2019
DOI: 10.1021/acs.jpcc.8b12081
|View full text |Cite
|
Sign up to set email alerts
|

Counterintuitive Short Uphill Transitions in Single-File Diffusion

Abstract: A universal feature of single-file transport in micropores is the anomalous diffusion of a tracer particle. Here, we report on a new inherent property of the tracer dynamics in periodic free energy landscapes, which manifests itself in the kinetics of local transitions between neighboring energy minima: in the presence of a drift, transitions uphill against the drift are faster than along the more favorable downhill direction. The inequality between the uphill and downhill transition times holds for all densit… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

2
18
0

Year Published

2020
2020
2023
2023

Publication Types

Select...
5
2
1

Relationship

3
5

Authors

Journals

citations
Cited by 17 publications
(20 citation statements)
references
References 60 publications
(71 reference statements)
2
18
0
Order By: Relevance
“…In contrast to expectations, it takes longer to go along the bias than against the bias. For example, such phenomena have been reported in the single-file diffusion [16], in the biased random walk with exclusion interactions [17], in the single-molecule motion with two different dynamic modes [18] and in the particle dynamics on cycle processes with strong coupling to the environment [19]. It was proposed that the asymmetry in the transition times is the sign that the system is out of equilibrium [18], as well as the consequence of the multi-particle interactions in the system [16,19].…”
Section: Introductionmentioning
confidence: 84%
See 1 more Smart Citation
“…In contrast to expectations, it takes longer to go along the bias than against the bias. For example, such phenomena have been reported in the single-file diffusion [16], in the biased random walk with exclusion interactions [17], in the single-molecule motion with two different dynamic modes [18] and in the particle dynamics on cycle processes with strong coupling to the environment [19]. It was proposed that the asymmetry in the transition times is the sign that the system is out of equilibrium [18], as well as the consequence of the multi-particle interactions in the system [16,19].…”
Section: Introductionmentioning
confidence: 84%
“…For example, such phenomena have been reported in the single-file diffusion [16], in the biased random walk with exclusion interactions [17], in the single-molecule motion with two different dynamic modes [18] and in the particle dynamics on cycle processes with strong coupling to the environment [19]. It was proposed that the asymmetry in the transition times is the sign that the system is out of equilibrium [18], as well as the consequence of the multi-particle interactions in the system [16,19]. These theoretical studies, however, involved mostly numerical simulations or considered special simplified systems, raising the question if the observed phenomena are valid for more general cases.…”
Section: Introductionmentioning
confidence: 84%
“…The case f e = f corresponds to particle flow in the environment as in the system and for g → +∞ resembles the situations in the single file models studied in previous work, i.e. in the BASEP 21 and ASEP. 22 The case f e = 0 corresponds to an equilibrium environment, where the flow has no preferred direction.…”
mentioning
confidence: 84%
“…In the extreme case g → ∞, the particles would mutually block each other, corresponding to a single-file diffusion, where similar effects have been reported recently for times of single transitions in crowded environments. 21,22 For attractive interactions, the particles form a low-energy bound state when encountering each other. To escape from such a bound state requires a longer time on average.…”
mentioning
confidence: 99%
“…ψ ± (t) = ψ(t). In the presence of hidden dissipative mechanisms the symmetry may be lifted counterintuitively [64,65]. Denoting the mean waiting time by t = ∞ 0 tψ(t)dt, the steady state current becomes J M = φ + / t −φ − / t = J.…”
mentioning
confidence: 99%