Oxford, UK, 3-6 April 2017
Open Calls for Papers
- Published on Thursday, 29 September 2016 14:32
This EPJ B Topical Issue aims to highlight the versatility and wide range of achievements of the continuous-time random walk (CTRW) formalism on the occasion of its fiftieth anniversary.
Deadline for submission: 31 May 2017
List of confirmed authors
Eli Barkai (Bar-Ilan University)
Stas Burov (Bar-Ilan University)
The concept of continuous-time random walk is generalized into the quantum approach using a completely positive map. This approach introduces in a phenomenological way the concept of disorder in the transport problem of a quantum open system. If the waiting-time of the continuous-time Renewal approach is exponential we recover a semigroup for a dissipative quantum walk. Two models of non-Markovian evolution have been solved considering different types of disorder.
Aleksei Chechkin (National Academy of Sciences of Ukraine, Kiev)
Sergey Denisov (Universität Augsburg)
Marco Dentz (Center for Strategic and International Studies, Washington)
Bartlomiej Dybiec (Jagiellonian University)
Sergei Fedotov (The University of Manchester)
Katarzyna Górska (Institute of Nuclear Physics, Polish Academy of Sciences, Kraków)
The linear Boltzmann equation approach is generalized to describe fractional superdiffusive transport of the Levy walk type in arbitrary force fields. The time distribution between scattering events is assumed to have a mean value and infinite variance. It is completely characterized by two intermittent scattering rates, one normal and one fractional. Because the mean time between scattering events can be made arbitrary small, the retardation effects can be neglected, like in the standard linear Boltzmann equation. We formulate a general fractional linear Boltzmann equation approach, and exemplify it with a particularly simple case having the Bohm and Gross scattering integral. Here, at each scattering event the particle velocity is completely randomized and takes a value from equilibrium Maxwell distribution at a given finite temperature. We argue that this novel fractional kinetic equation provides a viable alternative to the fractional Kramers equation by Silbey and Barkai based on the picture of divergent mean time between scattering events. The range of applications is discussed.
A novel version of the Continuous-Time Random Walk (CTRW) model with memory is developed. This memory means the dependence between arbitrary number of successive jumps of the process, while waiting times between jumps are considered as i.i.d. random variables. The dependence was found by analysis of empirical histograms for the stochastic process of a single share price on a market within the high frequency time scale, and justified theoretically by considering bid-ask bounce mechanism containing some delay characteristic for any double-auction market. Our model turns out to be exactly analytically solvable, which enables a direct comparison of its predictions with their empirical counterparts, for instance, with empirical velocity autocorrelation function. Thus this paper significantly extends the capabilities of the CTRW formalism. (https://arxiv.org/abs/1305.6797)
Reiner Klages (Queen Mary, University of London)
Diego Krapf (Colorado State University)
Katja Lindeberg (University of California, San Diego)
Marcin Magdziarz (Wrocław University of Technology)
Francesco Mainardi (Università di Bologna)
Ralf Metzler (Universität Potsdam)
Miquel Montereo (Universitat de Barcelona)
Takashi Odagaki (CEO, Research Institute for Science Education, Inc., Japan)
Enrico Scalas (University of Sussex)
Harvey Scher (Weizmann Institute of Science)
The Continuous Time Random Walk (CTRW) was introduced by Montroll and Weiss in 1965 in a purely mathematical paper. Its antecedents and later applications beginning in 1973 are discussed, especially for the case of fractal time where the mean waiting time between jumps is infinite.
Using the fact that the continuous time random walk (CTRW) scheme is a random process subordinated to a simple random walk under the operational time given by the number of steps taken by the walker up to a given time, we revisit the problem of strongly dispersive transport in disordered media, which first lead Scher and Montroll to introducing the power law waiting time distributions. Using subordination approach allows for disentangling the complexity of the problem, separating the solution of the boundary value problem (which is solved on the level of normal diffusive transport) from the influence of the waiting times, which allows for the solution of the direct problem in the whole time domain (including short times, out of reach of the initial approach), and simplifying strongly the analysis of the inverse problem. The analysis of the last shows that the current traced do not contain information sufficient for unique restoration of the waiting time probability densities, but define a single-parametric family of functions, all leading to the same photocurrent forms. The members of the family have the power-law tails which differ only by a prefactor, but may look astonishingly different at their body. The same applies to the multiple trapping model, mathematically equivalent to a special the limiting case of CTRW.
The problem of 1/f noise has been with us for about a century. Because it is so often framed in Fourier spectral language, the most famous solutions have tended to be the stationary long range dependent (LRD) models such as Mandelbrot's fractional Gaussian noise. In view of the increasing importance to physics of non-ergodic fractional renewal models, I present preliminary results of my research into the history of Mandelbrot's very little known work in that area from 1963-67. I speculate about how the lack of awareness of this work in the physics and statistics communities may have affected the development of complexity science, and I discuss the differences between the Hurst effect, 1/f noise and LRD, concepts which are often treated as equivalent. See http://arxiv.org/abs/1603.00738
Vasily Zaburdaev (Max-Planck-Institute for the Physics of Complex Systems)