Symplectic geometry originated in Hamiltonian dynamics. Symplectic geometry is the study of symplectic structures. These are certain topological structures, but these can only exist on even dimensional manifolds. Since symplectic structures are purely topological structures, they do not depend on any metric structure of the underlying space. In the earlier work, Nazimuddin and Rifat (2014) developed a comparison between symplectic and Riemannian geometry [1] . After summarizing the basic definitions, examples and facts concerning symplectic geometry, this article will proceed to discuss the connections between symplectic geometry and contact geometry, Riemannian geometry, Kähler geometry.

Let M be a even dimensional smooth closed manifold, that is a compact smooth manifold without boundary. A symplectic structure ω on M is a closed, nondegenerate smooth 2-form. The nondegeneracy condition is equivalent to the fact that ω induces an isomorphism. In symplectic geometry, conformal changes to ω (i.e., multiplying by g) would usually force.

Example 2.1. The standard symplectic structure on is given by

where are the coordinates of. It is clear that ω₀ is closed.

Example 2.2. All manifolds are not symplectic. For instance, S⁴ is not. If ω₀ is a symplectic form on S⁴, then ω₀ is exact, since the second homology class of S⁴ vanishes [2] . In other words, since ω₀ is a closed 2-form, for some 1-form α₀ and. Since is a volume form on S⁴, Stokes theorem implies that

Since S⁴ has no boundary, the last integral vanishes and ω₀ can have no symplectic form.

The natural equivalence between symplectic structures is symplectomorphism. Two symplectic structures ω₁ and ω₂ on manifolds M₁ and M₂, respectively, are symplectomorphic if there exists a diffeomorphism satisfying. All symplectic structures are locally symplectomorphic. In consequence, there are no local invariants in symplectic geometry according to the following theorems. In particular case, We have Darboux’s theorem which states that, all symplectic structures on a 2n dimensional manifold are locally symplectomorphic to the standard structure on.

Theorem 3.1 (Darboux’s theorem) Let M be a manifold of dimension 2n with a closed non-degenerate 2-form ω₀. For any point p on a symplectic manifold, there exists a chart U with local coordinates, such that on U

Thus locally all symplectic structures are symplectomorphic to Example 2.1.

Theorem 3.2 (Weinstein’s Theorem) If a submanifold L of a symplectic manifold (M, ω), then there exists a neighborhood of L which is symplectomorphic to a neighborhood of the zero section in the cotangent bundle.

Furthermore symplectic structures are “local in time”. That is symplectic deformations of symplectic structures do not produce new symplectic structures.

Theorem 3.3 (Moser’s theorem) Let M be a closed manifold and ω_t, is a family of cohomologous symplectic forms on M then there is an isotopy with such that for all t.

In particular, on a symplectic manifold all deformations of symplectic structures come from diffeomorphisms of the underlying manifold. The theorem is not true if the symplectic structures do not agree off of a compact set.

If a symplectic vector bundle is a pair (E, ω) over a smooth manifold M of rank 2n, where E ® M is a real vector bundle, then ω_q (skew-symmetric and non-degenerate) is a symplectic form on each fiber E_q, depending smoothly on q. Each of the following two characteristics is equivalent to the existence of a symplectic structure (a) the existence of a reduction of the structure group of E from general linear group to symplectic group and (b) the existence of an (almost) complex structure on such that.

Now we discuss some recent results on the existence of symplectic structures on both open and closed manifolds. The existence problem of symplectic structures on even dimensional closed manifolds is quite difficult. However, Gromov has shown that symplectic structures on open manifolds obey an h-principle rule. As the existence problem of symplectic structures is based on a differential equation, but it can be reduced to a differential inequality and then solved by the h-principle.

Theorem 4.1 (Gromov’s Theorem) Every 2n dimensional manifold M with almost symplectic structure is homotopic through almost symplectic structures to a symplectic structure, if M is open.

If the manifolds are closed, then the existence problem is much more subtle. Often there are no h-principle rules. The following result was obtained using Seiberg-Witten theory:

Theorem 4.2 (Taubes Theorem) The connected sum of an odd number of copies of does not admit a symplectic structure (even though it admits an almost symplectic structure and a cohomology class such that).

In higher dimensions the uniqueness problem for symplectic forms on closed manifolds does not reduce to topological obstruction theory. There is often a dramatic difference between the space of non-degenerate two-forms and the space of symplectic forms [3] .

The even dimensional analogue theory to contact geometry is symplectic geometry. In general, contact manifolds come naturally as boundaries of symplectic manifolds. Also a contact manifold by symplectic means by looking at its symplectization [4] [5] .

Consider (X, ω) be a symplectic manifold. A vector field v satisfying

where L_vω is the Lie derivative of ω in the direction of v, is called a symplectic dilation. A compact hypersurface M in (X, ω) is said to have contact type if there exists a symplectic dilation v in a neighborhood of M that is transverse to M. Given a hypersurface M in (X, ω) the characteristic line field LM in the tangent bundle of M is the symplectic complement of TM in TX. (Since M is codimension one it is coisotropic and thus the symplectic complement lies in TM and is one dimensional.)

Theorem 5.1. Let M be a compact hypersurface in a symplectic manifold (X, ω) and denote the inclusion map. Then M has contact type if and only if there exists a 1-form α on M such that and the form α is never zero on the characteristic line field.

If M is a hypersurface of contact type, then the 1-form α is obtained by contracting the symplectic dilation v into the symplectic form:. It is easy to verify the 1-form α is a contact from on M. Thus a hypersurface of contact type in a symplectic manifold inherits a co-oriented contact structure.

