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基质晶体的真空紫外光谱研究 被引量:8
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作者 洪广言 曾小青 +1 位作者 尤洪鹏 吴雪艳 《硅酸盐学报》 EI CAS CSCD 北大核心 2004年第3期233-238,共6页
初步总结了基质晶体中吸收带位置的规律 ,即氧化物 (CaO∶Eu ,Y2 O3∶Eu ,≈ 2 0 0nm) >多铝酸盐 (BaMgAl1 0 O1 7∶Eu ,≈ 175nm)≥硅酸盐 (Ca2 SiO4 ∶Tb ,160~ 170nm) >硼酸盐 [(Y ,Gd)BO3∶Eu ,15 0~ 160nm]≥钒酸盐 (YVO4 ... 初步总结了基质晶体中吸收带位置的规律 ,即氧化物 (CaO∶Eu ,Y2 O3∶Eu ,≈ 2 0 0nm) >多铝酸盐 (BaMgAl1 0 O1 7∶Eu ,≈ 175nm)≥硅酸盐 (Ca2 SiO4 ∶Tb ,160~ 170nm) >硼酸盐 [(Y ,Gd)BO3∶Eu ,15 0~ 160nm]≥钒酸盐 (YVO4 ∶Eu ,≈ 15 5nm)≈正磷酸盐 [(La,Gd)PO4 ∶Eu ,≈ 15 5nm] >五磷酸盐 (TbP5O1 4∶Eu ,≈ 13 5nm) >二磷酸盐 [Sr3(PO4 ) 2 ∶Eu或K3Tb(PO4 ) 2 ∶Eu ,≈ 12 5nm] >氟化物 (LaF3∶Eu或LiYF4 ∶Eu ,≈ 12 0nm)。基质吸收带的位置主要取决于基质的阴离子、阴离子基团 ,以及基质的组成、结构和键能 ,也受基质中阳离子的影响。这一初步规律将有助于人们寻找优质的新型紫外晶体和新型等离子体平板显示器件用的荧光粉。 展开更多
关键词 基质晶体 真空紫外光谱 基质吸收带 激发光谱
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Y_(1.95-x)Gd_xSiO_5:Eu_(0.05)的真空紫外光谱 被引量:2
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作者 宋桂兰 尤洪鹏 +8 位作者 洪广言 曾小青 甘树才 金昌弘 卞钟洪 庾炳容 裴贤淑 权一亿 朴哲熙 《发光学报》 EI CAS CSCD 北大核心 2000年第2期145-149,共5页
利用高温固相法合成了 Y1.95-xGdxSiO5:Eu0.05(x=0.6mol%)荧光体。结构测定表明所合成的荧光体为单斜晶系的X2型Y2SiO5相,空间群为B2/b。真空紫外光谱表明:随着Gd3+含量的增加,在... 利用高温固相法合成了 Y1.95-xGdxSiO5:Eu0.05(x=0.6mol%)荧光体。结构测定表明所合成的荧光体为单斜晶系的X2型Y2SiO5相,空间群为B2/b。真空紫外光谱表明:随着Gd3+含量的增加,在192um附近,出现了Gd+的激发峰,且此峰的强度随着Gd3+含量的增加而增大;同时位于150~185nm之间的基质吸收带的强度也增大;而位于200~300nm之间的Eu的电行迁移带的强度却随着Gd3+含量的增加而降低。 展开更多
关键词 真空紫外光谱 基质吸收带 荧光粉
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Investigation of Modification Effect of B_2O_3 Component on Optical Spectroscopy of Er^(3+) Doped Tellurite Glasses 被引量:2
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作者 杨艳民 陈宝玖 +2 位作者 王成 任国仲 王晓君 《Journal of Rare Earths》 SCIE EI CAS CSCD 2007年第1期31-35,共5页
To investigate the modification effect of the B2O3 component on tellurite glass, a series of glasses with a composition of xB2O3-(80-x)TeO2-10ZnO-10Na20 (x = 0, 10, 20, 30, 40, 50, 60, 70, 80) and an additional am... To investigate the modification effect of the B2O3 component on tellurite glass, a series of glasses with a composition of xB2O3-(80-x)TeO2-10ZnO-10Na20 (x = 0, 10, 20, 30, 40, 50, 60, 70, 80) and an additional amount of 0.5% Er2Os(in molar) were prepared. The refractive index, the absorption edge of the host, the J-O parameters of Er^3+ , the fluorescent decay time, the bandwidth, and the quantum efficiency for the 4Ⅰ13/2→4Ⅰ15/2 transition were obtained theoretically and experimentally. These results indicated that the introduction of B2O3 modified the performance of the tellurite glass. For example, with increasing content of B2O3, the refractive index of the host decreases from 1.9 to 1.5, the absorption edge of the host shifted toward the blue regime, the intensity parameter Ω6 changed from 1.08 × 10^-20(for the pure tellurite glass) to 1.98 ×10^-20 cm^2(for the pure borate glass), the bandwidth of the 4Ⅰ13/2→4Ⅰ15/2 transition increased, and the quantum efficiency of the 4Ⅰ13/2→4Ⅰ15/2 transition decreased. 展开更多
关键词 Er^3+ glass J-O theory bandWIDTH host absorption band gap quantum efficiencv rare earths
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(Y,Gd)BO_3∶Eu的真空紫外光谱特性 被引量:8
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作者 吴雪艳 洪广言 +7 位作者 曾小青 尤洪鹏 金昌弘 卞锺洪 裴淑贤 庾炳容 权一亿 朴哲熙 《高等学校化学学报》 SCIE EI CAS CSCD 北大核心 2000年第11期1658-1660,共3页
The (Y,Gd)BO 3∶Eu phosphor was synthesized by solid state reaction. The UV spectra showed that in a certain range of Gd 3+ concentration, more Gd 3+ absorbed energy and transferred it to Eu 3+ with its increasing con... The (Y,Gd)BO 3∶Eu phosphor was synthesized by solid state reaction. The UV spectra showed that in a certain range of Gd 3+ concentration, more Gd 3+ absorbed energy and transferred it to Eu 3+ with its increasing concentration. From the spectra in VUV region, it was observed that both the doping and the concentrations of Gd 3+ , Eu 3+ greatly affected the absorption of the host lattice. The absorbances at 147 nm and 170 nm increased when the Gd 3+ was doped which can be explained as that Gd 3+ transferred energy to BO 4. The optical properties of (Y,Gd)BO 3∶Eu were the best when the concentration of Eu 3+ was about 0.04. 展开更多
关键词 VUV光谱 基质吸收带 稀土发光材料 荧光粉
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