2007
DOI: 10.1103/physreve.76.031135
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Dynamic boundaries in asymmetric exclusion processes

Abstract: We investigate the dynamics of a one-dimensional asymmetric exclusion process with Langmuir kinetics and a fluctuating wall. At the left-hand boundary, particles are injected onto the lattice; from there, the particles hop to the right. Along the lattice, particles can adsorb or desorb, and the right-hand boundary is defined by a wall particle. The confining wall particle has intrinsic forward and backward hopping, a net leftward drift, and cannot desorb. Performing Monte Carlo simulations and using a moving-f… Show more

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Cited by 30 publications
(41 citation statements)
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“…In order to compute Q 100 and Q 001 (defined in the frame of the particle), we use finitesegment MFT in the moving frame of the transported particle. We consider a sliding window of m sites always centered about the driven particle [10]. As before, we explicitly enumerate all configurations of the m sites surrounding the particle and assign appropriate rates to create the transition matrix M. Transitions generated by the motion of the particle are reflected in the modifications of M to include terms corresponding to sliding of the m-site window.…”
Section: Prl 99 248302 (2007) P H Y S I C a L R E V I E W L E T T E R Smentioning
confidence: 99%
“…In order to compute Q 100 and Q 001 (defined in the frame of the particle), we use finitesegment MFT in the moving frame of the transported particle. We consider a sliding window of m sites always centered about the driven particle [10]. As before, we explicitly enumerate all configurations of the m sites surrounding the particle and assign appropriate rates to create the transition matrix M. Transitions generated by the motion of the particle are reflected in the modifications of M to include terms corresponding to sliding of the m-site window.…”
Section: Prl 99 248302 (2007) P H Y S I C a L R E V I E W L E T T E R Smentioning
confidence: 99%
“…However, in practice there could be many active particles moving along the same track, which could interact with each other and exhibit some form of collective behavior. This has motivated a number of studies that model the movement of multiple motor particles as an asymmetric exclusion process (ASEP) (Evans et al, 2003;Klumpp and Lipowsky, 2003;Kolomeisky, 1998;Lipowsky et al, 2001;Nowak et al, 2007a;Parmeggiani et al, 2003Parmeggiani et al, , 2004Popkov et al, 2003;Pronina and Kolomeisky, 2007). In the simplest version of such models, each particle hops unidirectionally at a uniform rate along a 1D lattice; the only interaction between particles is a hard-core repulsion that prevents more than one particle occupying the same lattice site at the same time.…”
Section: G Exclusion Processesmentioning
confidence: 99%
“…This motivates an approach called the finite segment mean field theory (FSMFT) approximation (Nowak et al, 2007b). Consider a small segment within the track containing m sites so that the number of states in the system is M = 2 m .…”
Section: Local Target Signalingmentioning
confidence: 99%
“…Solving for the length L yields the main result of this Section, Eq. (13). From the analysis it becomes apparent that the relevant length scale, denoted by λ [Eq.…”
Section: B Mathematical Analysis: Adiabatic Limitmentioning
confidence: 99%