Symplectic Topology Math 705 Notes by Patrick Lei, Spring 2020
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Density of Thin Film Billiard Reflection Pseudogroup in Hamiltonian Symplectomorphism Pseudogroup Alexey Glutsyuk
Density of thin film billiard reflection pseudogroup in Hamiltonian symplectomorphism pseudogroup Alexey Glutsyuk To cite this version: Alexey Glutsyuk. Density of thin film billiard reflection pseudogroup in Hamiltonian symplectomor- phism pseudogroup. 2020. hal-03026432v2 HAL Id: hal-03026432 https://hal.archives-ouvertes.fr/hal-03026432v2 Preprint submitted on 6 Dec 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Density of thin film billiard reflection pseudogroup in Hamiltonian symplectomorphism pseudogroup Alexey Glutsyuk∗yzx December 3, 2020 Abstract Reflections from hypersurfaces act by symplectomorphisms on the space of oriented lines with respect to the canonical symplectic form. We consider an arbitrary C1-smooth hypersurface γ ⊂ Rn+1 that is either a global strictly convex closed hypersurface, or a germ of hy- persurface. We deal with the pseudogroup generated by compositional ratios of reflections from γ and of reflections from its small deforma- tions. In the case, when γ is a global convex hypersurface, we show that the latter pseudogroup is dense in the pseudogroup of Hamiltonian diffeomorphisms between subdomains of the phase cylinder: the space of oriented lines intersecting γ transversally. We prove an analogous local result in the case, when γ is a germ. -
The Extension Problem in Complex Analysis II; Embeddings with Positive Normal Bundle Author(S): Phillip A
The Extension Problem in Complex Analysis II; Embeddings with Positive Normal Bundle Author(s): Phillip A. Griffiths Source: American Journal of Mathematics, Vol. 88, No. 2 (Apr., 1966), pp. 366-446 Published by: The Johns Hopkins University Press Stable URL: http://www.jstor.org/stable/2373200 Accessed: 25/10/2010 12:00 Your use of the JSTOR archive indicates your acceptance of JSTOR's Terms and Conditions of Use, available at http://www.jstor.org/page/info/about/policies/terms.jsp. JSTOR's Terms and Conditions of Use provides, in part, that unless you have obtained prior permission, you may not download an entire issue of a journal or multiple copies of articles, and you may use content in the JSTOR archive only for your personal, non-commercial use. Please contact the publisher regarding any further use of this work. Publisher contact information may be obtained at http://www.jstor.org/action/showPublisher?publisherCode=jhup. Each copy of any part of a JSTOR transmission must contain the same copyright notice that appears on the screen or printed page of such transmission. JSTOR is a not-for-profit service that helps scholars, researchers, and students discover, use, and build upon a wide range of content in a trusted digital archive. We use information technology and tools to increase productivity and facilitate new forms of scholarship. For more information about JSTOR, please contact [email protected]. The Johns Hopkins University Press is collaborating with JSTOR to digitize, preserve and extend access to American Journal of Mathematics. http://www.jstor.org THE EXTENSION PROBLEM IN COMPLEX ANALYSIS II; EMBEDDINGS WITH POSITIVE NORMAL BUNDLE. -
Symplectic Structures on Gauge Theory?
