{"title":"动力系统理论中的三个例子","authors":"M. Sevryuk","doi":"10.3842/SIGMA.2022.084","DOIUrl":null,"url":null,"abstract":". We present three explicit curious simple examples in the theory of dynamical systems. The first one is an example of two analytic diffeomorphisms R , S of a closed two-dimensional annulus that possess the intersection property but their composition RS does not ( R being just the rotation by π/ 2). The second example is that of a non-Lagrangian n -torus L 0 in the cotangent bundle T ∗ T n of T n ( n ≥ 2) such that L 0 intersects neither its images under almost all the rotations of T ∗ T n nor the zero section of T ∗ T n . The third example is that of two one-parameter families of analytic reversible autonomous ordinary differential equations of the form ˙ x = f ( x, y ), ˙ y = µg ( x, y ) in the closed upper half-plane { y ≥ 0 } such that the corresponding phase portraits for 0 < µ < 1 and for µ > 1 are topologically non-equivalent. The first two examples are expounded within the general context of symplectic topology.","PeriodicalId":49453,"journal":{"name":"Symmetry Integrability and Geometry-Methods and Applications","volume":" ","pages":""},"PeriodicalIF":0.9000,"publicationDate":"2022-09-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Three Examples in the Dynamical Systems Theory\",\"authors\":\"M. Sevryuk\",\"doi\":\"10.3842/SIGMA.2022.084\",\"DOIUrl\":null,\"url\":null,\"abstract\":\". We present three explicit curious simple examples in the theory of dynamical systems. The first one is an example of two analytic diffeomorphisms R , S of a closed two-dimensional annulus that possess the intersection property but their composition RS does not ( R being just the rotation by π/ 2). The second example is that of a non-Lagrangian n -torus L 0 in the cotangent bundle T ∗ T n of T n ( n ≥ 2) such that L 0 intersects neither its images under almost all the rotations of T ∗ T n nor the zero section of T ∗ T n . The third example is that of two one-parameter families of analytic reversible autonomous ordinary differential equations of the form ˙ x = f ( x, y ), ˙ y = µg ( x, y ) in the closed upper half-plane { y ≥ 0 } such that the corresponding phase portraits for 0 < µ < 1 and for µ > 1 are topologically non-equivalent. The first two examples are expounded within the general context of symplectic topology.\",\"PeriodicalId\":49453,\"journal\":{\"name\":\"Symmetry Integrability and Geometry-Methods and Applications\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":0.9000,\"publicationDate\":\"2022-09-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Symmetry Integrability and Geometry-Methods and Applications\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.3842/SIGMA.2022.084\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATHEMATICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Symmetry Integrability and Geometry-Methods and Applications","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.3842/SIGMA.2022.084","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATHEMATICS","Score":null,"Total":0}
. We present three explicit curious simple examples in the theory of dynamical systems. The first one is an example of two analytic diffeomorphisms R , S of a closed two-dimensional annulus that possess the intersection property but their composition RS does not ( R being just the rotation by π/ 2). The second example is that of a non-Lagrangian n -torus L 0 in the cotangent bundle T ∗ T n of T n ( n ≥ 2) such that L 0 intersects neither its images under almost all the rotations of T ∗ T n nor the zero section of T ∗ T n . The third example is that of two one-parameter families of analytic reversible autonomous ordinary differential equations of the form ˙ x = f ( x, y ), ˙ y = µg ( x, y ) in the closed upper half-plane { y ≥ 0 } such that the corresponding phase portraits for 0 < µ < 1 and for µ > 1 are topologically non-equivalent. The first two examples are expounded within the general context of symplectic topology.
期刊介绍:
Scope
Geometrical methods in mathematical physics
Lie theory and differential equations
Classical and quantum integrable systems
Algebraic methods in dynamical systems and chaos
Exactly and quasi-exactly solvable models
Lie groups and algebras, representation theory
Orthogonal polynomials and special functions
Integrable probability and stochastic processes
Quantum algebras, quantum groups and their representations
Symplectic, Poisson and noncommutative geometry
Algebraic geometry and its applications
Quantum field theories and string/gauge theories
Statistical physics and condensed matter physics
Quantum gravity and cosmology.