Diffusion in spatially rough, confining, one-dimensional continuous energy landscapes is treated using Zwanzig's proposal, which is based on the Smoluchowski equation. We show that Zwanzig's conjecture agrees with Brownian dynamics simulations only in the regime of small roughness. Our correction of Zwanzig's framework corroborates well with numerical results. A numerical simulation scheme based on our coarse-grained Langevin dynamics offers significant reductions in computational time. The mean first-passage time problem in the case of random roughness is treated. Finally, we address the validity of the separation of length scales assumption for the case of polynomial backgrounds and cosine-based roughness. Our results are applicable to hi...
The propagation of gradient flow structures from microscopic to macroscopic models is a topic of hig...
Most methods for modelling dynamics posit just two time scales: a fast and a slow scale. But many ap...
Abstract. Non-interacting brownian particles follows Langevin equations fullfiling fluctuation–dissi...
Rugged energy landscapes find wide applications in diverse fields ranging from astrophysics to prote...
We consider the problem of an overdamped Brownian particle moving in multiscale potential with N + 1...
Diffusion in one dimensional rugged energy landscape (REL) is predicted to be pathologically differe...
AbstractThe potential energy profile for many complex reactions of proteins, such as folding or allo...
Diffusion-a measure of dynamics, and entropy-a measure of disorder in the system are found to be int...
Almost all processes in life are governed by proteins which are biomolecules consisting of a chain o...
In recent work, we have illustrated the construction of an exploration geometry on free energy surfa...
Non-interacting Brownian particles obey Langevin equations fulfilling a fluctuation–dissipation rela...
We introduce and analyze a model for the transport of particles or energy in extended lattice system...
Several years ago Zwanzig considered the diffusion in a potential that is spatially rough due to hie...
This thesis explores the effects of fluctuations and discreteness on the growth of physical systems ...
International audienceOwing to their complex morphology and surface, disordered nanoporous media pos...
The propagation of gradient flow structures from microscopic to macroscopic models is a topic of hig...
Most methods for modelling dynamics posit just two time scales: a fast and a slow scale. But many ap...
Abstract. Non-interacting brownian particles follows Langevin equations fullfiling fluctuation–dissi...
Rugged energy landscapes find wide applications in diverse fields ranging from astrophysics to prote...
We consider the problem of an overdamped Brownian particle moving in multiscale potential with N + 1...
Diffusion in one dimensional rugged energy landscape (REL) is predicted to be pathologically differe...
AbstractThe potential energy profile for many complex reactions of proteins, such as folding or allo...
Diffusion-a measure of dynamics, and entropy-a measure of disorder in the system are found to be int...
Almost all processes in life are governed by proteins which are biomolecules consisting of a chain o...
In recent work, we have illustrated the construction of an exploration geometry on free energy surfa...
Non-interacting Brownian particles obey Langevin equations fulfilling a fluctuation–dissipation rela...
We introduce and analyze a model for the transport of particles or energy in extended lattice system...
Several years ago Zwanzig considered the diffusion in a potential that is spatially rough due to hie...
This thesis explores the effects of fluctuations and discreteness on the growth of physical systems ...
International audienceOwing to their complex morphology and surface, disordered nanoporous media pos...
The propagation of gradient flow structures from microscopic to macroscopic models is a topic of hig...
Most methods for modelling dynamics posit just two time scales: a fast and a slow scale. But many ap...
Abstract. Non-interacting brownian particles follows Langevin equations fullfiling fluctuation–dissi...