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采用助熔剂法生长高质量的Sm3+:YAl3(BO3)4晶体,并通过吸收光谱、荧光光谱对它的光谱特性进行表征,采用Judd–Offelt理论分析了该晶体的光谱参数。结果表明:Sm:YAl3(BO3)4晶体的t(t=2,4,6)参数分别为2=0.058×10–20,4=1.28×10–20,6=1.06×10–20。6H7/2能级的辐射寿命为520.2μs。热学性能测试表明:Sm:YAl3(BO3)4晶体具有较高的热导率,沿c轴方向是5.30W/(m K)。 相似文献
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《硅酸盐学报》2012,40(9)
以 K2W2O7为助熔剂,采用泡生法生长出了 Pr3+掺杂量为 5% (摩尔分数)的 KYb(WO4)2(Pr:KYbW)自激活激光晶体。X 射线衍射分析表明:生长的晶体为单斜晶系的 Pr:KYbW,晶格常数为 a = 1.065 nm、b = 1.031 nm、c = 0.753 nm、β = 130.65°。由样品的 Raman 光谱和红外光谱确认 Pr:KYbW晶体内共有 WO6和 YbO8两种畸变多面体结构,验证了晶体中钨氧桥键的存在。吸收光谱表明:在 945、975nm 处出现了 2 个最强的吸收峰,对应于Yb3+的2F7/2→2F5/2能级跃迁。晶体的上转换荧光谱表明:在 481nm 处的蓝光来自于 Pr3+的3P0→3H4能级跃迁;在 645nm 处的红光来自于 Pr3+的3P0→3F2能级跃迁。 相似文献
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《硅酸盐学报》2012,40(9)
以金属硝酸盐和钛酸丁酯为原料,乙酰丙酮为螯合剂,采用溶胶–凝胶法制备了 Y2O2S:Eu3+,Mg2+,Ti4+红色长余辉发光粉体。采用 X 射线衍射仪、扫描电子显微镜和荧光分光光度计对不同温度合成的样品性能进行测试与表征。结果表明:干凝胶在 600 ℃保温 2 h 生成了立方相的前驱体Y2O3:Eu3+,Mg2+,Ti4+。前驱体在 1050~1150 ℃硫化后的产物为 Y2O3与 Y2O2S 的混合相,在 1 200 ℃时,硫化生成纯相的 Y2O2S:Eu3+,Mg2+,Ti4+,产物平均粒径约为 150nm,1300 ℃时再次出现 Y2O3相。与高温固相法相比,溶胶–凝胶法制备的样品主激发峰出现蓝移,主发射峰位于 616nm 和 626nm处,对应于 Eu3+的5D0→7F2跃迁;硫化温度为 1200 ℃时,样品的余辉时间为 40min。 相似文献
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以尿素为燃料,采用快速燃烧法在650℃合成了Tb3+掺杂的SrAl2O4:Eu2+,Dy3+新型长余辉光致发光材料。研究了Tb3+掺杂对Eu2+,Dy3+共激活的铝酸盐长余辉发光材料的发光特性的影响。X射线衍射分析结果表明:当Tb3+的掺杂量x=0.17%时,合成的样品结构为单相SrAl2O4单斜晶系。光致发光测试结果表明:样品的激发光谱为峰值位于345nm附近的连续宽带谱,发射光谱为峰值位于510nm左右的连续宽带谱。余辉衰减曲线结果表明:Tb3+的适量掺杂可以提高铝酸锶的余辉性能。与SrAl2O4:Eu2+,Dy3+相比,掺杂Tb3+有利于形成结晶度良好的固溶体,样品中的晶体细密紧凑,颗粒粒径约为100nm。 相似文献
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采用溶胶–凝胶法制备Li+取代(K0.5Na0.5)+及Ta5+取代Nb5+的(K0.5Na0.5)NbO3陶瓷粉体,采用无压烧结工艺制备(Na0.50+xK0.50–2xLix)Nb0.9Ta0.1O3(x=0,0.02,0.04)陶瓷样品。研究了前驱体煅烧温度对陶瓷粉体物相组成的影响。分析了不同Li+掺杂量对样品物相组成、微观结构、体积密度及电学性能的影响。结果表明:前驱体的最佳煅烧温度为600℃,通过透射电子显微镜分析陶瓷粉体的粒径为49nm;不同Li+掺杂量制备的(Na0.50+xK0.50–2xLix)Nb0.9Ta0.1O3陶瓷样品均为正交相钙钛矿结构;随着Li+掺杂量的增加,(Na0.50+xK0.50–2xLix)Nb0.9Ta0.1O3陶瓷的体积密度先增大后减小,介电常数逐渐升高,压电常数先降低再升高,剩余极化强度逐渐升高。Li+掺杂量x为0.04时样品的压电常数(d33=94pC/N)、相对介电常数(εr=684.33)及剩余极化强度(Pr=98.27μC/cm2)较好。 相似文献
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The electrical properties of Sr0.5 Ba0.3 TiO3 in the presence of Nb2 O5 as a donor, 3Li2 O · 2SiO2 as a sintering agent, and Bi2 O3 as a dopant have been studied. When the compositions of the ceramics were 1 mol Sr0.7 Ba0.3 TiO3 + 0.5 mol% Nb2 O5 + 2 mol% 3Li2 O · 2SiO2 + 0.2 mol% Bi2 O3 , the ceramics were sintered at 1100°C and exhibited the following characteristics: apparent dielectric constant ɛ, 25000; loss factor tan δ, 2%; insulating resistivity ρj , 1010 Ω· cm; variation of dielectric constant with temperature Δɛ/ɛ (−25° to +85°C), +10%, −14%. ɛ and tan δ show only small changes with frequency. The study shows this ceramic can be used in multilayer technology. 相似文献
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Hong-Soo Kim Gun Yong Sung Chong Hee Kim 《Journal of the American Ceramic Society》1992,75(3):587-591
The effect of the cooling rate on the PTCR (positive temperature coefficient of resistivity) characteristics of 0.1 mol% Sb2 O3 -doped BaTiO3 ceramics has been investigated. Resistances both below and above the Curie temperature were increased by slow cooling, which indicated that the resistive layer width at the grain boundary increased as the cooling rate decreased. Concentration profiles of the Ba vacancies as a function of distance from the grain boundary have been simulated by the finite difference method. The inversion temperature of the 0.1 mol% Sb2 O3 -doped BaTiO3 system was determined to be 1160°C from the measured electrical properties and computed concentration profiles. 相似文献
