掺铒 Bi2O3-GeO2-Ga2O3-Na2O玻璃中激发态吸收的抑制

对应用于1.55μm波段宽带放大的掺Er³⁺:Bi₂O₃-GeO₂-Ga₂O₃-Na₂O玻璃中激发态吸收的抑制进行了研究. 为此, 在该玻璃中分别引入了Ce³⁺离子和B₂O₃组分. 研究表明, 随着玻璃中Ce₂O₃的掺杂或B₂O₃组分的引入, Er³⁺:⁴I_11/2能级与Ce³⁺:²F_5/2能级间的能量传递或Er³⁺:⁴I_11/2→⁴I_13/2能级间多声子弛豫速率相应提高, Er ³⁺离子⁴I_11/2能级荧光寿命显著减小, 激发态吸收得到有效抑制. 同时, 实验发现, Ce₂O₃的掺杂进一步提高了Er ³⁺离子⁴I_13/2→⁴I_15/2能级间总量子效率, 增强了1.55mum波段荧光发射强度, 而荧光发射谱宽基本保持不变. B2O3组分的引入虽在一定程度上削弱了1.55μm波段荧光发射强度, 但进一步拓展了其荧光发射谱, 且增益截面峰值波长移向长波段.     

高声子能量氧化物对掺铒碲酸盐玻璃光谱性质的影响

在研制的Er3+/Ce3+共掺低声子能量碲酸盐玻璃(TeO2-Bi2O3-TiO2)中,分别引入高声子能量WO3、SiO2和B2O3氧化物组分,测试了玻璃样品400~1700 nm范围内的吸收光谱、1.53μm波段荧光谱、Er3+离子荧光寿命和拉曼光谱,结合McCumber理论计算了Er3+离子光谱参数.结果表明:高声子能量氧化物组分的引入,能使声子参与的Er3+/Ce3+离子间能量传递过程变得更为有效,增加了Er3+离子亚稳态能级4I13/2上粒子数积累,从而增强1.53μm波段荧光发射.另外,高声子能量氧化物组分的引入还可以增加荧光半高宽(FWHM)和带宽品质因子(σe×FWHM).研究结果对于获取具有优异光谱特性的掺Er3+光纤放大器(EDFA)的玻璃基质具有实际意义.     

P2O3-B2O3-Al2O3-SrO-BaO玻璃中Yb3+非辐射能量转移下Er3+离子的增强发射

本文研究了共掺Er3 +/Yb3 +P2 O3 -B2 O3 -Al2 O3 -SrO -BaO玻璃的能量转移过程。实验中制备了高掺杂Yb3 +离子的双掺Er3 +/Yb3 +的磷酸盐玻璃样品。在Er3 +/Yb3 +掺杂比率 >1 :1 8(mol% )时 ,观测到了基于Yb3 +离子至Er3 +离子能量转移下Er3 +( 4 I13 / 2 →4I15 / 2 )的增强发射和Yb3 +( 2 F7/ 2 →2 F5 / 2 )发射的减弱 ,当Yb3 +离子掺杂浓度超过 2 .1× 1 0 2 1ions/cm3 时 (Er3 +/Yb3 +≤ 1 :1 8,mol% ) ,由于Yb3 +离子的自淬灭效应 ,Er3 +离子的发射强度降低。实验中得到了Yb3 +离子的最佳掺杂浓度为1 .74× 1 0 2 1ions/cm3     

掺铒TeO2-Nb2O5-ZnO系统玻璃的上转换发光性能

稀土离子掺杂碲酸盐系统玻璃是一类应用前景良好的上转换发光材料.研究了含铒TeO2-Nb2O5-ZnO系统玻璃在980nm抽运下的上转换光谱,结果发现存在3个上转换荧光谱带,分别对应于2H11/2→4I15/2、4S3/2→4I15/2和4F9/2→4I15/2,而且Er3 含量的增加可明显提高材料在530、550和660nm附近的发光性能.少量的ZnO引入既可以大幅提升材料的上转换发光强度,又能保持铌碲酸盐玻璃良好的化学稳定性.材料的发光机制主要是激发态吸收(ESA)和能量转移(ET),最大声子能量的降低是上转换发光增强的主要原因.     

Er~(3+)掺杂透明微晶玻璃光谱性质的研究

通过高温熔融法和热处理制备了含有-γBi2WO6纳米晶的Er3+掺杂透明硼铋酸盐微晶玻璃.根据X射线粉末衍射结果和Scherrer公式计算得到-γBi2WO6晶粒大小约为15 nm.由于部分Er3+离子取代Bi3+进入-γBi2WO6纳米晶相中,使得Er3+离子在1.5μm的有效发射带宽由78 nm增加到85 nm,同时Er3+离子在4I13/2能级的荧光寿命由0.67 ms增加到1.43 ms.此外,与原始玻璃相比,在Er3+掺杂硼铋酸盐微晶玻璃中观察到强烈的绿光上转换发光,其上转换发光机制可以归为双光子过程.     

