EXERCISES IN POISSON GEOMETRY

Similar documents
LIE ALGEBROIDS AND POISSON GEOMETRY, OLIVETTI SEMINAR NOTES

Lie groupoids and Lie algebroids

Dirac structures. Henrique Bursztyn, IMPA. Geometry, mechanics and dynamics: the legacy of J. Marsden Fields Institute, July 2012

BRST 2006 (jmf) 7. g X (M) X ξ X. X η = [ξ X,η]. (X θ)(η) := X θ(η) θ(x η) = ξ X θ(η) θ([ξ X,η]).

HAMILTONIAN ACTIONS IN GENERALIZED COMPLEX GEOMETRY

INTRODUCTION TO POISSON GEOMETRY LECTURE NOTES, WINTER 2017

Exercises in Geometry II University of Bonn, Summer semester 2015 Professor: Prof. Christian Blohmann Assistant: Saskia Voss Sheet 1

A BRIEF INTRODUCTION TO DIRAC MANIFOLDS

Deformations of coisotropic submanifolds in symplectic geometry

Symplectic and Poisson Manifolds

On the Van Est homomorphism for Lie groupoids

LECTURE 1: LINEAR SYMPLECTIC GEOMETRY

Integrating exact Courant Algebroids

A MARSDEN WEINSTEIN REDUCTION THEOREM FOR PRESYMPLECTIC MANIFOLDS

Patrick Iglesias-Zemmour

On the holonomy fibration

Constant symplectic 2-groupoids

Reduction of Symplectic Lie Algebroids by a Lie Subalgebroid and a Symmetry Lie Group

LIE GROUPOIDS AND LIE ALGEBROIDS LECTURE NOTES, FALL Contents 1. Lie groupoids Definitions 30

Hamiltonian flows, cotangent lifts, and momentum maps

Lie theory of multiplicative structures.

INTEGRATION OF TWISTED POISSON STRUCTURES ALBERTO S. CATTANEO AND PING XU

From momentum maps and dual pairs to symplectic and Poisson groupoids

The BRST complex for a group action

Math 550 / David Dumas / Fall Problems

Quasi-Poisson structures as Dirac structures

Twisted Poisson manifolds and their almost symplectically complete isotropic realizations

Lie groupoids, cyclic homology and index theory

Dirac Structures on Banach Lie Algebroids

On the geometry of coisotropic submanifolds of Poisson manifolds

Lecture 5 - Lie Algebra Cohomology II

Deformations of Coisotropic Submanifolds of Jacobi Manifolds

The Atiyah bundle and connections on a principal bundle

INTEGRABILITY OF POISSON BRACKETS arxiv:math/ v2 [math.dg] 23 Dec 2003

Atiyah classes and homotopy algebras

Generalized complex geometry

BACKGROUND IN SYMPLECTIC GEOMETRY

SYMPLECTIC MANIFOLDS, GEOMETRIC QUANTIZATION, AND UNITARY REPRESENTATIONS OF LIE GROUPS. 1. Introduction

GEOMETRIC BRST QUANTIZATION

Many of the exercises are taken from the books referred at the end of the document.

THE NEWLANDER-NIRENBERG THEOREM. GL. The frame bundle F GL is given by x M Fx

LECTURE 28: VECTOR BUNDLES AND FIBER BUNDLES

Locally conformal Dirac structures and infinitesimal automorphisms

MANIN PAIRS AND MOMENT MAPS

In this short note we prove that any Dirac structure can be realized as the push-forward of a presymplectic form via a

Doubled Aspects of Vaisman Algebroid and Gauge Symmetry in Double Field Theory arxiv: v1 [hep-th] 15 Jan 2019

SYMPLECTIC GEOMETRY: LECTURE 5

LECTURE 3 MATH 261A. Office hours are now settled to be after class on Thursdays from 12 : 30 2 in Evans 815, or still by appointment.

R-flux string sigma model and algebroid duality on Lie 3-algebroids

LECTURE 11: SYMPLECTIC TORIC MANIFOLDS. Contents 1. Symplectic toric manifolds 1 2. Delzant s theorem 4 3. Symplectic cut 8

