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The pentagram map that associates to a projective polygon a new one formed by intersections of short diagonals was introduced by R. Schwartz and was shown to be integrable by V. Ovsienko, R. Schwartz and S. Tabachnikov. Recently, M. Glick…

Quantum Algebra · Mathematics 2016-05-19 Michael Gekhtman , Michael Shapiro , Serge Tabachnikov , Alek Vainshtein

The pentagram map was introduced by R. Schwartz in 1992 for convex planar polygons. Recently, V. Ovsienko, R. Schwartz, and S. Tabachnikov proved Liouville integrability of the pentagram map for generic monodromies by providing a Poisson…

Algebraic Geometry · Mathematics 2019-10-30 Fedor Soloviev

The pentagram map is a discrete integrable system first introduced by Schwartz in 1992. It was proved to be intregable by Schwartz, Ovsienko, and Tabachnikov in 2010. Gekhtman, Shapiro, and Vainshtein studied Poisson geometry associated to…

Quantum Algebra · Mathematics 2019-02-05 Nicholas Ovenhouse

The pentagram map is a projectively natural iteration defined on polygons, and also on objects we call twisted polygons (a twisted polygon is a map from Z into the projective plane that is periodic modulo a projective transformation). We…

Dynamical Systems · Mathematics 2009-10-14 Valentin Ovsienko , Richard Schwartz , Serge Tabachnikov

The pentagram map, introduced by Schwartz in 1992, is a dynamical system on the moduli space of polygons in the projective plane. Its real and complex dynamics have been explored in detail. We study the pentagram map over an arbitrary…

Dynamical Systems · Mathematics 2023-01-27 Max H. Weinreich

We introduce twisted triple crossing diagram maps, collections of points in projective space associated to bipartite graphs on the cylinder, and use them to provide geometric realizations of the cluster integrable systems of Goncharov and…

Exactly Solvable and Integrable Systems · Physics 2025-06-04 Niklas Christoph Affolter , Terrence George , Sanjay Ramassamy

The pentagram map was introduced by R. Schwartz in 1992 and is now one of the most renowned discrete integrable systems. In the present paper we prove that this map, as well as all its known integrable multidimensional generalizations, can…

Exactly Solvable and Integrable Systems · Physics 2022-05-10 Anton Izosimov

We consider nonlinear recurrences generated from cluster mutations applied to quivers that have the property of being cluster mutation-periodic with period 1. Such quivers were completely classified by Fordy and Marsh, who characterised…

Exactly Solvable and Integrable Systems · Physics 2015-06-05 Allan Fordy , Andrew Hone

The pentagram map is a discrete dynamical system on planar polygons. By definition, the image of a polygon $P$ under the pentagram map is the polygon $P'$ whose vertices are the intersection points of consecutive shortest diagonals of $P$.…

Exactly Solvable and Integrable Systems · Physics 2025-09-29 Leaha Hand , Anton Izosimov

The pentagram map is a discrete dynamical system defined on the moduli space of polygons in the projective plane. This map has recently attracted a considerable interest, mostly because its connection to a number of different domains, such…

Dynamical Systems · Mathematics 2019-12-19 Valentin Ovsienko , Richard Evan Schwartz , Serge Tabachnikov

Cluster algebras are a class of commutative algebras whose generators are defined by a recursive process called mutation. We give a brief introduction to cluster algebras, and explain how discrete integrable systems can appear in the…

Combinatorics · Mathematics 2019-03-21 Andrew N. W. Hone , Philipp Lampe , Theodoros E. Kouloukas

We introduce a rich family of generalizations of the pentagram map sharing the property that each generates an infinite configuration of points and lines with four points on each line. These systems all have a description as $Y$-mutations…

Dynamical Systems · Mathematics 2017-05-17 Max Glick , Pavlo Pylyavskyy

We consider a class of complex manifolds constructed as multiplicative quiver varieties associated with a cyclic quiver extended by an arbitrary number of arrows starting at a new vertex. Such varieties admit a Poisson structure, which is…

Exactly Solvable and Integrable Systems · Physics 2026-01-07 Maxime Fairon

One of the remarkable properties of cluster algebras is that any cluster, obtained from a sequence of mutations from an initial cluster, can be written as a Laurent polynomial in the initial cluster (known as the "Laurent phenomenon").…

Mathematical Physics · Physics 2014-04-01 Allan P Fordy

The pentagram map was invented by Richard Schwartz in his search for a projective-geometric analogue of the midpoint map. It turns out that the dynamical behavior of the pentagram map is totally different from that of the midpoint map.…

Dynamical Systems · Mathematics 2018-08-02 Quang-Nhat Le

We consider a class of map, recently derived in the context of cluster mutation. In this paper we start with a brief review of the quiver context, but then move onto a discussion of a related Poisson bracket, along with the Poisson algebra…

Exactly Solvable and Integrable Systems · Physics 2011-05-17 Allan P Fordy

The pentagram map, introduced by R. Schwartz, is defined by the following construction: given a polygon as input, draw all of its "shortest" diagonals, and output the smaller polygon which they cut out. We employ the machinery of cluster…

Combinatorics · Mathematics 2011-04-18 Max Glick

The pentagram map is a projectively natural iteration defined on polygons, and also on a generalized notion of a polygon which we call {\it twisted polygons}. In this note we describe our recent work on the pentagram map, in which we find a…

Dynamical Systems · Mathematics 2009-01-13 Valentin Ovsienko , Richard Schwartz , Serge Tabachnikov

It is known that there is a one-to-one mapping between oriented directed graphs and zero-sum replicator dynamics (Lotka-Volterra equations) and that furthermore these dynamics are Hamiltonian in an appropriately defined nonlinear Poisson…

Exactly Solvable and Integrable Systems · Physics 2024-11-26 Matthew Visomirski , Christopher Griffin

We discuss the relation between the cluster integrable systems and $q$-difference Painlev\'e equations. The Newton polygons corresponding to these integrable systems are all 16 convex polygons with a single interior point. The Painlev\'e…

Mathematical Physics · Physics 2018-02-19 M. Bershtein , P. Gavrylenko , A. Marshakov
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