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Saddle-node bifurcation
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Saddle-node bifurcation : ウィキペディア英語版
Saddle-node bifurcation
In the mathematical area of bifurcation theory a saddle-node bifurcation, tangential bifurcation or fold bifurcation is a local bifurcation in which two fixed points (or equilibria) of a dynamical system collide and annihilate each other. The term 'saddle-node bifurcation' is most often used in reference to continuous dynamical systems. In discrete dynamical systems, the same bifurcation is often instead called a fold bifurcation. Another name is blue skies bifurcation in reference to the sudden creation of two fixed points.
If the phase space is one-dimensional, one of the equilibrium points is unstable (the saddle), while the other is stable (the node).
Saddle-node bifurcations may be associated with hysteresis loops and catastrophes.
==Normal form==

A typical example of a differential equation with a saddle-node bifurcation is:
:\frac=r+x^2.
Here x is the state variable and r is the bifurcation parameter.
*If r<0 there are two equilibrium points, a stable equilibrium point at -\sqrt and an unstable one at +\sqrt.
*At r=0 (the bifurcation point) there is exactly one equilibrium point. At this point the fixed point is no longer hyperbolic. In this case the fixed point is called a saddle-node fixed point.
*If r>0 there are no equilibrium points.
In fact, this is a normal form of a saddle-node bifurcation. A scalar differential equation \tfrac = f(r,x) which has a fixed point at x = 0 for r = 0 with \tfrac(0,0) = 0 is locally topological equivalent to \frac = r \pm x^2 , provided it satisfies \tfrac(0,0) \ne 0 and \tfrac(0,0) \ne 0 . The first condition is the nondegeneracy condition and the second condition is the transversality condition.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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