Transient Periodicity in a Morris-Lecar Neural System

Figure 3

(a) The strange chaotic attractor at 𝑏=0.15 and 𝑉^𝐾=−0.7. (b) The time histories for two nearby initial conditions. The nonoverlap between the two signals and positive Lyapunov establishes that the underlying attractor supports chaotic dynamics.

(a)

(b)