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Erbium doped GaSe crystal for mid-IR applications

dc.citation.epage5491en_US
dc.citation.issue12en_US
dc.citation.spage5484en_US
dc.citation.volume14en_US
dc.citation.woscount19
dc.contributor.authorHsu, YKen_US
dc.contributor.authorChen, CWen_US
dc.contributor.authorHuang, JYen_US
dc.contributor.authorPan, CLen_US
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Photonicsen_US
dc.date.accessioned2014-12-08T15:16:24Z
dc.date.available2014-12-08T15:16:24Z
dc.date.issued2006-06-12en_US
dc.description.abstractWe reported a type-I difference-frequency generator (DFG), based on erbium doped GaSe (Er: GaSe) crystals as a coherent infrared source tunable from 2.4 mu m to 28 mu m. The two mixing beams used for the DFG are a tunable near infrared output (1.1-1.8 mu m) from an optical parametric amplifier (OPA) and the fundamental beam of a picosecond Nd: YAG laser at 1.064 mu m. The system can produce a maximum output pulse energy of 5 mu J at wavelength of 3.5 mu m, corresponding to a photon conversion efficiency of 8% at a pump intensity of 1.7 GW/cm(2). The nonlinear coefficient (d(eff)) of 0.5 atom % erbium doped GaSe crystal was found to be 55.3 pm/V or 24 % higher than that of a pure GaSe crystal. The improvement of deff is attributed to the substitutive and interstitial doping of Er ion in GaSe unit cell. The optical properties of GaSe influenced by the erbium doping are also presented. (c) 2006 Optical Society of America.en_US
dc.identifier.doi10.1364/OE.14.005484en_US
dc.identifier.issn1094-4087en_US
dc.identifier.journalOPTICS EXPRESSen_US
dc.identifier.urihttp://dx.doi.org/10.1364/OE.14.005484en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/12155
dc.identifier.wosnumberWOS:000238437800061
dc.language.isoen_USen_US
dc.titleErbium doped GaSe crystal for mid-IR applicationsen_US
dc.typeArticleen_US

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