Among all the Hamiltonian systems, the integrable ones have
special geometric properties; in particular, their solutions are
very regular and quasi-periodic. The quasi-periodicity of the
solutions of an integrable system is a result of the fact that the
system is invariant under a (semi-global) torus action. It is thus
natural to investigate the symplectic manifolds that can be endowed
with a (global) torus action. This leads to symplectic toric
manifolds (Part B of this book). Physics makes a surprising
come-back in Part A: to describe Mirror Symmetry, one looks for a
special kind of Lagrangian submanifolds and integrable systems, the
special Lagrangians. Furthermore, integrable Hamiltonian systems on
punctured cotangent bundles are a starting point for the study of
contact toric manifolds (Part C of this book).
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