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Preparation And Luminesence Properties Of Rare-earth Doped Li2LaxBnO3n+1 Phosphors

Posted on:2018-08-05Degree:MasterType:Thesis
Country:ChinaCandidate:X Y ZhaoFull Text:PDF
GTID:2321330515454651Subject:physics
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With the development of technique,luminescent materials are widely applied for many fields of human life such as fluorescence detection,light illumination and display screen.Perovskite compounds as an activator possesses because of stable chemical and thermal properties,are widely uesed for phophors.The general struc-ture of Ruddlesden-Popper?RP?phase is An+1BnO3n+1,which could be written here as Li2[AxBnO3n+1]:?n = 2,3 and 4;A = La;B = Nb/Ti?.High temperature synthesis of the sample were prepared by Solid-state Method.The structure and lu-minescent properties of Li2Lao,889Nb1.5Ti0.75O7?n = 2?and Li2La2.25Nb1.25Ti2.75O13?n = 2?doped with Tb3+/Pr3+ ions are studied by characterization methods in-cluding X-ray diffraction?XRD?and fluorescence spectrum,respectively.The main contents are as follows:Li2La0.889Nb1.5Ti0.5O7?n = 2?fluorescent powder was characterizated by XRD and fluorescence spectra.The results show that which was doped with a small amount of Pr3+ ions did not change the structure significantly.The excitation spectrum of Li2La0.889Nb1.5Ti0.75O7:Pr3+ were mainly consisted of a wide band range from 200 to 400 nm.The peak is located at 278 and 339 nm,where the former peak near 278 nm originated from the 4f?5d transition of the Pr3+ ion;the latter peat near 339 nm is due to the valence-to-conduction.The emission band at 495 nm originated from 3P0?P3H4 transition of Pr3+ ions,the main peak in the emission spectrum located at 609 nm,which resulted from 1D2?3H4 transition of Pr3+ ions.According to the XRD analysis,the main diffraction peaks of samples are con-sistent with the standard card?ICSD 88968?of the diffraction peak data.This showed doped rare earth ions did not change matrix lattice structure.The ex-citation spectrum of Li2La2.25Nb1.25Ti2.75O13:Pr3+/Tb3+ consists of the 4f-5d excitation transition?278 nm?and valence-to-conduction?339 nm?and the valence charge transfer?IVCT?transition?360 nm?of Pr3+ to Ti4+.The emission spectra excited by 278 nm exhibit sharp lines peaking at 495 and 609 nm may assigned to the 3P0?3H4 and 1D2?3H4 transition of pr3+ ions.In ordered to investigated the mechanism of energy transfer in host,excited under 237 nm,the emission spectrum of Li2La2.25Nb1.25Ti2.75O13:Pr3+ sample has a broad emission band centered at 404 nm which can be assigned to the NbO67-complex transition of the host.Other weak peaks located in 495 and 609 nm as-cribed to the 3P0?3H4 and 1D2?3H4 transition of Pr3+ ions.Furthermore,the luminescence of Tb3+-doped Li2La2.25Nb1.25Ti2.75O13 has been investigated.As can be seen from the emission spectrum,there are a broad emission band centered at 404 nm and two shaxpe peaks located at 495 and 609 nm.Compared to Pr3+ ions,the substrate energy transfer to Tb3+ ions is more easy to occur.
Keywords/Search Tags:Layered perovskite, Niobate, Energy transfer, charge transfer tran-sition
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