Quantum-classical transition in dissipative systems through scaled trajectories
arXiv:1711.07207 · doi:10.1088/2399-6528/aab521
Abstract
A nonlinear quantum-classical transition wave equation is proposed for dissipative systems within the Caldirola-Kanai model. Equivalence of this transition equation to a scaled Schrödinger equation is proved. The dissipative dynamics is then studied in terms of what we call scaled trajectories following the standard procedure used in Bohmian mechanics. These trajectories depend on a continuous parameter allowing us a smooth transition from Bohmian to classical trajectories. Arrival times and actual momentum distribution functions are also analyzed. The propagation of a Gaussian wave packet in a viscid medium under the presence of constant, linear and harmonic potentials is studied. The gradual decoherence process and localization are easily visualized and understood within this theoretical framework.
References in corpus (1)
Cited by in corpus (10)
- Dissipative tunneling by means of scaled trajectories
- Dissipative quantum backflow
- Dissipative two-identical-particle systems: diffraction and interference
- Stochastic Bohmian and Scaled Trajectories
- Quantum Classical Transition for Mixed States: The Scaled Von Neumann Equation
- Different routes to the classical limit of backflow
- Quantum surface diffusion in Bohmian Mechanics
- Scaled quantum theory. The bouncing ball problem
- Momentum-space decoherence of distinguishable and identical particles in the Caldeira-Leggett formalism
- Identical damped harmonic oscillators described by coherent states