Liouville integrability refers to a type of integrability in Hamiltonian systems where there exist enough independent conserved quantities (integrals of motion) that are in involution, allowing the system to be fully solved by quadrature. This concept is fundamental in the study of dynamical systems, particularly in symplectic geometry, as it ties together the existence of conservation laws with the structural properties of the phase space. It provides a systematic way to identify integrable systems and is closely related to the analysis of their symplectic structures and normal forms.
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