In mathematics, a symplectic manifold is a smooth manifold, M, equipped with a closed nondegenerate differential 2-form, ω, called the symplectic form. The study of symplectic manifolds is called symplectic geometry or symplectic topology. Symplectic manifolds arise naturally in abstract formulations of classical mechanics and analytical mechanics as the cotangent bundles of manifolds. For example, in the Hamiltonian formulation of classical mechanics, which provides one of the major motivations for the field, the set of all possible configurations of a system is modeled as a manifold, and this manifold's cotangent bundle describes the phase space of the system.
Contents
- Motivation
- Definition
- Linear symplectic manifold
- Lagrangian and other submanifolds
- Special Lagrangian submanifolds
- Lagrangian fibration
- Lagrangian mapping
- Special cases and generalizations
- References
Any real-valued differentiable function, H, on a symplectic manifold can serve as an energy function or Hamiltonian. Associated to any Hamiltonian is a Hamiltonian vector field; the integral curves of the Hamiltonian vector field are solutions to Hamilton's equations. The Hamiltonian vector field defines a flow on the symplectic manifold, called a Hamiltonian flow or symplectomorphism. By Liouville's theorem, Hamiltonian flows preserve the volume form on the phase space.
Motivation
Symplectic manifolds arise from classical mechanics, in particular, they are a generalization of the phase space of a closed system. In the same way the Hamilton equations allow one to derive the time evolution of a system from a set of differential equations, the symplectic form should allow one to obtain a vector field describing the flow of the system from the differential dH of a Hamiltonian function H. So we require a linear map TM → T*M, or equivalently, an element of T*M ⊗ T*M. Letting ω denote a section of T*M ⊗ T*M, the requirement that ω be non-degenerate ensures that for every differential dH there is a unique corresponding vector field VH such that dH = ω(VH, · ). Since one desires the Hamiltonian to be constant along flow lines, one should have dH(VH) = ω(VH, VH) = 0, which implies that ω is alternating and hence a 2-form. Finally, one makes the requirement that ω should not change under flow lines, i.e. that the Lie derivative of ω along VH vanishes. Applying Cartan's formula, this amounts to
which is equivalent to the requirement that ω should be closed.
Definition
A symplectic form on a manifold M is a closed non-degenerate differential 2-form ω. Here, non-degenerate means that for all p ∈ M, if there exists an X ∈ TpM such that ω(X,Y) = 0 for all Y ∈ TpM, then X = 0. The skew-symmetric condition (inherent in the definition of differential 2-form) means that for all p ∈ M we have ω(X,Y) = −ω(Y,X) for all X,Y ∈ TpM. In odd dimensions, antisymmetric matrices are not invertible. Since ω is a differential two-form, the skew-symmetric condition implies that M has even dimension. The closed condition means that the exterior derivative of ω vanishes, dω = 0. A symplectic manifold consists of a pair (M,ω), of a manifold M and a symplectic form ω. Assigning a symplectic form ω to a manifold M is referred to as giving M a symplectic structure.
Linear symplectic manifold
There is a standard linear model, namely a symplectic vector space R2n. Let R2n have the basis {v1, ..., v2n}. Then we define our symplectic form ω so that for all 1 ≤ i ≤ n we have ω(vi,vn+i) = 1, ω(vn+i,vi) = −1, and ω is zero for all other pairs of basis vectors. In this case the symplectic form reduces to a simple quadratic form. If In denotes the n × n identity matrix then the matrix, Ω, of this quadratic form is given by the (2n × 2n) block matrix:
Lagrangian and other submanifolds
There are several natural geometric notions of submanifold of a symplectic manifold.
The most important case of the isotropic submanifolds is that of Lagrangian submanifolds. A Lagrangian submanifold is, by definition, an isotropic submanifold of maximal dimension, namely half the dimension of the ambient symplectic manifold. One major example is that the graph of a symplectomorphism in the product symplectic manifold (M × M, ω × −ω) is Lagrangian. Their intersections display rigidity properties not possessed by smooth manifolds; the Arnold conjecture gives the sum of the submanifold's Betti numbers as a lower bound for the number of self intersections of a smooth Lagrangian submanifold, rather than the Euler characteristic in the smooth case.
Special Lagrangian submanifolds
In the case of Kahler manifolds (or Calabi-Yau manifolds) we can make a choice
- complex Lagrangian submanifolds of hyperKahler manifolds,
- fixed points of a real structure of Calabi-Yau manifolds.
The SYZ conjecture has been proved for special Lagrangian submanifolds but in general, it is open, and brings a lot of impacts to the study of mirror symmetry. see (Hitchin 1999)
Lagrangian fibration
A Lagrangian fibration of a symplectic manifold M is a fibration where all of the fibres are Lagrangian submanifolds. Since M is even-dimensional we can take local coordinates (p1,…,pn,q1,…,qn), and by Darboux's theorem the symplectic form ω can be, at least locally, written as ω = ∑ dpk ∧ dqk, where d denotes the exterior derivative and ∧ denotes the exterior product. Using this set-up we can locally think of M as being the cotangent bundle T*Rn, and the Lagrangian fibration as the trivial fibration π : T*Rn ↠ Rn. This is the canonical picture.
Lagrangian mapping
Let L be a Lagrangian submanifold of a symplectic manifold (K,ω) given by an immersion i : L ↪ K (i is called a Lagrangian immersion). Let π : K ↠ B give a Lagrangian fibration of K. The composite (π ∘ i) : L ↪ K ↠ B is a Lagrangian mapping. The critical value set of π ∘ i is called a caustic.
Two Lagrangian maps (π1 ∘ i1) : L1 ↪ K1 ↠ B1 and (π2 ∘ i2) : L2 ↪ K2 ↠ B2 are called Lagrangian equivalent if there exist diffeomorphisms σ, τ and ν such that both sides of the diagram given on the right commute, and τ preserves the symplectic form. Symbolically:
where τ*ω2 denotes the pull back of ω2 by τ.