Fundamentals of Heterodyne Detection in Laser Communications

International Telemetering Conference Proceedings / November 19-21, 1979 / Town and Country Hotel, San Diego, California === The use of optical heterodyne detection in a communication system requires a local oscillator laser beam to be coincident with the incoming signal on the detector. After detec...

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Main Author: Goodwin, Frank E.
Other Authors: Hughes Aircraft Company
Language:en_US
Published: International Foundation for Telemetering 1979
Online Access:http://hdl.handle.net/10150/613886
http://arizona.openrepository.com/arizona/handle/10150/613886
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spelling ndltd-arizona.edu-oai-arizona.openrepository.com-10150-6138862016-06-23T03:01:32Z Fundamentals of Heterodyne Detection in Laser Communications Goodwin, Frank E. Hughes Aircraft Company International Telemetering Conference Proceedings / November 19-21, 1979 / Town and Country Hotel, San Diego, California The use of optical heterodyne detection in a communication system requires a local oscillator laser beam to be coincident with the incoming signal on the detector. After detection, the signal behaves in every way like a classical microwave or radio signal which has been detected with a heterodyne receiver. This discussion of the use of optical heterodyne detection in laser communications thus includes consideration of modulation formats as well as the special geometrical requirements of combining the local oscillator and signal. Modulation formats of interest are amplitude modulation, frequency modulation and phase modulation, and both heterodyne and homodyne detection techniques are considered. The physical and geometric treatment of optical heterodyne detection is given. General equations are derived for the signal to noise ratio of a coherent receiver in terms of the distribution functions of the signal and local oscillator fields and the size of the detector. The most efficient local oscillator field distribution function is when it exactly matches that of the signal field distribution over the detector surface. A special case of interest is when the signal field is an Airy function and the local oscillator field is uniform. This special case is shown to be feasible with a small penalty in heterodyne mixing efficiency. An analysis of the heterodyne NEP includes factors from geometrical mixing efficiency, thermal noise, dark current, and electrical load mismatch. The degree of degradation is then a function of the amount of local oscillator power. Practical limits on heterodyne NEP's are established. 1979-11 text Proceedings 0884-5123 0074-9079 http://hdl.handle.net/10150/613886 http://arizona.openrepository.com/arizona/handle/10150/613886 International Telemetering Conference Proceedings en_US http://www.telemetry.org/ Copyright © International Foundation for Telemetering International Foundation for Telemetering
collection NDLTD
language en_US
sources NDLTD
description International Telemetering Conference Proceedings / November 19-21, 1979 / Town and Country Hotel, San Diego, California === The use of optical heterodyne detection in a communication system requires a local oscillator laser beam to be coincident with the incoming signal on the detector. After detection, the signal behaves in every way like a classical microwave or radio signal which has been detected with a heterodyne receiver. This discussion of the use of optical heterodyne detection in laser communications thus includes consideration of modulation formats as well as the special geometrical requirements of combining the local oscillator and signal. Modulation formats of interest are amplitude modulation, frequency modulation and phase modulation, and both heterodyne and homodyne detection techniques are considered. The physical and geometric treatment of optical heterodyne detection is given. General equations are derived for the signal to noise ratio of a coherent receiver in terms of the distribution functions of the signal and local oscillator fields and the size of the detector. The most efficient local oscillator field distribution function is when it exactly matches that of the signal field distribution over the detector surface. A special case of interest is when the signal field is an Airy function and the local oscillator field is uniform. This special case is shown to be feasible with a small penalty in heterodyne mixing efficiency. An analysis of the heterodyne NEP includes factors from geometrical mixing efficiency, thermal noise, dark current, and electrical load mismatch. The degree of degradation is then a function of the amount of local oscillator power. Practical limits on heterodyne NEP's are established.
author2 Hughes Aircraft Company
author_facet Hughes Aircraft Company
Goodwin, Frank E.
author Goodwin, Frank E.
spellingShingle Goodwin, Frank E.
Fundamentals of Heterodyne Detection in Laser Communications
author_sort Goodwin, Frank E.
title Fundamentals of Heterodyne Detection in Laser Communications
title_short Fundamentals of Heterodyne Detection in Laser Communications
title_full Fundamentals of Heterodyne Detection in Laser Communications
title_fullStr Fundamentals of Heterodyne Detection in Laser Communications
title_full_unstemmed Fundamentals of Heterodyne Detection in Laser Communications
title_sort fundamentals of heterodyne detection in laser communications
publisher International Foundation for Telemetering
publishDate 1979
url http://hdl.handle.net/10150/613886
http://arizona.openrepository.com/arizona/handle/10150/613886
work_keys_str_mv AT goodwinfranke fundamentalsofheterodynedetectioninlasercommunications
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