Lp. Hughston, GEOMETRY OF STOCHASTIC STATE-VECTOR REDUCTION, Proceedings - Royal Society. Mathematical, physical and engineering sciences, 452(1947), 1996, pp. 953-979
The state space of a quantum mechanical system is a complex projective
space, the space of rays in the associated Hilbert space. The state s
pace comes equipped with a natural Riemannian metric (the Fubini-Study
metric) and a compatible symplectic structure. The operations of ordi
nary quantum mechanics can thus be reinterpreted in the language of di
fferential geometry. It is interesting in this spirit to scrutinize th
e probabilistic assumptions that are brought ill at various stages in
the analysis of quantum dynamics, particularly in connection with stat
e vector reduction. A promising approach to understanding reduction, s
tudied recently by a number of authors, involves the use of nonlinear
stochastic dynamics to modify the ordinary linear Schrodinger evolutio
n. Here we use stochastic differential geometry to give a systematic g
eometric formulation for such stochastic models of state vector collap
se. In this picture, the conventional Schrodinger evolution; which cor
responds to the unitary flow associated with a Killing vector of the F
ubini-Study metric, is replaced by a more general stochastic flow on t
he state manifold. In the simplest example of such a flow, the volatil
ity term in the stochastic differential equation for the state traject
ory is proportional to the gradient of the expectation of the Hamilton
ian. The conservation of energy is represented by the requirement that
the actual process followed by the expectation of the Hamiltonian, as
the state evolves: should be a martingale. This requirement implies t
he existence of a nonlinear term in the drift vector of the state proc
ess, which is always oriented opposite to the direction of increasing
energy uncertainty. As a consequence, the state vector necessarily col
lapses to an energy eigenstate, and a martingale argument call be used
to show that the probability of collapse to a given eigenstate, from
any particular initial state, is, in fact, given by precisely the usua
l quantum mechanical probability.