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hal.structure.identifierLASMEA
dc.contributor.authorDERBAL, M.
hal.structure.identifierUnité de Développement de la Technologie du Silicium [UDTS]
dc.contributor.authorOUADJAOUT, Djamel
hal.structure.identifierCentre de Développement des Technologies Avancées [CDTA]
dc.contributor.authorSISERIR, F.
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorJUBERA, Veronique
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorCHAMINADE, Jean-Pierre
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorGARCIA, Alain
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorVIRAPHONG, Oudomsack
hal.structure.identifierFaculté de Physique
dc.contributor.authorKADI HANNIFI, M.
dc.date.issued2010
dc.identifier.issn0925-3467
dc.description.abstractEnCrystal growth and spectroscopic study of the new compound Yb<sup>3+</sup>:LiLu(WO<sub>4</sub>)<sub>2</sub> have been undertaken for the first time. Preliminary growth using flux method with Li<sub>2</sub>W<sub>2</sub>O<sub>7</sub> as solvent allows us to obtain small single crystals. As a promising laser crystal, Yb<sup>3+</sup>:LiLu(WO<sub>4</sub>)<sub>2</sub> have characteristics of a low concentration quenching effect and low laser threshold owing to the existence of covalent bands in WO<sub>4</sub> group. Its absorption peak at 977 nm, corresponding to <sup>2</sup>F<sub>7/2</sub>(1) → <sup>2</sup>F<sub>5/2</sub>(5) transition, is suitable for laser diode pumping. Emission spectrum shows large bands extending from 900 to 1100 nm, five peaks centred respectively at 959, 978, 997, 1025 and 1056 nm are well resolved. The FWHM of the most intense emission band located at 997 nm is about 20 nm. Energy Stark levels are: 0, 201, 469 and 749 cm<sup>−1</sup> for the <sup>2</sup>F<sub>7/2</sub> component and: 10,230, 10,427 and 10,890 cm<sup>−1</sup> for the <sup>2</sup>F<sub>5/2</sub> component. The overall splitting of <sup>2</sup>F<sub>7/2</sub> ground-state manifold is 749 cm<sup>−1</sup>, which is larger than that observed in similar systems such as Yb<sup>3+</sup>:LiLa(WO<sub>4</sub>)<sub>2</sub> (632 cm<sup>−1</sup>). Such large crystal-field splitting of the <sup>2</sup>F<sub>7/2</sub> ground-state will be advantageous to lower laser thermal effect and re-absorption losses. As we can see, the stark electronic levels are characterized by relatively large crystal-field splitting favourable to laser crystal applications in the near infrared spectral region.
dc.language.isoen
dc.publisherElsevier
dc.subject.enEmission spectrum
dc.subject.enAbsorption cross-section
dc.subject.enMonoclinic double tungstates
dc.subject.enYb<sup>3+</sup>:LiLu(WO<sub>4</sub>)<sub>2</sub> laser crystal
dc.title.enEmission spectrum and simulated laser parameters of Yb<sup>3+</sup>:LiLu(WO<sub>4</sub>)<sub>2</sub> crystal
dc.typeArticle de revue
dc.identifier.doi10.1016/j.optmat.2010.02.009
dc.subject.halChimie/Matériaux
bordeaux.journalOptical Materials
bordeaux.page756-758
bordeaux.volume32
bordeaux.issue7
bordeaux.peerReviewedoui
hal.identifierhal-00480913
hal.version1
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-00480913v1
bordeaux.COinSctx_ver=Z39.88-2004&amp;rft_val_fmt=info:ofi/fmt:kev:mtx:journal&amp;rft.jtitle=Optical%20Materials&amp;rft.date=2010&amp;rft.volume=32&amp;rft.issue=7&amp;rft.spage=756-758&amp;rft.epage=756-758&amp;rft.eissn=0925-3467&amp;rft.issn=0925-3467&amp;rft.au=DERBAL,%20M.&amp;OUADJAOUT,%20Djamel&amp;SISERIR,%20F.&amp;JUBERA,%20Veronique&amp;CHAMINADE,%20Jean-Pierre&amp;rft.genre=article


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