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Similarly, when a stable limit cycle is at the \"margin\" of a chaotic attractor in a single system, a certain coupling strength can induce the potential chaotic attractor such that the coupled system has a synchronous chaotic behavior. This excitation mechanism is different from the traditional function of coupling in that the latter mainly drives the coupled system to synchronize with the ongoing dynamics of a single system but does not recover its disappearing dynamics. This newly observed synchronization is called coherent synchronization to distinguish it from various common types of synchronization. Several numerical examples are presented for quantitative description of this interesting phenomenon.<\/jats:p>","DOI":"10.1142\/s0218127406015362","type":"journal-article","created":{"date-parts":[[2006,8,21]],"date-time":"2006-08-21T11:10:02Z","timestamp":1156158602000},"page":"1375-1387","source":"Crossref","is-referenced-by-count":2,"title":["COHERENT SYNCHRONIZATION IN LINEARLY COUPLED NONLINEAR SYSTEMS"],"prefix":"10.1142","volume":"16","author":[{"given":"TIANSHOU","family":"ZHOU","sequence":"first","affiliation":[{"name":"Department of Mathematics, Zhongshan University, Guangzhou 510275, P. R. China"}]},{"given":"GUANRONG","family":"CHEN","sequence":"additional","affiliation":[{"name":"Department of Electronic Engineering, City University of Hong Kong, P. R. 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