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Physical Review Letters

New model for dissipation in quantum mechanics

A. H. Castro Neto, A. O. Caldeira

Published Oct 7, 1991• 37 citations
Publisher

Abstract

We propose a new model for studying dissipation in quantum-mechanical systems. The mechanism of dissipation is solely due to the scattering of the environment excitations by the particle of interest. We treat the problem via the functional integral formalism. It is shown that the model gives a damping parameter which is temperature dependent.

DOI
10.1103/physrevlett.67.1960

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We propose a new model for studying dissipation in quantum-mechanical systems. The mechanism of dissipation is solely due to the scattering of the environment excitations by the particle of interest. We treat the problem via the functional integral formalism. It is shown that the model gives a damping parameter which is temperature dependent.
The usual treatment of damping forces in quantum mechanics starts from the introduction of the explicitly time dependent Kanai Hamiltonian, which actually represents a variable mass particle, and the misinterpretation of this Hamiltonian as representing a particle of constant mass leads to certain physical difficulties. However the Hamiltonian can be modified so that it can be reinterpreted as describing a constant mass particle. Here we explicitly introduce the mass as a new dynamical variable, which allows us to write a linear, time independent Hamiltonian for the system, which can be solved by conventional methods. The damped harmonic oscillator and damped free particle are treated in detail, both for the Kanai Hamiltonian and for our case, and the solutions are compared. Our solution can be reduced to the Kanai one in appropriate circumstances, but in general it has a much greater versatility, as a result of which it can be more easily reinterpreted as describing a constant mass particle subject to a damping force, which reinterpretation is of course necessary if the method is to have practical applicability. We also show how such a reinterpretation can be carried out in detail by introducing a ’’dissipation variable’’, in terms of which one may avoid the concept of a variable mass altogether.
Phenomenological Equations of Motion for Dissipative Systems Lagrangian Hamiltonian and Hamilton-Jacobi Formulation of the Classical Dissipative Systems Noether's Theorem and Non-Noether Conservation Laws Dissipative Forces Derived from Many-Body Problems A Particle Coupled to a Field and the Damped Motion of a Central Particle Coupled to a Heat Bath Quantization of Dissipative Systems in General and of Explicitly Time-Dependent Hamiltonians in Particular Density Matrix and the Wigner Distribution Function for Damped Systems Path Integral Formulation of a Damped Harmonic Oscillator Quantization of the Motion of an Infinite Chain Heisenberg's Equations of Motion for a Particle Coupled to a Heat Bath Quantum Mechanical Models of Dissipative Systems and the Concept of Optical Potential.
A new minimal coupling method is introduced. A general dissipative quantum system is investigated consistently and systematically. Some coupling functions describing the interaction between the system and the environment are introduced. Based on coupling functions, some susceptibility functions are attributed to the environment explecitly. Transition probabilities relating the way energy flows from the system to the environment are calculated and the energy conservation is explecitly examined. This new formalism is generalized to the dissipative scalar and vector field theories along the ideas developed for the quantum dissipative systems
This paper presents a comprehensive model for quantum decoherence, grounded in the principles of quantum field theory (QFT) and statistical mechanics. The core argument is that traditional decoherence models often oversimplify the process, failing to adequately capture the intricate interactions arising from the quantum effects of the surrounding environment. This work introduces a framework that explicitly incorporates the scattering of quantum states by the environment, treated as a QFT system, and then analyzes the resultant impact using statistical mechanics. The model aims to provide a more accurate and nuanced understanding of decoherence, particularly in scenarios involving strong environmental interactions. Specifically, the model utilizes the formalism of quantum scattering theory to describe the interaction between a quantum system and its environment. The resulting dynamics are then analyzed using the framework of statistical mechanics, allowing for the calculation of decoherence rates as a function of environmental parameters such as temperature and density. The key contributions of this work include a detailed mathematical description of the decoherence process, a clear separation of the quantum and classical aspects of the problem, and a framework for extending the model to more complex systems. The model predicts that decoherence is not simply a loss of quantum information, but rather a fundamental process of state transformation driven by the statistical properties of the environment. This work offers a significant step forward in our ability to understand and potentially mitigate the effects of decoherence in quantum technologies.
It is difficult to incorporate the concept of interacting physical particles in the frame of conventional quantum mechanics. It comes from the fact that in this formalism the Hamiltonian plays a dual role as the generator of motion and as the observable associated with the energy. As a result it is easy to define either a representation in which particles interact but are not well defined (a representation in which the Hamiltonian is not diagonal) or a representation in which the units are well defined but do not interact. We expect that in the search for a representation in which we may speak of both well defined and still interacting particles, the distinction between reversible and irreversible processes should play a basic role. Certainly we do not want to eliminate irreversible processes such as scattering, production or decay which are basically related to the mechanisms through which we observe particles. To distinguish between reversible and irreversible processes we have to work in a representation such that a Liapounov function (the entropy) may be ascribed to the time evolution of the system. The introduction of such a representation through a specific class of non-unitary transforms is described. We then propose newmore » quantum rules directly applicable to dissipative systems with a Liapounov function. For systems with a discrete spectrum these new quantum rules reduce trivially to the usual quantum rules as formulated by Born, Jordan and Heisenberg. The theory is applied to a simple field theoretical model - the so-called Friedrichs model-for which all calculations can be performed exactly.« less
A new method to treat the energy dissipation into electron excitations by time-dependent local perturbations is presented. The probability P( epsilon ) for the electron system to be excited to a state epsilon is expressed in terms of new Green functions given by extending the Keldysh Green function formalism. As an example, the method is applied to the slowly varying noninteracting Wolff model at zero temperature. The Muskhelishvili technique, which has been used for X-ray problems, is used to solve the resulting integral equations of the Green functions. The results are identical to those given by a time-dependent Tomonagon approach and by solving directly the equation of motion for field operators.