Commun. Math. Phys. 193, 47 – 67 (1998) Communications in Mathematical Physics c Springer-Verlag 1998 Symplectic Structures on Gauge Theory? Nai-Chung Conan Leung School of Mathematics, 127 Vincent Hall, University of Minnesota, Minneapolis, MN 55455, USA Received: 27 February 1996 / Accepted: 7 July 1997 [ ] Abstract: We study certain natural differential forms ∗ and their equivariant ex- tensions on the space of connections. These forms are defined usingG the family local index theorem. When the base manifold is symplectic, they define a family of sym- plectic forms on the space of connections. We will explain their relationships with the Einstein metric and the stability of vector bundles. These forms also determine primary and secondary characteristic forms (and their higher level generalizations). Contents 1 Introduction ............................................... 47 2 Higher Index of the Universal Family ........................... 49 2.1 Dirac operators ............................................. 50 2.2 ∂-operator ................................................ 52 3 Moment Map and Stable Bundles .............................. 53 4 Space of Generalized Connections ............................. 58 5 Higer Level Chern–Simons Forms ............................. 60 [ ] 6 Equivariant Extensions of ∗ ................................ 63 1. Introduction In this paper, we study natural differential forms [2k] on the space of connections on a vector bundle E over X, A i [2k] FA (A)(B1,B2,...,B2 )= Tr[e 2π B1B2 B2 ] Aˆ(X). k ··· k sym ZX They are invariant closed differential forms on . They are introduced as the family local indexG for universal family of operators. A ? This research is supported by NSF grant number: DMS-9114456 48 N-C. C. Leung We use them to define higher Chern-Simons forms of E: [ ] ch(E; A0,...,A )=∗ L(A0,...,A ), l l ◦ l l and discuss their properties. -
1.10 Partitions of Unity and Whitney Embedding 1300Y Geometry and Topology
1.10 Partitions of unity and Whitney embedding 1300Y Geometry and Topology Theorem 1.49 (noncompact Whitney embedding in R2n+1). Any smooth n-manifold may be embedded in R2n+1 (or immersed in R2n). Proof. We saw that any manifold may be written as a countable union of increasing compact sets M = [Ki, and that a regular covering f(Ui;k ⊃ Vi;k;'i;k)g of M can be chosen so that for fixed i, fVi;kgk is a finite ◦ ◦ cover of Ki+1nKi and each Ui;k is contained in Ki+2nKi−1. This means that we can express M as the union of 3 open sets W0;W1;W2, where [ Wj = ([kUi;k): i≡j(mod3) 2n+1 Each of the sets Ri = [kUi;k may be injectively immersed in R by the argument for compact manifolds, 2n+1 since they have a finite regular cover. Call these injective immersions Φi : Ri −! R . The image Φi(Ri) is bounded since all the charts are, by some radius ri. The open sets Ri; i ≡ j(mod3) for fixed j are disjoint, and by translating each Φi; i ≡ j(mod3) by an appropriate constant, we can ensure that their images in R2n+1 are disjoint as well. 0 −! 0 2n+1 Let Φi = Φi + (2(ri−1 + ri−2 + ··· ) + ri) e 1. Then Ψj = [i≡j(mod3)Φi : Wj −! R is an embedding. 2n+1 Now that we have injective immersions Ψ0; Ψ1; Ψ2 of W0;W1;W2 in R , we may use the original argument for compact manifolds: Take the partition of unity subordinate to Ui;k and resum it, obtaining a P P 3-element partition of unity ff1; f2; f3g, with fj = i≡j(mod3) k fi;k. -
Lecture 1: Basic Concepts, Problems, and Examples
LECTURE 1: BASIC CONCEPTS, PROBLEMS, AND EXAMPLES WEIMIN CHEN, UMASS, SPRING 07 In this lecture we give a general introduction to the basic concepts and some of the fundamental problems in symplectic geometry/topology, where along the way various examples are also given for the purpose of illustration. We will often give statements without proofs, which means that their proof is either beyond the scope of this course or will be treated more systematically in later lectures. 1. Symplectic Manifolds Throughout we will assume that M is a C1-smooth manifold without boundary (unless specific mention is made to the contrary). Very often, M will also be closed (i.e., compact). Definition 1.1. A symplectic structure on a smooth manifold M is a 2-form ! 