WO3/Nb2O5掺杂对碲酸盐玻璃热学性质和拉曼光谱特性的影响

报道了钨碲酸盐玻璃系统TeO₂-ZnO-Na₂O-WO₃ 和钨铌碲酸盐玻璃系统TeO₂- ZnO-Na₂O-Nb₂O₅-WO₃抗析晶热稳定性和拉曼光谱特性. 实验研究了掺杂WO₃和Nb₂O₅对碲酸盐玻璃抗析晶热稳定性和拉曼光谱特性的影响, 并分析讨论了掺杂碲酸盐玻璃拉曼谱带展宽机制. 结果表明, 掺杂WO₃和Nb₂O₅较大地提高了碲酸盐玻璃的抗析晶热稳定性, 钨铌碲酸盐玻璃最大抗析晶热稳定性ΔT达154℃. 拉曼光谱研究表明,WO₃和Nb₂O₅的加入使碲酸盐玻璃在921和862cm^-1附近出现特征谱带, 导致拉曼光谱中高频移区从550cm^-1延伸扩展到950cm^-1, 从而有效地拓宽了碲酸盐玻璃的拉曼带宽, 钨铌碲酸盐玻璃最大拉曼光谱半高宽可达355cm^-1. 实验研究表明,钨铌碲酸盐玻璃是宽带拉曼光纤放大器的候选材料之一.     

1.55μm光纤放大器用掺Er3+碲酸盐玻璃光谱性能研究

制备了TeO2-BaO(Li2O,Na2O)-La2O3掺铒碲酸盐玻璃系统,测量玻璃的密度、折射率和DSC曲线,以及玻璃的吸收光谱和荧光光谱.由测得的密度和折射率等参数,应用Judd-Ofelt理论和McCumber理论,计算出碲酸盐玻璃的各光学性能参数与受激发射截面.且从测得热稳定性能较好的TBLE3荧光发射谱图中得到该碲酸盐玻璃荧光半高宽(FWHM)为～60nm,σepeak×FHWM值高达～600,明显大于掺铒硅酸盐玻璃和磷酸盐玻璃,表明该种碲酸盐玻璃是光纤发大器用的理想基质材料.     

WO3/Nb2O5掺杂对碲酸盐玻璃热学性质和拉曼光谱特性的影响

报道了钨碲酸盐玻璃系统TeO₂-ZnO-Na₂O-WO₃ 和钨铌碲酸盐玻璃系统TeO₂- ZnO-Na₂O-Nb₂O₅-WO₃抗析晶热稳定性和拉曼光谱特性. 实验研究了掺杂WO₃和Nb₂O₅对碲酸盐玻璃抗析晶热稳定性和拉曼光谱特性的影响, 并分析讨论了掺杂碲酸盐玻璃拉曼谱带展宽机制. 结果表明, 掺杂WO₃和Nb₂O₅较大地提高了碲酸盐玻璃的抗析晶热稳定性, 钨铌碲酸盐玻璃最大抗析晶热稳定性ΔT达154℃. 拉曼光谱研究表明,WO₃和Nb₂O₅的加入使碲酸盐玻璃在921和862cm^-1附近出现特征谱带, 导致拉曼光谱中高频移区从550cm^-1延伸扩展到950cm^-1, 从而有效地拓宽了碲酸盐玻璃的拉曼带宽, 钨铌碲酸盐玻璃最大拉曼光谱半高宽可达355cm^-1. 实验研究表明,钨铌碲酸盐玻璃是宽带拉曼光纤放大器的候选材料之一.     

