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Microring resonator channel dropping filters
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Optical all-pass filters for phase response design with applications for dispersion compensation
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84894004428
-
-
note
-
r≈1 π/1 - r.
-
-
-
-
14
-
-
84893996067
-
-
note
-
Implicit in this assumption is that each resonator is not strongly driven; i.e., the transmitted phase shift φ per resonator is small with respect to unity.
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15
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Dispersive properties of optical filters for WDM systems
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G. Lenz, B. J. Bggleton, C. R. Giles, C. K. Madsen, and R. B. Slusher, "Dispersive properties of optical filters for WDM systems," IEEE J. Quantum Electron. 34, 1390-1402 (1998).
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16
-
-
84894010051
-
-
note
-
γPL is the nonlinear phase shift acquired for a power level of P over a distance L.
-
-
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17
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0032615102
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Enhanced all-optical switching by use of a nonlinear fiber ring resonator
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19
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84893991031
-
-
note
-
eff are lowered by factors of 3/4 and 9/16, respectively, from their given maximum values when operating at dispersion extremum points.
-
-
-
-
20
-
-
84893992339
-
-
note
-
The simulations used to study pulse evolution in a sequence of waveguide-coupled resonators were carried out by an iterative method in which each iteration consisted of linear and nonlinear phase accumulation during one round trip within the resonator followed by interference at the coupler. Traditional beam or pulse propagation split-step Fourier methods are unnecessary, as structural dispersion possessing a discrete impulse response, is more readily treated in the time domain.
-
-
-
-
21
-
-
84894008807
-
-
note
-
Additionally, higher-order dispersive or nonlinear effects render the scattering of solitons inelastic. Under these conditions, the term "solitary wave" is more appropriate.
-
-
-
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22
-
-
84894005702
-
-
note
-
To expand Eq. (18) correctly, the B term must also be expanded, which will generate more time derivative terms within the square brackets. Thus the SS contribution will consist of not only two m = 2 terms but also one m = 1 term. For terms such that m > 1, the time derivatives implicitly appear to the far left of each term when the square brackets are expanded.
-
-
-
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24
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0001655211
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Wavelength conversion in GaAs micro-ring resonators
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26
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84893993451
-
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note
-
2' where a is the transmission coefficient for a single pass around the resonator. If the attenuation is comparable with the cross coupling, light is resonantly attenuated strongly. Under the condition known as critical coupling (r = a), the finesse drops by a factor of 2 and, more important, the transmission drops to zero.
-
-
-
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27
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0001366258
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Ultimate Q of optical microsphere resonators
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