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. 2016 Jun 16;7:11887. doi: 10.1038/ncomms11887

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The total number of modes (stable and unstable) admitted by equation (1) is shown in colour as a function of the energy detuning divided by the hopping energy J, and of the driving power (F/γ)², with F being the driving amplitude and γ the loss rate of each cavity. Identical cavities with eigenfrequency are assumed. The dashed line indicates the driving energy used in Figs 3 and 4.

Inline graphic — The total number of modes (stable and unstable) admitted by equation (1) is shown in colour as a function of the energy detuning divided by the hopping energy J, and of the driving power (F/γ)², with F being the driving amplitude and γ the loss rate of each cavity. Identical cavities with eigenfrequency are assumed. The dashed line indicates the driving energy used in Figs 3 and 4.