Order the phase-space coordinates as
Then Hamilton's equations are
The Poisson bracket is
For with Jacobian , the chain rule gives
This has Hamiltonian form with the same canonical matrix for every exactly when
Taking determinants gives ; the symplectic condition fixes the orientation, so . Hence the change-of-variables formula shows that the phase-space volume element is invariant. This is Liouville theorem in Hamiltonian mechanics.

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