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Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

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spik<strong>in</strong>gBurst<strong>in</strong>g 367foldbifurcationxurestsaddlehomocl<strong>in</strong>icorbitbifurcationfold bifurcationsaddle homocl<strong>in</strong>icorbit bifurcationFigure 9.25: “Fold/homocl<strong>in</strong>ic” burst<strong>in</strong>g: The rest<strong>in</strong>g state disappears via saddle-node(fold) bifurcation and the spik<strong>in</strong>g limit cycle disappears via saddle homocl<strong>in</strong>ic orbitbifurcation.tential corresponds to the left stable equilibrium, which is the <strong>in</strong>tersection of the leftknee of the fast N-shaped nullcl<strong>in</strong>e with the slow nullcl<strong>in</strong>e. Dur<strong>in</strong>g rest<strong>in</strong>g, the N-shapenullcl<strong>in</strong>e slowly moves up, until its knee touches the slow nullcl<strong>in</strong>e at a saddle-nodepo<strong>in</strong>t. Right after this moment, the rest<strong>in</strong>g state disappears via saddle-node (fold) bifurcation,hence the part “fold” <strong>in</strong> the name of the burster. After the fold bifurcation,the membrane potential jumps up to the stable limit cycle correspond<strong>in</strong>g to repetitivespik<strong>in</strong>g. Dur<strong>in</strong>g the spik<strong>in</strong>g state, the N-shaped nullcl<strong>in</strong>e slowly moves down, and themiddle (saddle) equilibrium moves away from the rest<strong>in</strong>g state toward the limit cycle.After a while, the limit cycle becomes a homocl<strong>in</strong>ic trajectory to the saddle, and thenthe cycle disappears via saddle homocl<strong>in</strong>ic orbit bifurcation, hence the part “homocl<strong>in</strong>ic”<strong>in</strong> the name of the burster. After this bifurcation, the membrane potentialjumps down to the rest<strong>in</strong>g state and closes the hysteresis loop.

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