2 Ω2(M), which is (1) nondegenerate, and (2) closed (i.e. d! = 0). (Recall that a 2-form ! 2 Ω2(M) is said to be nondegenerate if for every point p 2 M, !(u; v) = 0 for all u 2 TpM implies v 2 TpM equals 0.) The pair (M; !) is called a symplectic manifold. Before we discuss examples of symplectic manifolds, we shall first derive some im- mediate consequences of a symplectic structure. (1) The nondegeneracy condition on ! is equivalent to the condition that M has an even dimension 2n and the top wedge product !n ≡ ! ^ ! · · · ^ ! is nowhere vanishing on M, i.e., !n is a volume form. In particular, M must be orientable, and is canonically oriented by !n. The nondegeneracy condition is also equivalent to the condition that M is almost complex, i.e., there exists an endomorphism J of TM such that J 2 = −Id. -
Characteristic Classes and K-Theory Oscar Randal-Williams
Characteristic classes and K-theory Oscar Randal-Williams https://www.dpmms.cam.ac.uk/∼or257/teaching/notes/Kthy.pdf 1 Vector bundles 1 1.1 Vector bundles . 1 1.2 Inner products . 5 1.3 Embedding into trivial bundles . 6 1.4 Classification and concordance . 7 1.5 Clutching . 8 2 Characteristic classes 10 2.1 Recollections on Thom and Euler classes . 10 2.2 The projective bundle formula . 12 2.3 Chern classes . 14 2.4 Stiefel–Whitney classes . 16 2.5 Pontrjagin classes . 17 2.6 The splitting principle . 17 2.7 The Euler class revisited . 18 2.8 Examples . 18 2.9 Some tangent bundles . 20 2.10 Nonimmersions . 21 3 K-theory 23 3.1 The functor K ................................. 23 3.2 The fundamental product theorem . 26 3.3 Bott periodicity and the cohomological structure of K-theory . 28 3.4 The Mayer–Vietoris sequence . 36 3.5 The Fundamental Product Theorem for K−1 . 36 3.6 K-theory and degree . 38 4 Further structure of K-theory 39 4.1 The yoga of symmetric polynomials . 39 4.2 The Chern character . 41 n 4.3 K-theory of CP and the projective bundle formula . 44 4.4 K-theory Chern classes and exterior powers . 46 4.5 The K-theory Thom isomorphism, Euler class, and Gysin sequence . 47 n 4.6 K-theory of RP ................................ 49 4.7 Adams operations . 51 4.8 The Hopf invariant . 53 4.9 Correction classes . 55 4.10 Gysin maps and topological Grothendieck–Riemann–Roch . 58 Last updated May 22, 2018. -
Double Groupoids and the Symplectic Category
JOURNAL OF GEOMETRIC MECHANICS doi:10.3934/jgm.2018009 c American Institute of Mathematical Sciences Volume 10, Number 2, June 2018 pp. 217{250 DOUBLE GROUPOIDS AND THE SYMPLECTIC CATEGORY Santiago Canez~ Department of Mathematics Northwestern University 2033 Sheridan Road Evanston, IL 60208-2730, USA (Communicated by Henrique Bursztyn) Abstract. We introduce the notion of a symplectic hopfoid, a \groupoid-like" object in the category of symplectic manifolds whose morphisms are given by canonical relations. Such groupoid-like objects arise when applying a version of the cotangent functor to the structure maps of a Lie groupoid. We show that such objects are in one-to-one correspondence with symplectic double groupoids, generalizing a result of Zakrzewski concerning symplectic double groups and Hopf algebra objects in the aforementioned category. The proof relies on a new realization of the core of a symplectic double groupoid as a symplectic quotient of the total space. The resulting constructions apply more generally to give a correspondence between double Lie groupoids and groupoid- like objects in the category of smooth manifolds and smooth relations, and we show that the cotangent functor relates the two constructions. 1. Introduction. The symplectic category is the category-like structure whose objects are symplectic manifolds and morphisms are canonical relations, i.e. La- grangian submanifolds of products of symplectic manifolds. Although compositions in this \category" are only defined between certain morphisms, this concept has nonetheless proved to be useful for describing many constructions in symplectic ge- ometry in a more categorical manner; in particular, symplectic groupoids can be characterized as certain monoid objects in this category, and Hamiltonian actions can be described as actions of such monoids. -