Er3+离子掺杂透明的LaF3-SiO2纳米玻璃-陶瓷的上转换发光

采用溶胶-凝胶法成功制备了一系列Er3 掺杂的透明纳米LaF3-SiO2玻璃-陶瓷样品,并研究了其上转换发光性质与发光机制.研究得到了Er3 浓度对上转换发光的影响规律,拟合了上转换荧光强度与LD工作电流的关系,发现所得结果与理论值能够很好地一致.在980nm激光二极管激发下,获得了发射波长为520、540、660nm的有效上转换发光.在较低的功率泵浦下,540nm波长的绿光波段发射最强,其发光主要过程是处于4F7/2态的Er3 离子能量大部分被弛豫到4S3/2态,再由此激发态跃迁到基态4I15/2态所致.     

Tm3+掺杂Bi2O3-SiO2-PbO玻璃的～2μm发光光谱性质

用高温熔融法制备了Tm2O3摩尔掺杂浓度分别为0.1%、0.25%、0.5%、0.75%和1%的33Bi2O3-50SiO2-17PbO玻璃。采用DSC方法对该种玻璃的析晶性能进行研究,发现其Tx–Tg为138℃,说明该玻璃抗析晶性能良好。基于其吸收光谱,采用Judd-Ofelt理论计算了Tm3+离子的J-O参数和部分激发态能级的跃迁几率、荧光寿命和分支比等光谱参量。分析3F4能级寿命随掺杂浓度变化关系,发现产生自淬灭的临界浓度为3.54×1020ions/cm3。用McCumber理论计算在33Bi2O3-50SiO2-17PbO玻璃中Tm3+离子3F4→3H6能级跃迁的吸收截面和发射截面,最大吸收截面和最大受激发射截面分别为3.7×10-21和7.2×10-21cm2。研究结果表明33Bi2O3-50SiO2-17PbO玻璃具有较好的光谱性质,是一种实现~2μm激光的较理想玻璃基质。     

Er3+掺杂的MFT玻璃材料2H11/2、4S3/2→4I15/2荧光性质

计算了Er^3 掺杂的氟氧化物玻璃材料MFT的J－O参数,进而获得了一些能级间跃迁的跃迁几率、分支比、及寿命等数据,测量了室温下Er^3 的较强的两个绿色发射^2H11／2、^4S3／2→^4I15／2及红色发射^4F9／2→^4I15／2的激发光谱,观测了^2H11／2、^4S2／2→^4I15/2跃迁荧光强度随着温度的变化,测量了室温下这两筹这衰减曲线,计算了这两个能级的无辐射跃迁几率及量子效率。     

Y_2O_2S∶Er,Yb纳米晶的制备及其上转换和下转换发光

采用共沉淀法,结合固-气硫化工艺制备了平均粒径约40nm的类球形Y2O2S∶Er,Yb纳米晶,并对其在980nm红外激发下的上转换和下转换发射进行了较为详细的研究。Er3+的上转换特征发射分别位于530、550和660nm附近。在表面吸附OH-和CO32-所形成的特殊声子环境下,Er3+的4S3/2→4F9/2和4I11/2→4I13/2多声子弛豫显著提高了4F9/2能级的粒子布居,致使纳米晶具有很强的660nm红光发射。并且红绿光荧光分支比会随Yb3+浓度的提高而显著增大。首次报导了Y2O2S纳米晶中Er3+的红外特征发射。源于Er3+离子4I13/2→4I15/2辐射跃迁的较强红外发射,在晶场作用下分化为峰位分别位于1501、1534和1577nm的3个发射峰。由于4I13/2能级是660nm红光发射的主要布居能级之一,该红外发射与红光发射存在明显竞争。但在较高Yb3+掺杂浓度下,高效的Yb3+→Er3+能量传递可有效削弱红外发射的竞争作用。     

掺铒铋基玻璃的荧光俘获和浓度猝灭效应研究

用高温熔融法制备了系列掺铒铋硼锗酸盐玻璃,测试分析了不同铒离子掺杂浓度下玻璃样品的吸收光谱和荧光光谱.结果显示,掺铒铋硼锗酸盐玻璃中存在着强烈的荧光俘获和浓度猝灭效应.随着铒离子掺杂浓度的增加,1.53 μm波段荧光谱展宽,1 560 nm波长处荧光次峰相对增强.对此用一个等效的四能级模型予以了定性分析.同时,随着铒离子掺杂浓度的增加,4I13/2能级荧光寿命和1.53 μm波段荧光强度呈现出先增加后减小趋势.依据Dexter能量转移理论,计算了该玻璃系统中铒离子发生浓度猝灭的临界距离R0及相互作用参数CEr-Er,并与其它玻璃基质进行了比较.     