掺Er3+氟铅硅酸盐玻璃的光谱性质和热稳定性研究

制备了掺Er^3 氟铅硅酸盐玻璃，研究了玻璃的物理性质、热稳定性、吸收光谱、荧光光谱和荧光寿命，应用McCumber理论，计算了能级^4I13／2→^4I15／2跃迁的吸收和受激发射截面．结果表明：以PbF2等分子替代PbO含量，样品密度、折射率、热稳定性、吸收截面和受激发射截面降低，但荧光半高宽和荧光寿命增加，对Er^3 离子在不同玻璃基质中带宽特性的比较发现，Er^3 掺杂50SiO2—50PbF2玻璃的带宽特性与碲酸盐和铋酸盐玻璃相当，大于磷酸盐，锗酸盐和硅酸盐玻璃，表明掺Er^3 氟铅硅酸盐玻璃可作为宽带光纤放大器的基质材料。     

OH- 对 Tm3+/Yb3+ 共掺碲酸盐玻璃上转换发光的影响

研究了Tm3 /Yb3 共掺碲酸盐玻璃的Raman光谱、红外光谱和上转换发光光谱,分析了OH-对Tm3 上转换发光的影响。结果表明,氧氯碲酸盐玻璃的声子能量高于氧氟碲酸盐玻璃的声子能量,但是Tm3 /Yb3 共掺氧氟碲酸盐玻璃的上转换发光强度高于Tm3 /Yb3 共掺氧氯碲酸盐玻璃。分析认为这主要是由于OH-的影响,在氧氟碲酸盐玻璃中OH-的浓度较低,导致Tm3 的荧光寿命高,从而提高Tm3 的上转换发光。在一定程度上,OH-对Tm3 上转换发光的影响大于声子能量对Tm3 上转换发光的影响。研究结果有助于进一步提高Tm3 的发光效率。     

碱金属和碱土金属对掺Tm3+碲酸盐玻璃光谱性质的影响

研究了碱金属和碱土金属离子修饰的掺铥碲酸盐玻璃的光谱性质,讨论了碱金属和碱土金属对掺铥碲酸盐玻璃J-O强度参数、1.46μm荧光发射强度、荧光半高宽、受激发射截面等光谱性质的影响,并与一些传统氧化物玻璃进行了比较.研究表明碱金属Li 和碱土金属Ba2 掺碲酸盐玻璃更适宜用作掺铥光放大器基质.含Li 的碲酸盐玻璃展现出7.90×10-21cm2的高发射截面;含Ba2 碲酸盐玻璃具有7.55×10-21cm2的高发射截面、103nm的荧光半高宽.     

TeO2-Nb2O5-BaCl2-AlF3玻璃系统结构及光学性能研究

用传统熔融法制备了一种新型的氧卤碲酸盐玻璃:(80-x)TeO2-10Nb2O5-10BaCl2-xAlF3(x=10、20和30),用密度比重天平、玻璃热膨胀仪、棱镜耦合仪、显微拉曼光谱仪和红外-可见-紫外分光光度计研究了组分变化对物理性能、结构及光学性质的影响。研究结果表明,随着玻璃中AlF3含量增加,玻璃的密度和折射率减小;在Tg温度前,玻璃的平均线膨胀系数α减小;玻璃的热稳定性增强;玻璃结构中的双三角锥体[TeO4]和变形的双三角锥体[TeO3+1]以及三角棱锥体[TeO3]相对含量都相应减少;玻璃在紫外吸收边出现了蓝移现象,玻璃的直接和间接光学帯隙都增大。     

TeO2对氟铝酸盐玻璃性质和结构的影响

以10MgF2—20CaF2—10SrF2—10BaF2—15YF3—35AlF3氟铝酸盐玻璃为基玻璃引入不同含量的TeO2得到了新的氟碲铝酸盐玻璃．用差热分析方法研究了TeO2对氟铝酸盐玻璃性能的影响，通过拉曼光谱和红外吸收谱来研究玻璃的结构变化．差热分析表明TeO2的增加使玻璃开始析晶温度瓦升高，融化温度％降低，成玻璃能力增加．玻璃结构分析表明氟碲铝酸盐玻璃的结构中存在[FnAl-O—AlFn]、[TeO3]、[TeO2F]和[TeOF2]等多面体，这些多面体由F^-和O^2-离子连接．这种新的氟碲铝酸盐玻璃有着良好的成玻璃能力，在0．75～5．00μm范围内玻璃具有很高的透过率，是一种具有应用前景的新的红外光学玻璃材料．     