Given a co-orientable contact manifold (M, ξ) its symplectization Symp (M, ξ) = (X, ω) is constructed as follows. The manifold and given a global contact form α for ξ the symplectic form is, where t is the coordinate on.

Example 5.2. The symplectization of the standard contact structure on the unit cotangent bundle is the standard symplectic structure on the complement of the zero section in the cotangent bundle.

The symplectization is independent of the choice of contact from α. To see this fix a co-orientation for ξ and note the manifold X can be identified (in may ways) with the subbundle of whose fiber over is { and β > 0 on vectors positively transverse to ξ_x} and restricting dλ the this subspace yields a symplectic form ω, where λ is the Liouville form on. A choice of contact form α fixes an identification of X with the subbundle of under which is taken to dλ.

The vector field on (X, ω) is a symplectic dilation that is transverse to. Clearly. Thus we see that any co-orientable contact mani-

fold can be realized as a hypersurface of contact type in a symplectic manifold. In summary we have the following theorem.

Theorem 5.3. If (M, ξ) is a co-oriented contact manifold, then there is a symplectic manifold Symp (M, ξ) in which M sits as a hypersurface of contact type. Moreover, any contact form α for ξ gives an embedding of M into Symp (M, ξ) that realizes M as a hypersurface of contact type.

We also note that all the hypersurfaces of contact type in (X, ω) look locally, in X, like a contact manifold sitting inside its symplectification.

Theorem 5.4. Given a compact hypersurface M of contact type in a symplectic manifold (X, ω) with the symplectic dilation given by v there is a neighborhood of M in X symplectomorphic to a neighborhood of M × {1} in Symp (M, ξ) where the symplectization is identified with using the contact form and.

The following proposition shows how symplectic structures can be generated from contact structures.

Proposition 5.5. [6] Let α be a contact structure on a 3-manifold. Then is a symplectic form on the 4-dimensional manifold, where θ is the coordinate on. (Here α is written as a form on).

Proof. We have. Thus,

Since is never zero and since does not contain differentials of θ, the claim follows.

There are also other relations between contact and symplectic geometry [7] .

The differentiable structure of a smooth manifold M gives rise to a canonical symplectic form on its cotangent bundle. Giving a Riemannian metric g on M is equivalent to prescribing its unit cosphere bundle and the restriction of the canonical 1-form from gives the structure of a contact manifold.

The following examples of known results are closely related to Riemannian and symplectic aspects of geometry.

1) A submanifold L of a symplectic manifold (M, ω) is called lagrangian if ω = 0 on TL.

a) Endow complex projective space with the usual Kähler metric and the usual Kähler form. The volume of submanifolds is taken with respect to this Riemannian metric. According to a result of Givental-Kleiner-Oh, the standard in has minimal volume among all its Hamiltonian deformations [8] . A partial result for the Clifford torus in can be found in [9] . The torus formed by the equators is also volume minimizing among its Hamiltonian deformations [10] . If L is a closed Lagrangian submanifold of there exists according to [11] a constant C depending on L such that Vol for all Hamiltonian deformations of L.

b) The mean curvature form of a Lagrangian submanifold L in a Kähler-Einstein manifold can be expressed through symplectic invariants of L [12] .

2) To estimate the first eigenvalue of the Laplacian operator on functions for certain Riemannian manifolds, symplectic methods can be used [13] .

3) Consider a bounded domain with smooth boundary. There exists a periodic billiard trajectory on of length l with

where C_n is an explicit constant depending only on n [14] .

4) Also Jacobi identity is satisfied as a consequence of the closure of the symplectic form, dω = 0.

Kähler manifolds are the remarkable class of symplectic manifolds. M. Gromov [15] observed that some of the tools used in the Kähler context can be used for the study of symplectic manifolds. One part of his wondering work has grown into which is now called Gromov-Witten theory [16] . All Kähler manifolds are symplectic, since the Kähler form is closed and non-degenerate For instance, the complex projective space is Kähler so that this space is also symplectic. But The converse need not be true, but we have the following theorem:

Theorem 7.1. A structure (M, ω, J) on a smooth manifold X is a Kähler structure if ω is a symplectic form, J is a complex structure, g is a Riemannian metric such that.

Many techniques and constructions from complex geometry are most useful in symplectic geometry. For instance, there is a symplectic version of blowing-up, which is closely related to the symplectic packing problem [17] [18] , also Donaldson’s construction of symplectic submanifolds [19] .

Also any complex surface admits a Kähler structure if and only if the first Betti number is even [20] . There are many symplectic 4-manifolds with even b1 (or b1 = 0) admitting no Kähler structure [21] . For a minimal Kähler surface we have the following theorem.

Theorem 7.2 Let (X, J) be a minimal Kähler surface. Then inside the symplectic cone, the Kähler cone can be enlarged across any of its open face determined by an irreducible curve with negative self-intersection. In fact, if the curve is not a rational curve with odd self-intersection, then the reflection of the Kähler cone along the corresponding face is in the symplectic cone.

In addition, for a minimal surface of general type, the canonical class K_J is shown to be in the symplectic cone in [22] [23] .

Symplectic geometry is a rather new and vigorously developing mathematical discipline. One can very roughly say that if the fundamental quantity in Riemannian geometry is length, then the fundamental quantity in symplectic geometry is directed area and the fundamental quantity in contact geometry is a certain twisting behavior. In this work, we have developed a connection between various branches of differential geometry with symplectic geometry.

Nazimuddin, A.K.M. and Ali, Md.S. (2016) Connections with Symplectic Structures. American Journal of Computational Mathematics, 6, 313-319. http://dx.doi.org/10.4236/ajcm.2016.64032