玻璃中结构弛豫的红外发散响应

本文将红外发散响应理论应用到玻璃中结构缺陷的二能级模型,解释了超声吸收的双峰结构,特别是提出了小峰的存在对频率的依赖关系。并且在引入热激活有效势的基础上,对SiO₂在整个温区的吸收曲线进行了成功的拟合。 关键词：     

Bi离子掺杂GeO2-Al2O3-M(M=Na2O，BaO，Y2O3)玻璃的光学性质

用高温熔融法制备了Bi离子掺杂浓度为1mol%的GeO-B₂O₃-Na₂O (GBNB)，GeO₂-Al₂O₃-Na₂O(GANB)，GeO₂-Al₂O₃-BaO(GABB)和GeO₂-Al₂O₃-Y₂O₃(GAYB)玻璃.测定了样品玻璃的差热曲线、吸收、发射光谱及荧光衰减曲线.实验发现GBNB，GANB，GAYB，GABB的吸收边带逐步发生红移.由于这些吸收边带是由Bi³⁺的6s²电子到Bi⁵⁺ 6s⁰空轨道的跃迁引起.因此推断GBNB，GANB，GAYB，GABB玻璃中Bi⁵⁺离子的含量逐步增加.在GABB，GAYB，GANB三个样品中观察到发光中心约1220nm超宽带荧光发射.荧光强度从GABB，GAYB，GANB逐步减弱，荧光半高宽和荧光寿命逐步变小.这些超宽带的荧光归属为Bi⁵⁺离子的发光所致.从吸收与荧光光谱的变化，推断在GeO₂-Al₂O₃玻璃中引入BaO，Y₂O₃组分有利于Bi⁵⁺离子的形成.讨论了BaO，Y₂O₃化学组分对Bi离子在玻璃中的价态影响的内在机理. 关键词： 5+离子')" href="#">Bi⁵⁺离子 超宽带发光 吸收带 荧光寿命     

PbI2对远红外Te基硫系玻璃光学性能的影响

用传统的熔融淬冷法制备了一系列新型Ge-Te-PbI₂硫系玻璃,并且讨论了玻璃的形成区域. 利用X射线衍射(XRD)、差热分析(DTA)、可见/近红外吸收光谱、红外透过光谱等技术,研究重金属卤化物PbI₂对Ge-Te硫系玻璃组成、结构和性能的影响. 利用Tauc方程计算了样品的直接和间接光学带隙,根据金属标准和能量带隙理论讨论了玻璃光学带隙与组分变化的关系. 结果表明:PbI₂的引入,提高了Te玻璃的形成能力,而且玻璃的热稳定性良好;随着PbI₂含量的增加,玻璃的密度和折射率均增大,光学带隙减小,短波吸收截止边发生红移,玻璃的红外截止波长基本不变,达到了25 μm. 该系列玻璃可用于制备远红外长波波导器件. 关键词： Te基玻璃 2')" href="#">PbI₂ 光学带隙 红外光谱     

Ga2S3-Sb2S3-Ag2S硫系玻璃和光纤的制备及性能研究

本工作确定了一种新型的Ga₂S₃-Sb₂S₃-Ag₂S硫系玻璃体系的玻璃形成区,研究了玻璃的热稳定性和光学性能、稀土离子掺杂玻璃的中红外发光特性以及玻璃的成纤性能,评估了该玻璃在中红外波段的应用潜力.实验结果表明,Ga₂S₃-Sb₂S₃-Ag₂S体系的玻璃形成区为～10%—30%Ga₂S₃,～60%—80%Sb₂S₃和～0—15%Ag₂S(均为摩尔分数);该玻璃具有较宽的红外透过范围(～0.8—13.5μm)、较高的线性折射率(～2.564—2.713@10μm)和较大的三阶非线性折射率(～9.7×10^-14—15.7×10^-14 cm²/W@1.55μm);使用1.32μm激光抽运,稀土离子Dy...     

AgI(Cr2O3)复合离子导体的光谱研究

本文研究了AgI(Cr₂O₃)复合离子导体的红外吸收光谱,近紫外、可见反射光谱。发现复合离子导体的两种谱图均与纯AgI,Cr₂O₃的不同。红外吸收光谱在882—889cm^-1处有一新吸收峰。电子谱中,AgI从430nm开始向长波方向表现的光离解特性消失。本来Cr₂O₃由配位场效应而引起的d—d吸收跃迁以410nm,530nm为中心的反射谱带,现在410nm处的谱带消失。530nm处的谱带稍有红移,且随加入Cr₂O₃量的增多而强度减弱。代之以整个紫外、可见区的较强吸收。对此,结合透射电子显微镜的分析,用双声子耦合和介质的变形极化以及配位场理论对AgI(Cr₂O₃)复合离子导体的声子谱和电子谱进行了解析。 关键词：     

