Fig. 3.

A solution of (21) for <a onClick="popup('http://www.mathematical-neuroscience.com/content/1/1/13/mathml/M276','MathML',630,470);return false;" target="_blank" href="http://www.mathematical-neuroscience.com/content/1/1/13/mathml/M276">View MathML</a> and <a onClick="popup('http://www.mathematical-neuroscience.com/content/1/1/13/mathml/M290','MathML',630,470);return false;" target="_blank" href="http://www.mathematical-neuroscience.com/content/1/1/13/mathml/M290">View MathML</a> approaching to a heteroclinic cycle between two cluster states with the same clustering <a onClick="popup('http://www.mathematical-neuroscience.com/content/1/1/13/mathml/M277','MathML',630,470);return false;" target="_blank" href="http://www.mathematical-neuroscience.com/content/1/1/13/mathml/M277">View MathML</a> but a different effective phase difference. In the upper graph, synchronization indices for neuron pairs <a onClick="popup('http://www.mathematical-neuroscience.com/content/1/1/13/mathml/M292','MathML',630,470);return false;" target="_blank" href="http://www.mathematical-neuroscience.com/content/1/1/13/mathml/M292">View MathML</a> and <a onClick="popup('http://www.mathematical-neuroscience.com/content/1/1/13/mathml/M293','MathML',630,470);return false;" target="_blank" href="http://www.mathematical-neuroscience.com/content/1/1/13/mathml/M293">View MathML</a> are plotted (after block averaging of size 1000), whereas in the lower graph a shorter time series of membrane voltages shows transitions between different synchronized clusters.

Ashwin et al. The Journal of Mathematical Neuroscience 2011 1:13   doi:10.1186/2190-8567-1-13
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