Shaping Light in Nonlinear Optical Fibers 2017
DOI: 10.1002/9781119088134.ch9
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All‐Optical Pulse Shaping in the Sub‐Picosecond Regime Based on Fiber Grating Devices

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Cited by 1 publication
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“…The first and last transfer matrices characterize the interface between the unperturbed fiber core and the first/last layer of the grating. Finally, the grating's reflection and transmission spectral responses H R ( f ) and H T ( f ) are readily obtained from the elements of M FBG using the Equations ( 16) and (17). As previously stated, ML-TMM is a general algorithm useful for the characterization of any arbitrary grating profile, including a non-cosenoidal or even non-periodic refractive index perturbation.…”
Section: Multilayer-based Analysis Methodsmentioning
confidence: 99%
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“…The first and last transfer matrices characterize the interface between the unperturbed fiber core and the first/last layer of the grating. Finally, the grating's reflection and transmission spectral responses H R ( f ) and H T ( f ) are readily obtained from the elements of M FBG using the Equations ( 16) and (17). As previously stated, ML-TMM is a general algorithm useful for the characterization of any arbitrary grating profile, including a non-cosenoidal or even non-periodic refractive index perturbation.…”
Section: Multilayer-based Analysis Methodsmentioning
confidence: 99%
“…The performance of the FBG-based optical signal processor has been typically evaluated by three parameters [17]: the energy efficiency, the cross-correlation coefficient, C C ; and the Time-Bandwidth Product (TBP). The energy efficiency is obtained as the outputto-input waveform energy ratio.…”
Section: Survey Of Signal Processing Units Based On Fbgsmentioning
confidence: 99%
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