Sheaves of Lie Algebras of Vector Fields

Generalized complex geometry

Comparison for infinitesimal automorphisms. of parabolic geometries

THE MOMENTUM MAP IN POISSON GEOMETRY

class # MATH 7711, AUTUMN 2017 M-W-F 3:00 p.m., BE 128 A DAY-BY-DAY LIST OF TOPICS

GEOMETRIC QUANTIZATION

Poisson geometry of b-manifolds. Eva Miranda

(g 1, g 2 ) g 1 g 2. i : G G

THE MODULAR CLASS OF A LIE ALGEBROID COMORPHISM

Math 535a Homework 5

Normal forms in Poisson geometry

Geometry 9: Serre-Swan theorem

Integrability and Associativity

arxiv: v1 [math.dg] 24 Oct 2015

The Hitchin map, local to global

LECTURES ON PURE SPINORS AND MOMENT MAPS. Contents 1. Introduction Volume forms on conjugacy classes

arxiv:math.dg/ v2 24 Oct 2002

Lie, symplectic and Poisson groupoids and their Lie algebroids

Solutions to the Hamilton-Jacobi equation as Lagrangian submanifolds

Poisson Manifolds Bihamiltonian Manifolds Bihamiltonian systems as Integrable systems Bihamiltonian structure as tool to find solutions

Archivum Mathematicum

Stratified Symplectic Spaces and Reduction

From Poisson to Quantum Geometry

We can choose generators of this k-algebra: s i H 0 (X, L r i. H 0 (X, L mr )

Eva Miranda. UPC-Barcelona. (joint with Victor Guillemin and Ana Rita Pires) Zaragoza, February

DERIVED HAMILTONIAN REDUCTION

Modern Geometric Structures and Fields

Chap. 1. Some Differential Geometric Tools

Hamiltonian Systems of Negative Curvature are Hyperbolic

Poisson Structures. concerning their singularities

Dynamical systems on Leibniz algebroids

Stable generalized complex structures

arxiv:math/ v1 [math.ag] 18 Oct 2003

On Embedding Singular Poisson Spaces. Aaron Fraenkel McMillan

A little taste of symplectic geometry

Quantising noncompact Spin c -manifolds

Deformation Quantization and Reduction

Geometric Quantization

Poisson Geometry in Constrained Systems

(1) Let π Ui : U i R k U i be the natural projection. Then π π 1 (U i ) = π i τ i. In other words, we have the following commutative diagram: U i R k

arxiv: v2 [math.dg] 6 Aug 2018

On algebraic index theorems. Ryszard Nest. Introduction. The index theorem. Deformation quantization and Gelfand Fuks. Lie algebra theorem

CHARLES-MICHEL MARLE. Calculus on Lie algebroids, Lie groupoids and Poisson manifolds

COTANGENT MODELS FOR INTEGRABLE SYSTEMS

Representing Representations up to Homotopy

DIRAC STRUCTURES FROM LIE INTEGRABILITY

M4P52 Manifolds, 2016 Problem Sheet 1

HOLONOMY GROUPOIDS OF SINGULAR FOLIATIONS

PREQUANTIZATION OF SYMPLECTIC SUPERMANIFOLDS

LECTURE 16: LIE GROUPS AND THEIR LIE ALGEBRAS. 1. Lie groups

Transcription:

EXERCISES IN POISSON GEOMETRY The suggested problems for the exercise sessions #1 and #2 are marked with an asterisk. The material from the last section will be discussed in lecture IV, but it s possible (and good) to do the problems beforehand. 1. Poisson manifolds 1.1. Poisson bracket and Poisson bivector field. 1.1.1. Problem. Let {, } be a skew-symmetric bilinear form on C (M), and denote by Jac(f, g, h) = {f, {g, h}} + {g, {h, f}} + {h, {f, g}} the Jacobiator. Show that if X f = {f, } is a derivation, then Jac(f, g, h) is a derivation in each of its arguments. Consequently, the value of Jac(f, g, h) at m depends only on the differentials of f, g, h at m. In particular, if dim M = 2 it follows that Jac(f, g, h) = 0; thus {, } is a Poisson bracket. 1.1.2. Problem. (Poisson pencils.) Let {, } 0 and {, } 1 be two Poisson brackets on M,with the property that the sum {f, g} 0 + {f, g} 1 is again a Poisson bracket. Prove that all linear combinations are Poisson brackets. a 0 {f, g} 0 + a 1 {f, g} 1 1.1.3. Problem. Let π be a Poisson structure on a vector space V, and π 0 the leading term of its Taylor expansion at 0. Show that π 0 is again a Poisson structure. 1.1.4. Problem. ( ) Classify the translation invariant (i.e., constant ) Poisson structures on a vector space V. 1.1.5. Problem. ( ) Let π be a Poisson structure on a manifold M, and x 0 a point with π x0 = 0. Show that the cotangent space T x 0 M acquires a Lie bracket. 1.1.6. Problem. ( ) A vector field X on a Poisson manifold M is called a Poisson vector field if it satisfies L X {f, g} = {L X f, g} + {f, L X g} for all f, g. In particular, all Hamiltonian vector fields are Poisson vector fields. a) Give an example, as simple as possible, of a Poisson manifold and a Poisson vector field that is not a Hamiltonian vector field. b) Show that the Hamiltonian vector field are a Lie algebra ideal in the Lie algebra of Poisson vector fields. 1

