Anomalous diffusion in coupled viscoelastic media: A fractional Langevin equation approach
arXiv:2507.08291 · doi:10.1103/thv9-s9mq
Abstract
Anomalous diffusion often arises in complex environments where viscoelastic or crowded conditions influence particle motion. In many biological and soft-matter systems, distinct components of the medium exhibit unique viscoelastic responses, resulting in time-dependent changes in the observed diffusion exponents. Here, we develop a theoretical model of two particles, each embedded in a distinct viscoelastic medium, and coupled via a harmonic potential. By formulating and solving a system of coupled fractional Langevin equations (FLEs) with memory exponents , we uncover rich transient anomalous diffusion phenomena arising from the interplay of memory kernels and bilinear coupling. Notably, we identify recovery dynamics, where a subdiffusive particle () transiently accelerates and eventually regains its intrinsic long-time mobility. This recovery emerges only when memory exponents differ (), whereas identical exponents () suppress recovery. Our theoretical predictions offer insight into experimentally observed transient anomalous diffusions, such as polymer--protein complexes and cross-linked cytoskeletal networks, highlighting the critical role of memory heterogeneity and mechanical interactions in biological anomalous diffusion.
References in corpus (9)
- Why the Mittag-Leffler function can be considered the Queen function of the Fractional Calculus?
- Anomalous Polymer Dynamics Is Non-Markovian: Memory Effects and The Generalized Langevin Equation Formulation
- Generalized Elastic Model yields Fractional Langevin Equation
- Intracellular microrheology of motile Amoeba proteus
- On the generalized Langevin equation for a Rouse bead in a nonequilibrium bath
- Single cell visualization of transcription kinetics variance of highly mobile identical genes using 3D nanoimaging
- Diffusion of intrinsically disordered proteins within viscoelastic membraneless droplets
- Nonequilibrium diffusion of active particles bound to a semi-flexible polymer network: simulations and fractional Langevin equation
- Hyperphosphorylation-Induced Phase Transition in Vesicle Delivery Dynamics of Motor Proteins in Neuronal Cells