\(QS10_{3}^{(0)}\)
Description
Topological configuration of singularities: \(s,s,a,a;S,N,N\)
Phase Portrait
Topological Invariants
| TCSP | Fin Sep | Inf Sep |
| \(10\) | \(4431\) | \(411110\) |
Example
The quadratic differential system
\[\begin{cases} \dot{x} = y+x^{2} \\ \dot{y} = e^{2} \, x/5-e \, y+x^{2}-y^{2} \end{cases}\]
with parameters: \(e = -0.5\)
has the following phase portrait done with P4. If you want, you may download the P4 file here.
The phase portrait appears in the following papers
- With name \(Fig 5.204 S^2_{10,03}\) in {J. C. Artés, J. Llibre and A. C. Rezende}, Structurally unstable quadratic vector fields of codimension one, Birkhäuser/Springer, Cham, 2018, vi+267 pp.Note (for name \(Fig 5.204 S^2_{10,03}\)): The system has limit cycles with distribution \((0,1)\).
- With name \(S^2_{10,03}\) in {J. C. Artés, R. E. Kooij and J. Llibre}, Structurally stable quadratic vector fields, Mem. Amer. Math. Soc. { bf 134} (1998), no.~639, viii+108 pp.; MR1432139
- With name \(V5\) in {J. C. Artés, J. Llibre and D. Schlomiuk}, The geometry of quadratic polynomial differential systems with a weak focus and an invariant straight line, emph{ Internat. J. Bifur. Chaos Appl. Sci. Engrg.}, textbf{20}, no. 11 (2010), 3627--3662.
Neighbours of Codimension 1
- Through the border \(QS11_{4}^{(1)}\), by means of a bifurcation of type \(B\), we reach the neighbor \(QS8_{1}^{(0)}\).
- Through the border \(QS76_{2}^{(1)}\), by means of a bifurcation of type \(C\), we reach the neighbor \(QS1_{4}^{(0)}\).
- Through the border \(QS38_{6}^{(1)}\), by means of a bifurcation of type \(A\), we reach the neighbor \(QS25_{1}^{(0)}\).
- Through the border \(QS38_{7}^{(1)}\), by means of a bifurcation of type \(A\), we reach the neighbor \(QS25_{1}^{(0)}\).
- Through the border \(QS10_{1}^{(1)}\), by means of a bifurcation of type \(D(a)\), we reach the neighbor \(QS10_{5}^{(0)}\).
- Through the border \(QS10_{10}^{(1)}\), by means of a bifurcation of type \(D\), we reach the neighbor \(QS10_{10}^{(0)}\).
- Through the border \(QS74_{1}^{(1)}\), by means of a bifurcation of type \(C\), we reach the neighbor \(QS5_{1}^{(0)}\).
- Through the border \(QS74_{4}^{(1)}\), by means of a bifurcation of type \(C\), we reach the neighbor \(QS5_{2}^{(0)}\).
Comments
This phase portrait appears in J. C. Artés, J. Llibre and D. Schlomiuk (emph{ Internat. J. Bifur. Chaos Appl. Sci. Engrg.}, textbf{20}, no. 11 (2010), 3627--3662) featuring a weak focus of first order. Consequently, a configuration structurally equivalent to \(QS10_{3}^{(0)}\) could potentially exhibit an additional limit cycle bifurcating from the focus.