文摘
In this paper we make it mathematically rigorous the formulation of the following quantum Schrxf6;dinger–Langevin nonlinear operator for the wavefunction in bounded domains via its mild interpretation. The a priori ambiguity caused by the presence of the multi-valued potential λSψ, proportional to the argument of the complex-valued wavefunction is circumvented by subtracting its positional expectation value, as motivated in the original derivation (Kostin, 1972 [45]). The problem to be solved in order to find Sψ is mostly deduced from the modulus-argument decomposition of ψ and dealt with much like in Guerrero et al. (2010) [37]. Here is the (reduced) Planck constant, m is the particle mass, λ is a friction coefficient, nψ=ψ2 is the local probability density, denotes the electric current density, and Θ is a general operator (eventually nonlinear) that only depends upon the macroscopic observables nψ and Jψ. In this framework, we show local well-posedness of the initial-boundary value problem associated with the Schrxf6;dinger–Langevin operator in bounded domains. In particular, all of our results apply to the analysis of the well-known Kostin equation derived in Kostin (1972) [45] and of the Schrxf6;dinger–Langevin equation with Poisson coupling and enthalpy dependence (Jxfc;ngel et al., 2002 [41]).