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Physica Scripta

Quantum Hydrodynamic Analysis of Decoherence

Kyungsun Na, Róbert E. Wyatt

Published Jan 1, 2003• 12 citations
Publisher

Abstract

The hydrodynamic formulation of quantum mechanics is used to analyze the mechanism of decoherence for a system interacting with a bath in which the initial system wavefunction is a superposition of spatially separated components. In order to study the decoherence, the various time-evolving hydrodynamic fields are monitored for the two composite systems, each having a single bath mode. In one of these, the system and bath are uncoupled, but in the other they are coupled through an interaction term. For the uncoupled system, a large interference feature develops between the two separated components of the initial superposition. The reduced density matrix for the system initially displays two large off-diagonal peaks and as time proceeds, these peaks broaden but do not disappear. For the coupled system, the interference feature that attempts to form between the two initially separated wavepackets is largely suppressed. Although the quantum force again tends to push fluid elements toward the interference region, this is counteracted by the classical force, which attempts to separate the centers of the two wavepackets into two descending valleys. An essential feature of flux maps for this case is that in the mid-region between the two initial density peaks, an intersecting set of attractors and repellors for flux vectors form and these funnel density away from the central region. As time proceeds, the reduced density matrix for the system shows increasing concentration along the diagonal. The Wigner function for the system shows gradually decaying ripples lying between the two density maxima which themselves are separating with opposite momenta. Finally, at later times, the reduced density matrix for the system is very similar to that obtained from a mixture of independently evolving components.

