{"id":169,"date":"2023-09-26T15:18:49","date_gmt":"2023-09-26T15:18:49","guid":{"rendered":"https:\/\/creol.ucf.edu\/sdl\/?page_id=169"},"modified":"2025-03-20T15:26:11","modified_gmt":"2025-03-20T15:26:11","slug":"nonlinear-dynamics-and-synchronization","status":"publish","type":"page","link":"https:\/\/creol.ucf.edu\/sdl\/research\/nonlinear-dynamics-and-synchronization\/","title":{"rendered":"Nonlinear Dynamics and Synchronization"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"169\" class=\"elementor elementor-169\" data-elementor-post-type=\"page\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-e89be57 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"e89be57\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-254ea63\" data-id=\"254ea63\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-f63ed4a elementor-widget elementor-widget-text-editor\" data-id=\"f63ed4a\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>Temporal nonlinear dynamics have been studied for more than 40 years in a wide range of domains, from physics to economics to biology [1]. In some cases, observing nonlinear dynamics is seen as a drawback, as it disrupts the steady state of the system. However, in some other cases, nonlinear dynamics are intrinsic to the nominal behavior of the system, for instance in the case of spiking neurons [2]. In large coupled nonlinear systems, the advent of nonlinear dynamics in one component of the system can lead to the propagation of the dynamical features to neighboring components and this is called synchronization. Some standard systems that show synchronizing behavior are metronomes on a common platform, chirping crickets, and clapping audiences. It is now a well-established fact that synchronization in various systems emerges through nonlinear interactions and subsequent dynamics [3]. Synchronization in nonlinear networks is central to many interesting spatiotemporal phenomena, namely, in-phase synchrony, intensity synchronization, time-delayed synchronization, and cluster synchronization [4]. In addition, the time evolution of synchronized networks exhibits diversified behaviors such as periodic or fixed-point behaviors, chaotic synchronization [5], and formation of chimera states [6].<\/p><p>Our team studies nonlinear dynamics and synchronization for two different types of large coupled nonlinear systems, namely diode laser arrays and Josephson junction arrays. For laser diode arrays we have the capabilities to carry out numerical simulations on large arrays of semiconductor lasers made of more than one thousand devices. We also have components made of a few dozens of laser diodes, either in a 1D configuration or in a 2D stack configuration, for conducting experimental research.<\/p><p>Semiconductor diode lasers are reliable nonlinear systems as they are well-tested and verified experimentally [7]. Under the effect of external perturbations (such as those induced by optical feedback and current modulation), semiconductor lasers display a wide variety of nonlinear behaviors and make them a good testing ground for studying nonlinear dynamics, including chaotic behavior. A semiconductor diode array is fundamentally a network of coupled nonlinear oscillators [8]. Due to the nonlinear interaction, phase can be synchronized between nearest-neighbor coupled semiconductor lasers. For systems with two and three lasers, chaotic synchronization is shown to be induced. For a small diode network with two lasers, the stability properties of in-phase and anti-phase synchronization states are well established using the Lang-Kobayashi rate equations and ab-initio coupled mode theory [9]. When the array size is significantly large, the in-phase solutions are destabilized in favor of anti-phase, and travelling-wave solutions. The degree and characteristics of phase synchronization in large semiconductor laser arrays and its dependence on the size of the array remains an open question, especially in the experimental case, thus is the topic of our numerical and experimental research.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-10242d8 elementor-widget elementor-widget-image\" data-id=\"10242d8\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t<figure class=\"wp-caption\">\n\t\t\t\t\t\t\t\t\t\t<img fetchpriority=\"high\" decoding=\"async\" width=\"768\" height=\"416\" src=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/ThumbnailResearchArea2-768x416.png\" class=\"attachment-medium_large size-medium_large wp-image-148\" alt=\"\" srcset=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/ThumbnailResearchArea2-768x416.png 768w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/ThumbnailResearchArea2-300x163.png 300w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/ThumbnailResearchArea2-1024x555.png 1024w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/ThumbnailResearchArea2-1536x832.png 1536w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/ThumbnailResearchArea2-2048x1110.png 2048w\" sizes=\"(max-width: 768px) 100vw, 768px\" \/>\t\t\t\t\t\t\t\t\t\t\t<figcaption class=\"widget-image-caption wp-caption-text\">Fig. 1: Illustration of a coupled array of semiconductor lasers emitting in-phase train of pulses. The array of lasers is biased with the combination of a DC current and an electrical sine wave, resulting in gain switching of each individual emitter. The strong mutual coupling through a feedback mirror (not shown here) allows synchronization of the emitted pulses. The evolution of the real part of the field has been obtained with our optimized code.