Noise and dissipation in quantum theory

A model independent generalization of usual quantum mechanics, including the usual as well as the dissipative quantum systems, is proposed. The theory is developed deductively from the basic principles of the standard quantum theory, the only new qualitative assumption being that we allow the wave operator at time $t$ of a quantum system to be non differentiable (in $t$ ) in the usual sense, but only in an appropriately defined (Section (5.) ) stochastic sense. The resulting theory is shown to lead to a natural generalization of the usual quantum equations of motion, both in the form of the Schr\"odinger equation in interaction representation (Section (6.) ) and of the Heisenberg equation (Section (8.) ). The former equation leads in particular to a quantum fluctuation-dissipation relation of Einstein' s type. The latter equation is a generalized Langevin equation, from which the known form of the generalized master equation can be deduced via the quantum Feynman-Kac technique (Sections (9.) and (10.) ). For quantum noises with increments commuting with the past the quantum Langevin equation defines a closed system of (usually nonlinear) stochastic differential equations for the observables defining the coefficients of the noises. Such systems are parametrized by certain Lie algebras of observables of the system (Section (10.) ). With appropriate choices of these Lie algebras one can deduce generalizations and corrections of several phenomenological equations previously introduced at different times to explain different phenomena . Two examples are considered : the Lie algebra $[q, p]=i$ (Section (12.) ) , which is shown to lead to the equations of the damped harmonic oscillator ; and the Lie algebra of $SO(3)) $ (Section (13.) ) which is shown to lead to the Bloch equations . In both cases the equations obtained are independent of the model of noise. Moreover, in the former case, it is proved that the only possible noises which preserve the commutation relations of $p,q$ are the quantum Brownian motions, commonly used in Laser theory and solid state physics.