DOI
10.1238/physica.regular.067a00169

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The hydrodynamic formulation of quantum mechanics is used to analyze the mechanism of decoherence for a system interacting with a bath in which the initial system wavefunction is a superposition of spatially separated components. In order to study the decoherence, the various time-evolving hydrodynamic fields are monitored for the two composite systems, each having a single bath mode. In one of these, the system and bath are uncoupled, but in the other they are coupled through an interaction term. For the uncoupled system, a large interference feature develops between the two separated components of the initial superposition. The reduced density matrix for the system initially displays two large off-diagonal peaks and as time proceeds, these peaks broaden but do not disappear. For the coupled system, the interference feature that attempts to form between the two initially separated wavepackets is largely suppressed. Although the quantum force again tends to push fluid elements toward the interference region, this is counteracted by the classical force, which attempts to separate the centers of the two wavepackets into two descending valleys. An essential feature of flux maps for this case is that in the mid-region between the two initial density peaks, an intersecting set of attractors and repellors for flux vectors form and these funnel density away from the central region. As time proceeds, the reduced density matrix for the system shows increasing concentration along the diagonal. The Wigner function for the system shows gradually decaying ripples lying between the two density maxima which themselves are separating with opposite momenta. Finally, at later times, the reduced density matrix for the system is very similar to that obtained from a mixture of independently evolving components.
The hydrodynamic formulation of quantum mechanics is used to analyze the mechanism of decoherence for a system interacting with a bath in which the initial system wavefunction is a superposition of spatially separated components. In order to study the decoherence, the various time-evolving hydrodynamic fields are monitored for the two composite systems, each having a single bath mode. In one of these, the system and bath are uncoupled, but in the other they are coupled through an interaction term. For the uncoupled system, a large interference feature develops between the two separated components of the initial superposition. The reduced density matrix for the system initially displays two large off-diagonal peaks and as time proceeds, these peaks broaden but do not disappear. For the coupled system, the interference feature that attempts to form between the two initially separated wavepackets is largely suppressed. Although the quantum force again tends to push fluid elements toward the interference region, this is counteracted by the classical force, which attempts to separate the centers of the two wavepackets into two descending valleys. An essential feature of flux maps for this case is that in the mid-region between the two initial density peaks, an intersecting set of attractors and repellors for flux vectors form and these funnel density away from the central region. As time proceeds, the reduced density matrix for the system shows increasing concentration along the diagonal. The Wigner function for the system shows gradually decaying ripples lying between the two density maxima which themselves are separating with opposite momenta. Finally, at later times, the reduced density matrix for the system is very similar to that obtained from a mixture of independently evolving components.
The hydrodynamic formulation of quantum mechanics is used to elucidate the mechanism for decoherence, the suppression of interference effects in a system evolving from an initial coherent superposition. Analysis of time-dependent trajectory ensembles, flux maps, and elements of the stress tensor for two composite systems, in one of which the system is uncoupled to the environment, leads to the decoherence mechanism. For the uncoupled case, the quantum force acting on the fluid elements directs flux toward an attractor where the interference feature arises. For the coupled case, the classical force acting on each fluid element counters the quantum force and leads to gradual separation of the components of the initial superposition. Concomitantly, fluid stress is relieved when flux vectors diverge from a repellor in the mid-region between the separating wavepackets, thus suppressing formation of the interference feature.
We study a formulation of quantum mechanics in which the central notion is that of a quantum-mechanical history---a sequence of events at a succession of times. The primary aim is to identify sets of ``decoherent'' (or ``consistent'') histories for the system. These are quantum-mechanical histories suffering negligible interference with each other, and, therefore, to which probabilities may be assigned. These histories may be found for a given system using the so-called decoherence functional. When the decoherence functional is exactly diagonal, probabilities may be assigned to the histories, and all probability sum rules are satisfied exactly. We propose a condition for approximate decoherence, and argue that it implies that most probability sum rules will be satisfied to approximately the same degree. We also derive an inequality bounding the size of the off-diagonal terms of the decoherence functional. We calculate the decoherence functional for some simple one-dimensional systems, with a variety of initial states. For these systems, we explore the extent to which decoherence is produced using two different types of coarse graining. The first type of coarse graining involves imprecise specification of the particle's position. The second involves coupling the particle to a thermal bath of harmonic oscillators and ignoring the details of the bath (the Caldeira-Leggett model). We argue that both types of coarse graining are necessary in general. We explicitly exhibit the degree of decoherence as a function of the temperature of the bath, and of the width to within which the particle's position is specified. We study the diagonal elements of the decoherence functional, representing the probabilities for the possible histories of the system. To the extent that the histories decohere, we show that the probability distributions are peaked about the classical histories of the system, with the distribution of their initial positions and momenta given by a smeared version of the Wigner function. We discuss this result in connection with earlier uses of the Wigner function in this context. We find that there is a certain amount of tension between the demands of decoherence and peaking about classical paths.
In recent years trajectory based methodologies have become increasingly popular for evaluating the time evolution of quantum systems. A revival of the de Broglie Bohm interpretation of quantum mechanics has spawned several such techniques for examining quantum dynamics from a hydrodynamic perspective. Using techniques similar to those found in computational fluid dynamics one can construct the wavefunction of a quantum system at any time from the trajectories of a discrete ensemble of hydrodynamic fluid elements (Bohm particles) which evolve according to non-classical equations of motion. Until very recently these schemes have been limited to closed systems. In this paper we present our methodology for including the effects of a thermal environment into the hydrodynamic formulation of quantum dynamics. We derive hydrodynamic equations of motion from the Caldeira-Leggett master equation for the reduced density matrix and give a brief overview of our computational scheme which incorporates an adaptive Lagrangian mesh. Our applications focus upon the dissipative dynamics of open unbounded quantum systems. Using both the Wigner phase space representation and the linear entropy we probe the breakdown of the Markov approximation of the bath dynamics at low temperatures. We suggest a criteria for rationalizing the validity of the Markov approximation in open unbound systems and discuss decoherence, energy relaxation, and quantum/classical correspondence in the context of the Bohmian paths.
In recent years trajectory based methodologies have become increasingly popular for evaluating the time evolution of quantum systems. A revival of the de Broglie--Bohm interpretation of quantum mechanics has spawned several such techniques for examining quantum dynamics from a hydrodynamic perspective. Using techniques similar to those found in computational fluid dynamics one can construct the wave function of a quantum system at any time from the trajectories of a discrete ensemble of hydrodynamic fluid elements (Bohm particles) which evolve according to nonclassical equations of motion. Until very recently these schemes have been limited to conservative systems. In this paper, we present our methodology for including the effects of a thermal environment into the hydrodynamic formulation of quantum dynamics. We derive hydrodynamic equations of motion from the Caldeira-Leggett master equation for the reduced density matrix and give a brief overview of our computational scheme that incorporates an adaptive Lagrangian mesh. Our applications focus upon the dissipative dynamics of open unbounded quantum systems. Using both the Wigner phase space representation and the linear entropy, we probe the breakdown of the Markov approximation of the bath dynamics at low temperatures. We suggest a criteria for rationalizing the validity of the Markov approximation in open unbound systems and discuss decoherence, energy relaxation, and quantum/classical correspondence in the context of the Bohmian paths.
Hydrodynamic reformulations of the Schrödinger equation suggest an interpretation of quantum mechanics in terms of a fluid flowing on configuration space. In the discrete hydrodynamic view, this fluid is not fundamental but emerges from many underlying microscopic fluid components whose collective behavior reproduces quantum phenomena. The most developed realization of this idea is the discrete many interacting worlds (MIW) framework, in which discrete particle-like worlds interact via inter-world forces and quantum probabilities are grounded in direct world counting. But there is also an older, continuous version of MIW. After reviewing the hydrodynamic and MIW formalisms, and emphasizing some of their interpretational advantages over the Everettian Many Worlds and Bohmian approaches, we argue that all discrete hydrodynamic models face a generic structural difficulty, which we call the problem of sparse ontology. Because wavefunctions typically branch under decoherence, the discrete components of the fluid are repeatedly partitioned into sub-ensembles, thereby thinning their density in configuration space and driving the dynamics away from the quantum regime once the components become sufficiently sparse. We conclude that successful hydrodynamic completions of quantum mechanics plausibly require an essentially continuous ontology.