2004
DOI: 10.1109/jlt.2003.822007
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Simulating and Designing Brillouin Gain Spectrum in Single-Mode Fibers

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Cited by 193 publications
(68 citation statements)
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“…For 10% Ge-doped silica if the acoustic wave damping time is considered as T B = 6.469 ns [29], then we have, v B = 49.205 MHz. For such a structure, often it is assumed that v B to be equal for all acoustic modes and is assumed to be around MHz for all silica based fibers [27].…”
Section: Resultsmentioning
confidence: 99%
“…For 10% Ge-doped silica if the acoustic wave damping time is considered as T B = 6.469 ns [29], then we have, v B = 49.205 MHz. For such a structure, often it is assumed that v B to be equal for all acoustic modes and is assumed to be around MHz for all silica based fibers [27].…”
Section: Resultsmentioning
confidence: 99%
“…These can reach 100 K or more. Another possibility is to use a transversally varying speed for the acoustic wave involved in the Brillouin interaction, e.g., with varying germanium and aluminum concentrations across the core [7], [8], [9], [10]. This way, it is possible to independently control propagation of the acoustic and optical waves, and an acoustic speed variation as large as 9% has been achieved [10].…”
Section: Single-frequency Fiber Mopas and Synthetic-aperture Lasersmentioning
confidence: 99%
“…Several approaches have been exploited for the computation of the BGS starting from the modal properties of the fiber [2,3]. The usual assumption is that the fiber can support a single optical mode so that only a limited set of axially-symmetric acoustic modes are evaluated.…”
Section: Introductionmentioning
confidence: 99%