the definition of a Lax representation for the map, to be used to establish its integrability. arXiv:1303.4295v1 [math.DS]
“…For some of these maps, for example, T (2,2),(1,1) , T (2,1), (1,1) , and T (3,1), (1,1) , complete integrability has been established [131,133,156]. Other cases were studied numerically in [132].…”
The paper surveys open problems and questions related to different aspects of integrable systems with finitely many degrees of freedom. Many of the open problems were suggested by the participants of the conference 'Finite-dimensional Integrable Systems, FDIS 2017' held at CRM, Barcelona in July 2017.This article is part of the theme issue 'Finite dimensional integrable systems: new trends and methods'.
“…For some of these maps, for example, T (2,2),(1,1) , T (2,1), (1,1) , and T (3,1), (1,1) , complete integrability has been established [131,133,156]. Other cases were studied numerically in [132].…”
The paper surveys open problems and questions related to different aspects of integrable systems with finitely many degrees of freedom. Many of the open problems were suggested by the participants of the conference 'Finite-dimensional Integrable Systems, FDIS 2017' held at CRM, Barcelona in July 2017.This article is part of the theme issue 'Finite dimensional integrable systems: new trends and methods'.
“…The pentagram map has seen a spike in popularity in the current decade thanks largely to the discovery that it is a discrete integrable system [1,9,10,14], and also because of emerging connections with cluster algebras [1,2]. In a sense, the recent work differs significantly from the first paper [11] in that (1) for the purposes of integrability and cluster algebras, it is more natural to have the pentagram map act not on individual polygons but on projective equivalence classes of polygons, and (2) there has been a focus on generalized pentagram maps [3][4][5][6][7][8], which are not known to possess a property analogous to preserving convexity. The present paper returns to the matter of the limit point (X, Y ) of the pentagram map acting on a convex polygon A.…”
The pentagram map is a discrete dynamical system defined on the space of polygons in the plane. In the first paper on the subject, R. Schwartz proved that the pentagram map produces from each convex polygon a sequence of successively smaller polygons that converges exponentially to a point. We investigate the limit point itself, giving an explicit description of its Cartesian coordinates as roots of certain degree three polynomials.
“…In [MB1], Mari-Beffa defines higher dimensional generalizations of the pentagram map and relates their continuous limits to various families of integrable PDEs. See also [MB2].…”
The pentagram map is now known to be a discrete integrable system. We show that the integrals for the pentagram map are constant along Poncelet families. That is, if P 1 and P 2 are two polygons in the same same Poncelet family, and f is a monodromy invariant for the pentagram map, then f (P 1 ) = f (P 2 ). Our proof combines complex analysis with an analysis of the geometry of a degenerating sequence of Poncelet polygons.
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