2012
DOI: 10.1063/1.4757278
|View full text |Cite
|
Sign up to set email alerts
|

Some Hamiltonian models of friction II

Abstract: In the present paper we consider the motion of a very heavy tracer particle in a medium of a very dense, non-interacting Bose gas. We prove that, in a certain mean-field limit, the tracer particle will be decelerated and come to rest somewhere in the medium. Friction is caused by emission of Cerenkov radiation of gapless modes into the gas. Mathematically, a system of semilinear integro-differential equations, introduced in [FSSG10], describing a tracer particle in a dispersive medium is investigated, and deca… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
18
0

Year Published

2012
2012
2015
2015

Publication Types

Select...
5
1

Relationship

5
1

Authors

Journals

citations
Cited by 10 publications
(18 citation statements)
references
References 6 publications
0
18
0
Order By: Relevance
“…In [12] and in [10] (where a more general result going beyond the weak-coupling limit is proven), some of the authors have analyzed particle motion in an ideal Bose gas, that is, for µ = 0. In an ideal Bose gas, the speed of sound is zero, hence there is only supersonic particle motion.…”
Section: Introductionmentioning
confidence: 99%
“…In [12] and in [10] (where a more general result going beyond the weak-coupling limit is proven), some of the authors have analyzed particle motion in an ideal Bose gas, that is, for µ = 0. In an ideal Bose gas, the speed of sound is zero, hence there is only supersonic particle motion.…”
Section: Introductionmentioning
confidence: 99%
“…The following models are of interest (see [5,4]): B -Model: κ = 0 (ideal Bose gas), g → 0, see [4]. C -Model: κ = 0, but g = 0; see [3]. E -Model: 2κρ 0 /g 2 := λ =const., with g, κ → 0 ("Bogolubov limit").…”
mentioning
confidence: 99%
“…The following models are of interest (see [8,7]): B -Model: κ = 0 (ideal Bose gas), g → 0; see [7]. C -Model: κ = 0, but g = 0; see [5]. E -Model: 2κρ 0 /g 2 := λ =const., with g, κ → 0 ("Bogolubov limit"); this paper.…”
Section: Background From Physics and Equations Of Motionmentioning
confidence: 99%