2 EXERCISES IN POISSON GEOMETRY 1.1.7. Problem. Let G be a connected Lie group acting on a symplectic manifold (M, ω), preserving the symplectic structure. A map Φ: Q g is called a moment map for the action if it is G-equivariant, and the generating vector fields satisfy ι(ξ M )ω = d Φ, ξ for all ξ g. Show that Φ is a Poisson map with respect to the Lie-Poisson structure on g. Conversely, show that any Poisson map Φ: M g generates a (local) G-action having Φ as its moment map. 1.1.8. Problem. Given a Poisson manifold M, and a free and proper action of a Lie group G by Poisson diffeomorphisms, show that the quotient space M/G inherits a Poisson structure. As an example, show that the Kirillov Poisson structure on g may be obtained from a G-action on the symplectic manifold T G. 1.2. Submanifolds. Suppose (M, π) is a Poisson manifold. A submanifold N M is called a coisotropic submanifold if it has the property π (ann(t N)) T N. It is called a Poisson submanifold if π (T M N ) T N. 1.2.1. Problem. ( ) Let (M, π) be a Poisson manifold. (a) Show that N is coisotropic, if for all f, g C (M) vanishing on N, the restriction {f, g} N vanishes on N. (b) Show that N M is a Poisson submanifold if and only if for all f, g C (M), the restriction {f, g} N depends only on f N, g N. 1.2.2. Problem. ( ) Show that for any coisotropic submanifold N M, the conormal bundle ν(m, N) = ann(t N) T M N acquires a Lie algebroid structure. Remark: This problem becomes easier once you know about the Lie algebroid structure on T M, for a Poisson manifold M cf. Lecture II. What happens for a Poisson submanifold? 1.3. The Schouten bracket. 1.3.1. Problem. Let g be a Lie algebra, and g its exterior algebra. Prove the following Theorem 1.1 (Schouten bracket). There is a unique structure of a Z-graded super Lie algebra on g := 1 g, such that (i) The bracket extends that on g 0 = g; (ii) For fixed u k (M), the bracket [u, ] is a graded derivation of the wedge product on g, of degree k 1. Here, super Lie algebra means that the Jacobi identity and skew-symmetry hold with signs. Thus, [u, v] = ( 1) u v [v, u] and [u, [v, w]] + ( 1) u ( v + w ) [v, [w, u]] + ( 1) w ( u + v ) [w, [u, v]] = 0 for homogeneous elements u, v, w.

EXERCISES IN POISSON GEOMETRY 3 1.3.2. Problem. Let X (M) = Γ( T M) be the Z-graded vector space of multi-vector fields. Prove the following Theorem 1.2 (Schouten bracket). There is a unique structure of a Z-graded super Lie algebra on k := X 1 (M), with the following properties: (i) for fixed u X k (M), the bracket [u, ] is a graded derivation of degree k 1, with respect to the wedge product on X (M). (ii) For X X 1 (M), the Schouten bracket [X, ] is the Lie derivative. Note that the grading for the graded Lie algebra structure on multi-vector fields differs from the grading for the graded algebra structure! For example, [, ] is a bilinear map from X k (M) X l (M) to X k+l 1 (M), while the wedge product is a bilinear map X k (M) X l (M) to X k+l (M). Property (ii) above means that [u, v w] = [u, v] w + ( 1) (k 1)l v [u, w] if u, v, w are multivector fields of degrees k, l, m. 1.3.3. Problem. Using the defining properties of the Schouten bracket, show that for all f C (M) and u X (M). [f, u] = ι(df)u 1.3.4. Problem. Given a bivector field π X 2 (M), define {f, g} = π(df, dg). Show that [π, π](df, dg, dh) = 2 Jac(f, g, h). 1.3.5. Problem. From the properties of the Schouten bracket, it follows that d π := [π, ] is a differential on the Z-graded superalgebra X (M): That is, d 2 π = 1 2 [d π, d π ] = 1 [[π, π], ] = 0. 2 (a) Give a geometric interpretation to the cocycles in degree 1 and 2, as well as the coboundaries in degree 1. (b) Show that the map π : Ω(M) X(M) is a cochain map. 1.4. Poisson Lie groups. A Poisson Lie group is a Lie group G, together with a Poisson structure π such that the group multiplication is Poisson. A G-action on a Poisson manifold is called Poisson if the action map G M M is a Poisson map. 1.4.1. Problem. ( ) Show that for any Poisson Lie group G, the Poisson structure vanishes at the group unit e. 1.4.2. Problem. Show that for a Poisson Lie group G, the inversion map Inv: G G is anti- Poisson. That is, it becomes a Poisson map (G, π G ) (G, π G ). 1.4.3. Problem. ( ) Let G be a Poisson Lie group with a Poisson action on a Poisson manifold M. Show that the space C (M) G of invariant functions is closed under the Poisson bracket.