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Cihangir Duran Susan Trolier-McKinstry Gary L. Messing 《Journal of the American Ceramic Society》2000,83(9):2203-2213
Textured Sr0.53 Ba0.47 Nb2 O6 ceramics with a relative density of >95% were fabricated using templated grain growth (TGG). Acicular KSr2 Nb5 O15 template particles synthesized via a molten salt process were aligned by tape casting in a mixture of solid-state-synthesized SrNb2 O6 and BaNb2 O6 powders. The resulting ceramics possessed strong fiber texture along the polar axis ([001]) of the strontium barium niobate. Samples with 15.4 wt% templates attained a textured fraction of 0.82 after sintering at a temperature of 1450°C for 4 h. These materials showed peak dielectric constants of 7550 at 1 kHz, remanent polarizations of 13.2 μC/cm2 , saturation polarizations of 21 μC/cm2 (60%–85% of the single-crystal value), piezoelectric strain coefficients of 78 pC/N (70%–85% of the single-crystal value), and room-temperature pyroelectric coefficients of 2.9 × 10−2 μC·(cm2 ·°C)−1 (52% of the single-crystal value). These results show that TGG is a viable option for accessing single-crystal properties in polycrystalline ceramics. 相似文献
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Charles A. Bateman Lijie Zhang Helen M. Chan Martin P. Harmer 《Journal of the American Ceramic Society》1992,75(5):1281-1283
It is experimentally observed that the peritectic reaction, 211 + liquid → 123, can be driven essentially to completion in 1 h at an undercooling of only ∽30°C. The kinetic data, together with the observed microstructures, are inconsistent with the normal mechanism of the peritectic reaction. It is proposed that the mechanism of the reaction involves dissolution of 211 particles into the liquid and precipitation of solid 123. The aligned grain structure is explained through sympathetic nucleation of new 123 grains on existing grains. 相似文献
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采用垂直梯度凝固法成功生长出直径为27mm、长为110mm,具有可控形状和形态的F-和Y3+共掺钨酸铅[PbWO4∶(F,Y)]晶体。通过透射光谱、荧光光谱、光产额、衰减时间等对钨酸铅晶体光学性能进行了表征。结果表明:与纯钨酸铅晶体相比,垂直梯度凝固法生长的PbWO4∶(F,Y)晶体在320~420nm的短波范围的光学透过率明显提高,光吸收边更尖锐;荧光光谱为350~580nm范围的宽峰,发射主峰为420nm;光产额达到50p.e/MeV(1 000ns内),发光衰减时间为5ns。 相似文献
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The crystal-growth process and growth conditions of β-alumina (Na2 O · Al2 O3 ) were investigated using the Na2 B4 O7 -Na3 AlF6 flux method. β-Alumina (electric fusion brick) was used as both nutrient and seed. Weight loss of the flux varied widely for various runs: ≅ 10 wt% of flux evaporated at 100 h, ≅ 17 wt% at 150 h, and 43 wt% at 600 h. When β-alumina crystal was grown, only 20 wt% Na2 B4 O7 was added to the Na3 AlF6 flux. The linear growth rates of the β-alumina single crystal grown by an Na3 AlF6 -20 wt% Na2 B4 O7 flux method at 1040°C and Δ t = 18°C were ≅ 1.0 × 10−3 mm/h ( a face) and ≅0.3 × 10−3 mm/h ( c face). The β-alumina single crystals grown were bounded by only c [001] and a [100] and were colorless and transparent. 相似文献