TeO_2-Nb_2O_5-BaO-BaCl_2系统玻璃结构及银纳米晶引入研究

碲酸盐氧卤玻璃具有低声子能以及较好的稳定性和析晶性能等优秀的综合品质,是一类很有前途的光学玻璃材料。采用熔融法制备了不同组成的TeO2-Nb2O5-BaO-BaCl2系统玻璃,研究了网络结构变化和组成对该系统玻璃的成玻璃性能和析晶性能的影响,同时探讨了向玻璃基体内引入银纳米晶体的可能性。结果表明,BaCl2的引入使得玻璃网络结构中键合及基团种类增多,碲氧链间的连接加强,网络结构更加紧密,并且成玻璃区域有所扩展。TeO2-Nb2O5-BaO-BaCl2系统玻璃基体在保持自身结构稳定性的同时,更有利于AgCl纳米晶体析出,是一种适合金属纳米晶掺杂的优良光学玻璃基体材料。     

Pr3+掺杂铋碲酸盐玻璃的热膨胀与可见荧光发射

制备了Pr3 掺杂的高折射率7.5Li2O-7.5K2O-5BaO-5Bi2O3-75TeO2重金属铋碲酸盐玻璃.测定了玻璃的热膨胀曲线,计算了样品的热膨胀系数α,转变温度Tg和软化温度Tf.紫外灯下观察,Pr3 掺杂的玻璃样品发出橙红光.室温下记录了玻璃样品的吸收、激发和荧光发射光谱.光谱分析表明:紫外灯、蓝色激光二极管、蓝色发光二极管,以及氩离子激光器是Pr3 掺杂铋碲酸盐玻璃的有效激发光源.     

Thermodynamic properties of seven gaseous halogenated hydrocarbons from acoustic measurements: CHClFCF3, CHF2 CF3, CF3 CH3, CHF2CH3, CF3CHFCHF2, CF3CH2CF3, and CHF2CF2CH2F

Measurements of the speed of sound in seven halogenated hydrocarbons are presented. The compounds in this study are 1-chloro-1,2,2,2-tetrafluoroethane (CHClFCF₃ or HCFC-124), pentafluoroethane (CHF₂ CF₃ or HFC-125), 1,1,1-trifluoroethane (CF₃CH₃ or HFC-143a), 1,1-difluoroethane (CHF₂CH₃ or HFC-152a), 1,1,1,2,3,3-hexafluoropropane (CF₃CHFCHF₂ or HFC-236ea), 1,1,1,3,3,3-hexafluoropropane (CF₃CH₂CF₃ or HFC-236fa), and 1,1,2,2,3-pentafluoropropane (CHF₂CF₂CH₂F or HFC-245ca). The measurements were performed with a cylindrical resonator at temperatures between 240 and 400 K and at pressures up to 1.0 MPa. Ideal-gas heat capacities and acoustic virial coefficients were directly deduced from the data. The ideal-gas heat capacity of HFC-125 from this work differs from spectroscopic calculations by less than 0.2% over the measurement range. The coefficients for virial equations of state were obtained from the acoustic data and hard-core square-well intermolecular potentials. Gas densities that were calculated from the virial equations of state for HCFC-124 and HFC-125 differ from independent density measurements by at most 0.15%, for the ranges of temperature and pressure over which both acoustic and Burnett data exist. The uncertainties in the derived properties for the other five compounds are comparable to those for HCFC-124 and HFC-125.     

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.     

