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Outer billiards

Outer billiards is a dynamical system based on a convex shape in the plane. Classically, this system is defined for the Euclidean plane[1] but one can also consider the system in the hyperbolic plane[2] or in other spaces that suitably generalize the plane. Outer billiards differs from a usual dynamical billiard in that it deals with a discrete sequence of moves outside the shape rather than inside of it.

Definitions edit

The outer billiards map edit

Let P be a convex shape in the plane. Given a point x0 outside P, there is typically a unique point x1 (also outside P) so that the line segment connecting x0 to x1 is tangent to P at its midpoint and a person walking from x0 to x1 would see P on the right. (See Figure.) The map F: x0 -> x1 is called the outer billiards map.

 
Outer billiards defined relative to a pentagon

The inverse (or backwards) outer billiards map is also defined, as the map x1 -> x0. One gets the inverse map simply by replacing the word right by the word left in the definition given above. The figure shows the situation in the Euclidean plane, but the definition in the hyperbolic plane is essentially the same.

Orbits edit

An outer billiards orbit is the set of all iterations of the point, namely ... x0 <--> x1 <--> x2 <--> x3 ... That is, start at x0 and iteratively apply both the outer billiards map and the backwards outer billiards map. When P is a strictly convex shape, such as an ellipse, every point in the exterior of P has a well defined orbit. When P is a polygon, some points might not have well-defined orbits, on account of the potential ambiguity of choosing the midpoint of the relevant tangent line. Nevertheless, in the polygonal case, almost every point has a well-defined orbit.

  • An orbit is called periodic if it eventually repeats.
  • An orbit is called aperiodic (or non-periodic) if it is not periodic.
  • An orbit is called bounded (or stable) if some bounded region in the plane contains the whole orbit.
  • An orbit is called unbounded (or unstable) if it is not bounded.

Higher-dimensional spaces edit

Defining an outer billiards system in a higher-dimensional space is beyond the scope of this article. Unlike the case of ordinary billiards, the definition is not straightforward. One natural setting for the map is a complex vector space. In this case, there is a natural choice of line tangent to a convex body at each point. One obtains these tangents by starting with the normals and using the complex structure to rotate 90 degrees. These distinguished tangent lines can be used to define the outer billiards map roughly as above.[1]

History edit

Most people attribute the introduction of outer billiards to Bernhard Neumann in the late 1950s,[3] though it seems that a few people cite an earlier construction in 1945, due to M. Day. Jürgen Moser popularized the system in the 1970s as a toy model for celestial mechanics.[4][5] This system has been studied classically in the Euclidean plane, and more recently in the hyperbolic plane. One can also consider higher-dimensional spaces, though no serious study has yet been made. Bernhard Neumann informally posed the question as to whether or not one can have unbounded orbits in an outer billiards system, and Moser put it in writing in 1973.[4] Sometimes this basic question has been called the Moser-Neumann question. This question, originally posed for shapes in the Euclidean plane and solved only recently, has been a guiding problem in the field.

Moser-Neumann question edit

Bounded orbits in the Euclidean plane edit

In the 70's, Jürgen Moser sketched a proof, based on K.A.M. theory, that outer billiards relative to a 6-times-differentiable shape of positive curvature has all orbits bounded. In 1982, Raphael Douady gave the full proof of this result.[6] A big advance in the polygonal case came over a period of several years when three teams of authors, Vivaldi-Shaidenko,[7] Kolodziej,[8] and Gutkin-Simanyi,[9] each using different methods, showed that outer billiards relative to a quasirational polygon has all orbits bounded. The notion of quasirational is technical (see references) but it includes the class of regular polygons and convex rational polygons, namely those convex polygons whose vertices have rational coordinates. In the case of rational polygons, all the orbits are periodic. In 1995, Sergei Tabachnikov showed that outer billiards for the regular pentagon has some aperiodic orbits, thus clarifying the distinction between the dynamics in the rational and regular cases.[1] In 1996, Philip Boyland showed that outer billiards relative to some shapes can have orbits which accumulate on the shape.[10] In 2005, Daniel Genin showed that all orbits are bounded when the shape is a trapezoid, thus showing that quasirationality is not a necessary condition for the system to have all orbits bounded.[11] (Not all trapezoids are quasirational.)