A C1 Arnol'd-Liouville Theorem
A C1 Arnol’d-Liouville theorem Marie-Claude Arnaud, Jinxin Xue To cite this version: Marie-Claude Arnaud, Jinxin Xue. A C1 Arnol’d-Liouville theorem. 2016. hal-01422530v2 HAL Id: hal-01422530 https://hal-univ-avignon.archives-ouvertes.fr/hal-01422530v2 Preprint submitted on 16 Aug 2017 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. A C1 ARNOL’D-LIOUVILLE THEOREM MARIE-CLAUDE ARNAUD†, JINXIN XUE Abstract. In this paper, we prove a version of Arnol’d-Liouville theorem for C1 commuting Hamiltonians. We show that the Lipschitz regularity of the foliation by invariant Lagrangian tori is crucial to determine the Dynamics on each Lagrangian torus and that the C1 regularity of the foliation by invariant Lagrangian tori is crucial to prove the continuity of Arnol’d- Liouville coordinates. We also explore various notions of C0 and Lipschitz integrability. Dedicated to Jean-Christophe Yoccoz 1. Introduction and Main Results. This article elaborates on the following question. Question. If a Hamiltonian system has enough commuting integrals1, can we precisely describe the Hamiltonian Dynamics, even in the case of non C2 integrals? When the integrals are C2, Arnol’d-Liouville Theorem (see [4]) gives such a dynamical description. -
Topological K-Theory
TOPOLOGICAL K-THEORY ZACHARY KIRSCHE Abstract. The goal of this paper is to introduce some of the basic ideas sur- rounding the theory of vector bundles and topological K-theory. To motivate this, we will use K-theoretic methods to prove Adams' theorem about the non- existence of maps of Hopf invariant one in dimensions other than n = 1; 2; 4; 8. We will begin by developing some of the basics of the theory of vector bundles in order to properly explain the Hopf invariant one problem and its implica- tions. We will then introduce the theory of characteristic classes and see how Stiefel-Whitney classes can be used as a sort of partial solution to the problem. We will then develop the methods of topological K-theory in order to provide a full solution by constructing the Adams operations. Contents 1. Introduction and background 1 1.1. Preliminaries 1 1.2. Vector bundles 2 1.3. Classifying Spaces 4 2. The Hopf invariant 6 2.1. H-spaces, division algebras, and tangent bundles of spheres 6 3. Characteristic classes 8 3.1. Definition and construction 9 3.2. Real projective space 10 4. K-theory 11 4.1. The ring K(X) 11 4.2. Clutching functions and Bott periodicity 14 4.3. Adams operations 17 Acknowledgments 19 References 19 1. Introduction and background 1.1. Preliminaries. This paper will presume a fair understanding of the basic ideas of algebraic topology, including homotopy theory and (co)homology. As with most writings on algebraic topology, all maps are assumed to be continuous unless otherwise stated. -
Homotopy Type of Symplectomorphism Groups of S2 × S2 S´Ilvia Anjos
ISSN 1364-0380 (on line) 1465-3060 (printed) 195 Geometry & Topology Volume 6 (2002) 195–218 Published: 27 April 2002 Homotopy type of symplectomorphism groups of S2 × S2 S´ılvia Anjos Departamento de Matem´atica Instituto Superior T´ecnico, Lisbon, Portugal Email: [email protected] Abstract In this paper we discuss the topology of the symplectomorphism group of a product of two 2–dimensional spheres when the ratio of their areas lies in the interval (1,2]. More precisely we compute the homotopy type of this sym- plectomorphism group and we also show that the group contains two finite dimensional Lie groups generating the homotopy. A key step in this work is to calculate the mod 2 homology of the group of symplectomorphisms. Although this homology has a finite number of generators with respect to the Pontryagin product, it is unexpected large containing in particular a free noncommutative ring with 3 generators. AMS Classification numbers Primary: 57S05, 57R17 Secondary: 57T20, 57T25 Keywords: Symplectomorphism