Anomalous transport and diffusion of coupled Brownian particles with periodic driving forces

2021 ◽  
Vol 136 (10) ◽  
Author(s):  
Ying Wang ◽  
Chunhua Zeng ◽  
Bao-Quan Ai
2020 ◽  
Vol 541 ◽  
pp. 123284
Author(s):  
M.F. Kepnang Pebeu ◽  
R.L. Woulaché ◽  
C.B. Tabi ◽  
T.C. Kofane

2012 ◽  
Vol 11 (04) ◽  
pp. 1250026 ◽  
Author(s):  
M. SUÑÉ SIMON ◽  
J. M. SANCHO ◽  
A. M. LACASTA

The study of transport and diffusion of Brownian particles in disorder media needs the generation of random potentials with well prescribed statistical properties. Here we present a straightforward method to build a Gaussian potential landscape with an arbitrary spatial correlation with the only requirement of isotropy. The method has the particularity that, although it uses the Fourier space, all its constraints and information are in real space. As practical applications we construct three types of Gaussian disordered correlations: Normal, exponential and power-law. These three cases cover a variety of physical situations.


2011 ◽  
Vol 106 (9) ◽  
Author(s):  
M. Khoury ◽  
A. M. Lacasta ◽  
J. M. Sancho ◽  
Katja Lindenberg

Author(s):  
André L.P. Livorati ◽  
Matheus S. Palmero ◽  
Gabriel Díaz-I ◽  
Carl P. Dettmann ◽  
Iberê L. Caldas ◽  
...  

2017 ◽  
Vol 16 (02) ◽  
pp. 1750011 ◽  
Author(s):  
A. M. Fopossi Mbemmo ◽  
G. Djuidjé Kenmoé ◽  
T. C. Kofané

We investigate the diffusion of a particle subjected to a non-sinusoidal periodic potential and driven by an external constant force. To study the dynamic of the Brownian particles, we modify the shape of the potential as well as the temperature. This allows us to observe the dependence of the mean square displacement on the shape parameter as well as the diffusion coefficient. For a particular set of the system parameters, the dispersionless transport, normal diffusion and hyperdiffusion are generated in the system. We show that there exists a potential shape where some parameters of the system weakly affect the type of diffusion. The diffusion coefficient reaches its maximum around a critical value of the external field. This pronounced peak of the diffusion coefficient depends on the shape of the potential, so we have evaluated the critical force as a function of the potential features.


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