The original paper is in English. Non-English content has been machine-translated and may contain typographical errors or mistranslations. ex. Some numerals are expressed as "XNUMX".
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The original paper is in English. Non-English content has been machine-translated and may contain typographical errors or mistranslations. Copyrights notice
Visant la génération de supercontinuum (SC) large bande et plat à partir de fibres optiques dans la région de longueur d'onde de 1.55, 280 µm, nous étudions à la fois expérimentalement et théoriquement comment les spectres SC sont influencés par la dispersion de vitesse de groupe (GVD) des fibres. Dans la région anormale du GVD, étant donné que la puissance maximale des impulsions de pompe est maintenue élevée pendant la propagation à travers la fibre par l'effet soliton d'ordre supérieur, l'effet Raman a un effet néfaste sur la génération de SC plats et à large bande. Dans la région zéro GVD, l'interaction de la dispersion du troisième ordre (TOD) et de la modulation d'auto-phase divise le spectre SC en deux composantes principales. D'autre part, dans la région GVD normale, bien que le spectre SC soit plus large et plus lisse que celui des régions GVD anormales et nulles, il est toujours asymétrique lorsque le TOD de la fibre ne peut être ignoré. À partir de ces résultats, nous constatons qu’une fibre à dispersion aplatie avec GVD normale est la plus adaptée à la génération de SC plates et à large bande. Un spectre SC de 10 nm de large avec une fluctuation de densité spectrale inférieure à XNUMX dB est en réalité généré à partir d'une telle fibre.
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Fumio FUTAMI, Yuichi TAKUSHIMA, Kazuro KIKUCHI, "Generation of Wideband and Flat Supercontinuum over a 280-nm Spectral Range from a Dispersion-Flattened Optical Fiber with Normal Group-Velocity Dispersion" in IEICE TRANSACTIONS on Electronics,
vol. E82-C, no. 8, pp. 1531-1538, August 1999, doi: .
Abstract: Aiming at wideband and flat supercontinuum generation (SC) from optical fibers in the 1.55-µm wavelength region, we study both experimentally and theoretically how SC spectra are influenced by group-velocity dispersion (GVD) of fibers. In the anomalous GVD region, since the peak power of pump pulses is kept high during propagation through the fiber by the higher-order soliton effect, the Raman effect has an adverse effect to flat and wideband SC generation. In the zero GVD region, the interplay of the third-order dispersion (TOD) and the self-phase modulation splits the SC spectrum into two main components. On the other hand, in the normal GVD region, nevertheless the SC spectrum broadens wider and smoother than those in anomalous and zero GVD regions, it is still asymmetric when TOD of the fiber can not be ignored. From these results, we find that a dispersion-flattened fiber with normal GVD is the most suitable for flat and wideband SC generation. A 280-nm wide SC spectrum with the spectral-density fluctuation less than 10 dB is actually generated from such a fiber.
URL: https://global.ieice.org/en_transactions/electronics/10.1587/e82-c_8_1531/_p
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@ARTICLE{e82-c_8_1531,
author={Fumio FUTAMI, Yuichi TAKUSHIMA, Kazuro KIKUCHI, },
journal={IEICE TRANSACTIONS on Electronics},
title={Generation of Wideband and Flat Supercontinuum over a 280-nm Spectral Range from a Dispersion-Flattened Optical Fiber with Normal Group-Velocity Dispersion},
year={1999},
volume={E82-C},
number={8},
pages={1531-1538},
abstract={Aiming at wideband and flat supercontinuum generation (SC) from optical fibers in the 1.55-µm wavelength region, we study both experimentally and theoretically how SC spectra are influenced by group-velocity dispersion (GVD) of fibers. In the anomalous GVD region, since the peak power of pump pulses is kept high during propagation through the fiber by the higher-order soliton effect, the Raman effect has an adverse effect to flat and wideband SC generation. In the zero GVD region, the interplay of the third-order dispersion (TOD) and the self-phase modulation splits the SC spectrum into two main components. On the other hand, in the normal GVD region, nevertheless the SC spectrum broadens wider and smoother than those in anomalous and zero GVD regions, it is still asymmetric when TOD of the fiber can not be ignored. From these results, we find that a dispersion-flattened fiber with normal GVD is the most suitable for flat and wideband SC generation. A 280-nm wide SC spectrum with the spectral-density fluctuation less than 10 dB is actually generated from such a fiber.},
keywords={},
doi={},
ISSN={},
month={August},}
Copier
TY - JOUR
TI - Generation of Wideband and Flat Supercontinuum over a 280-nm Spectral Range from a Dispersion-Flattened Optical Fiber with Normal Group-Velocity Dispersion
T2 - IEICE TRANSACTIONS on Electronics
SP - 1531
EP - 1538
AU - Fumio FUTAMI
AU - Yuichi TAKUSHIMA
AU - Kazuro KIKUCHI
PY - 1999
DO -
JO - IEICE TRANSACTIONS on Electronics
SN -
VL - E82-C
IS - 8
JA - IEICE TRANSACTIONS on Electronics
Y1 - August 1999
AB - Aiming at wideband and flat supercontinuum generation (SC) from optical fibers in the 1.55-µm wavelength region, we study both experimentally and theoretically how SC spectra are influenced by group-velocity dispersion (GVD) of fibers. In the anomalous GVD region, since the peak power of pump pulses is kept high during propagation through the fiber by the higher-order soliton effect, the Raman effect has an adverse effect to flat and wideband SC generation. In the zero GVD region, the interplay of the third-order dispersion (TOD) and the self-phase modulation splits the SC spectrum into two main components. On the other hand, in the normal GVD region, nevertheless the SC spectrum broadens wider and smoother than those in anomalous and zero GVD regions, it is still asymmetric when TOD of the fiber can not be ignored. From these results, we find that a dispersion-flattened fiber with normal GVD is the most suitable for flat and wideband SC generation. A 280-nm wide SC spectrum with the spectral-density fluctuation less than 10 dB is actually generated from such a fiber.
ER -