The fundamental aspect of measurement, that a measurement always results in a record, is analysed. Recording implies irreversibility and entropy production in the combined system of instrument and object. In elementary particle physics the record itself is all important, and therefore the entropy production due to measurement, hitherto neglected in fundamental theories, is essential. The conjecture is advanced that, just as in relativity the signal is of prime importance and in quantum theory the measuring interaction is fundamental, this (third) aspect of measurement will play a central role in a new fundamental theory of elementary particles. Some basic notions of this new theory are proposed. The stable particle, for example, can be conceived of as a steady state of an open system, characterized by minimal entropy production. Finally the meaning of irreversibility on the micro-level of elementary particles is discussed.
The fundamental aspect of measurement, that a measurement always results in a record, is analysed. Recording implies irreversibility and entropy production in the combined system of instrument and object. In elementary particle physics the record itself is all important, and therefore the entropy production due to measurement, hitherto neglected in fundamental theories, is essential. The conjecture is advanced that, just as in relativity the signal is of prime importance and in quantum theory the measuring interaction is fundamental, this (third) aspect of measurement will play a central role in a new fundamental theory of elementary particles. Some basic notions of this new theory are proposed. The stable particle, for example, can be conceived of as a steady state of an open system, characterized by minimal entropy production. Finally the meaning of irreversibility on the micro-level of elementary particles is discussed.
Within the general formalism of quantum theory irreversibility and the arrow of time and the in the evolution of various physical systems are studied. Irreversible behavior often manifests itself in the guise of “entropy production.” This motivates me to begin this chapter with a brief review of quantum-mechanical entropy, a subject that Elliott Lieb has made outstanding contributions to, followed by an enumeration of examples of irreversible behavior and of an arrow of time analyzed in later sections. Subsequently, a derivation of the laws of thermodynamics from (quantum) statistical mechanics, and, in particular, of the Second Law of thermodynamics, in the forms given to it by Clausius and Carnot, is presented. In a third part, results on diffusive (Brownian) motion of a quantum particle interacting with a quasi-free quantum-mechanical heat bath are reviewed. This is followed by an outline of a theory of friction by emission of Cherenkov radiation of sound waves in a system consisting of a particle moving through a Bose–Einstein condensate and interacting with it. In what may be the most important section of this chapter, the fundamental arrow of time inherent in Quantum Mechanics is discussed.
Abstract We consider the temporal evolution of an isolated system of N particles from a non-equilibrium state of entropy S = S′ to the equilibrium state of maximum entropy, S = S max, S′ ≤ S max. The application of usual density matrix theory to the temporal development of S leads us to dS/dt = 0: The entropy S does not change in time t. Thereby it is irrelevant, whether we consider a non-equilibrium state or an equilibrium state. Consequently, the system cannot irreversibly change by entropy production dS/dt > 0 from S′ to S max. This is a paradoxial result, which contradicts the experience. It can be traced back to the von Neumann equation, which in principle describes reversible processes and hence is unsuitable for calculating the irreversible evolution of the entropy S in time t. Each irreversible process is accompanied by a positive entropy production P = dS/dt ≥ 0 inside the system, which only vanishes in case of the equilibrium state. In order to overcome the above mentioned difficulties, we assign an operator P to the entropy production P, which is defined by the eigenvalue equation P |u〉 = P|u〉 with the state vector |u〉 of the N-particle system. There was an extensive discussion about the relation between the production of entropy P on one hand and the progression of time t on the other. Making use of this concept, we combine the operator of entropy production P with the time-development operator U (t, t 0) of the system and finally deduce the infinitesimal unitary operator U (t+τ,t) = 1 + (i/k)τ P by means of very general assumptions. Here P means the generator of the infinitesimal progression of time τ = t − t 0 and k the Boltzmann constant, representing the atomic entropy unit. Similarly to P we also treat the time t as an observable, defined by t |u〉 = t|u〉. We apply the infinitesimal time-evolution operator U (t+τ,t) to the operator of time t and finally obtain the P – t commutation relation i[ P , t ] = k, which is independent of τ. It shows that the operators P and t do not commute, and hence P and t are not sharply defined simultaneously. Instead we have uncertainties ΔP and Δt on measuring P and t, which are given by the P–t uncertainty relation ΔPΔt ≥ k/2. It readily allows a discussion of the evolution of the entropy S of the isolated system in time t from S′ to S max. Now, the irreversible steps are correctly described by the entropy production P = dS/dt > 0, while the thermal equilibrium is given by P = 0, ΔP = 0, and thus the lifetime of the equilibrium state Δt = ∞. According to the P–t uncertainty relation, the Boltzmann constant k is similarly important to the quantum thermodynamics of irreversible processes like Planck′s constant h to usual quantum mechanics.
