37 research outputs found
Langevin analysis for time-nonlocal Brownian motion with algebraic memories and delay interactions
Starting from a Langevin equation with memory describing the attraction of a particle to
a center, we investigate its transport and response properties corresponding to two
special forms of the memory: one is algebraic, i.e., power-law, and the other involves a
delay. We examine the properties of the Green function of the Langevin equation and
encounter Mittag-Leffler and Lambert W-functions well-known in the literature. In the
presence of white noise, we study two experimental situations, one involving the motional
narrowing of spectral lines and the other the steady-state size of the particle under
consideration. By comparing the results to counterparts for a simple exponential memory,
we uncover instructive similarities and differences. Perhaps surprisingly, we find that
the Balescu-Swenson theorem that states that non-Markoffian equations do not add anything
new to the description of steady-state or equilibrium
observables is violated for our system in that the saturation size of the
particle in the steady-state depends on the memory function utilized. A natural
generalization of the Smoluchowski equation for the time-local case is examined and found
to satisfy the Balescu-Swenson theorem and describe accurately the first moment but not
the second and higher moments. We also calculate two-time correlation functions for all
three cases of the memory, and show how they differ from (tend to) their Markoffian
counterparts at small (large) values of the difference between the two times
Langevin analysis for time-nonlocal Brownian motion with algebraic memories and delay interactions
Starting from a Langevin equation with memory describing the attraction of a particle to
a center, we investigate its transport and response properties corresponding to two
special forms of the memory: one is algebraic, i.e., power-law, and the other involves a
delay. We examine the properties of the Green function of the Langevin equation and
encounter Mittag-Leffler and Lambert W-functions well-known in the literature. In the
presence of white noise, we study two experimental situations, one involving the motional
narrowing of spectral lines and the other the steady-state size of the particle under
consideration. By comparing the results to counterparts for a simple exponential memory,
we uncover instructive similarities and differences. Perhaps surprisingly, we find that
the Balescu-Swenson theorem that states that non-Markoffian equations do not add anything
new to the description of steady-state or equilibrium
observables is violated for our system in that the saturation size of the
particle in the steady-state depends on the memory function utilized. A natural
generalization of the Smoluchowski equation for the time-local case is examined and found
to satisfy the Balescu-Swenson theorem and describe accurately the first moment but not
the second and higher moments. We also calculate two-time correlation functions for all
three cases of the memory, and show how they differ from (tend to) their Markoffian
counterparts at small (large) values of the difference between the two times
Quantum dynamics in strong fluctuating fields
A large number of multifaceted quantum transport processes in molecular
systems and physical nanosystems can be treated in terms of quantum relaxation
processes which couple to one or several fluctuating environments. A thermal
equilibrium environment can conveniently be modelled by a thermal bath of
harmonic oscillators. An archetype situation provides a two-state dissipative
quantum dynamics, commonly known under the label of a spin-boson dynamics. An
interesting and nontrivial physical situation emerges, however, when the
quantum dynamics evolves far away from thermal equilibrium. This occurs, for
example, when a charge transferring medium possesses nonequilibrium degrees of
freedom, or when a strong time-dependent control field is applied externally.
Accordingly, certain parameters of underlying quantum subsystem acquire
stochastic character. Herein, we review the general theoretical framework which
is based on the method of projector operators, yielding the quantum master
equations for systems that are exposed to strong external fields. This allows
one to investigate on a common basis the influence of nonequilibrium
fluctuations and periodic electrical fields on quantum transport processes.
Most importantly, such strong fluctuating fields induce a whole variety of
nonlinear and nonequilibrium phenomena. A characteristic feature of such
dynamics is the absence of thermal (quantum) detailed balance.Comment: review article, Advances in Physics (2005), in pres
Confining Domains Lead to Reaction Bursts: Reaction Kinetics in the Plasma Membrane
Confinement of molecules in specific small volumes and areas within a cell is likely to be a general strategy that is developed during evolution for regulating the interactions and functions of biomolecules. The cellular plasma membrane, which is the outermost membrane that surrounds the entire cell, was considered to be a continuous two-dimensional liquid, but it is becoming clear that it consists of numerous nano-meso-scale domains with various lifetimes, such as raft domains and cytoskeleton-induced compartments, and membrane molecules are dynamically trapped in these domains. In this article, we give a theoretical account on the effects of molecular confinement on reversible bimolecular reactions in a partitioned surface such as the plasma membrane. By performing simulations based on a lattice-based model of diffusion and reaction, we found that in the presence of membrane partitioning, bimolecular reactions that occur in each compartment proceed in bursts during which the reaction rate is sharply and briefly increased even though the asymptotic reaction rate remains the same. We characterized the time between reaction bursts and the burst amplitude as a function of the model parameters, and discussed the biological significance of the reaction bursts in the presence of strong inhibitor activity