4 EXERCISES IN POISSON GEOMETRY 1.5. Tangent lifts. Given a vector field X X(M), let X T X(T M) denote its tangent lift. That is, the (local) flow of X is obtained by applying the tangent functor to the flow of X. The vertical lift of X, denoted X V X(T M), is the vertical vector field whose restriction to each fiber T m M is given by X m, regarded as a constant vector field. For f C (M), let its tangent lift f T C (T M) be the function such that f T (v) = v(f) for all v T M. We define the vertical lift f V C (T M) to be simply the pullback. 1.5.1. Problem. (a) Express X T and f T in local coordinates. (b) Show that X X T is a Lie algebra morphism X(M) X(T M). (c) Show that (X(f)) T = X T (f T ) for all X X(M) and f C (M). (d) Give formulas for (fg) T, (fx) T, for all X X(M) and f, g C (M). (e) Extend the tangent lift operation to a morphism of graded Lie algebras, relative to the Schouten bracket, X 1 (M) X 1 (T M), u u T. Express this lift operation in local coordinates. 1.5.2. Problem. As application of the previous problem, every Poisson structure π X 2 (M) has a tangent lift to a Poisson structure π T X 2 (T M). (a) Given a local coordinate expression for π, find the corresponding local coordinate expression for π T. (b) Show that if π is nondegenerate, then so is π T. (c) More generally, show that if N M is a symplectic leaf of π, then T N T M is a symplectic leaf of π T. 1.5.3. Problem. As we saw, the dual bundle E of any Lie algebroid E M inherits a Poisson structure. If M is a Poisson manifold, and E = T M its cotangent Lie algebroid, show that this Poisson structure on E = T M is the tangent lift. 1.5.4. Problem. Given a Lie algebroid E over M, construct a tangent lift Lie algebroid E T over T M. 2.1. Dirac manifolds. 2. Dirac manifolds 2.1.1. Problem. ( ) Prove that for any closed 2-form ω Ω 2 (M), with corresponding map ω : T M T M, v ω(v, ), the graph E = Gr(ω) = {v + ω (v) v T M} is a Dirac structure, with E T M = 0. Conversely, every Dirac structure E with E T M = 0 is the graph of a closed 2-form.

EXERCISES IN POISSON GEOMETRY 5 2.1.2. Problem. ( ) Describe a Dirac structure E TM associated to any (regular) foliation F of M. 2.1.3. Problem. ( ) Show that a smooth map Φ: M M between Poisson manifolds is a Poisson map if and only if the pull-back map on 1-forms Ω 1 (M) Ω 1 (M ) is a Lie algebra homomorphism. 2.1.4. Problem. ( ) Let E TM be a Dirac structure, with the property that E m = T mm for some m M. Show that the Lie bracket on Γ(E) induces a Lie algebra structure on T mm. 2.1.5. Problem. (Linear Dirac geometry) A metrized vector space is a vector space V with a non-degenerate metric. A subspace E V is Lagrangian, is E = E. Let V be the same vector space with the opposite metric. A Lagrangian relation between metrized vector spaces V and V is a Lagrangian subspaces L V V. Write v L v if (v, v) L. We define ker(l) to be the set of all v such that v L 0. (a) Given a Lagrangian subspace E V, show that its forward image E V, consisting of all v V such that v L v for some v E, is Lagrangian. (b) Similarly, for a Lagrangian F V, define its backward image and show that it is Lagrangian. (c) Suppose that in a) we have ker(l) E = 0, and let E be the forward image. If F V with E F = 0, show that the backward image F V satisfies E F = 0. 2.1.6. Problem. ( ) Let Φ C (M, N). Sections σ = X +α Γ(TM) and τ = Y +β Γ(TN) are called Φ-related if σ Φ τ : X Φ Y, α = Φ β. Show that σ 1 Φ τ 1, σ 2 Φ τ 2 [σ 1, σ 2 ] Φ [τ 1, τ 2 ]. 2.1.7. Problem. Show that the integrability of Lagrangian subbundles E TM is measured by a certain 3-tensor Υ E Γ( 3 E ). 2.1.8. Problem. (Mackenzie-Xu) Let E, F TM be two Dirac structures, with E F = 0. Let e 1,..., e n be a (local) basis of sections of E, and f 1,..., f n the dual basis of sections of F. Letting a: TM T M be the projection to the vector field part, show that π = i a(e i ) a(f i ) is a Poisson structure. 3. Symplectic groupoids 3.1. Lie groupoid cochains. Let G M be a Lie groupoid, and G (k) G k its space of k-arrows. Define maps i : G (k+1) G (k), i = 0,..., k + 1 by i (g 1,....g k+1 ) = (g 1,..., g i g i+1,..., g k+1 )