<\/figcaption>\n\t\t\t\t\t\t\t\t\t\t<\/figure>\n\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-4527ffb elementor-widget elementor-widget-image\" data-id=\"4527ffb\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t<figure class=\"wp-caption\">\n\t\t\t\t\t\t\t\t\t\t<img decoding=\"async\" width=\"768\" height=\"611\" src=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/Fig2-768x611.png\" class=\"attachment-medium_large size-medium_large wp-image-149\" alt=\"\" srcset=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/Fig2-768x611.png 768w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/Fig2-300x239.png 300w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/Fig2-1024x814.png 1024w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/Fig2-1536x1222.png 1536w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/09\/Fig2-2048x1629.png 2048w\" sizes=\"(max-width: 768px) 100vw, 768px\" \/>\t\t\t\t\t\t\t\t\t\t\t<figcaption class=\"widget-image-caption wp-caption-text\">Fig. 2: Illustration of a cluster dynamics in an array of semiconductor lasers. This experimental result shows that lasers subject to optical feedback in the array are governed by group behavior, or clustering, as can be seen from the electrical spectrum of their temporal dynamics. For instance, laser #2 to laser #10 show main contributions of the external cavity frequency and its harmonics while laser #12 shows a broad spectral component, usually observed in chaotic patterns.<\/figcaption>\n\t\t\t\t\t\t\t\t\t\t<\/figure>\n\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-989f75c elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"989f75c\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-c919f58\" data-id=\"c919f58\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-8883df6 elementor-widget elementor-widget-text-editor\" data-id=\"8883df6\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><strong>Works Cited<\/strong><\/p><p>1. Strogatz, S. H., [<em>Nonlinear dynamics and chaos: with applications to physics, biology, chemistry and engineering<\/em>], CRC Press (2018).<\/p><p>2. Montbrio, E., Pazo, D., and Roxin, A., \u201cMacroscopic description for networks of spiking neurons,\u201d <em>Physical Review X<\/em> 5(2), 021028 (2015).<\/p><p>3. Pikovsky, A., Rosenblum, M., and Kurths, J., [<em>Synchronization: A universal concept in nonlinear science<\/em>], Cambridge University Press (2002).<\/p><p>4. Dahms, T., Lehnert, J., and Scholl, E., \u201cCluster and group synchronization in delay-coupled networks,\u201d <em>Physical Review E<\/em> 86(1), 016202 (2012).<\/p><p>5. Pecora, L. M., and Carroll, T. L., \u201cSynchronization in chaotic systems,\u201d <em>Physical Review Letters<\/em> 64(8), 821 (1990).<\/p><p>6. Hart, J. D., Bansal, K., Murphy, T. E., and Roy, R., \u201cExperimental observation of chimera and cluster states in a minimal globally coupled network,\u201d <em>Chaos: an Interdisciplinary Journal of Nonlinear Science<\/em> 26(9), 094801 (2016).<\/p><p>7. Lang, R., and Kobayashi, K., \u201cExternal optical feedback effects on semiconductor injection laser properties,\u201d <em>IEEE Journal of Quantum Electronics<\/em> 16(3), 347-355 (1980).<\/p><p>8. Soriano, M. C., Garcia-Ojalvo, J., Mirasso, C. M., and Fischer, I., \u201cComplex photonics: dynamics and applications of delay-coupled semiconductor lasers,\u201d <em>Reviews of Modern Physics<\/em> 85(1), 421 (2013).<\/p><p>9. Adams, M., Li, N., Cemlyn, B., Susanto, H., and Henning, I., \u201cEffect of detuning, gain guiding and index antiguiding on the dynamics of two laterally coupled semiconductor lasers,\u201d <em>Physical Review A<\/em> 95(5), 053869 (2017).<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"Temporal nonlinear dynamics have been studied for more than 40 years in a wide range of domains, from physics to economics to biology [1]. In some cases, observing nonlinear dynamics is seen as a drawback, as it disrupts the steady state of the system. However, in some other cases, nonlinear dynamics are intrinsic to the&hellip;","protected":false},"author":83,"featured_media":0,"parent":15,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"footnotes":""},"class_list":["post-169","page","type-page","status-publish","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/pages\/169","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/users\/83"}],"replies":[{"embeddable":true,"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/comments?post=169"}],"version-history":[{"count":21,"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/pages\/169\/revisions"}],"predecessor-version":[{"id":728,"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/pages\/169\/revisions\/728"}],"up":[{"embeddable":true,"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/pages\/15"}],"wp:attachment":[{"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/media?parent=169"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}