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Laser chimeras as a paradigm for multistable patterns in complex systems
A chimera state is a rich and fascinating class of self-organized solutions developed in high-dimensional networks. Necessary features of the network for the emergence of such complex but structured motions are non-local and symmetry breaking coupling. An accurate understanding of chimera states is...
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Published in: | Nature communications 2015-07, Vol.6 (1), p.7752-7752, Article 7752 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | A chimera state is a rich and fascinating class of self-organized solutions developed in high-dimensional networks. Necessary features of the network for the emergence of such complex but structured motions are non-local and symmetry breaking coupling. An accurate understanding of chimera states is expected to bring important insights on deterministic mechanism occurring in many structurally similar high-dimensional dynamics such as living systems, brain operation principles and even turbulence in hydrodynamics. Here we report on a powerful and highly controllable experiment based on an optoelectronic delayed feedback applied to a wavelength tuneable semiconductor laser, with which a wide variety of chimera patterns can be accurately investigated and interpreted. We uncover a cascade of higher-order chimeras as a pattern transition from
N
to
N
+1 clusters of chaoticity. Finally, we follow visually, as the gain increases, how chimera state is gradually destroyed on the way to apparent turbulence-like system behaviour.
Chimera states are a class of self-organized solutions of high-dimensional networks with non-local and symmetry breaking coupling. Here the authors study the chimera patterns generated in a non-linear optical setup and uncover the transition between chimera orders as a pattern across clusters of chaoticity. |
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ISSN: | 2041-1723 2041-1723 |
DOI: | 10.1038/ncomms8752 |