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Hamiltonian Isotopy


A Hamiltonian isotopy on a symplectic manifold (M,omega) is a smooth family of diffeomorphisms phi_H^t, starting at the identity, generated by a time-dependent real function H_t through

 partial_tphi_H^t=X_(H_t) degreesphi_H^t,

where the Hamiltonian vector field is defined by omega(X_(H_t),v)=dH_t(v). The opposite sign convention changes H_t to -H_t and gives the same class of isotopies. Each map in the family preserves the symplectic form. Its time-one map is a Hamiltonian diffeomorphism. On a noncompact manifold, compact support of the Hamiltonian function is commonly required. Hamiltonian isotopy is stronger than merely being a smooth isotopy or a symplectic diffeomorphism.


See also

Hamiltonian Diffeomorphism, Hamiltonian System, Symplectic Diffeomorphism, Symplectic Manifold

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References

Cannas da Silva, A. Lectures on Symplectic Geometry. Berlin: Springer-Verlag, 2001. https://people.math.ethz.ch/~acannas/Papers/lsg.pdf.

Cite this as:

Weisstein, Eric W. "Hamiltonian Isotopy." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/HamiltonianIsotopy.html

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