How to show nonlinear Schrodinger equation is an infinite dimensional Hamiltonian system?

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The nonlinear Schrodinger equation is $$ ih\frac{\partial \psi}{\partial t} = -\frac{h^2}{2}\Delta \psi + V\psi-|\psi|^{p-1}\psi $$ From Wiki, I know the Hamiltonian system is

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And from Stability of semiclassical bound states of nonlinear Schrödinger equations with potentials, the author say the nonlinear Schrodinger equation (NLS) is Hamiltonian system. But for the given $E(\phi)$ , what is $p$ and $q$ as in definition of Hamiltonian system?

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Define the Hamiltonian density functional $\mathcal{H}$ as $$ \mathcal{H}=\frac{\hbar^2}{2}\nabla\Psi\cdot\nabla\Psi^*+(V-|\Psi|^p)\Psi^*\Psi. $$ The evolution equation is given by $$ i\hbar\frac{\partial\Psi}{\partial t}=\frac{\delta\mathcal{H}}{\delta\Psi^*}=\{\Psi,\mathcal{H}\}, $$ where the commutator between two functionals $\mathcal{F}$ and $\mathcal{G}$ is given by $$ \{\mathcal{F},\mathcal{G}\}=\frac{\delta\mathcal{F}}{\delta\Psi}\frac{\delta\mathcal{G}}{\delta\Psi^*}-\frac{\delta\mathcal{F}}{\delta\Psi^*}\frac{\delta\mathcal{G}}{\delta\Psi}, $$ with $\frac{\delta\mathcal{F}}{\delta\Psi}$ being the functional derivative. The canonical pair analogous to $(q,p)$ is given here by $(\Psi,\Psi^*)$.