In view of the fact that physical measurements represent transmission of information, a general definition based on the measure of lack of knowledge in information theory can be introduced for different entropies each of them corresponding to one particular kind of measurement. By means of this entropy concept the problem of the consistency of microscopic reversibility and maeroscopic irreversibility is studied. Under certain conditions it can be shown that the reversible microscopic equation of motion leads to the result that all entropies corresponding to reduced quantities, i.e., to quantities which do not determine the microscopic state of the system completely, can never decrease. However, it is to be noted that this behavior is symmetric in time, in the classical as well as in the quantum mechanical case. Irreversibility is so related on the one hand to incomplete description of a system, but on the other also to the fact that theoretical statements can be verified by experiments in the future only. The validity of the results obtained within the framework of ensemble theory for a single physical system is dtscussed. As applications of the general ideas a system of free particles and the Boltzmann gas are treated. (auth)
Decoherence theory explains the suppression of interference between branches of a quantum state but does not explain why any particular branch persists as a stable classical history under continued environmental interaction. This unresolved gap lies at the core of the quantum measurement problem. Here we demonstrate that irreversible record formation is a necessary structural condition for the stabilization of quantum histories. Using a minimal open quantum system consisting of a measured qubit coupled to a memory degree of freedom, we show that decoherence alone fails to produce persistent measurement records in the presence of ongoing noise. By contrast, when the memory subsystem is allowed to irreversibly export entropy, stable and distinguishable records emerge robustly. We introduce an operational recordability metric based on the trace-distance distinguishability of conditional memory states and observe a pronounced transition between recordable and non-recordable regimes. These results establish that measurement outcomes do not become classical merely by decohering; they become classical only when they are irreversibly maintained. This mechanism resolves a structural incompleteness in decoherence-based accounts of measurement without invoking wavefunction collapse, observers, or interpretational postulates. Keywords: quantum measurement problem, decoherence, irreversible record formation, open quantum systems, Lindblad dynamics, classical emergence, quantum histories, record stabilization, entropy export, measurement records, trace distance, quantum information, environment-induced decoherence, thermodynamic irreversibility
The microscopic theory of irreversible processes that we developed is summarized and illustrated, using as a simple example the Friedrichs model. Our approach combines the Poincaré's point of view (dynamical interpretation of irreversibility) with the Gibbs-Einstein ensemble point of view. It essentially consists in a nonunitary transformation theory based on the symmetry properties of the Liouville equation and dealing with continuous spectrum. The second law acquires a microscopic content in terms of a Liapounov function which is a quadratic functional of the density operator. In our new representation of dynamics, which is defined for a restricted set of observables and states, this functional takes a universal form. We obtain, in this way, a semi-group description, the generator of which contains a part directly related to the microscopic entropy production. The Friedrichs model gives us a simple field theoretical example for which the entropy production can be evaluated. The thermodynamical meaning of life-times is explicitly displayed. The transition from pure states to mixtures, as well as the occurrence of long tails in thermodynamic systems, are also briefly discussed.
Many-particle systems play a fundamental role in physics where we encounter systems of molecules or systems of elementary particles in quantum field theory. Many-particle theories provide the basis for understanding the macroscopic behaviour of vast assemblies of interacting particles starting from their microscopic properties and leads to descriptions of entropy, statistical mechanics and fluid mechanics. Covering a wide range of topics and including more than 400 problems and solutions, this book is an ideal resource for students specialising in many-particle systems. Key features • Several hundred problems with solutions in each volume. • Problems range from basic introductory to advanced level. • Features worked examples as well as solutions to many problems. • Includes key concepts. • Covers essential complete physics course.