group, Pontryagin ring, homotopy equiva- lence Proposed:YashaEliashberg Received:1October2001 Seconded: TomaszMrowka,JohnMorgan Revised: 11March2002 c Geometry & Topology Publications 196 S´ılvia Anjos 1 Introduction In general symplectomorphism groups are thought to be intermediate objects between Lie groups and full groups of diffeomorphisms. Although very little is known about the topology of groups of diffeomorphisms, there are some cases when the corresponding symplectomorphism groups are more understandable. For example, nothing is known about the group of compactly supported dif- feomorphisms of R4 , but in 1985, Gromov showed in [4] that the group of compactly supported symplectomorphisms of R4 with its standard symplectic structure is contractible. -
Hamiltonian and Symplectic Symmetries: an Introduction
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 54, Number 3, July 2017, Pages 383–436 http://dx.doi.org/10.1090/bull/1572 Article electronically published on March 6, 2017 HAMILTONIAN AND SYMPLECTIC SYMMETRIES: AN INTRODUCTION ALVARO´ PELAYO In memory of Professor J.J. Duistermaat (1942–2010) Abstract. Classical mechanical systems are modeled by a symplectic mani- fold (M,ω), and their symmetries are encoded in the action of a Lie group G on M by diffeomorphisms which preserve ω. These actions, which are called sym- plectic, have been studied in the past forty years, following the works of Atiyah, Delzant, Duistermaat, Guillemin, Heckman, Kostant, Souriau, and Sternberg in the 1970s and 1980s on symplectic actions of compact Abelian Lie groups that are, in addition, of Hamiltonian type, i.e., they also satisfy Hamilton’s equations. Since then a number of connections with combinatorics, finite- dimensional integrable Hamiltonian systems, more general symplectic actions, and topology have flourished. In this paper we review classical and recent re- sults on Hamiltonian and non-Hamiltonian symplectic group actions roughly starting from the results of these authors. This paper also serves as a quick introduction to the basics of symplectic geometry. 1. Introduction Symplectic geometry is concerned with the study of a notion of signed area, rather than length, distance, or volume. It can be, as we will see, less intuitive than Euclidean or metric geometry and it is taking mathematicians many years to understand its intricacies (which is work in progress). The word “symplectic” goes back to the 1946 book [164] by Hermann Weyl (1885–1955) on classical groups. -
Symplectic Embedding Problems, Old and New
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 55, Number 2, April 2018, Pages 139–182 http://dx.doi.org/10.1090/bull/1587 Article electronically published on August 11, 2017 SYMPLECTIC EMBEDDING PROBLEMS, OLD AND NEW FELIX SCHLENK Abstract. We describe old and new motivations to study symplectic embed- ding problems, and we discuss a few of the many old and the many new results on symplectic embeddings. Contents 1. Introduction 139 2. Meanings of “symplectic” 146 3. From Newtonian mechanics to symplectic geometry 148 4. Why study symplectic embedding problems 152 5. Euclidean symplectic volume preserving 158 6. Symplectic ellipsoids 162 7. The role of J-holomorphic curves 166 8. The fine structure of symplectic rigidity 170 9. Packing flexibility for linear tori 174 10. Intermediate symplectic capacities or shadows do not exist 176 Acknowledgments 178 About the author 178 References 178 1. Introduction 4 Consider Table 1.1 where pk is the percentage of the volume of the box [0, 1] ⊂ R4 thatcanbefilledbyk disjoint symplectically embedded balls of equal radius. What does symplectic mean? Why do we care about knowing these numbers? How can one find them? How can one understand them? The first goal of this text is to answer these questions. Table 1.1 k 1234 5 6 7 8 1 2 8 9 48 224 pk 2 1 3 9 10 49 225 1 Received by the editors February 18, 2017. 2010 Mathematics Subject Classification. Primary 53D35; Secondary 37B40, 53D40. The author is partially supported by SNF grant 200020-144432/1. c 2017 American Mathematical Society