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By specular nature we here mean that the conditions under which the system has to be prepared are exactly the opposite of those giving rise to Chimera states. Chimera states emerge, indeed, for locally coupled identical oscillators, while here one needs globally coupled nonidentical oscillators, and actually our Letter shows that the more different the ensemble's units are, the best is the case for the observation of Bellerophon states
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By specular nature we here mean that the conditions under which the system has to be prepared are exactly the opposite of those giving rise to Chimera states. Chimera states emerge, indeed, for locally coupled identical oscillators, while here one needs globally coupled nonidentical oscillators, and actually our Letter shows that the more different the ensemble's units are, the best is the case for the observation of Bellerophon states.
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Numerical values are obtained by a fourth order Runge-Kutta integration method, with an integration time step of 0.005. (Equation presented)
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Numerical values are obtained by a fourth order Runge-Kutta integration method, with an integration time step of 0.005. (Equation presented).
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See Supplemental Material at for the analytical treatment, characterization of other Bellerophon states, and the animated movies
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See Supplemental Material at http://link.aps.org/supplemental/10.1103/PhysRevLett.117.204101 for the analytical treatment, characterization of other Bellerophon states, and the animated movies.
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