DocumentCode
1123530
Title
Decision-driven phase-locked loop for optical homodyne receivers: Performance analysis and laser linewidth requirements
Author
Kazovsky, Leonid G.
Author_Institution
Bell communications Research, Navesing Research and Engineering Center, Red Bank, NJ, USA
Volume
3
Issue
6
fYear
1985
fDate
12/1/1985 12:00:00 AM
Firstpage
1238
Lastpage
1247
Abstract
Optical homodyne receivers based on decision-driven phase-locked loops are investigated. The performance of these receivers is affected by two phase noises due to the laser transmitter and laser local oscillator, and by two shot noises due to the two detectors employed in the receiver. The impact of these noises is minimized if the loop bandwidth
is chosen optimally. The value of Bopt and the corresponding optimum loop performance are evaluated in this paper. It is shown that second-order phase-locked loops require at least 0.8 pW of signal power per every kilohertz of laser linewidth (this number refers to the system with the detector responsivity 1 A/W, dumping factor 0.7, and rms phase error 10°). This signal power is used for phase locking, and is, therefore, lost from the data receiver. Further, the maximum permissible laser linewidth
is evaluated and for second order loops with the dumping factor 0.7 found to be
, where Rb (bit/s) is the system bit rate. For
Mbit/s, this leads to
kHz. For comparison, heterodyne receivers with noncoherent postdetection processing only require
MHz for
Mbit/s. Thus, the homodyne systems impose much more stringent requirements on the laser linewidth than the heterodyne systems. However, homodyne systems have several important advantages over heterodyne systems, and the progress of laser technology may make homodyning increasingly attractive. Even today, homodyne reception is feasible with experimental external cavity lasers, which have been demonstrated to have
as low as 10 kHz.
is chosen optimally. The value of B
is evaluated and for second order loops with the dumping factor 0.7 found to be
, where R
Mbit/s, this leads to
kHz. For comparison, heterodyne receivers with noncoherent postdetection processing only require
MHz for
Mbit/s. Thus, the homodyne systems impose much more stringent requirements on the laser linewidth than the heterodyne systems. However, homodyne systems have several important advantages over heterodyne systems, and the progress of laser technology may make homodyning increasingly attractive. Even today, homodyne reception is feasible with experimental external cavity lasers, which have been demonstrated to have
as low as 10 kHz.Keywords
Homodyne detection; Optical fiber receivers; PLLs; Phase-locked loop (PLL); Laser noise; Local oscillators; Optical mixing; Optical noise; Optical receivers; Optical transmitters; Performance analysis; Phase detection; Phase locked loops; Phase noise;
fLanguage
English
Journal_Title
Lightwave Technology, Journal of
Publisher
ieee
ISSN
0733-8724
Type
jour
DOI
10.1109/JLT.1985.1074338
Filename
1074338
Link To Document