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A calcium vapor cell for atomic spectroscopy

dc.citation.epage3749en_US
dc.citation.issue11en_US
dc.citation.spage3747en_US
dc.citation.volume73en_US
dc.citation.woscount5
dc.contributor.authorHuang, MSen_US
dc.contributor.authorLu, MHen_US
dc.contributor.authorShy, JTen_US
dc.contributor.department物理研究所zh_TW
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.contributor.departmentDepartment of Photonicsen_US
dc.date.accessioned2014-12-08T15:41:48Z
dc.date.available2014-12-08T15:41:48Z
dc.date.issued2002-11-01en_US
dc.description.abstractA calcium vapor cell used in laser spectroscopy usually suffers from calcium coating on the cell windows. To solve the problem, we add two mirrors in the cell to reflect the laser beam, then the calcium will coat on these mirrors instead of on the windows. Calcium coating degrades the reflectivity of the mirrors at the beginning, but the mirrors become calcium mirrors after a certain period of coating and their reflectivity will not change by further calcium coating. Using this cell in a conventional saturated-absorption spectroscopy, the observed saturated-absorption peak at 657 nm is about 2.4% of the probe beam power and its linewidth is below 300 kHz. Therefore, a portable secondary calcium-wavelength standard at 657 nm having an accuracy better than 1x10(-11) is possible. In addition, our cell has a continuous working time longer than 3 d and it can be easily extended to 10 d. (C) 2002 American Institute of Physics.en_US
dc.identifier.doi10.1063/1.1511800en_US
dc.identifier.issn0034-6748en_US
dc.identifier.journalREVIEW OF SCIENTIFIC INSTRUMENTSen_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.1511800en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/28426
dc.identifier.wosnumberWOS:000178818200004
dc.language.isoen_USen_US
dc.titleA calcium vapor cell for atomic spectroscopyen_US
dc.typeArticleen_US

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