Er3+/Yb3+共掺碲硼硅酸盐玻璃的光谱性质和热稳定性研究

制备了系列Er³⁺/Yb³⁺共掺碲硼硅酸盐玻璃样品(85-x)TeO₂-15B₂O₃-xSiO₂ (TBS x=0,5,10,15,20 mol%).测试和分析了样品的吸收光谱、荧光光谱、能级寿命、红外透射光谱及差热特性.并通过对Er³⁺离子⁴I_13/2→⁴I_15/2跃迁发射谱线的高斯拟合，设计了一个简单的四能级结构估算了Er³⁺离子⁴I_13/2和⁴I_15/2能级在碲硼硅酸盐中的Stark分裂情况.研究表明SiO₂的引入能有效地改善玻璃的热稳定性和光谱性能，玻璃析晶温度T_x与玻璃转变温度T_g之差(ΔT=T_x-T_g)可达178℃，说明碲硼硅酸盐是一种适合于光纤拉制的玻璃基质材料.比较了不同基质玻璃中Er³⁺离子的荧光半高宽和受激发射截面，结果表明TBS玻璃系统具有较好的带宽性能，是一种优良的宽带光纤放大器候选基质材料. 关键词： 碲硼硅酸盐 热稳定性 高斯拟合 -基')" href="#">OH^-基     

Ag@SiO2纳米核壳结构对铒碲发光玻璃的发光增强机制

本研究首次把预先制备好的Ag@SiO₂纳米核壳结构成功地引进到碲化物发光玻璃70TeO₂-25ZnO-5La₂O₃-0.5Er₂O₃体内,发现(A)Ag(1.6×10^?6mol/L)@SiO₂(40 nm)@Er³⁺(0.5%):铒碲发光玻璃相对于样品(B)Er³⁺(0.5%):铒碲发光玻璃的可见光与红外光的激发光谱强度的最大增强依次为149.0%与161.5%,可见光与红外光的发光光谱强度则依次最大增强了155.2%与151.6%,同时还发现样品(A)相对于样品(B)的寿命显著变长。由于Ag@SiO₂的表面等离子体吸收峰恰好位于546.0 nm,它与铒离子的发光峰546.0 nm完全共振,因此,Ag@SiO₂对铒碲发光玻璃的发光共振增强作用显著。由于银的纳米核壳结构与玻璃的制作具有分步实现的优点,它既能成功控制Ag@SiO₂的尺寸,而且在Ag@SiO₂@Er:铒碲发光玻璃的制作过程中还具有可操作性强的优点,同时价格也更加便宜。在保证银不被氧化的前提下,还可控制稀土离子发光中心与银的表面等离子体之间的距离,因此能够成功地减少背向能量反传递。上述优点促成了Ag@SiO₂纳米核壳结构表面等离子体有效加强了Ag@SiO₂@Er³⁺:铒碲发光玻璃的常规光致发光强度。     

垂直排列液晶盒中反铁电液晶TFMHxPOCBC-D2偏振红外光谱研究

本文通过偏振红外吸收光谱研究了铁电与反铁电液晶分子TFMHxPOCBC-D₂(4-(trifluoromethylhexy-3-d₂ carbonyl)phenyl 4′-octyloxybiphenyl caboxylate)在垂直排列取向液晶盒中CD₂基团绕手征性烷基链转动的受阻行为.实验结果显示CD₂的偏振红外吸收在Sm-C相不同于Sm-C_A相.建立了一个CD₂转动受阻模型,在这一模型的基础上,对CD₂的偏振红外吸收进行了模拟计算,较好地解释了CD₂红外吸收在铁电和反铁电液晶相下的行为差异,得到了CD₂基团绕手征性烷基链转动受阻的结论. 关键词： 反铁电液晶 红外光谱 受阻转动     

Er3+掺杂的Bi2O3-B2O3-SiO2玻璃的光谱性质

测试了Bi₂O₃-B₂O₃-SiO₂玻璃中的Er³⁺离子的吸收光谱、发射光谱、⁴I_13/2的荧光寿命、拉曼光谱,及OH^-的傅里叶红外吸收光谱。应用Judd-Ofelt理论计算了该玻璃中的Er³⁺离子的J-O参数、振子强度、⁴I_13/2能级的寿命,从而利用测得的⁴I_13/2的荧光寿命得出了⁴I_13/2能级的量子效率(15%)。由于较低量子效率可能与OH^-有关,所以计算了玻璃中的OH^-浓度,发现其浓度较高(1.66×10¹⁹cm^-1,相当于Er³⁺浓度的3倍)。应用McCumber理论和四能级模型计算了Er³⁺离子的受激发射截面和荧光发射光谱的半峰全宽,结果与通过吸收光谱计算所得基本吻合。根据透射率和折射率的关系计算了折射率,发现和测量值相差很大,说明有较大的散射,通过拉曼光谱和显微镜测试,认为是玻璃中的微小气泡造成的。     

