  With many Hamiltonians one can naturally associate a |Psi|^2-distributed
Markov process. For nonrelativistic quantum mechanics, this process is in fact
deterministic, and is known as Bohmian mechanics. For the Hamiltonian of a
quantum field theory, it is typically a jump process on the configuration space
of a variable number of particles. We define these processes for regularized
quantum field theories, thereby generalizing previous work of John S. Bell
[Phys. Rep. 137, 49 (1986)] and of ourselves [J. Phys. A: Math. Gen. 36, 4143
(2003)]. We introduce a formula expressing the jump rates in terms of the
interaction Hamiltonian, and establish a condition for finiteness of the rates.
