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Giant Second-Harmonic Generation Response and Large Band Gap in the Partially Fluorinated Mid-Infrared Oxide RbTeMo2O8F

dc.contributor.authorHu, Yilei
dc.contributor.authorWu, Chao
dc.contributor.authorJiang, Xingxing
dc.contributor.authorWang, Zujian
dc.contributor.authorHuang, Zhipeng
dc.contributor.authorLin, Zheshuai
dc.contributor.authorLong, Xifa
dc.contributor.authorHumphrey, Mark
dc.contributor.authorZhang, Chi
dc.date.accessioned2021-11-05T02:46:20Z
dc.date.issued2021-08-18
dc.description.abstractStrong second-harmonic generation (SHG) and a wide band gap are two crucial but often conflicting parameters that must be optimized for practical nonlinear optical (NLO) materials. We report herein the first d0-transition-metal (TM) tellurite with half of the d0-TM-octahedra partially fluorinated, namely, quinary RbTeMo2O8F, which exhibits giant SHG responses (27 times that of KH2PO4 (KDP) and 2.2 times that of KTiOPO4 (KTP) with 1064 and 2100 nm laser radiation, respectively), the largest SHG values among all reported metal tellurites. RbTeMo2O8F also possesses a large band gap (3.63 eV), a wide optical transparency window (0.34-5.40 μm), and a significant birefringence (Δn = 0.263 at 546 nm). Theoretical calculations and crystal structure analysis demonstrate that the outstanding SHG responses can be definitively attributed to the uniform alignment of the polarized [MoO5F]/[MoO6] octahedra and the seesaw-like [TeO4], and the consequent favorable summative polarization of the three distinct SHG-active polyhedra, both induced by partial fluorine substitution on the [MoO6] octahedra.en_AU
dc.description.sponsorshipThis research was financially supported by National Natural Science Foundation of China (no. 51432006), Ministry of Education of China for Changjiang Innovation Research Team (no. IRT14R23), Ministry of Education and State Administration of Foreign Experts Affairs for 111 Project (no. B13025), and the Innovation Program of Shanghai Municipal Education Commission. M.G.H. thanks the Australian Research Council for support (DP170100411).en_AU
dc.format.mimetypeapplication/pdfen_AU
dc.identifier.issn0002-7863en_AU
dc.identifier.urihttp://hdl.handle.net/1885/251604
dc.language.isoen_AUen_AU
dc.provenancehttps://v2.sherpa.ac.uk/id/publication/7788..."The Accepted Version can be archived in a Non-Commercial Institutional Repository. 12 months embargo." from SHERPA/RoMEO site (as at 5/11/2021). This document is the Accepted Manuscript version of a Published Work that appeared in final form in [Journal of the American Chemical Society], copyright © American Chemical Society after peer review and technical editing by the publisher. To access the final edited and published work see https://dx.doi.org/10.1021/jacs.1c06061en_AU
dc.publisherAmerican Chemical Societyen_AU
dc.relationhttp://purl.org/au-research/grants/arc/DP170100411en_AU
dc.rights© 2021 American Chemical Societyen_AU
dc.sourceJournal of the American Chemical Societyen_AU
dc.titleGiant Second-Harmonic Generation Response and Large Band Gap in the Partially Fluorinated Mid-Infrared Oxide RbTeMo2O8Fen_AU
dc.typeJournal articleen_AU
dcterms.accessRightsOpen Accessen_AU
local.bibliographicCitation.issue32en_AU
local.bibliographicCitation.lastpage12459en_AU
local.bibliographicCitation.startpage12455en_AU
local.contributor.affiliationHumphrey, M., Research School of Chemistry, The Australian National Universityen_AU
local.contributor.authoruidu9400918en_AU
local.identifier.citationvolume143en_AU
local.identifier.doi10.1021/jacs.1c06061en_AU
local.identifier.essn1520-5126en_AU
local.publisher.urlhttp://pubs.acs.org/journal/jacsat/about.htmlen_AU
local.type.statusAccepted Versionen_AU

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