s the subsystem J shares the beable value with I. We find the momenta are given by which satisfy the Poisson brackets with the Hamiltonian nr = Of($, n) (41) {4,/,71j} = (42) I / / f 2 H = i ; [ (Ir )2 + n-QiWn)+ 2 sin2(4r - 4r) (43) cri The Hamilton equations of motion follow from th