In this paper we give explicit examples of long-range correlated stationary Markovian processes y(t) where the stationary probability density function (pdf) shows tails which are Gaussian or exponential. These processes are obtained by simply performing appropriate coordinate transformations of a specific power-law correlated additive process x(t) , already known in the literature, whose pdf shows power-law tails. We give analytical and numerical evidences that although the new processes are Markovian and have Gaussian or exponential tails, their autocorrelation function shows a power-law decay with logarithmic corrections. For a generic continuous and monotonously increasing coordinate transformation, we also analytically investigate what is the relationship between the asymptotic decay of the autocorrelation function and the tails of the stationary pdf. Extreme events seem to be associated to long-range correlated processes with power-law decaying autocorrelation function. However, the occurrence of extreme events is not necessary in order to have more general long-range correlated processes in which the autocorrelation shows a slow decay characterized by a power-law times a correction function such as the logarithm. Our results help in clarifying that even in the context of stationary Markovian processes long-range dependencies are not necessarily associated to the occurrence of extreme events. Moreover, our results can be relevant in the modeling of complex systems with long memory. In fact, we provide simple stationary processes associated to Langevin equations with white noise thus confirming that long-memory effects can be modeled in the context of continuous time stationary Markovian processes.
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http://dx.doi.org/10.1103/PhysRevE.79.031116 | DOI Listing |
Entropy (Basel)
November 2024
Department of Physics and Astronomy and London Centre for Nanotechnology, University College London, Gower Street, London WC1E 6BT, UK.
The reduced density matrix that characterises the state of an open quantum system is a projection from the full density matrix of the quantum system and its environment, and there are many full density matrices consistent with a given reduced version. Without a specification of relevant details of the environment, the time evolution of a reduced density matrix is therefore typically unpredictable, even if the dynamics of the full density matrix are deterministic. With this in mind, we investigate a two-level open quantum system using a framework of quantum state diffusion.
View Article and Find Full Text PDFHeliyon
July 2024
Department of Mathematics, School of Advanced Sciences, Vellore Institute of Technology, Vellore - 632014, Tamilnadu, India.
The present study delves into the dynamics of a specific form of queueing system described as an retrial queue. Here, the queue comprises two distinct categories of clients: transit clients and recurrent clients. Transit clients are those who appear at the queue following a Poisson process, reflecting a random arrival pattern commonly seen in queueing scenarios.
View Article and Find Full Text PDFPhys Rev E
October 2024
Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem 91904, Israel.
Sci Rep
October 2024
Faculty of Physics, Urmia University of Technology, Urmia, Iran.
Ergotropy, which represents the maximum amount of work that can be extracted from a quantum system, has become a focal point of interest in the fields of quantum thermodynamics and information processing. In practical scenarios, the interaction of quantum systems with their surrounding environment is unavoidable. Recent studies have increasingly focused on analyzing open quantum systems affected by non-stationary environmental fluctuations due to their significant impact on various physical scenarios.
View Article and Find Full Text PDFJ Chem Phys
October 2024
H. H. Wills Physics Laboratory, University of Bristol, Bristol BS8 1TL, United Kingdom.
The most general description of quantum evolution up to a time τ is a completely positive tracing preserving map known as a dynamical mapΛ̂(τ). Here, we consider Λ̂(τ) arising from suddenly coupling a system to one or more thermal baths with a strength that is neither weak nor strong. Given no clear separation of characteristic system/bath time scales, Λ̂(τ) is generically expected to be non-Markovian; however, we do assume the ensuing dynamics has a unique steady state, implying the baths possess a finite memory time τm.
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