Unbounded orbits in the Euclidean plane edit

In 2007, Richard Schwartz showed that outer billiards has some unbounded orbits when defined relative to the Penrose Kite, thus answering the original Moser-Neumann question in the affirmative.[12] The Penrose kite is the convex quadrilateral from the kites-and-darts Penrose tilings. Subsequently, Schwartz showed that outer billiards has unbounded orbits when defined relative to any irrational kite.[13] An irrational kite is a quadrilateral with the following property: One of the diagonals of the quadrilateral divides the region into two triangles of equal area and the other diagonal divides the region into two triangles whose areas are not rational multiples of each other. In 2008, Dmitry Dolgopyat and Bassam Fayad showed that outer billiards defined relative to the semidisk has unbounded orbits.[14] The semidisk is the region one gets by cutting a disk in half. The proof of Dolgopyat-Fayad is robust, and also works for regions obtained by cutting a disk nearly in half, when the word nearly is suitably interpreted.

Unbounded orbits in the hyperbolic plane edit

In 2003, Filiz Doǧru and Sergei Tabachnikov showed that all orbits are unbounded for a certain class of convex polygons in the hyperbolic plane.[15] The authors call such polygons large. (See the reference for the definition.) Filiz Doǧru and Samuel Otten then extended this work in 2011 by specifying the conditions under which a regular polygonal table in the hyperbolic plane have all orbits unbounded, that is, are large.[16]

Existence of periodic orbits edit

In ordinary polygonal billiards, the existence of periodic orbits is a major unsolved problem. For instance, it is unknown if every triangular shaped table has a periodic billiard path. More progress has been made for outer billiards, though the situation is far from well understood. As mentioned above, all the orbits are periodic when the system is defined relative to a convex rational polygon in the Euclidean plane. Moreover, it is a recent theorem of Chris Culter (written up by Sergei Tabachnikov) that outer billiards relative to any convex polygon has periodic orbits—in fact a periodic orbit outside of any given bounded region.[17]

Open questions edit

Outer billiards is a subject still in its beginning phase. Most problems are still unsolved. Here are some open problems in the area.

  • Show that outer billiards relative to almost every convex polygon has unbounded orbits.
  • Show that outer billiards relative to a regular polygon has almost every orbit periodic. The cases of the equilateral triangle and the square are trivial, and Tabachnikov answered this for the regular pentagon. These are the only cases known.
  • more broadly, characterize the structure of the set of periodic orbits relative to the typical convex polygon.
  • understand the structure of periodic orbits relative to simple shapes in the hyperbolic plane, such as small equilateral triangles.

