bibtype |
J -
Journal Article
|
ARLID |
0442871 |
utime |
20240903170533.7 |
mtime |
20150415235959.9 |
WOS |
000353527000015 |
SCOPUS |
84925451822 |
DOI |
10.1214/14-AAP1032 |
title
(primary) (eng) |
A particle system with cooperative branching and coalescence |
specification |
page_count |
34 s. |
media_type |
P |
|
serial |
ARLID |
cav_un_epca*0255426 |
ISSN |
1050-5164 |
title
|
Annals of Applied Probability |
volume_id |
25 |
volume |
3 (2015) |
page_num |
1616-1649 |
publisher |
name |
Institute of Mathematical Statistics |
|
|
keyword |
interacting particle system |
keyword |
cooperative branching |
keyword |
coalescence |
keyword |
phase transition |
keyword |
upper invariant law |
keyword |
survival |
keyword |
extinction |
author
(primary) |
ARLID |
cav_un_auth*0244526 |
name1 |
Sturm |
name2 |
A. |
country |
DE |
share |
50 |
|
author
|
ARLID |
cav_un_auth*0217893 |
name1 |
Swart |
name2 |
Jan M. |
full_dept (cz) |
Stochastická informatika |
full_dept |
Department of Stochastic Informatics |
department (cz) |
SI |
department |
SI |
institution |
UTIA-B |
full_dept |
Department of Stochastic Informatics |
share |
50 |
fullinstit |
Ústav teorie informace a automatizace AV ČR, v. v. i. |
|
source |
|
cas_special |
project |
project_id |
GAP201/10/0752 |
agency |
GA ČR |
ARLID |
cav_un_auth*0263519 |
|
abstract
(eng) |
In this paper, we introduce a one-dimensional model of particles performing independent random walks, where only pairs of particles can produce offspring ("cooperative branching") and particles that land on an occupied site merge with the particle present on that site ("coalescence"). We show that the system undergoes a phase transition as the branching rate is increased. For small branching rates the upper invariant law is trivial and the process started with finitely many particles a.s. ends up with a single particle. Both statements are not true for high branching rates. An interesting feature of the process is that the spectral gap is zero even for low branching rates. Indeed, if the branching rate is small enough, then we show that for the process started in the fully occupied state, the particle density decays as one over the square root of time, and the same is true for the decay of the probability that the process still has more than one particle at a later time if it started with two particles. |
reportyear |
2016 |
RIV |
BA |
num_of_auth |
2 |
mrcbC52 |
4 A hod 4ah 20231122140906.8 |
inst_support |
RVO:67985556 |
permalink |
http://hdl.handle.net/11104/0246064 |
mrcbC64 |
1 Department of Stochastic Informatics UTIA-B 10103 STATISTICS & PROBABILITY |
confidential |
S |
mrcbT16-e |
STATISTICSPROBABILITY |
mrcbT16-j |
2.039 |
mrcbT16-s |
2.617 |
mrcbT16-4 |
Q1 |
mrcbT16-B |
87.561 |
mrcbT16-C |
84.959 |
mrcbT16-D |
Q1 |
mrcbT16-E |
Q1* |
arlyear |
2015 |
mrcbTft |
\nSoubory v repozitáři: swart-0442871.pdf |
mrcbU14 |
84925451822 SCOPUS |
mrcbU34 |
000353527000015 WOS |
mrcbU63 |
cav_un_epca*0255426 Annals of Applied Probability 1050-5164 Roč. 25 č. 3 2015 1616 1649 Institute of Mathematical Statistics |
|