1994
DOI: 10.1070/pu1994v037n08abeh000038
|View full text |Cite
|
Sign up to set email alerts
|

Nonlinear Brownian motion

Abstract: Contents 1. Introduction 2. Two ways of describing Brownian motion 2.1 The Langevin equation; 2.2 The Fokker-Planck equation 3. Brownian motion in a medium with nonlinear friction. Three forms of the Fokker-Planck equation 4. The Fokker-Planck equation for a Boltzmann gas 5. The Smoluchowski equation. The master equation 6. Two ways of transition from the master equation to the Fokker-Planck equation 6.1 The kinetic form of the Fokker-Planck equation; 6.2 Stationary solution of the Fokker-Planck equation 7. Th… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
103
0

Year Published

2005
2005
2024
2024

Publication Types

Select...
5
2
1

Relationship

0
8

Authors

Journals

citations
Cited by 148 publications
(103 citation statements)
references
References 27 publications
(10 reference statements)
0
103
0
Order By: Relevance
“…However, in general, it cannot be expected that such a 'truncated' LE yields the correct relaxation behavior and/or the correct stationary solution [59,62]. Furthermore, also under such simplifying approximations, the results will depend on the choice of the discretization rule [50,53,54,55,56,57,58,59,60] because of the multiplicative coupling between 2 D(P ) and ζ(t). Loosely speaking, this discretization dilemma is the price that one has to pay for mapping the large number of collisions between t and t + τ into a single instant of time.…”
Section: Resumementioning
confidence: 99%
See 1 more Smart Citation
“…However, in general, it cannot be expected that such a 'truncated' LE yields the correct relaxation behavior and/or the correct stationary solution [59,62]. Furthermore, also under such simplifying approximations, the results will depend on the choice of the discretization rule [50,53,54,55,56,57,58,59,60] because of the multiplicative coupling between 2 D(P ) and ζ(t). Loosely speaking, this discretization dilemma is the price that one has to pay for mapping the large number of collisions between t and t + τ into a single instant of time.…”
Section: Resumementioning
confidence: 99%
“…II B) suggests that the "transport-form", i.e. the post-point discretization rule [50,58,59,60] should be preferable in the relativistic case as well.…”
Section: Resumementioning
confidence: 99%
“…Commonly used values of the parameter γ are γ = 0 corresponding to pre-point Itô convention, γ = 1/2 corresponding to mid-point Stratonovich convention and γ = 1 corresponding to post-point Hänggi-Klimontovich [52,53], kinetic or isothermal convention [54][55][56]. The integration convention should be determined from the experimental data or derived from another model [57].…”
Section: External Force That Does Not Limit the Anomalous Diffusionmentioning
confidence: 99%
“…The dynamics of the systems studied here is based on Langevin equations, known from the theory of conventional Brownian motion (Hänggi et al, 1990;Langevin, 1908). For the two-dimensional space we get four first order coupled differential equations in the phase space {x 1 , x 2 , v 1 , v 2 }:…”
Section: Dynamic Equations For Two-dimensional Oscillatorsmentioning
confidence: 99%
“…Simple models composed of active Brownian particles were studied in many ear- * Electronic address: udo.erdmann@physik.hu-berlin.de lier works (e.g. Helbing and Molnár, 1995;Klimontovich, 1994;Schienbein and Gruler, 1993).…”
Section: Introductionmentioning
confidence: 99%