Conley conjecture

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Template:Short description

Template:Expert needed The Conley conjecture, named after mathematician Charles Conley, is a mathematical conjecture in the field of symplectic geometry, a branch of differential geometry.

Background

Let (M,ω) be a compact symplectic manifold. A vector field V on M is called a Hamiltonian vector field if the 1-form ω(V,) is exact (i.e., equals to the differential of a function H. A Hamiltonian diffeomorphism ϕ:MM is the integration of a 1-parameter family of Hamiltonian vector fields Vt,t[0,1].

In dynamical systems one would like to understand the distribution of fixed points or periodic points. A periodic point of a Hamiltonian diffeomorphism ϕ (of periodic k) is a point xM such that ϕk(x)=x. A feature of Hamiltonian dynamics is that Hamiltonian diffeomorphisms tend to have infinitely many periodic points. Conley first made such a conjecture for the case that M is a torus. Template:Refn

The Conley conjecture is false in many simple cases. For example, a rotation of a round sphere S2 by an angle equal to an irrational multiple of π, which is a Hamiltonian diffeomorphism, has only 2 geometrically different periodic points.Template:R On the other hand, it is proved for various types of symplectic manifolds.

History of studies

The Conley conjecture was proved by Franks and Handel for surfaces with positive genus. [1] The case of higher dimensional torus was proved by Hingston. [2] Hingston's proof inspired the proof of Ginzburg of the Conley conjecture for symplectically aspherical manifolds. Later Ginzburg--Gurel and Hein proved the Conley conjecture for manifolds whose first Chern class vanishes on spherical classes. Finally, Ginzburg--Gurel proved the Conley conjecture for negatively monotone symplectic manifolds.

References

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