
For a certain c ∗ > 1.4 {c_ * } > 1.4 and c ∈ ( 1.4 , c ∗ ) c \in \left ( {1.4,{c_ * }} \right ) the quadratic system x ˙ = − y + x y , y ˙ = x + 2 y 2 − c x 2 \dot x = - y + xy,\dot y = x + 2{y^2} - c{x^2} has a center at the origin surrounded by a one-parameter family of periodic trajectories. We show the period is not a monotone function of the parameter.
Local and nonlocal bifurcation theory for dynamical systems, center, Nonlinear oscillations and coupled oscillators for ordinary differential equations, Topological structure of integral curves, singular points, limit cycles of ordinary differential equations, periodic trajectories, Periodic solutions to ordinary differential equations
Local and nonlocal bifurcation theory for dynamical systems, center, Nonlinear oscillations and coupled oscillators for ordinary differential equations, Topological structure of integral curves, singular points, limit cycles of ordinary differential equations, periodic trajectories, Periodic solutions to ordinary differential equations
| citations This is an alternative to the "Influence" indicator, which also reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically). | 24 | |
| popularity This indicator reflects the "current" impact/attention (the "hype") of an article in the research community at large, based on the underlying citation network. | Average | |
| influence This indicator reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically). | Top 10% | |
| impulse This indicator reflects the initial momentum of an article directly after its publication, based on the underlying citation network. | Average |