See also edit

References edit

  1. ^ a b c Tabachnikov, Serge (1995). Billiards. Panoramas et Synthèses. Société Mathématique de France. ISBN 978-2-85629-030-9.
  2. ^ Tabachnikov, Sergei (2002). "Dual Billiards in the Hyperbolic Plane". Nonlinearity. 15 (4): 1051–1072. Bibcode:2002Nonli..15.1051T. CiteSeerX 10.1.1.408.9436. doi:10.1088/0951-7715/15/4/305. S2CID 250758250.
  3. ^ Neumann, Bernhard H. (25 Jan 1959). "Sharing Ham and Eggs". Iota: The Manchester University Mathematics Students' Journal.
  4. ^ a b Moser, Jürgen (1973). Stable and random motions in dynamical systems. Annals of Mathematics Studies. Vol. 77. Princeton University Press.
  5. ^ Moser, Jürgen (1978). "Is the Solar System Stable?". Mathematical Intelligencer. 1 (2): 65–71. doi:10.1007/BF03023062.
  6. ^ R. Douady (1982). "these de 3-eme cycle". University of Paris 7. {{cite journal}}: Cite journal requires |journal= (help)
  7. ^ Vivaldi, Franco; Shaidenko, Anna V. (1987). "Global Stability of a class of discontinuous billiards". Communications in Mathematical Physics. 110 (4): 625–640. Bibcode:1987CMaPh.110..625V. doi:10.1007/BF01205552. S2CID 111386812.
  8. ^ Kołodziej, Rafał (1989). "The antibilliard outside a polygon". Bull. Polish Acad. Sci. Math. 34: 163–168.
  9. ^ Gutkin, Eugene; Simanyi, Nandor (1991). "Dual polygonal billiard and necklace dynamics". Communications in Mathematical Physics. 143 (3): 431–450. Bibcode:1992CMaPh.143..431G. doi:10.1007/BF02099259. S2CID 121776396.
  10. ^ Boyland, Philip (1996). "Dual billiards, twist maps, and impact oscillators". Nonlinearity. 9 (6): 1411–1438. arXiv:math/9408216. Bibcode:1996Nonli...9.1411B. doi:10.1088/0951-7715/9/6/002. S2CID 18709638.
  11. ^ Genin, Daniel I. (2005). Regular and chaotic dynamics of outer billiards (Ph.D. Thesis). Pennsylvania State University.
  12. ^ Schwartz, Richard E. (2007). "unbounded orbits for outer billiards I". Journal of Modern Dynamics. 1 (3): 371–424. arXiv:math/0702073. Bibcode:2007math......2073S. doi:10.3934/jmd.2007.1.371. S2CID 119146537.
  13. ^ Schwartz, Richard E. (2009). "outer billiards on kites". Annals of Mathematics Studies. 171. Princeton University Press. {{cite journal}}: Cite journal requires |journal= (help)
  14. ^ Dolgopyat, Dmitry; Fayad, Bassam (2009). "unbounded orbits for semicircular outer billiards". Annales Henri Poincaré. 10 (2): 357–375. Bibcode:2009AnHP...10..357D. doi:10.1007/s00023-009-0409-9.
  15. ^ Doǧru, Filiz; Tabachnikov, Sergei (2003). "On Polygonal Dual Billiards in the Hyperbolic Plane". Regular and Chaotic Dynamics. 8 (1): 67–82. Bibcode:2003RCD.....8...67D. doi:10.1070/RD2003v008n01ABEH000226.
  16. ^ Doǧru, Filiz; Otten, Samuel (2011). "Sizing Up Outer Billiard Tables". American Journal of Undergraduate Research. 10: 1–8. doi:10.33697/ajur.2011.008.
  17. ^ Tabachnikov, Serge (2007). "A proof of Culter's theorem on existence of periodic orbits in polygonal outer billiards". Geometriae Dedicata. 129: 83–87. arXiv:0706.1003. Bibcode:2007arXiv0706.1003T. doi:10.1007/s10711-007-9196-y.

