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Lemma 2.3
Under a hamiltonian deformation J d h ~ J\,\widetilde{\!dh\,} of a
Lagrangian L L , we have
d d t θ \displaystyle{d\over dt}\theta\!
= \displaystyle=
− Δ L ( h ) , \displaystyle\!-\Delta_{L}(h),
(2.4)
d d t vol L \displaystyle{d\over dt}\vol_{L}\!
= \displaystyle=
− ⟨ d θ , d h ⟩ vol L . \displaystyle\!-\langle d\theta,dh\rangle\vol_{L}.