Er3+离子掺杂钡镓锗玻璃上转换发光机理研究

研究了Er³⁺离子掺杂钡镓锗玻璃的吸收光谱、拉曼光谱和上转换光谱.分析了Er³⁺离子在钡镓锗玻璃中的上转换发光机理.结果表明：玻璃的最大声子能量为828cm^-1，紫外截止波长为275nm.采用800nm和980nmLD激发玻璃样品，在室温下观察到强烈的上转换绿光和红光发射.随着Er³⁺离子浓度的增加，绿光发光强度先增加后减小，而红光发光强度呈单调递增趋势.能量分析表明：800nmLD激发产生的绿光主要源于Er³⁺离子4I_13/2能级的激发态吸收过程；红光发射主要源于Er³⁺离子4I_13/2能级与4I_11/2能级之间的能量转移过程.980nmLD激发产生的绿光主要源于Er³⁺离子4I_11/2能级之间的能量转移过程；而红光发射主要源于Er³⁺离子4I_13/2能级与4I_11/2能级之间的能量转移过程和4I_13/2能级的激发态吸收过程.通过量子效率分析，发现采用800nmLD激发Er³⁺离子掺杂浓度为1mol% 的样品时，上转换绿光发光效率最高. 关键词： 上转换发光机理 3+离子掺杂')" href="#">Er³⁺离子掺杂 钡镓锗玻璃     

Low activation energies in superionic glasses in the 4.2–77 K temperature region

The peaks in the ultrasonic attenuation observed in AgI-doped superionic glasses at temperatures higher than 77 K have always been explained in terms of classical, thermally activated, relaxation processes due to silver ions which are mobile in the glassy matrix. Here we complete an ultrasonic study with the loss characteristics and sound velocity in “binary” (Ag₂O·nB₂O₃) and “ternary” [(AgI)_x(Ag₂O·nB₂O₃) _{1 − x}] glasses in the 4.2–77 K temperature region. In such a way we obtain useful information about defects having low activation energy.     

Structure and elastic properties of TeO2-BaF2 glasses

Binary tellurite (100−x)TeO₂-xBaF₂ glasses for different compositions of BaF₂ (x=8, 10, 12, 15, 18 and 20 wt%) have been prepared by rapid quenching method. The velocities and attenuation during the propagation of the ultrasonic waves in all glasses were measured using a transducer operated at a fundamental frequency of 5 MHz at room temperature. A progressive increase in BaF₂ content leads to a decrease in ultrasonic velocities and density, which is followed by an increase in attenuation. The existence of depolymerisation of Te co-ordination leads to the transformation of TeO₄ trigonal bipyramid units through TeO₃₊₁ polyhedron to TeO₃ trigonal pyramid units. This is responsible for the observed decrease in the measured and determined parameters with the addition of the modifier content.     

Structural investigation of bismuth borate glasses under the influence of γ-irradiation through ultrasonic studies

The ultrasonic velocity and attenuation measurements for different compositions of irradiated heavy metal oxide (HMO) borate glasses xBi₂O₃ (1−x) B₂O₃ (where x=0.25, 0.30, 0.35, 0.40, 0.45) has been investigated at room temperature (303 K) using pulse echo overlap method. The elastic moduli, Debye temperature, Poisson's ratio and other acoustical parameters have been obtained from experimental data. Structural changes after irradiation have been investigated by using FTIR spectroscopy and ultrasonic studies. As the changes are strongly dependent on the internal structure of the absorbing substance, in the present investigation ultrasonic velocities before and after γ-irradiation in bismuth borate glasses are measured as a function of composition, from which the structural changes in the network former B₂O₃ and modifier Bi₂O₃ due to irradiation are obtained.     

Ultrasonic relaxation in Zinc-Borate glasses

Borate glasses in the system (1 − x) [29Na₂O − 4Al₂O₃ − 67B₂O₃] − x ZnO with (x = 0, 5, 10, 15, 20, 25, 30, and 35 mol%), have been prepared by the melt quenching technique. The longitudinal ultrasonic attenuation of the prepared sample has been measured using the pulse echo technique at ultrasonic frequencies 2, 4, 6 and 8 MHz in the temperature range between 160 and 300 K. The results showed well-defined peak whose position shifts toward higher temperature with increasing frequency. The mean activation energy is strongly composition sensitive. The position and overall shape of the loss peaks in dependence on composition were analyzed in terms of an assumed loss of standard linear solid type with low dispersion, and a broad distribution of Arrhenius-type relaxation with temperature independent relaxation strength. The dependence of ultrasonic attenuation on temperature has been interpreted in terms of a thermally activated relaxation process which arises when ultrasonic waves disturb the equilibrium of an atom moving in a double-well potential in the glass network. The dependence of activation energy on composition suggests that the structure of these glasses changes at 15 mol% ZnO concentration.     

