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Novel method to stabilize a laser wavelength unaffected by Fabry-Perot etalon angle drift

dc.citation.epage1226en_US
dc.citation.issue5en_US
dc.citation.spage1221en_US
dc.citation.volume43en_US
dc.citation.woscount6
dc.contributor.authorHuang, MSen_US
dc.contributor.authorLu, MHen_US
dc.contributor.authorShy, JTen_US
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Photonicsen_US
dc.date.accessioned2014-12-08T15:39:18Z
dc.date.available2014-12-08T15:39:18Z
dc.date.issued2004-05-01en_US
dc.description.abstractA laser with its wavelength stabilized to a Fabry-Perot etalon has many industrial applications. An ideal error signal for laser stabilization is the dispersion-like signal generated without wavelength modulation. We present a technique, by which the error signal is generated by the difference of two resonance peaks of a Fabry-Perot etalon. A laser beam is split into two beams, which pass through an etalon with a small optical path length difference to generate two partially overlapped resonance peaks. Subtracting one peak from the other yields a dispersion-like error signal. The zero crossing of the differential signal is insensitive to the angle drift of the etalon if the incident angles of the two laser beams are nearly equal but with opposite sign. (C) 2004 Society of Photo-Optical Instrumentation Engineers.en_US
dc.identifier.doi10.1117/1.1690278en_US
dc.identifier.issn0091-3286en_US
dc.identifier.journalOPTICAL ENGINEERINGen_US
dc.identifier.urihttp://dx.doi.org/10.1117/1.1690278en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/26846
dc.identifier.wosnumberWOS:000221456900033
dc.language.isoen_USen_US
dc.subjectFabry-Peroten_US
dc.subjectetalonen_US
dc.subjectdifferential signalen_US
dc.subjectlaser stabilizationen_US
dc.titleNovel method to stabilize a laser wavelength unaffected by Fabry-Perot etalon angle driften_US
dc.typeArticleen_US

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