I recently asked two questions, Q. [1] and Q. [2], regarding reformulating non-local Lagrangians as Hamiltonians.
In these questions, the Hamiltonian is formulated as an integral because of it's non-local nature. Additionally, all of the partial derivatives must be replaced by functional derivatives, for the same reason.
My question is, how does one formulate a symplectic integrator for such a Hamiltonian?
In all symplectic integrator derivations I've seen, the Hamiltonian function is used, not the integral. Is there a more generalized approach one can take in this case?
Take for example the case where:
$$ \mathbb{H}=\frac{1}{2}\int^t_0 \left(p(\tau)p(t-\tau)+q(\tau)q(t-\tau)\right)\,\text{d}\tau \tag{1}$$
This Hamiltonian has the associated Hamilton's equations of (as per Q. [2]) :
$$ \dot{q}(\tau)=p(\tau),\,\dot{p}(\tau)=q(\tau) \tag{2}$$
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[1] This question deals with the Legendre transform for non-local Lagrangian formulations.
[2] This question (and answer) deals the derivation of the Euler-Lagrange equations and Hamilton's equations for non-local Lagrangians.