outer, billiards, this, article, includes, list, references, related, reading, external, links, sources, remain, unclear, because, lacks, inline, citations, please, help, improve, this, article, introducing, more, precise, citations, june, 2013, learn, when, r. This article includes a list of references related reading or external links but its sources remain unclear because it lacks inline citations Please help to improve this article by introducing more precise citations June 2013 Learn how and when to remove this template message Outer billiards is a dynamical system based on a convex shape in the plane Classically this system is defined for the Euclidean plane 1 but one can also consider the system in the hyperbolic plane 2 or in other spaces that suitably generalize the plane Outer billiards differs from a usual dynamical billiard in that it deals with a discrete sequence of moves outside the shape rather than inside of it Contents 1 Definitions 1 1 The outer billiards map 1 2 Orbits 1 3 Higher dimensional spaces 2 History 3 Moser Neumann question 3 1 Bounded orbits in the Euclidean plane 3 2 Unbounded orbits in the Euclidean plane 3 3 Unbounded orbits in the hyperbolic plane 4 Existence of periodic orbits 5 Open questions 6 See also 7 ReferencesDefinitions editThe outer billiards map edit Let P be a convex shape in the plane Given a point x0 outside P there is typically a unique point x1 also outside P so that the line segment connecting x0 to x1 is tangent to P at its midpoint and a person walking from x0 to x1 would see P on the right See Figure The map F x0 gt x1 is called the outer billiards map nbsp Outer billiards defined relative to a pentagonThe inverse or backwards outer billiards map is also defined as the map x1 gt x0 One gets the inverse map simply by replacing the word right by the word left in the definition given above The figure shows the situation in the Euclidean plane but the definition in the hyperbolic plane is essentially the same Orbits edit An outer billiards orbit is the set of all iterations of the point namely x0 lt gt x1 lt gt x2 lt gt x3 That is start at x0 and iteratively apply both the outer billiards map and the backwards outer billiards map When P is a strictly convex shape such as an ellipse every point in the exterior of P has a well defined orbit When P is a polygon some points might not have well defined orbits on account of the potential ambiguity of choosing the midpoint of the relevant tangent line Nevertheless in the polygonal case almost every point has a well defined orbit An orbit is called periodic if it eventually repeats An orbit is called aperiodic or non periodic if it is not periodic An orbit is called bounded or stable if some bounded region in the plane contains the whole orbit An orbit is called unbounded or unstable if it is not bounded Higher dimensional spaces edit Defining an outer billiards system in a higher dimensional space is beyond the scope of this article Unlike the case of ordinary billiards the definition is not straightforward One natural setting for the map is a complex vector space In this case there is a natural choice of line tangent to a convex body at each point One obtains these tangents by starting with the normals and using the complex structure to rotate 90 degrees These distinguished tangent lines can be used to define the outer billiards map roughly as above 1 History editMost people attribute the introduction of outer billiards to Bernhard Neumann in the late 1950s 3 though it seems that a few people cite an earlier construction in 1945 due to M Day Jurgen Moser popularized the system in the 1970s as a toy model for celestial mechanics 4 5 This system has been studied classically in the Euclidean plane and more recently in the hyperbolic plane One can also consider higher dimensional spaces though no serious study has yet been made Bernhard Neumann informally posed the question as to whether or not one can have unbounded orbits in an outer billiards system and Moser put it in writing in 1973 4 Sometimes this basic question has been called the Moser Neumann question This question originally posed for shapes in the Euclidean plane and solved only recently has been a guiding problem in the field Moser Neumann question editBounded orbits in the Euclidean plane edit In the 70 s Jurgen Moser sketched a proof based on K A M theory that outer billiards relative to a 6 times differentiable shape of positive curvature has all orbits bounded In 1982 Raphael Douady gave the full proof of this result 6 A big advance in the polygonal case came over a period of several years when three teams of authors Vivaldi Shaidenko 7 Kolodziej 8 and Gutkin Simanyi 9 each using different methods showed that outer billiards relative to a quasirational polygon has all orbits bounded The notion of quasirational is technical see references but it includes the class of regular polygons and convex rational polygons namely those convex polygons whose vertices have rational coordinates In the case of rational polygons all the orbits are periodic In 1995 Sergei Tabachnikov showed that outer billiards for the regular pentagon has some aperiodic orbits thus clarifying the distinction between the dynamics in the rational and regular cases 1 In 1996 Philip Boyland showed that outer billiards relative to some shapes can have orbits which accumulate on the shape 10 In 2005 Daniel Genin showed that all orbits are bounded when the shape is a trapezoid thus showing that quasirationality is not a necessary condition for the system to have all orbits bounded 11 Not all trapezoids are quasirational Unbounded orbits in the Euclidean plane edit In 2007 Richard Schwartz showed that outer billiards has some unbounded orbits