Phase-splitting in the idealized model is not stable. In (
a–
c), 20 globally coupled oscillators are simulated with


rad s
−1 (corresponding to a cycle period of 24.2 hours),


,


,


and


hours, and feedback starts on day 0. Numerical integration is by fourth-order Runge–Kutta method with a time step of 0.1 hours. (
a) The idealized model exhibits phase-splitting of globally coupled, noiseless, identical oscillators. (
b) Phase-splitting is not achieved with variability of the intrinsic oscillator period (the Lorentzian distribution mean period is 24.2±2 hours (s.d.)). (
c) Phase-splitting is not achieved with noisy perturbations of phase (the Gaussian variance is 0.005 rad, resulting in s.d. in the period of 0.46 hours).