Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Foundations of Physics

On the Concept of Entropy for Quantum Decaying Systems

Osvaldo Civitarese, Manuel Gadella

Published Sep 27, 2013• 8 citations
Publisher
DOI
10.1007/s10701-013-9746-0

Related papers

Dynamical entropy for quantum systems

Göran Lindblad

Lecture notes in mathematics•Jan 1, 1988•9 citations

AN APPROXIMATION TO THE ENTROPY FOR QUANTUM DECAYING STATES

Osvaldo Civitarese, Manuel Gadella

The concept of entropy was initially defined for systems with thermodynamical equilibrium. We try to extend this notion for quantum non-relativistic decaying states. We use a technique based on path integration on coherent states in order to obtain an approximation to the entropy of a decaying state.

International Journal of Geometric Methods in Modern Physics•Apr 30, 2013•2 citations

The influence of quantization on the onset of chaos in Hamiltonian systems: The Kolmogorov entropy interpretation

Ronnie Kosloff, Stuart A. Rice

An extension of the concept of Kolmogorov entropy to quantum mechanical systems is given. Using the Kolmogorov entropy as a common basis for discussion, the onset of chaotic motion in classical mechanical and quantum mechanical systems is compared. It is found that if the spectrum of the system is discrete, the Kolmogorov entropy is zero, and therefore that a bounded quantum mechanical system cannot have chaotic motion like that observed for a corresponding classical mechanical system. This analysis leads to the prediction that if the distributions of states are similar for two bounded systems which in the classical limit have, respectively, quasiperiodic and chaotic motion, wave packets for the two systems decay at similar rates as found by Brumer and Shapiro. The relationship between the defined Kolmogorov entropy, previous interpretations of ’’KAMlike’’ onset of chaos in quantum mechanical systems, and the role played by preparation and observation of a system in influencing the intramolecular dynamics, are discussed.

The Journal of Chemical Physics•Jan 15, 1981•92 citations

NOTES ON QUANTUM ENTROPY

Makoto Ohya, D�nes Petz

WORLD SCIENTIFIC eBooks•Feb 1, 2008•2 citations

Entropy in quantum mechanics

Ugo Farinelli, A. Gamba

Il Nuovo Cimento•May 1, 1956•2 citations

Coherence theory and coherence phenomena in a closed spin 1/2 system

Dannenberg, O

We study a simplified Heisenberg spin model in order to clarify the idea of decoherence in closed quantum systems. For this purpose, we define a new concept: the coherence function $\\Xi(t)$, which describes the dynamics of coherence in the whole system, and which is linked with the total coarse-grained (von Neumann) entropy of all particles. We discuss in some detail a general coherence theory and its elementary results. For example, in the particular setup, decoherence diagonalises reduced density matrices in all possible basis sets. As expected, decoherence is understood as a statistical process that is caused by the dynamics of the system, similar to entropy. Moreover, the concept of decoherence time is applicable in closed systems. However, in most cases, the decay of off-diagonal elements differs from the usual $\\exp(-t/\\tau_d)$ behaviour. We have solved the form of decoherence time $\\tau_d$ in an infinite Heisenberg model with respect to density $\\rho$, spatial dimension $D$ and $\\epsilon$ in a $1/r^{\\epsilon}$ -type of potential.

•May 18, 2006•1 citation
An extension of the concept of Kolmogorov entropy to quantum mechanical systems is given. Using the Kolmogorov entropy as a common basis for discussion, the onset of chaotic motion in classical mechanical and quantum mechanical systems is compared. It is found that if the spectrum of the system is discrete, the Kolmogorov entropy is zero, and therefore that a bounded quantum mechanical system cannot have chaotic motion like that observed for a corresponding classical mechanical system. This analysis leads to the prediction that if the distributions of states are similar for two bounded systems which in the classical limit have, respectively, quasiperiodic and chaotic motion, wave packets for the two systems decay at similar rates as found by Brumer and Shapiro. The relationship between the defined Kolmogorov entropy, previous interpretations of ’’KAMlike’’ onset of chaos in quantum mechanical systems, and the role played by preparation and observation of a system in influencing the intramolecular dynamics, are discussed.
We study a simplified Heisenberg spin model in order to clarify the idea of decoherence in closed quantum systems. For this purpose, we define a new concept: the coherence function Xi(t)\\Xi(t)Xi(t), which describes the dynamics of coherence in the whole system, and which is linked with the total coarse-grained (von Neumann) entropy of all particles. We discuss in some detail a general coherence theory and its elementary results. For example, in the particular setup, decoherence diagonalises reduced density matrices in all possible basis sets. As expected, decoherence is understood as a statistical process that is caused by the dynamics of the system, similar to entropy. Moreover, the concept of decoherence time is applicable in closed systems. However, in most cases, the decay of off-diagonal elements differs from the usual exp(−t/taud)\\exp(-t/\\tau_d)exp(−t/taud​) behaviour. We have solved the form of decoherence time taud\\tau_dtaud​ in an infinite Heisenberg model with respect to density rho\\rhorho, spatial dimension DDD and epsilon\\epsilonepsilon in a 1/repsilon1/r^{\\epsilon}1/repsilon -type of potential.