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Reduction of parasitic lasingA technique was developed which carefully retro-reflects precisely controlled amounts of light back into a laser system thereby intentionally forcing the laser system components to oscillate in a new resonator called the parasitic oscillator. The parasitic oscillator uses the laser system to provide the gain and an external mirror is used to provide the output coupling of the new resonator. Any change of gain or loss inside the new resonator will directly change the lasing threshold of the parasitic oscillator. This change in threshold can be experimentally measured as a change in the absolute value of reflectivity, provided by the external mirror, necessary to achieve lasing in the parasitic oscillator. Discrepancies between experimental data and a parasitic oscillator model are direct evidence of optical misalignment or component performance problems. Any changes in the optical system can instantly be measured as a change in threshold for the parasitic oscillator. This technique also enables aligning the system for maximum parasitic suppression with the system fully operational.
Document ID
19950011907
Acquisition Source
Legacy CDMS
Document Type
Other - Patent
Authors
Storm, Mark E.
(NASA Langley Research Center Hampton, VA, United States)
Date Acquired
August 16, 2013
Publication Date
November 29, 1994
Subject Category
Lasers And Masers
Report/Patent Number
Patent Number: NASA-CASE-LAR-14645-1-SB
Patent Number: US-PATENT-5,369,662
Patent Application Number: US-PATENT-APPL-SN-105528
Accession Number
95N18322
Distribution Limits
Public
Copyright
Work of the US Gov. Public Use Permitted.
Patent
NASA-CASE-LAR-14645-1-SB|US-PATENT-5,369,662
Patent Application
US-PATENT-APPL-SN-105528
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