Abstract
Abstract
The synchronization of the motion of microresonators has attracted considerable attention. In previous studies, the microresonators for synchronization were studied mostly in the linear regime. While the important problem of synchronizing nonlinear microresonators was rarely explored. Here we present theoretical methods to synchronize the motions of chaotic optical cavity modes in an optomechanical system, where one of the optical modes is strongly driven into chaotic motion and transfers chaos to other weakly driven optical modes via a common mechanical resonator. This mechanical mode works as a common force acting on each optical mode, which, thus, enables the synchronization of states. We find that complete synchronization can be achieved in two identical chaotic cavity modes. For two arbitrary nonidentical chaotic cavity modes, phase synchronization can also be achieved in the strong-coupling small-detuning regime.
Funder
United States Department of Defense | United States Army | U.S. Army Research, Development and Engineering Command | Army Research Office
MEXT | Japan Society for the Promotion of Science
MEXT | RIKEN
John Templeton Foundation
United States Department of Defense | United States Air Force | AFMC | Air Force Office of Scientific Research
the National Key R&D Program of China
Japan Society for the Promotion of Science London
Publisher
Springer Science and Business Media LLC
Cited by
13 articles.
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