We investigate the mean-square displacement (MSD) for random motion governed by the generalized Langevin equation for memory functions that contain two different time scales: In the first model, the memory kernel consists of a delta peak and a single-exponential and in the second model of the sum of two exponentials. In particular, we investigate the scenario where the long-time exponential kernel contribution is negative. The competition between positive and negative friction memory contributions produces an enhanced transient persistent regime in the MSD, which is relevant for biological motility and active matter systems
Abstract. Passive microrheology [12] utilizes measurements of noisy, entropic fluctuations (i.e., di...
To be published in Physical Review EThe over-passing probability across an inverted parabolic potent...
We show that the first order Langevin equation for the overdamped dynamics of an interacting system ...
We investigate the mean-square displacement (MSD) for random motion governed by the generalized Lang...
We study the dynamics of a particle in a fluid from a generalized Langevin equation (GLE) with a fri...
A generalized Langevin equation with fluctuating diffusivity (GLEFD) is proposed, and it is shown th...
We study the motion of a particle governed by a generalized Langevin equation. We show that, when no...
The memory kernel for a tagged particle in a fluid, computed from molecular dynamics simulations, de...
Any first course on polymer physics teaches that the dynamics of a tagged monomer of a polymer is an...
We show that for particles performing Brownian motion in a frozen array of scatterers long-time corr...
We propose a generalization of the widely used fractional Brownian motion (FBM), memory-multi-FBM (M...
International audienceStrong interaction with other particles or feedback from the medium on a Brown...
Generating an initial condition for a Langevin equation with memory is a non trivial issue. We intro...
Generating an initial condition for a Langevin equation with memory is a non trivial issue.We introd...
A number of random processes in various fields of science is described by phenomenological equations...
Abstract. Passive microrheology [12] utilizes measurements of noisy, entropic fluctuations (i.e., di...
To be published in Physical Review EThe over-passing probability across an inverted parabolic potent...
We show that the first order Langevin equation for the overdamped dynamics of an interacting system ...
We investigate the mean-square displacement (MSD) for random motion governed by the generalized Lang...
We study the dynamics of a particle in a fluid from a generalized Langevin equation (GLE) with a fri...
A generalized Langevin equation with fluctuating diffusivity (GLEFD) is proposed, and it is shown th...
We study the motion of a particle governed by a generalized Langevin equation. We show that, when no...
The memory kernel for a tagged particle in a fluid, computed from molecular dynamics simulations, de...
Any first course on polymer physics teaches that the dynamics of a tagged monomer of a polymer is an...
We show that for particles performing Brownian motion in a frozen array of scatterers long-time corr...
We propose a generalization of the widely used fractional Brownian motion (FBM), memory-multi-FBM (M...
International audienceStrong interaction with other particles or feedback from the medium on a Brown...
Generating an initial condition for a Langevin equation with memory is a non trivial issue. We intro...
Generating an initial condition for a Langevin equation with memory is a non trivial issue.We introd...
A number of random processes in various fields of science is described by phenomenological equations...
Abstract. Passive microrheology [12] utilizes measurements of noisy, entropic fluctuations (i.e., di...
To be published in Physical Review EThe over-passing probability across an inverted parabolic potent...
We show that the first order Langevin equation for the overdamped dynamics of an interacting system ...