6 EXERCISES IN POISSON GEOMETRY for 0 < i < k + 1, while the map 0 drops g 1 and k+1 drops g k+1. 1 Let Then δ δ = 0. (Exercise.) k+1 δ = ( 1) i i : Ω (G (k) ) Ω (G (k+1) ). i=0 3.1.1. Problem. A form α Ω l (G) is called multiplicative if it satisfies δα = 0. For l = 0 this means, f(g 1 g 2 ) = f(g 1 ) + f(g 2 ). Show that a symplectic 2-form ω on a groupoid G M is multiplicative if and only if the graph of the groupoid multiplication is a Lagrangian submanifold Gr(Mult G ) G G G. 3.2. Bisections. An embedded submanifold S G of a Lie groupoid G M is a bisection if both s and t restrict to diffeomorphisms S M. (Thus, S can be regarded as a section of s, and also of t.) Let Γ(G) be the set of all bisections. 3.2.1. Problem. (a) Show that Γ(G) is naturally a group, and define actions Γ(G) Diff(G) of left multiplication, right multiplication, and conjugation (adjoint action) on G. Show that the conjugation action is by automorphisms of the groupoid structure. (b) Describe the group Γ(G), and its actions, for the following basic examples: (i) G = G pt a Lie group, (ii) G = M M M a pair groupoid, (iii) G = G M M an action groupoid for a G-action on M, (iv) G M the gauge groupoid of a principal G-bundle P M. (c) For a symplectic groupoid (G, ω), show that the actions above preserve the symplectic form if and only if S is a Lagrangian submanfold. Show that the Lagrangian bisections form a subgroup Γ Lag (G) Γ(G). 3.3. Symplectic realization. Let (M, π) be a Poisson manifold. A symplectic realization of (M, π) is a Poisson manifold (P, π P ), with π P non-degenerate (i.e. symplectic), together with a Poisson map P M. It is called full if it is a surjective submersion. An important example is M = g with the standard Lie-Poisson structure: a full symplectic realization is given by P = T G, where G is a Lie group integrating g, and with the map given by left trivialization. T G g 3.3.1. Problem. ( ) (Following Cannas da Silva-Weinstein) Let M = R 2 with the Poisson structure π = x 1. x 1 x 2 Let P = R 4, with coordinates q 1, q 2, p 1, p 2, with the Poisson structure π P = + q 1 p 1 q 2 p 2 1 Intuitively, a k-arrow involves k + 1 base points x0,..., x k, and arrows g i going from x i to x i 1. The map i is such that it omits the i-th base point.

EXERCISES IN POISSON GEOMETRY 7 corresponding to the standard symplectic form. Let i: M P be the inclusion (x 1, x 2 ) (x 1, x 2, 0, 0). a) Show that the map t: P M, (q 1, p 1, q 2, p 2 ) (q 1, q 2 + p 1 q 1 ) is Poisson. Thus, t defines a symplectic realization, with t i = id M. b) Find a submersion s: P M, with s i = id M, such that the fibers are symplectically orthogonal to those of t. Verify that s is anti-poisson. c) Not using the formulas from parts a) and b), argue that M admits a global symplectic groupoid integrating it. (Hint: This Poisson structure on R 2 is a special case of...). 3.3.2. Problem. ( ) Find a full symplectic realization for any Poisson structure of the form on R 2, where f is a smooth function. f(q 1, q 2 ), q 1 q 2 3.3.3. Problem. ( ) Consider π = q 1 q 2 on R 2. Using the Poisson spray X = p 1 p 2, q 2 q 1 on P = T R 2, show that the Poisson structure from Crainic-Marcut s symplectic realization is π P = +, q 1 p 1 q 2 p 2 q 1 q 2 with s(q, p) = q and t(q, p) = (q 1 p 2, q 2 + p 1 ). 3.3.4. Problem. As a more interesting example, work out the Crainic-Marcut construction for g, the dual of a Lie algebra. (The result will be T G = g G, in exponential coordinates on G near e.)