Global dynamics of the May-Leonard system with a Darboux invariant

We study the global dynamics of the classic May-Leonard model in $\mathbb{R}^3$. Such model depends on two real parameters and its global dynamics is known when the system is completely integrable. Using the Poincare compactification on $\mathbb R^3$ we obtain the global dynamics of the classical...

Full description

Bibliographic Details
Main Authors: Regilene Oliveira, Claudia Valls
Format: Article
Language:English
Published: Texas State University 2020-06-01
Series:Electronic Journal of Differential Equations
Subjects:
Online Access:http://ejde.math.txstate.edu/Volumes/2020/55/abstr.html
id doaj-497279b376a44a2798dec9f1a1da47ba
record_format Article
spelling doaj-497279b376a44a2798dec9f1a1da47ba2020-11-25T03:31:13ZengTexas State UniversityElectronic Journal of Differential Equations1072-66912020-06-01202055,119Global dynamics of the May-Leonard system with a Darboux invariantRegilene Oliveira0Claudia Valls1 ICMC-Univ. de Sao Paulo, Brazil Univ. de Lisboa, Lisboa, Portugal We study the global dynamics of the classic May-Leonard model in $\mathbb{R}^3$. Such model depends on two real parameters and its global dynamics is known when the system is completely integrable. Using the Poincare compactification on $\mathbb R^3$ we obtain the global dynamics of the classical May-Leonard differential system in $\mathbb{R}^3$ when $\beta =-1-\alpha$. In this case, the system is non-integrable and it admits a Darboux invariant. We provide the global phase portrait in each octant and in the Poincar\'e ball, that is, the compactification of $\mathbb R^3$ in the sphere $\mathbb{S}^2$ at infinity. We also describe the $\omega$-limit and $\alpha$-limit of each of the orbits. For some values of the parameter $\alpha$ we find a separatrix cycle $F$ formed by orbits connecting the finite singular points on the boundary of the first octant and every orbit on this octant has $F$ as the $\omega$-limit. The same holds for the sixth and eighth octants.http://ejde.math.txstate.edu/Volumes/2020/55/abstr.htmllotka-volterra systemsmay-leonard systemsdarboux invariant phase portraitslimit setspoincare compactification
collection DOAJ
language English
format Article
sources DOAJ
author Regilene Oliveira
Claudia Valls
spellingShingle Regilene Oliveira
Claudia Valls
Global dynamics of the May-Leonard system with a Darboux invariant
Electronic Journal of Differential Equations
lotka-volterra systems
may-leonard systems
darboux invariant
phase portraits
limit sets
poincare compactification
author_facet Regilene Oliveira
Claudia Valls
author_sort Regilene Oliveira
title Global dynamics of the May-Leonard system with a Darboux invariant
title_short Global dynamics of the May-Leonard system with a Darboux invariant
title_full Global dynamics of the May-Leonard system with a Darboux invariant
title_fullStr Global dynamics of the May-Leonard system with a Darboux invariant
title_full_unstemmed Global dynamics of the May-Leonard system with a Darboux invariant
title_sort global dynamics of the may-leonard system with a darboux invariant
publisher Texas State University
series Electronic Journal of Differential Equations
issn 1072-6691
publishDate 2020-06-01
description We study the global dynamics of the classic May-Leonard model in $\mathbb{R}^3$. Such model depends on two real parameters and its global dynamics is known when the system is completely integrable. Using the Poincare compactification on $\mathbb R^3$ we obtain the global dynamics of the classical May-Leonard differential system in $\mathbb{R}^3$ when $\beta =-1-\alpha$. In this case, the system is non-integrable and it admits a Darboux invariant. We provide the global phase portrait in each octant and in the Poincar\'e ball, that is, the compactification of $\mathbb R^3$ in the sphere $\mathbb{S}^2$ at infinity. We also describe the $\omega$-limit and $\alpha$-limit of each of the orbits. For some values of the parameter $\alpha$ we find a separatrix cycle $F$ formed by orbits connecting the finite singular points on the boundary of the first octant and every orbit on this octant has $F$ as the $\omega$-limit. The same holds for the sixth and eighth octants.
topic lotka-volterra systems
may-leonard systems
darboux invariant
phase portraits
limit sets
poincare compactification
url http://ejde.math.txstate.edu/Volumes/2020/55/abstr.html
work_keys_str_mv AT regileneoliveira globaldynamicsofthemayleonardsystemwithadarbouxinvariant
AT claudiavalls globaldynamicsofthemayleonardsystemwithadarbouxinvariant
_version_ 1724572785010802688