“…Under the threshold gain, the trivial solution is stable meaning no oscillation, but it soon experiences a Hopf bifurcation at the threshold gain and the stability of the two solutions are switched. 4,5,9 Once the gain is further increased beyond the critical gain, the system undergoes a secondary Hopf bifurcation, also known as a Neimark-Sacker bifurcation and every solution becomes unstable. 4,12,13 We proceed the work by assuming that the gain is in the region where the oscillatory solution is stable, between the two critical points.…”