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By increasing the Fresnel number F of a ring cavity with photorefractive gain, we show the transition between a low-F regime, where a few modes compete with a periodic alternation which becomes irregular with increasing F (chaotic itinerancy), and a high-F regime, where many modes oscillate simultaneously, giving rise to chaotic domains spatially correlated over a length much shorter than the wave-front size (spatiotemporal chaos).
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Arecchi et al. (1990) studied this question.
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