2014
DOI: 10.1166/jctn.2014.3581
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Review and Theory of Optical Soliton Generation Used to Improve the Security and High Capacity of MRR and NRR Passive Systems

Abstract: We review the generation, application and theory of soliton pulses in a nonlinear fiber optic medium to improve the security and capacity of optical passive systems such as add/drop and PANDA ring resonators. The improvement of the ring resonator passive systems depends on the output signals, where the chaotic signal generation within the systems is the critical properties of the output signals which can be used to enhance the security and capacity. The passive ring resonator systems are constructed by a nonli… Show more

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Cited by 33 publications
(9 citation statements)
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“…). The electric fields are circulated within the system and described by the equations ( 1)-( 3) [12], the input electric field is fed into the z-axis, where = = − − + , is the initial electric field amplitude, Where is the electric field amplitude (real), is the wave number in the direction of propagation (z-axis) and is the angular frequency [27][28][29], where is the initial phase.…”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…). The electric fields are circulated within the system and described by the equations ( 1)-( 3) [12], the input electric field is fed into the z-axis, where = = − − + , is the initial electric field amplitude, Where is the electric field amplitude (real), is the wave number in the direction of propagation (z-axis) and is the angular frequency [27][28][29], where is the initial phase.…”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…The medium of the ring resonator has Kerr effect‐type nonlinearity; therefore, variation of the total refractive index can be presented in Equation . n=n0+n2I=n0+n2Aeffp. …”
Section: Multicarrier Generation Using Microring Resonatorsmentioning
confidence: 99%
“…where n 0 and n 2 are the linear and nonlinear refractive indices respectively, and I and P are the optical intensity and power respectively. The effective mode core area, A eff , ranges from 0.10 to 0.50 μm 2 in terms of material parameters for InGaAsP/InP 42 . A bright soliton with a 1.55 μm central frequency and 800 mW power is introduced into the first ring resonator, R 1 .…”
Section: Theoretical Backgroundmentioning
confidence: 99%