2019
DOI: 10.1364/oe.27.010320
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Supercontinuum noise reduction by fiber undertapering

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Cited by 23 publications
(12 citation statements)
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“…The spectral evolution in the first two nonlinear stages (EYDFA and TDF) of the cascade were simulated by solving the generalized nonlinear Schrödinger equation (GNLSE) using the fourth order Runge-Kutta integration scheme in the interaction picture with adaptive step size 38,56 . All simulations were performed with 2 19 time sampling points and a temporal resolution of dt = 0.92 fs.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The spectral evolution in the first two nonlinear stages (EYDFA and TDF) of the cascade were simulated by solving the generalized nonlinear Schrödinger equation (GNLSE) using the fourth order Runge-Kutta integration scheme in the interaction picture with adaptive step size 38,56 . All simulations were performed with 2 19 time sampling points and a temporal resolution of dt = 0.92 fs.…”
Section: Discussionmentioning
confidence: 99%
“…Standard SC sources use long pump pulses (picosecond or longer) that break into a sea of solitons initiated by noise seeded modulation instability (MI), and thus the entirety of the broad spectrum suffers from high RIN [35][36][37] . There have been several attempts to mitigate this noise, such as undertapering 38 , seeding of the MI 39,40 (limited low power 41 and a phase-coherent seed 42 ), and increasing the repetition rate to average over more pulses for an enhanced signal-to-noise-ratio (SNR) 20,43 . However, it has never been investigated what effect the SC cascading has on the noise.…”
mentioning
confidence: 99%
“…The MI is produced by breaking up of the pulse in many fundamental solitons, when they collide and re-combine in a chaotic manner. For this reason, the MI is a noisy process [54,55]. A direct comparison between the SLD, EDFA, and SC spectra in the wavelength band from 1510 to 1540 nm, where acetylene has strong absorption peaks, is shown in Figure 3.…”
Section: Methodsmentioning
confidence: 99%
“…The MI is produced by breaking up of the pulse in many fundamental solitons, when they collide and re-combine in a chaotic manner. For this reason, the MI is a noisy process [54,55].…”
Section: Methodsmentioning
confidence: 99%
“…Hollow core fibers overcome the damage threshold by generating a supercontinuum in a gas phase 14 . This results in a broad and bright spectrum, however, there are various competing nonlinear processes present in these fibers, such as the chaotic four-wave mixing and modulation instability 9,[15][16][17] . These mechanisms, combined with their sensitive input coupling, result in strong spectral fluctuations of the generated supercontinuum.…”
Section: Introductionmentioning
confidence: 99%