Abstract
Continuous quantum measurement theory is used to construct a phenomenological description of the interaction of a quasiclassical variable with a quantum variable , where the quasiclassical nature of is assumed to have come about as a result of decoherence. The state of the quantum subsystem evolves according to the stochastic nonlinear Schrödinger equation of a continuously measured system, and the classical system couples to a stochastic number representing the imprecisely measured value of . The theory gives intuitively sensible results even when the quantum system starts out in a superposition of well-separated localized states.
- Received 13 May 1997
DOI:https://doi.org/10.1103/PhysRevLett.81.2846
©1998 American Physical Society