The Hamiltonian vector field is symplectically dual to the differential of the energy. I will separate the object being defined from the consequence being claimed.
Objects and notation
A symplectic manifold \((M^{2n},\omega)\) has a closed nondegenerate two-form. A Hamiltonian \(H:M\to\mathbf R\) determines a vector field through contraction with \(\omega\).
I keep the defining relation \(\mathsf D\) above the derived relation \(\mathsf C\). This exposes whether cancellation used \(x\ne0\) and whether the conclusion is canonical.
Push the symbols
The middle display is intentionally dense: it is where signs, bounds, multiplicities, or normalising factors are most likely to be lost.
Structural reading
The two-row display is also a debugging tool: if the conclusion changes when only notation changes, some hidden choice has entered the argument.
A hypothesis worth keeping
Symplectic geometry has no preferred notion of distance. Nondegeneracy of a two-form is not positive definiteness of a metric.
The important habit is to remember what was fixed before the calculation began and what was proved only afterward. The final display preserves that order.