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VUV-excited Luminescence Properties Of MAl2B2O7: Re(M=Sr, Ba, Ca; Re=Eu~(3+), Tb~(3+), Eu~(2+))

Posted on:2008-06-01Degree:MasterType:Thesis
Country:ChinaCandidate:T HouFull Text:PDF
GTID:2120360212492316Subject:Optics
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In recent years, more attention has been paid to PDP (Plasma display panel )because of its potential market in the illumination. Special attention has been paid to the development of new and efficient VUV-excited phosphors. On the other hand, borates are of interest as host lattices for luminescent ions, because of their large band gap. Based on this consideration, it is valuable to investigate the alkaline borate family. In this paper, The VUV excitation and luminescence characteristics of MAl2B2O7:Re(M = Sr, Ba, Ca; Re= Eu3+,Tb3+, Eu2+) have been studied.In this work, a series of powder samples of MAl2B2O7:Re(M=Ca, Sr, Ba; Re= Eu3+,Tb3+, Eu2+)was prepared under a reducing atmosphere by solid-state reaction.. The X-ray powder diffraction data of MAl2B2O7:Re are in agreement of JCPDS standard card which indicates that single-phased phosphor can be obtained in such synthesis process.The excitation spectrum of MAl2B2O7: Eu3+ (M=Sr, Ba, Ca) are composed of two broad bands. One band in the range from 130 nm to 170 nm is attributed to the borate groups, and the other band at 230 nm is due to the charge-transfer state (CTS) of the Eu3+ ion. The excitation peak shifts from 167nm to 172nm when the Sr2+ ions are completely replaced by the Ba2+ and Ca2+ ions. It is obvious that the wavelength positions of the excitation bands depend much more on hosts. The lattice parameters of the phosphors increase and the crystal-field strength decrease with increasing of the ionic radius of Ca2+, Sr2+ and Ba2+.Because Eu3+ ions doped into CaAl2B2O7 occupy centrosymmetric site, the emission of magnetic dipole transition 5D0→7F1 is stronger than electric dipole transition. As Eu3+ ions doped into MAl2B2O7 (M=Sr, Ba) occupy Ba2+ or Sr2+ sites which is non-centrosymmetric site, so that the emission of electric dipole transition 5D0→7F2 is stronger than magnetic dipole transition in those series sample. The strong emission line at 613 nm is due to the hypersensitive electric dipole transition of 5D0→7F2. The weaker emission around 592 nm is due to the magnetic dipole transition 5D0→7F1.As for MAl2B2O7:Tb3+ (M=Sr, Ba, Ca) the VUV excited spectra consists of one broad band in the range from 120 nm to 170 nm and the band peaking around 226 nm, and 270 nm respectively. The band (130~170nm) is also assigned to absorption of the borate groups. The bands which cover the spectral range from 160 to 270nm are due to the transitions of Tb3+(4f8→4f75d ).When Ce3+ is doped into the samples, the absorption band of samples obviously decreased in VUV. In PL spectra of MAl2B2O7:Tb3+ (M=Sr, Ba, Ca), there are four peaks at 487 nm, 546 nm, 589 nm and 619 nm corresponding to 5D4 →7FJ (J=6,5,4,3) transition of Tb3+ respectively. Among these transitions, the green emission around 545 nm (5D4→7F5) is the strongest because it is a magnetic dipole allowed transition with △J=±1The excitation spectrum of BaAl2B2O7: Eu2+show a high absorption band which obviously decreased in VUV. The emission spectrum of Ba1-xSrxA12B2O7:Eu2+move to longer wavelength with increasing of Sr2+ mole concentration.
Keywords/Search Tags:rare earth, VUV-excited, Luminescence, spectrum
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