{"title":"Multistable and Time Sequencing Photorefractive Ring Resonators","authors":"Dana Z. Anderson, C. Benkert, A. Hermanns","doi":"10.1364/nldos.1990.dmmpcps478","DOIUrl":null,"url":null,"abstract":"In this presentation we discuss and demonstrate the performance of two novel multimode photorefractive systems. The first is a multimode resonator with “winner-takes-all” dynamics. The resonator has several (in our case five) stable steady state solutions in which one mode always oscillates while all the others are suppressed. The system makes a decision which of the modes it will support depending on the initial conditions. The state of the system can then be switched with an external light signal. A modification of the resonator results in a different all-optical system which is capable of recalling a stored sequence of oscillating modes. The dynamics of this sequential recall process is again completely controlled by photorefractive two beam coupling.","PeriodicalId":441335,"journal":{"name":"Nonlinear Dynamics in Optical Systems","volume":"13 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nonlinear Dynamics in Optical Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/nldos.1990.dmmpcps478","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
In this presentation we discuss and demonstrate the performance of two novel multimode photorefractive systems. The first is a multimode resonator with “winner-takes-all” dynamics. The resonator has several (in our case five) stable steady state solutions in which one mode always oscillates while all the others are suppressed. The system makes a decision which of the modes it will support depending on the initial conditions. The state of the system can then be switched with an external light signal. A modification of the resonator results in a different all-optical system which is capable of recalling a stored sequence of oscillating modes. The dynamics of this sequential recall process is again completely controlled by photorefractive two beam coupling.