12.07.2015 Views

Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

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196 Bifurcations0.80.60.4stable limit cyclen-nullcl<strong>in</strong>eI=7limit cyclesnVIV-nullcl<strong>in</strong>e0.20-80 -60 -40 -20 0membrane voltage, mVI=4nodesaddlestable limit cyclestable limit cyclenodesaddleI=3.08homocl<strong>in</strong>ic orbithomocl<strong>in</strong>ic orbitnodesaddleI=1m<strong>in</strong>/max of oscillations ofmembrane potential, mV0-20-40-60homocl<strong>in</strong>icbifurcationsaddlesnodeslimit cycles-800 2 4 6<strong>in</strong>jected dc-current, InodesaddleFigure 6.28: Saddle homocl<strong>in</strong>ic orbit bifurcation <strong>in</strong> the I Na,p +I K -model with parametersas <strong>in</strong> Fig. 4.1a and fast K + current (τ(V ) = 0.16). As the bifurcation parameter Idecreases, the stable limit cycle becomes a homocl<strong>in</strong>ic orbit to a saddle.

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