Plasma spraying of Al2O3 and Al2O3Y2O3

A microstructural study has been carried out of plasma-sprayed Al₂O₃ and mixed and sintered Al₂O₃Y₂O₃. In order to ascertain the degree of metastability achieved by plasma spraying, these results are compared with a similar experiment utilizing a CO₂ laser for melting and the hammer-and-anvil technique for quenching of the same materials. X-ray diffraction methods were used to determine the obtained phases and crystal structures. In addition, transmission electron microscopy was used to confirm the phases present and to study their morpology. The porosity was studied with both mercury intrusion porosimetry and small angle neutron scattering. The addition of Y₂O₃ is shown to decrease the porosity from 15% to 7.5%. Adhesion is likewise related to the addition of Y₂O₃ and it is seen that adhesion of the mixture is measurably improved over that of pure Al₂O₃. The implication of these results is discussed.     

Microstructure and Strength of Al2O3/Al2O3 Joints Bonded with ZnO-Al2O3-B2O3-SiO2 Glass-Ceramic

ZnO-Al2O3-B2O3-SiO2 （ZABS） glass powder was used as interlayer to join alumina ceramics. The effect of joining temperature on the microstructure and strength of joints was investigated. The results showed that the ZABS glass can react with alumina substrate to form a layer of ZnAl2O4 at Al2O3/glass interface. Bending test exhibited that low joining temperature （1150℃） led to low joint strength due to the formation of pores in the interlayer, originated by high viscosity of the glass. High joining temperature （1250 ℃） also resulted in low joint strength, because of large CTE （coefficient of thermal expansion） mismatch between amorphous interlayer and alumina substrate. Therefore, only when the joining temperature was appropriate （1200℃）, defect-free interface and high joint strength can be obtained. The optimum joint strength reached 285 MPa, which was the same as the base material strength.     

Surface tension of PbO-B2O3 and Bi2O3-B2O3 glass melts

The surface tensions of xPbO-(100?x) B₂O₃ (x = 30–80 mol%) and xBi₂O₃-(100?x) B₂O₃ (x = 0–100 mol%) melts were measured using the ring method over the temperature range 973 to 1373 K. The compositional and temperature dependences of surface tension were investigated. Addition of PbO and Bi₂O₃ to B₂O₃ increased the surface tensions of their respective PbO-B₂O₃ and Bi₂O₃-B₂O₃ melts. The surface tension showed a maximum at 60 mol% PbO in the PbO-B₂O₃ melts and at 70–80 mol% Bi₂O₃ in the Bi₂O₃-B₂O₃ melts. The temperature coefficient of surface tension was examined on the basis of its relationship to the structure, and it was suggested that the temperature coefficient of surface tension decreases with an increasing content of four-coordinated boron.     

Preparation of pressureless-sintered SiC-Y2O3-Al2O3

Sintering additives were prepared from aluminium hydroxide and yttrium hydroxide. These additives were soluble in water and resulted in a binder. A -SiC powder was mixed with the additive solution and sintered at 2150° C without pressure. The oxides formed from the additive promoted sintering. The sintered body contained no pores. Aluminium, silicon, and yttrium oxide were precipitated in the sintered body.     

Some physical properties of V2O5-Fe2O3 and V2O5-Fe2O3-Li2O systems

Various methods have been used to study the physical properties of the V₂O₅-Fe₂O₃ and V₂O₅-Fe₂O₃-Li₂O systems, including X-ray, electron microscope, Mössbauer effect, NMR and thermogravimetric measurements. The iron ions are approximately equally distributed in substitutional and interstitial sites in the V₂O₅ lattice. The maximum number of iron ions dissolved in the V₂O₅ matrix corresponds to 4 mol % Fe₂O₃. In all the samples a quantity of Fe₂O₃ which has not been included in lattice is observed. The V₂O₅-Fe₂O₃ and V₂O₅-Fe₂O₃-Li₂O systems are formed from solid solutions mixed with very small Fe₂O₃ particles. The analysis of the charge compensation of iron ions suggests that V₂O₅ is a quasi-amorphous semiconductor. Irradiation of V₂O₅-based samples with an electron beam induces the V₂O₅ platelets to convert to the VO _x phase.