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There are two bifurcations in , both at .
Near , append . The plane is invariant and tangent to the extended center subspace, so it is an extended center manifold. The reduced equation is exactly
Its leading terms have two branches, and , which cross and exchange their center-direction stability. Hence this is a transcritical bifurcation.
For the bifurcation at , set
The extended system becomes
Solving the centre-manifold invariance equation for gives
Substitution into the equation yields
For this has two nearby equilibria , while for it has none. It is therefore a saddle-node bifurcation. These reductions are collected in bifurcations of the 2022 Cambridge quadratic-cubic system.
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