Abstract

The Kuramoto model is a mathematical model for describing the collective synchronization phenomena of coupled oscillators. We theoretically demonstrate that an array of coupled photonic crystal lasers emulates the Kuramoto model with non-delayed nearest-neighbor coupling (the local Kuramoto model). Our novel strategy employs indirect coupling between lasers via additional cold cavities. By installing cold cavities between laser cavities, we avoid the strong coupling of lasers and realize ideal mutual injection-locking with effective non-delayed dissipative coupling. First, after discussing the limit cycle interpretation of laser oscillation, we demonstrate the synchronization of two indirectly coupled lasers by numerically simulating coupled-mode equations. Second, by performing a phase reduction analysis, we show that laser dynamics in the proposed device can be mapped to the local Kuramoto model. Finally, we briefly demonstrate that a chain of indirectly coupled photonic crystal lasers actually emulates the one-dimensional local Kuramoto chain. We also argue that our proposed structure, which consists of periodically aligned cold cavities and laser cavities, will best be realized by using state-of-the-art buried multiple quantum well photonic crystals.

Highlights

  • The Kuramoto model is a mathematical model for describing the collective synchronization phenomena of coupled oscillators

  • We demonstrate that the cold cavities play a crucial role in avoiding strong coupling between lasers, which results in ideal mutual injection-locking and dramatically simplifies the phase dynamics of laser oscillations

  • We argue that our proposed device can be realized best by using buried multiple quantum well (MQW) photonic crystal (PhC) ­cavities[47,48,49,50], where MQWs are locally embedded in a PhC slab

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Summary

Discussion

We discuss several details that will be of importance in a real device design and experiments. In this context, the spectral shape of laser emissions will be of interest. We may prove synchronization from the pump-power dependence of the change in spectral shape Another promising experimental strategy to prove synchronization may be to pump two lasers independently and tune the respective laser frequencies by making use of the carrier-induced blue s­ hift[49]. We found that even if all the parameters of the three cavities including β1,2 are moderately different, synchronization can occur (not shown)

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