We demonstrated 10-Gb/s dual-wavelength packets buffering in a dual-loop
optical buffer with a semiconductor optical amplifier. Confirmed
by experiments, the crosstalk between lambda1 and lambda2 signals,
which is the main reason of restraining the buffering time, is decreased
by using power equalization. The buffered data packets are retrieved
after they are buffered for one, two, and three cycles with the maximum
buffering time up to 3.75 mus. The power penalty, the extinction
ratio, and the signal-to-noise ratio are 2.1, 7.5, and 4 dB, respectively,
after three cycles. We obtain the eye diagrams for both wavelengths
with good results, and the buffer is transparent for either wavelength.
%0 Journal Article
%1 Tian2008
%A Tian, Changyong
%A Wu, Chongqing
%A Li, Zhengyong
%A Guo, Ning
%D 2008
%J Photonics Technology Letters, IEEE
%K 10 Gbit/s, amplifier amplifiersbit buffer, buffered buffering, communication, data dual fibre loop optical packet packet, rate semiconductor switching, wavelength
%N 8
%P 578-580
%R 10.1109/LPT.2008.918808
%T Dual-Wavelength Packets Buffering in Dual-Loop Optical Buffer
%V 20
%X We demonstrated 10-Gb/s dual-wavelength packets buffering in a dual-loop
optical buffer with a semiconductor optical amplifier. Confirmed
by experiments, the crosstalk between lambda1 and lambda2 signals,
which is the main reason of restraining the buffering time, is decreased
by using power equalization. The buffered data packets are retrieved
after they are buffered for one, two, and three cycles with the maximum
buffering time up to 3.75 mus. The power penalty, the extinction
ratio, and the signal-to-noise ratio are 2.1, 7.5, and 4 dB, respectively,
after three cycles. We obtain the eye diagrams for both wavelengths
with good results, and the buffer is transparent for either wavelength.
@article{Tian2008,
abstract = {We demonstrated 10-Gb/s dual-wavelength packets buffering in a dual-loop
optical buffer with a semiconductor optical amplifier. Confirmed
by experiments, the crosstalk between lambda1 and lambda2 signals,
which is the main reason of restraining the buffering time, is decreased
by using power equalization. The buffered data packets are retrieved
after they are buffered for one, two, and three cycles with the maximum
buffering time up to 3.75 mus. The power penalty, the extinction
ratio, and the signal-to-noise ratio are 2.1, 7.5, and 4 dB, respectively,
after three cycles. We obtain the eye diagrams for both wavelengths
with good results, and the buffer is transparent for either wavelength.},
added-at = {2009-11-19T14:40:48.000+0100},
author = {Tian, Changyong and Wu, Chongqing and Li, Zhengyong and Guo, Ning},
biburl = {https://www.bibsonomy.org/bibtex/2d932569b741a6988b1ca829107d7a1f7/photonics},
doi = {10.1109/LPT.2008.918808},
file = {Tian2008.pdf:Tian2008.pdf:PDF},
interhash = {5f448b44429795c7aee16385d635cd17},
intrahash = {d932569b741a6988b1ca829107d7a1f7},
issn = {1041-1135},
journal = {Photonics Technology Letters, IEEE},
keywords = {10 Gbit/s, amplifier amplifiersbit buffer, buffered buffering, communication, data dual fibre loop optical packet packet, rate semiconductor switching, wavelength},
month = {April15, },
number = 8,
owner = {gianluca},
pages = {578-580},
timestamp = {2009-11-19T14:41:05.000+0100},
title = {Dual-Wavelength Packets Buffering in Dual-Loop Optical Buffer},
volume = 20,
year = 2008
}