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
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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
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fullinstit Ústav teorie informace a automatizace AV ČR, v. v. i.
source
url http://library.utia.cas.cz/separaty/2015/SI/swart-0442871.pdf
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