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Intrinsic Randomness and Intrinsic Irreversibility in Classical Dynamical Systems

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TLDR
This work believes that its formulation permits a microscopic formulation of the second law of thermodynamics for well-defined classes of dynamical systems.
Abstract
We continue our previous work on dynamic “intrinsically random” systems for which we can derive dissipative Markov processes through a one-to-one change of representation. For these systems, the unitary group of evolution can be transformed in this way into two distinct Markov processes leading to equilibrium for either t→ + ∞ or t→ - ∞. To lift the degeneracy, we first formulate the second principle as a selection rule that is meaningful in intrinsically random systems. For these systems, this excludes a set of unrealizable states. As a result of this exclusion, permitted initial conditions correspond to a set of states that is not invariant through velocity inversion. In this way, the time-reversal symmetry of dynamics is broken and these systems acquire a new feature we may call “intrinsic irreversibility.” The set of admitted initial conditions can be characterized by an entropy displaying the amount of information necessary for their preparation. The initial conditions selected by the second law correspond to a finite amount of information, while the initial conditions that are rejected correspond to an infinite amount of information and are therefore “impossible.” We believe that our formulation permits a microscopic formulation of the second law of thermodynamics for well-defined classes of dynamical systems.

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Nonlinear quantum evolution equations to model irreversible adiabatic relaxation with maximal entropy production and other nonunitary processes

TL;DR: In this paper, a geometrical construction of the maximum entropy production/steepest-entropy-ascent nonlinear evolution equation for adiabatic systems is presented, where each component particle contributes an independent local tendency along the direction of steepest increase of the locally perceived entropy.
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Nonequilibrium statistical mechanics Brussels–Austin style

TL;DR: In this paper, the Brussels-Austin Group considered the observed direction of time to be a basic physical phenomenon due to the dynamics of physical systems and used rigged Hilbert space (whereas the older approaches used Hilbert space).
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How can quantum mechanics of material evolution be possible? Symmetry and symmetry-breaking in protobiological evolution.

TL;DR: In this article, the symmetry-breaking of the Hamiltonian in the interaction with the exterior through material flow has been observed in the evolution of a material system which is highly symmetrical and highly degenerate in its internal states.
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The second law as a selection principle: The microscopic theory of dissipative processes in quantum systems

TL;DR: The superposition principle of quantum mechanics has to be reconsidered as irreversible processes transform pure states into mixtures and unitary transformations are limited by the requirement that entropy remains invariant.
Journal ArticleDOI

Irreversibility and nonlocality

TL;DR: In this article, the second law of thermodynamics when formulated as a dynamical principle implies a departure from locality, and an extension of the theory to singular distribution functions is discussed.
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