Energy and canonical momentum conservation in non-local classical field theory Assume we have the following Lagrangian field density where $x, x'$ both three dimensional real vectors are coordinates and $t$ represents time, field is given by $\phi$. Assume for the sake of concreteness that $\phi$ is a function that returns three-dimensional real vector.
$$ \mathscr{L} = f(x) (\partial_t\phi)^2 + \int g(x, x', \phi(x), \phi(x')) dx'. $$
Define canonical momentum to be:
$$ \pi = \frac{\partial \mathscr{L}}{\partial(\partial_t\phi)} = 2f(x)\partial_t\phi. $$
Questions:


*

*Is it true that we can write equations of motion as:
$$ \partial_t \pi_i = - \sum \limits_j \frac{\partial}{\partial x_j} P_{ij}? $$
Here, $P_{ij}$ is some function.

*Is there an equivalent law of conservation of energy? How does it look like?
 A: *

*To keep the notation simple let us consider bi-local point-mechanics 
$$ S[q,v]~=~\int \! dt~dt^{\prime}~{\cal L}(t,t^{\prime}), \tag{A} $$ 
where we use the shorthand notation
$$ {\cal L}(t,t^{\prime})~=~{\cal L}(q(t),q(t^{\prime}),v(t),v(t^{\prime}),t,t^{\prime}).\tag{B}$$
(It is in principle straightforward to generalize to multi-local field theory.)

*Define momentum
$$p(t)~:=~\frac{\delta S[q,v]}{\delta v(t)}
~=~\int \! dt^{\prime}~\frac{\partial[{\cal L}(t,t^{\prime})+{\cal L}(t^{\prime},t)]}{\partial v(t)},\tag{C}$$
force
$$F(t)~:=~\frac{\delta S[q,v]}{\delta q(t)}~=~\int \! dt^{\prime}~\frac{\partial[{\cal L}(t,t^{\prime})+{\cal L}(t^{\prime},t)]}{\partial q(t)},\tag{D}$$
Lagrangian
$$ L(t)~:=~\int \! dt^{\prime}~[{\cal L}(t,t^{\prime})+{\cal L}(t^{\prime},t)], \tag{E}$$
and energy function
$$ H(t)~:=~p(t)v(t)-L(t).\tag{F}$$

*Next we identify
$$\dot{q}(t)~\approx~v(t),\tag{G}$$
and assume the stationary action principle (SAP). The Lagrangian EOM becomes
$$\dot{p}(t)~\approx~F(t).\tag{H}$$

*One may show that if ${\cal L}(t,t^{\prime})$ has no explicit time dependence, then the energy function $H(t)$ is conserved on-shell.

*For more on non-local action functionals, see e.g. this Phys.SE post.
