2008
DOI: 10.1016/j.optcom.2008.01.064
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SBS gain-based slow-light system with a Fabry–Perot resonator

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Cited by 11 publications
(9 citation statements)
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“…The challenge in achieving on-chip slow and fast light is that the short interaction length requires a very large value of n g to achieve an appreciable pulse delay. Thus far, large values of group index have been obtained using resonances of atomic transitions [3,7] or optical cavities [6,11,14] and multi-structured waveguides [1], however these techniques are fixed in frequency and/or limited in signal bandwidth, constraints which put severe restrictions on the maximum achievable pulse delay. In addition, the atomic transitions for which the largest values of n g are attained require specialized hardware, and have applications mainly in quantum information processing.…”
Section: Introductionmentioning
confidence: 99%
“…The challenge in achieving on-chip slow and fast light is that the short interaction length requires a very large value of n g to achieve an appreciable pulse delay. Thus far, large values of group index have been obtained using resonances of atomic transitions [3,7] or optical cavities [6,11,14] and multi-structured waveguides [1], however these techniques are fixed in frequency and/or limited in signal bandwidth, constraints which put severe restrictions on the maximum achievable pulse delay. In addition, the atomic transitions for which the largest values of n g are attained require specialized hardware, and have applications mainly in quantum information processing.…”
Section: Introductionmentioning
confidence: 99%
“…2 However, the transmission of spectrally pure, high optical energy through an optical medium requires the consideration and management of nonlinear effects, such as stimulated Brillouin scattering ͑SBS͒. 3 The influences of SBS on optical transmission systems performance and resultant systems impairments is a subject of continued interest and research, 4,5 as photonic based systems become the primary transmissions medium for an increasing number of diverse applications, such as radio over fiber, 6 data synchronizing and buffering, 7 and higher speed telecommunications, to support new domestic services. 8 This also leads to the development of new subsystem components, such as high-Q passband filters, 9 Raman fiber lasers, 10 and erbium doped fiber lasers.…”
Section: High Performance Laser Linewidth Broadening For Stimulated Bmentioning
confidence: 99%
“…To confirm this expectation, we propagate a super-Gaussian pulse through the SBS system and through the GAB1 system with the system parameters given above. A super-Gaussian pulse is defined using the field amplitude E sg ðtÞ ¼ expð−t α =σ α Þ, where σ ¼ T 0 =2 is the bit half-width at 1=e 2 intensity, T 0 is the bit period, and, for our study, we set α ¼ 4 [16]. Figure 4 shows the result of numerical simulations for the propagation of a pulse with T 0 ¼ 120 ps through these two delay systems.…”
Section: System Composed Of Sbs and A Single Uniform Fbgmentioning
confidence: 99%
“…Thus, these passive devices can provide delay. The time for which these structures can store energy depends on the cavity parameters [14][15][16][17][18][19][20]. In addition, the bandwidth of these structural resonances depends on the cavity parameters so that the bandwidth and resonance frequency can be tuned.…”
Section: Introductionmentioning
confidence: 99%
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