Cr4+在Al2O3多晶体中的光谱性能研究

Transparent polycrystalline Cr:Al2O3 ceramics were synthesized by conventional pressureless synthesis processing. The absorption and emission spectra of Cr:Al2O3 ceramics specimens before and after annealing were measured at room temperature. It was discovered that the emission spectra of Cr4+ in Al2O3 octahedral coordination site is in infrared wavelength range of 1100-1600 nm. The emission peak of Cr4+ is centered at 1223 nm, which is similar to that of Cr4+ in tetrahedral site. Al2O3 has smaller lattice constant, resulting in the larger crystal field strength, so there is a blue shift in the peak of Cr4+:Al2O3 ceramics compared to those of other Cr4+-doped crystals. And the emission band is much narrower with full width at half maximum Delta lambda 37 nm.

Nd：YAG透明陶瓷的烧成及其显微结构

由溶胶一凝胶／燃烧合成结合法合成了Nd：YAG(掺钕钇铝石榴石，neodymium—doped yttrium aluminium garnet)粉体，用真空烧结法制备了Nd：YAG透明陶瓷。研究了显微结构随烧结温度和保温时间的变化，并对透明陶瓷的晶界结构和成分分布进行了表征。随着烧结温度的提高和保温时间的延长，Nd：YAG陶瓷的密度增大，晶形发育完整，透过率提高。晶粒内部和晶界的化学组成基本相同。所制备的Nd：YAG透明陶瓷在激光工作波长1064nm的透过率达到75％。

掺Yb^3＋的氧化镧钇透明激光陶瓷的光谱特性

采用传统陶瓷烧结工艺，在无压还原气氛中低温制备了Yb^3＋掺杂量高达10％（按摩尔计）的透明性良好的氧化镧钇激光陶瓷，研究了其在室温的吸收光谱、发射光谱以及荧光寿命。结果表明：掺Yb^3＋氧化镧钇透明激光陶瓷具有宽的吸收和发射光谱以及长的荧光寿命。吸收峰位于902，942nm和968nm处，吸收截面分别为0.31×10^-20,0.45×10^-20cm^2和0.53×10^-20cm2：主发射峰位于1032nm和1075nm处，发射截面分别为1.05×10^-20cm^2和0.87×10^-20cm ^

氧化铝透明陶瓷中Cr3+的发光性能

采用传统无压烧结工艺制备出透明性良好的掺Cr3+氧化铝陶瓷;测定了陶瓷的吸收光谱、发射光谱和激发光谱。结果表明,氧化铝陶瓷吸收峰与红宝石单晶一致,吸收截面大小与单晶相近;陶瓷中Cr3+离子所处格位的晶体场强较单晶弱,但其发射谱仍有较好的锐线发射;陶瓷中微量添加剂以及晶界的存在使得Al2O3晶胞发生畸变,造成其发射峰宽化。

Yb:Y2-2xLa2xO3激光透明陶瓷的光谱性能

It was first reported the spectral properties of a low-temperature sintered transparent Yb: Y2-2x La-2x O-3 laser ceramics. Yb: Y2-2x La-2x O-3 laser ceramics have broad absorption band and large absorption cross- section of 4.0 x 10(-20) cm(2) at wavelengths 977nm of the highest absorption peak. Its fluorescence lifetime is 1.1 ms, and the emission cross-sections are 1.0 x 10(-20) cm(2) and 0.7 x 10(-20) cm(2) at wavelengths 1033nm and 1077nm, respectively. All the optical properties are similar to those of single crystals.

La2O3对氧化铝透明陶瓷显微结构和透光性能的影响

采用传统无压烧结工艺在氢气氛下制备Al2O3透明陶瓷。实验结果表明：MgO和La2O3复合添加时，随着La2O3掺杂量的增加体积密度总体上保持上升的趋势。随着保温时间的延长，陶瓷的致密化程度增大，残余气孔逐步排出，晶粒进一步长大。采用La2O3和MgO复合添加比单独掺入MgO陶瓷样品透过率更高，掺杂效果更好。在烧结温度为1750℃，保温时问为1h条件下，在波艮为300～800nm测试范围内，陶瓷样品的全透过率大于82％，最大值为86％。

Ti：Al2O3透明多晶陶瓷光谱特性分析

采用传统无压烧结工艺制备出透明性良好的掺Ti氧化铝陶瓷；测定了该陶瓷的吸收光谱、荧光光谱和激发光谱。结果表明，掺Ti氧化铝透明陶瓷样品在Mg与Ti掺入离子的摩尔比（NMg／NTi）较小时，表现出Ti^3＋离子的490nm特征吸收峰，即^2T2→^2E跃迁产生的宽带吸收；NMg／NTi较大时，陶瓷样品吸收光谱中不存在Ti^3＋离子吸收，其250nm处吸收为O^2-→Ti^4＋的转移吸收。掺Ti氧化铝透明陶瓷样品Ti^3＋离子的发射谱线与单晶的相吻合，同时Ti^3＋在氧化铝陶瓷中分布很均匀，且Ti^3＋浓度较

Cr^4＋在Al2O3透明陶瓷中的发光行为

采用传统无压烧结工艺制备出透明性良好的掺Cr的Al2O3透明陶瓷；测定了其吸收光谱和荧光光谱，发现在Al2O3六配位的八面体结构中，除了有Cr^3＋离子的特征吸收峰外，由于有Mg^2＋的电荷补偿作用，也有Cr^4＋离子，Cr^4＋的荧光发射峰位于1223nm附近，与Cr^4＋在四面体中的发光行为一致。但其荧光发射峰较窄，半高宽△λ仅为37nm。

Diode-pumped passively q-switched Nd : YAG ceramic laser with a Cr4+: YAG crystal-satiable absorber

Transparent polycrystalline Nd:YAG ceramics were fabricated by solid-state reactive sintering a mixture of commercial Al2O3,Y2O3, and Nd2O3 powders. The powders were mixed in ethanol and doped with 0.5 wt% tetraethoxysilane, dried, and pressed. Pressed samples were sintered at 1750 degrees C in vacuum. Transparent fully dense samples with average grain sizes of 10 mu m were obtained. The 1 at.% Nd:YAG ceramic was used to research passively Q-switched laser output with a Cr4+:YAG crystal as a saturable absorber. An average output power of 94 mW with a pulse width of 50 ns was obtained when the incident pump power was 750 mW. The slope efficiency was 13%. The pulse energy is 5 mu J, and the peak power is about 100 W.

