CHEN Chun-yi, NI Xiao-long, LIU Zhi etc. Research on scintillation and pulse distortion measurement of atmospheric optical transmission channel[J]. Editorial Office of Optics and Precision Engineering, 2016,24(10s): 330-337
CHEN Chun-yi, NI Xiao-long, LIU Zhi etc. Research on scintillation and pulse distortion measurement of atmospheric optical transmission channel[J]. Editorial Office of Optics and Precision Engineering, 2016,24(10s): 330-337 DOI: 10.3788/OPE.20162413.0330.
Research on scintillation and pulse distortion measurement of atmospheric optical transmission channel
To analyze the influence of atmosphere on optical signal transmission
the methods of measuring scintillation in the optical power received by a finite aperture and temporal pulse-waveform distortion have been researched
and the mathematical model for analyzing the measurement data has been established. Between two tall buildings standing 6.2 km apart
the measurement experiment on laser transmission has been carried out; a CCD sensor is used to detect the received optical pattern images
which are defocused; a high bandwidth digital oscilloscope is used to record the temporal waveform of received pulses. Based on the recorded pattern images and pulse waveforms
the probability density distribution of the optical-power scintillationreceived by a virtual circular aperture and the temporal waveform distortion of received optical pulses have been analyzed
respectively. It is shown that:the Nakagami distribution is more accurate than the lognormal distribution for characterizing relatively weak fluctuations in the received optical power; the negative exponential distribution can be appropriately used to describe very strong fluctuations in the received optical power; for a rectangular pulse train transmitted at a repetition rate of 100 MHz
the side lobes in the frequency spectrum of the transmitted temporal pulse waveform with a frequency related to their peaks equal to or larger than 0.48 GHz almost completely disappear when the pulses arrive at the receiver end
and meanwhile obvious spreading of the temporal intensity distribution of a single pulse can be observed with the peak intensity occurring at the moment when the trailing edge of the transmitted pulse reaches the receiver end.
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references
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