2008
DOI: 10.1103/physreve.78.016208
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Effect of multiple time delays on intensity fluctuation dynamics in fiber ring lasers

Abstract: The effect of time delay on nonlinear oscillators is an important problem in the study of dynamical systems. The dynamics of an erbium-doped fiber ring laser with an extra loop providing time-delayed feedback is studied experimentally by measuring the intensity of the laser. The delay time for the feedback is varied from approximately 0.3 to approximately 900 times the cavity round-trip time, over four orders of magnitude, by changing the length of fiber in the delay line. Depending on the delay, we observe ei… Show more

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Cited by 25 publications
(12 citation statements)
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“…For example, in a semiconductor laser with time-delayed feedback through an external mirror, the photon lifetime is significantly shorter than the feedback time, which can cause the laser intensity to oscillate chaotically [9]. From an experimental point of view, delay systems are particularly attractive because the complexity of the dynamics usually increases with the delay [10][11][12], which is typically easy to control.…”
Section: Introductionmentioning
confidence: 99%
“…For example, in a semiconductor laser with time-delayed feedback through an external mirror, the photon lifetime is significantly shorter than the feedback time, which can cause the laser intensity to oscillate chaotically [9]. From an experimental point of view, delay systems are particularly attractive because the complexity of the dynamics usually increases with the delay [10][11][12], which is typically easy to control.…”
Section: Introductionmentioning
confidence: 99%
“…The question of isochronal synchronization of these nonlinear oscillators (Fischer et al 2006;Klein et al 2006;Rogers-Dakin et al 2006;Schwartz & Shaw 2007;Zhou & Roy 2007;Franz et al 2008) is central to possible applications in sensor networks (Sorrentino & Ott 2008, 2009a. We thus consider coupled oscillators in §4, where the many different configurations, in which even two oscillators may be coupled, are outlined.…”
Section: Introductionmentioning
confidence: 99%
“…Pump light from the laser enters the fiber resonator through the fiber coupler, and an increase in the optical power induces first-order Stokes light waves, B 1 and B 2 , that propagate in a direction opposite to that of the pump light P 1 and P 2 . Both the Sagnac effect in the BFOG and changes to the resonant frequency will produce a difference in the resonance frequencies of B 1 and B 2 [9,10], which results in interference, and the interference signal is processed by the detection circuit. As the power of the pump light exceeds the Brillouin scattering threshold power, an increase in the pump power will result in an increase in the power of the first-order Stokes light [5,7] and stimulate the production of second-and higher-order Stokes light waves.…”
Section: Light Wave Characteristics In the Bfogmentioning
confidence: 99%