Diode-pumped Yb : YAG ceramic laser

Transparent polycrystalline Yb:YAG ceramics were fabricated by solid-state reactive sintering a mixture of commercial Al2O3, Y2O3, and Yb2O3 powders. The powders were mixed in ethanol and doped with 0.5 wt% tetraethoxysilane, dried, and pressed. Pressed samples were sintered at 1730 degrees C in vacuum. Transparent fully dense samples with grain sizes of several micrometers were obtained. The phase from 1500 degrees to 1700 degrees C was important for the grain growth, in which the grains grew quickly and a mass of pores were eliminated from the body of the sample. Annealing was an important step to remove the vacancies of oxygen and transform Yb2+ to Yb3+. The 1 at.% Yb:YAG ceramic sample was pumped by a diode laser to study the laser properties. The maximum output power of 1.02 W was obtained with a slope efficiency of 25% at 1030 nm. The size of the lasering sample was 4 mm x 4 mm x 3 mm.

Synthesis of CaCu3Ti4O12 ceramic via a sol-gel method

The novel nano-ultrafine powders for the preparation of CaCu3Ti4O12 ceramic were prepared by the sol-gel method and citrate auto-ignition method. The obtained precursor powders were pressed, sintered at 1000 degrees C to fabricate microcrystal CaCu3Ti4O12 ceramic. The microcrystalline phase of CaCu3Ti4O12 was confirmed by X-ray powder diffraction (XRD). The morphology and size of the grains of the powders and ceramics under different heat treatments were observed using scanning electron microscopy (SEM). The relative dielectric constant of the ceramic sintered at 1000 degrees C was measured with a magnitude of more than 10(4) at room temperature, which was approaching to those of Pb-containing complex perovskite ceramics, and the loss tangent was less than 0.20 in a broad frequency region. The relative dielectric constant and loss tangent were also compared with that of CaCu3Ti4O12 ceramic prepared by other reported methods. (c) 2006 Elsevier B.V. All rights reserved.

Investigation of the spectroscopic properties of Yb3+-doped yttrium lanthanum oxide transparent ceramic

Spectroscopic properties of (Y0.9-xLa0.1Ybx)(2)O-3 transparent ceramic were studied. Two main absorption peaks of the specimen are centered at 940 and 970 nm, which are suitable for InGaAs laser diode pumping. The main emission peaks were located at 1032 and 1075 nm with larger emission cross-section and longer fluorescence lifetime than those of Yb:Y2O3. These properties of (Y0.9-xLa0.1Ybx)(2)O-3 transparent ceramic are favorable to achieve high efficiency and high power laser output. (c) 2007 Elsevier B.V. All rights reserved.

掺Yb^3＋氧化镧钇透明激光陶瓷的光谱特性

采用传统陶瓷烧结工艺,在无压还原气氛下低温制备出透明性良好的掺Yb^3＋氧化镧钇透明激光陶瓷,测试了其在室温下的吸收光谱、发射光谱和荧光寿命.结果表明,掺Yb^3＋氧化镧钇透明激光陶瓷的吸收系数随着Yb^3＋掺杂浓度的增加而增大,最强吸收峰974 nm处的吸收截面为0.90～1.12×10^-20 cm^2;主发射峰1 032 nm和1 075 nm处的发射截面分别为1.05×10^-20 cm^2和0.87×10^-20 cm^2; Yb^3＋掺杂浓度为5at.%时荧光寿命为1.38 ms,并随Yb^3

用Judd-Ofelt理论计算Nd^3＋掺杂氧化镧钇透明陶瓷的光谱参量

采用传统无压烧结工艺制备Nd^3 ＋掺杂的氧化镧钇透明激光陶瓷,测试了其吸收和荧光光谱.采用Judd-Ofelt理论对Nd^3 ＋掺杂量为1 .5at %的样品光谱参量进行了计算.根据吸收光谱,拟合得到三个强度参量分别为：Ω2=6 .57×10^-20cm^2,Ω4=2 .04×10^-20cm^2,Ω6=4 .38×10^-20cm^2.根据这三个参量计算了样品的辐射寿命,跃迁几率,荧光分支比,量子效率和品质因子,并对结果作了分析.

用纳米粉制备Nd：Y1.84La0.16O3透明陶瓷Nd：Y1

用碳酸盐共沉淀法制备一种新的掺钕氧化镧钇（Nd：Y1.84La0.16O3）纳米粉体,得到颗粒细小、均匀、分散性好、粒径为50～60nm的Nd：Y1.84La0.16O3纳米粉体.分别采用Nd：Y1.84La0.16O3纳米粉料和商业粉料,用传统陶瓷无压烧结工艺制备Nd：Y1.84La0.16O3透明陶瓷.Nd：Y1.8vLa0.16O3纳米粉制备的陶瓷样品的组分均匀、几乎不存在第二相,具有较高的透过率.商业粉制备的陶瓷样品因混料不均匀而在晶界处存在部分第二相,降低了陶瓷的透过率.此外,还运用体视学法预测