Calculation of the Quasiternary Systems:Si_3N_4-Y_2O_3-SiO_2,Y_2O_3-SiO_2-BeO and Y_2O_3-Al_2O_3-BeO

Based on the thermodynamic model of Kaufman for the calculation of quasibinary and quasiternary system, numerical method for the calculation of stable equilibrium is developed and thermodynamic data of undefined phases are discussed in this work for several ceramic systems.The calculated isothermal sections in Si3N4-Y2O3-SiO2 system meet well with other previous calculated phase diagrams and experimental results. The diagrams in Y2O3-SiO2-BeO and Y2O3-Al2O3-BeO systems are calculated for the approach of prediction.     

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.     

溶胶凝胶法制备Er3+-Yb3+共掺纳米SiO2粉

利用溶胶-凝胶法合成了Er2O3-Yb2O3-SiO2纳米二氧化硅(SiO2)粉。Er3 和Yb3 直接加入有机酸催化的TEOS反应溶液中,凝胶后经过700~900℃,得到Er3 -Yb3 共掺纳米SiO2粉。样品经过红外光谱、XRD、TEM等分析,结果表明,纳米粉的粒径受有机酸比例和处理温度的影响。在室温PL谱上,样品可观察到较强的1530nm荧光,同时镱的引入对掺铒SiO2纳米粉在1.54μm的荧光发射有增强作用。     

Subsolidus,high temperature phase relations in the systems Al2O3-Cr2O3-ZrO2, MgO-Cr2O3-ZrO2 and MgO-Al2O3-ZrO2

In the temperature range 1600 to 1900° C, the system A₂O₃-Cr₂O₃-ZrO₂ is characterized by the coexistence of ZrO₂ (unstablilized) and an (Al, Cr)₂O₃ solid solution series. In the systems MgO-Cr₂O₃-ZrO₂ and MgO-Al₂O₃-ZrO₂ a nearly stoichiometric spinel coexists with both stabilized and unstabilized ZrO₂. At temperatures above 1600°C a new ternary Mg-Al-Zr oxide becomes stable in the MgO-rich part of the MgO-Al₂O₃-ZrO₂ system.     

Si_2N_2O-Al_2O_3-La_2O_3和Si_2N_2O-Al_2O_3-CaO系统的亚固相关系

本文给出了 Si_2N_2O-Al_2O_3-La_2O_3和 Si_2N_2O-Al_2O_3-CaO 系统的亚固相图。实验结果表明:在 Si_2N_2O-Al_2O_3-CaO 系统中有一个未知结构的新化合物 CaO·Si_2N_2O,在3CaO·Si_2N_2O 和3CaO·Al_2O_3两化合物之间形成连续立方固溶体。而 Si_2N_2O-Al_2O_3-La_2O_3系统中则没有发现新化合物。在两个系统的富 Si_2N_2O区,过量的 Si_2N_2O 与 La_2O_3和 CaO 分别反应形成 Si_3N_4与 La_(10)[SiO_4]_(?)N_2(H-相)(和 CaSiO_3。所研究的这两个三元系统中,分别形成了如下几个四元相容性区。在 Si_2N_2O-Al_2O_3-La_2O_3系统内有:H-Si_3N_4-La_2O_3·Si_2N_2O-La_2O_3·Al_2O_3;H-Si_3N_4-La_2O_3·Al_2O_3-La_2O_3·11 Al_2O_3;H-Si_3N_4-La_2O_3·11 Al_2O_3-Al_2O_3;H-Si_3N_4-Al_2O_3-O′s.s;H-Si_3N_4-O′s.s-Si_2N_2O在 Si_2N_2O-Al_2O_3-CaO 系统内有:Si_3N_4-CaSiO_3-CaO·Si_2N_2O-3CaO·Al_2O_3;Si_3N_3-CaSiO_3-3CaO·Al_2O_3-2CaO·Al_2O_3·SiO_(?);Si_(?)N_(?)-CaSiO_3-2CaO·Al_2O_3·SiO_2-Al_2O_3;Si_3N_4-CaSiO_3-Al_2O_(?)-O′s.s;Si_3N_4-CaSiO_3-O′s.s-Si_(?)N_(?)O