English
Related papers

Related papers: Pentagram maps and refactorization in Poisson-Lie …

200 papers

We introduce a family of generalizations of the pentagram maps related to $Q$-nets. A specific example is considered, and we find the map can be treated as a refactorization mapping in the Poisson-Lie group of pseudo-difference operators.…

Exactly Solvable and Integrable Systems · Physics 2024-12-12 Bao Wang

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 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, 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

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 was introduced by R. Schwartz more than 20 years ago. In 2009, V. Ovsienko, R. Schwartz and S. Tabachnikov established Liouville complete integrability of this discrete dynamical system. In 2011, M. Glick interpreted the…

Dynamical Systems · Mathematics 2017-10-25 Michael Gekhtman , Michael Shapiro , Serge Tabachnikov , Alek Vainshtein

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 on polygons in the projective plane was introduced by R. Schwartz in 1992 and is by now one of the most popular and classical discrete integrable systems. In the present paper we introduce and prove integrability of…

Exactly Solvable and Integrable Systems · Physics 2022-11-03 Anton Izosimov , Boris Khesin

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

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 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

The pentagram map, introduced by R. Schwartz, is a birational map on the configuration space of polygons in the projective plane. We study the singularities of the iterates of the pentagram map. We show that a "typical" singularity…

Combinatorics · Mathematics 2012-03-06 Max Glick

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

The Hamiltonian structure of a class of three-dimensional (3D) Lotka-Volterra (LV) equations is revisited from a novel point of view by showing that the quadratic Poisson structure underlying its integrability structure is just a real…

Exactly Solvable and Integrable Systems · Physics 2011-08-23 Angel Ballesteros , Alfonso Blasco , Fabio Musso

The pentagram map is a discrete integrable system on the moduli space of planar polygons. The corresponding first integrals are so-called monodromy invariants $E_1, O_1, E_2, O_2,\dots$ By analyzing the combinatorics of these invariants,…

Exactly Solvable and Integrable Systems · Physics 2016-10-03 Anton Izosimov

The theory of Poisson-Lie groups and Lie bialgebras plays a major role in the study of one dimensional integrable systems; many families of integrable systems can be recovered from a Lax pair which is constructed from a Lie bialgebra…

Mathematical Physics · Physics 2024-07-19 Hank Chen , Florian Girelli

The notion of Poisson manifold with compatible pseudo-metric was introduced by the author in [1]. In this paper, we introduce a new class of Lie algebras which we call a pseudo-Rieamannian Lie algebras. The two notions are strongly related:…

Differential Geometry · Mathematics 2007-05-23 Mohamed Boucetta

A class of Poisson embeddings of reduced, finite dimensional symplectic vector spaces into the dual space $\Lg_R^*$ of a loop algebra, with Lie Poisson structure determined by the classical split $R$--matrix $R=P_+ - P_-$ is introduced.…

High Energy Physics - Theory · Physics 2008-02-03 J. Harnad , M. -A. Wisse

We introduce a Lie bialgebra structure on the central extension of the Lie algebra of differential operators on the line and the circle (with scalar or matrix coefficients). This defines a Poisson--Lie structure on the dual group of…

High Energy Physics - Theory · Physics 2009-10-22 Boris Khesin , Ilya Zakharevich
‹ Prev 1 2 3 10 Next ›