The equilibria have and . Thus
At , the linearization has trace and determinant . Hence is a saddle equilibrium when , a sink equilibrium when , and a source equilibrium when . The sink equilibrium/source equilibrium may be a node equilibrium or a focus equilibrium; the node-focus discriminant is not a bifurcation curve. At , the trace and determinant are and . These points are sink equilibria for and source equilibria for .
The local bifurcation curves are therefore
For on the pitchfork curve, a leading centre-manifold equation is . For , with unfolding parameter , the pitchfork is supercritical and creates two sink equilibria from a sink equilibrium that becomes a saddle equilibrium. For it is subcritical in the centre direction; the nonzero branches are unstable, and the transverse eigenvalue is also positive. The origin of parameter space is a reflection-symmetric double-zero degeneration.
To determine Hopf criticality at the origin, use the energy , whose derivative is . For a small nearly harmonic oscillation , averaging gives . Thus this Hopf bifurcation is supercritical and creates an attracting periodic orbit for . By the supplied opposite-criticality fact, the simultaneous Hopf bifurcations at the two nonzero equilibria are subcritical. A direct calculation confirms this: writing , puts the cubic radial coefficient at , including the contribution from the quadratic terms.
The figure includes these local curves and the global curves derived below. All lines emerging from the double-zero point are local asymptotic sketches.
Figure 1.
Local and global curves near the symmetric double-zero point
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