The bandwidth of the single-mode fiber is derived for both the amplitude-modulation and the heterodyne-detection (AM) system and the intensity-modulation and the intensity-detection (IM) system, in case that the spectral width of the light source is much less than the modulation bandwidth. In the wavelength-division-multiplexing system, the bandwidth per carrier wave is given as a function of the wavelength, and also at the zero-dispersion wavelength. In case of IM system, the frequency dispersion of the fiber causes the harmonic distortion of the signal and reduces the bandwidth to about a third of that in case of AM system.
The copyright of the original papers published on this site belongs to IEICE. Unauthorized use of the original or translated papers is prohibited. See IEICE Provisions on Copyright for details.
Copy
Kazuhito FURUYA, Matsuhiro MIYAMOTO, Yasuharu SUEMATSU, "Bandwidths of Single Mode Optical Fibers" in IEICE TRANSACTIONS on transactions,
vol. E62-E, no. 5, pp. 305-310, May 1979, doi: .
Abstract: The bandwidth of the single-mode fiber is derived for both the amplitude-modulation and the heterodyne-detection (AM) system and the intensity-modulation and the intensity-detection (IM) system, in case that the spectral width of the light source is much less than the modulation bandwidth. In the wavelength-division-multiplexing system, the bandwidth per carrier wave is given as a function of the wavelength, and also at the zero-dispersion wavelength. In case of IM system, the frequency dispersion of the fiber causes the harmonic distortion of the signal and reduces the bandwidth to about a third of that in case of AM system.
URL: https://global.ieice.org/en_transactions/transactions/10.1587/e62-e_5_305/_p
Copy
@ARTICLE{e62-e_5_305,
author={Kazuhito FURUYA, Matsuhiro MIYAMOTO, Yasuharu SUEMATSU, },
journal={IEICE TRANSACTIONS on transactions},
title={Bandwidths of Single Mode Optical Fibers},
year={1979},
volume={E62-E},
number={5},
pages={305-310},
abstract={The bandwidth of the single-mode fiber is derived for both the amplitude-modulation and the heterodyne-detection (AM) system and the intensity-modulation and the intensity-detection (IM) system, in case that the spectral width of the light source is much less than the modulation bandwidth. In the wavelength-division-multiplexing system, the bandwidth per carrier wave is given as a function of the wavelength, and also at the zero-dispersion wavelength. In case of IM system, the frequency dispersion of the fiber causes the harmonic distortion of the signal and reduces the bandwidth to about a third of that in case of AM system.},
keywords={},
doi={},
ISSN={},
month={May},}
Copy
TY - JOUR
TI - Bandwidths of Single Mode Optical Fibers
T2 - IEICE TRANSACTIONS on transactions
SP - 305
EP - 310
AU - Kazuhito FURUYA
AU - Matsuhiro MIYAMOTO
AU - Yasuharu SUEMATSU
PY - 1979
DO -
JO - IEICE TRANSACTIONS on transactions
SN -
VL - E62-E
IS - 5
JA - IEICE TRANSACTIONS on transactions
Y1 - May 1979
AB - The bandwidth of the single-mode fiber is derived for both the amplitude-modulation and the heterodyne-detection (AM) system and the intensity-modulation and the intensity-detection (IM) system, in case that the spectral width of the light source is much less than the modulation bandwidth. In the wavelength-division-multiplexing system, the bandwidth per carrier wave is given as a function of the wavelength, and also at the zero-dispersion wavelength. In case of IM system, the frequency dispersion of the fiber causes the harmonic distortion of the signal and reduces the bandwidth to about a third of that in case of AM system.
ER -