Bohm-Bell processes, of interest in the foundations of quantum field theory,
form a class of Markov processes Qt generalizing in a natural way both
Bohm's dynamical system in configuration space for nonrelativistic quantum
mechanics and Bell's jump process for lattice quantum field theories. They are
such that at any time t the distribution of Qt is ∣ψt∣2 with ψ
the wave function of quantum theory. We extend this class here by introducing
the analogous Markov process for quantum mechanics on a graph (also called a
network, i.e., a space consisting of line segments glued together at their
ends). It is a piecewise deterministic process whose innovations occur only
when it passes through a vertex.Comment: 15 pages LaTeX, 1 figure; v2 minor correction