Piezoelectric constant and conductivity relaxation in n-type InP from ultrasonic attenuation measurements

Measurements have been made of the attenuation of 30, 90 and 150 MHz {111}; longitudinal ultrasonic waves and of the d.c. resistivity in chromium-doped, n-type InP from -50 to +150°C. From the attenuation maximum observed for 30 MHz waves we find γe₁₄γ = 0.040 C/m².     

Anelastic effects in (AgI)x(Ag2O·B2O3)1−x superionic glasses

We present here the first measurements of acoustic absorption in (AgI)_x(Ag₂O·B₂O₃)_1?x superionic glasses at ultrasonic frequencies (5–45 MHz) and in the 80–434 K temperature range. The attenuation shows, at decreasing temperature, an unusually high peak which seems to be attributed to a thermally activated relaxation process. A possible microscopic explanation of this anomaly is proposed, in connection with the presence of mobile ions in those materials.     

LaCoO3中自旋态转变现象的超声研究

测量了LaCoO₃单相多晶样品的纵波与横波超声声速和衰减随温度的变化关系, 在材料的自 旋态转变温度附近（≈90K），纵波声速出现明显的软化并伴随一个尖锐的衰减峰，但是在 横波的测量中却没有出现类似的超声异常，分析认为LaCoO₃在90K附近的自旋态 转变是由于Co³⁺离子是从低自旋态(LS,t⁶_2ge⁰ _g)转变到中等自旋态(IS,t⁵ _2ge¹_g )，而不是高等自旋态(HS,t⁴_2ge²_g).随着温度的升高，在 200K附近纵波和横波测量上都观察到一个伴随着微小声速软化的宽大的衰减峰，这可能是随 机分布的IS态Co³⁺离子的Jahn-Teller效应导致的局域晶格扭曲所造成的. 关键词： 超声声速与衰减 自旋态转变 Jahn-Teller效应     

Measurement of optical dephasing of Eu3+ and Pr3+ doped silicate glasses by spectral holeburning

Long-lived spectral holeburning has been observed in Eu³⁺ and Pr³⁺ doped silicate glasses, and used to measure homogeneous linewidths (φ_h). In the case of Eu³⁺, holes are burned by optical pumping of nuclear quadrupole levels, and our low temperature measurement of φ_h shows that the previously determined T^1.8 temperature dependence holds down to at least 1.6 K. On the other hand, in Pr³⁺ doped glass, holes are burned by optically induced local lattice rearrangements. In contrast to previously studied inorganic glasses, we find a linear temperature dependence of φ_h for the ³H₄ ? ¹D₂ transition from 1.6 K to 20 K. This was confirmed by picosecond accumulated grating photon echoes. Current theories of dephasing in glasses do not predict these temperature dependences. Holeburning has also been observed in Pr³⁺ doped BeF₂ and phosphate glasses and Nd³⁺ doped silicate glass and thus appears to be a rather general phenomenon in inorganic glasses, as has been found for molecules in organic glasses.     

Hypersonic secondary relaxation due to fast ion diffusion modes in xLiCl0.5Li2OB2O3 glasses

The hypersonic attenuation and the sound velocity for a high and a low conducting Li⁺-glass, 0.7LiCl0.5Li₂OB₂O₃ and 0.5Li₂OB₂O₃, respectively, have been measured as functions of temperature by Brillouin scattering. A large excess hypersonic attenuation was found at high temperatures in the LiCl rich glass compared to the low conducting glass. The effect is attributed to structural relaxation of fast ion diffusion modes involving Li⁺ ions jumping between different sites in the glass network. The sound velocity observed for the LiCl doped glass was 10% lower than the value for the undoped glass. This reflects considerable changes in the elastic properties of the glass network in accordance with a model which proposes that the high conductivity in these glasses can be explained by structural changes of the intermediate range order.     

非晶态快离子导体(AgI)x(Ag4P2O7)1-x的声学性质

用液氮骤冷方法制备了(AgI)_x(Ag₄P₂O₇)_1-x系列非晶态快离子导体。对AgI摩尔浓度x=0.50,0.60,0.67,0.75,0.80的样品,在77—300K温度范围及2,5,10,15MHz的频率上测量了纵波和横波的超声衰减和声速。发现在200—240K附近存在一个异常强的弛豫型超声吸收峰,随AgI含量的增加,该峰的位置向低温方向移动,且峰的高度增大。在实验的温度范围内,观察到纵波和 关键词：