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Our approach is based on a bi-directional comb-fiber architecture which is composed of a Sagnac-loop-based mirror and a comb-like combination of N sections of interleaved single-mode fibers and high nonlinear fibers.
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These fibers are less common than G.652 fiber but thanks to their slightly higher nonlinear character, there are suitable for simulation of the worst case which can arise in a real network.
The paper presents a high nonlinear photonic crystal fiber (HN-PCF) with highly duty ratio for time-stretch analog-to-digital conversion (TSADC).
According to simulation, the proposed fiber warrants a high nonlinear coefficient of the order 41 W−1 km−1 and a low dispersion of 0.25 ps/nm/km at 1550 nm wavelength.
This chapter discusses the design, performance and applications of various specialty fibers with special attention to dispersion compensation fibers, polarization maintaining and single-polarization fibers, highly nonlinear fibers, double clad fiber for high-power lasers and amplifiers, and photonic crystal fibers.
This novel substance is a suitable optical fiber material for nonlinear applications due to its high nonlinear coefficient.
Out of this, tellurite glass is a highly suitable fiber material for infrared nonlinear applications because of its high nonlinear coefficient compared to other non-silica glasses.
For the 1300 nm source, high-peak-power ultrashort pulses were coupled into normal-dispersion highly nonlinear fiber (ND-HNLF) to generate the SC.
The nonlinear analysis of columns is also conducted by means of nonlinear fiber section frame element.
The excitation-wavelength-tunable nonlinear fiber-optic spectrometer presented in this study allows performing nonlinear spectroscopy of human lung tissue ECM through the elastin 2PEF and the collagen SHG signals.
Because of its specificities, this nonlinear fiber spectrometer can be used for various studies of endogenous and exogenous fluorophores or harmonophores.
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