when defined relative to the Penrose Kite thus answering the original Moser Neumann question in the affirmative 12 The Penrose kite is the convex quadrilateral from the kites and darts Penrose tilings Subsequently Schwartz showed that outer billiards has unbounded orbits when defined relative to any irrational kite 13 An irrational kite is a quadrilateral with the following property One of the diagonals of the quadrilateral divides the region into two triangles of equal area and the other diagonal divides the region into two triangles whose areas are not rational multiples of each other In 2008 Dmitry Dolgopyat and Bassam Fayad showed that outer billiards defined relative to the semidisk has unbounded orbits 14 The semidisk is the region one gets by cutting a disk in half The proof of Dolgopyat Fayad is robust and also works for regions obtained by cutting a disk nearly in half when the word nearly is suitably interpreted Unbounded orbits in the hyperbolic plane edit In 2003 Filiz Doǧru and Sergei Tabachnikov showed that all orbits are unbounded for a certain class of convex polygons in the hyperbolic plane 15 The authors call such polygons large See the reference for the definition Filiz Doǧru and Samuel Otten then extended this work in 2011 by specifying the conditions under which a regular polygonal table in the hyperbolic plane have all orbits unbounded that is are large 16 Existence of periodic orbits editIn ordinary polygonal billiards the existence of periodic orbits is a major unsolved problem For instance it is unknown if every triangular shaped table has a periodic billiard path More progress has been made for outer billiards though the situation is far from well understood As mentioned above all the orbits are periodic when the system is defined relative to a convex rational polygon in the Euclidean plane Moreover it is a recent theorem of Chris Culter written up by Sergei Tabachnikov that outer billiards relative to any convex polygon has periodic orbits in fact a periodic orbit outside of any given bounded region 17 Open questions editOuter billiards is a subject still in its beginning phase Most problems are still unsolved Here are some open problems in the area Show that outer billiards relative to almost every convex polygon has unbounded orbits Show that outer billiards relative to a regular polygon has almost every orbit periodic The cases of the equilateral triangle and the square are trivial and Tabachnikov answered this for the regular pentagon These are the only cases known more broadly characterize the structure of the set of periodic orbits relative to the typical convex polygon understand the structure of periodic orbits relative to simple shapes in the hyperbolic plane such as small equilateral triangles See also editIllumination problemReferences edit a b c Tabachnikov Serge 1995 Billiards Panoramas et Syntheses Societe Mathematique de France ISBN 978 2 85629 030 9 Tabachnikov Sergei 2002 Dual Billiards in the Hyperbolic Plane Nonlinearity 15 4 1051 1072 Bibcode 2002Nonli 15 1051T CiteSeerX 10 1 1 408 9436 doi 10 1088 0951 7715 15 4 305 S2CID 250758250 Neumann Bernhard H 25 Jan 1959 Sharing Ham and Eggs Iota The Manchester University Mathematics Students Journal a b Moser Jurgen 1973 Stable and random motions in dynamical systems Annals of Mathematics Studies Vol 77 Princeton University Press Moser Jurgen 1978 Is the Solar System Stable Mathematical Intelligencer 1 2 65 71 doi 10 1007 BF03023062 R Douady 1982 these de 3 eme cycle University of Paris 7 a href Template Cite journal html title Template Cite journal cite journal a Cite journal requires journal help Vivaldi Franco Shaidenko Anna V 1987 Global Stability of a class of discontinuous billiards Communications in Mathematical Physics 110 4 625 640 Bibcode 1987CMaPh 110 625V doi 10 1007 BF01205552 S2CID 111386812 Kolodziej Rafal 1989 The antibilliard outside a polygon Bull Polish Acad Sci Math 34 163 168 Gutkin Eugene Simanyi Nandor 1991 Dual polygonal billiard and necklace dynamics Communications in Mathematical Physics 143 3 431 450 Bibcode 1992CMaPh 143 431G doi 10 1007 BF02099259 S2CID 121776396 Boyland Philip 1996 Dual billiards twist maps and impact oscillators Nonlinearity 9 6 1411 1438 arXiv math 9408216 Bibcode 1996Nonli 9 1411B doi 10 1088 0951 7715 9 6 002 S2CID 18709638 Genin Daniel I 2005 Regular and chaotic dynamics of outer billiards Ph D Thesis Pennsylvania State University Schwartz Richard E 2007 unbounded orbits for outer billiards I Journal of Modern Dynamics 1 3 371 424 arXiv math 0702073 Bibcode 2007math 2073S doi 10 3934 jmd 2007 1 371 S2CID 119146537 Schwartz Richard E 2009 outer billiards on kites Annals of Mathematics Studies 171 Princeton University Press a href Template Cite journal html title Template Cite journal cite journal a Cite journal requires journal help Dolgopyat Dmitry Fayad Bassam 2009 unbounded orbits for semicircular outer billiards Annales Henri Poincare 10 2 357 375 Bibcode 2009AnHP 10 357D doi 10 1007 s00023 009 0409 9 Doǧru Filiz Tabachnikov Sergei 2003 On Polygonal Dual Billiards in the Hyperbolic Plane Regular and Chaotic Dynamics 8 1 67 82 Bibcode 2003RCD 8 67D doi 10 1070 RD2003v008n01ABEH000226 Doǧru Filiz Otten Samuel 2011 Sizing Up Outer Billiard Tables American Journal of Undergraduate Research 10 1 8 doi 10 33697 ajur 2011 008 Tabachnikov Serge 2007 A proof of Culter s theorem on existence of periodic orbits in polygonal outer billiards Geometriae Dedicata 129 83 87 arXiv 0706 1003 Bibcode 2007arXiv0706 1003T doi 10 1007 s10711 007 9196 y Retrieved from https en wikipedia org w index php title Outer billiards amp oldid 1187436066, wikipedia, wiki, book, books, library,

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