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Chaos Solitons & Fractals

Dissipative behaviour and the interface between quantum and classical dynamical systems

A.M. Kowalski, Angel Ricardo Plastino, Araceli N. Proto

Published Jan 1, 1995• 0 citations
Publisher
DOI
10.1016/0960-0779(95)80032-c

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One way to look for complex behaviours in many‐body quantum systems is to let the number N of degrees of freedom become large and focus upon collective observables. Mean‐field quantities scaling as tend to commute, whence complexity at the quantum level can only be inherited from complexity at the classical level. Instead, fluctuations of microscopic observables scale as and exhibit collective Bosonic features, typical of a mesoscopic regime half‐way between the quantum one at the microscopic level and the classical one at the level of macroscopic averages. Here, we consider the mesoscopic behaviour emerging from an infinite quantum spin chain undergoing a microscopic dissipative, irreversible dynamics and from global states without long‐range correlations and invariant under lattice translations and dynamics. We show that, from the fluctuations of one site spin observables whose linear span is mapped into itself by the dynamics, there emerge bosonic operators obeying a mesoscopic dissipative dynamics mapping Gaussian states into Gaussian states. Instead of just depleting quantum correlations because of decoherence effects, these maps can generate entanglement at the collective, mesoscopic level, a phenomenon with no classical analogue that embodies a peculiar complex behaviour at the interface between micro and macro regimes.
This paper shows how classical transport dynamics arise naturally from the same variational dissipative–conservative framework that also supports quantum-analogue behaviour. In the transport-dominated regime, the oscillatory field reduces to Hamilton–Jacobi dynamics with well-defined trajectories and effective inertia, while coupling to auxiliary dissipative degrees of freedom suppresses interference and stabilises classical motion. No stochastic noise, no collapse postulates, and no hidden variables are introduced. Quantum, classical, and decoherent behaviour appear as distinct dynamical regimes of a single deterministic system, controlled by the balance between phase transport and amplitude curvature. Classical mechanics is recovered not as a foundational axiom, but as an effective description with a clear domain of validity.
The non-equilibrium dynamics of the critical behaviour of the Boson system undergoing the second order quantum phase transition is discussed. The analysis is carried out using the Keldysh technique of the non-equilibrium dynamics description. The critical behaviour close to the quantum critical point has been shown to be multi-critical. Crossover among three different critical regimes (modes) is possible: adiabatic quantum mode (AQM), dissipative classical mode (classical critical dynamics mode (CCDM) and dissipative quantum critical mode (QCDM). As a result, the observed critical behavior can essentially depend on the conditions of approaching the critical point.