硫系玻璃动力学强弱性评测方法

玻璃动力学强弱性指数m值的主要评测方法有两种:通过玻璃转变温度附近黏温关系测试直接获得mvis值;基于量热分析,根据不同升温速率获得假想温度,并假定玻璃转变温度范围内假想温度Tf符合Arrhenius关系,通过理论推导间接获得mDSC值。由于玻璃转变温度范围内假想温度Tf和黏度的关系实际上并非严格遵循Arrhenius关系,因此mDSC和mvis之间存在偏差。以系列商用硫系玻璃为例,通过两种评测方法比较,建立了通过mDSC推算mvis的经验公式,实现了准确、快速的评测硫系玻璃动力学强弱性。     

脉冲激光沉积Ge-Ga-S-CdS非晶薄膜

采用脉冲激光沉积(PLD)法在载玻片上沉积了Ge-Ga-S-CdS硫系非晶薄膜,利用XRD、分光光度计、扫描电镜、XPS等现代测试手段,研究薄膜的结晶形态、光学性质和成分。结果发现,利用脉冲激光沉积方法获得了可见光透过率为80%、光学质量优良、厚度均匀、没有明显缺陷的Ge-Ga-S-CdS硫系非晶薄膜,XPS光电子能谱结果显示薄膜成分与靶材的成分存在微小的偏差。     

ZnO·Al2O3·nSiO2玻璃抗裂纹萌生能力反常演化的结构起源探索

为探究ZnO·Al₂O₃·nSiO₂玻璃抗裂纹萌生能力(C_R)随SiO₂含量变化的演化规律,制备了一系列不同n值(n=2,2.35,2.5,2.65,3,3.5)的样品。基于C_R和结构表征发现,C_R随着n的增加呈先增大后减小的反常演化,并于n=2.5时出现极值(31.1 N)。这是源于随着n增大:(1)原子堆积份数逐渐减小,可致密化体积逐渐增加,从而导致C_R逐步提高;(2)Al—O多面体结构单元含量逐步减少,导致C_R逐步下降;(3)考虑到相界面对裂纹生长的强阻挡能力,中程异构分相(富Al和富Si相)致相界面数量呈先增多后减少的变化趋势,导致C_R产生类似的非单调演化。上述三个因素的竞争和协同作用是该体系中C_R呈反常演化的结构起源,但考虑到极值点附近较小的组分变化,中程异构致相界面数量随n增加呈现的非单调演变才应是C_R呈反常演化的主要结构根源。     

Na2O-Bi2O3-B2O3体系玻璃的形成和结构研究

采用熔融急冷法制备Na2 O -Bi2 O3-B2 O3体系玻璃。X射线粉末衍射表明该体系的成玻性能较好 ,成玻范围较宽 ;密度、粉末透红外光谱和TSDC研究表明 ,玻璃中的硼元素具有“硼反常”现象 ,铋元素有〔BiO3〕和〔BiO6 〕两种微结构 ,玻璃中的碱金属离子以及硼元素和铋元素的微结构在外场作用下定向排列 ,表现出明显的SHG效应。     

GeS2-Ga2S3-CdS玻璃的折射率与三阶非线性光学性能

采用熔融-急冷法制备了GeS2-Ga2S3-CdS硫系玻璃,用椭圆偏振仪、飞秒光Kerr技术分别测试了在室温玻璃的折射率和三阶非线性光学性能,分析了玻璃的组成、结构对玻璃的折射率与三阶非线性光学性能的影响.结果表明:玻璃的折射率主要决定于Ge的含量;玻璃的三阶非线性极化率χ(3)与玻璃中S-Ge,S--Ga键的数量有关,当玻璃中S-Ge,S-Ga键的数量最多时,离子极化程度最大.电子云的变形程度最大时,具有最大的χ(3).玻璃的超快三阶非线性光学系数与线性折射率n间的关系不遵循Miller规则.     

铝硅准二元玻璃硬度和抗碎裂性演化的结构起源

为探究准二元铝硅玻璃硬度和抗碎裂性随组分变化的结构起源,采用激光加热气动悬浮技术,制备了组分为xAl2O3·(100–x)SiO2(30≤x≤63,摩尔分数)的系列玻璃样品.利用显微维氏硬度仪对玻璃的硬度、抗碎裂性进行了详细表征.结果表明:随着Al2O3含量增加,玻璃硬度逐渐升高,于x=63时硬度最大(8.94 GPa...     

Effects of Six-fold Coordinated Silicon on Structure and Properties of BaO-SiO_2-P_2O_5 Glasses

We studied the local structure and properties of six-fold coordinated silicon(Si~([6])) in BaOSiO_2-P_2O_5 glasses. Nuclear magnetic resonance(NMR) and Raman spectroscopy revealed the existence of sixfold coordinated silicon species and network former units(NFUs) in the BaO-SiO_2-P_2O_5 glasses. The glass transition temperature(Tg), which was measured by differential scanning calorimetry, increased rapidly along with the increase of SiO_2 from 0 to 10 mol%, then declined and finally increased again, which showed a "Z" trend along with the increase of SiO_2 while the density of the glasses showed the opposite trend. When the addition of SiO_2 is 16 mol%, Tg decreased to an extremely low value(807.9 K). Besides, the Vickers indentation hardness(Hv) had been significantly enhanced from 4.66 to 6.63 GPa by adding 16 mol% SiO_2. Furthermore, the liquid fragility index(m) of the glasses declined slowly firstly and then increased rapidly when the amount of SiO_2 is greater than 13 mol%.     

脉冲激光沉积硫化锗-硫化稼-硫化镉非晶薄膜的结构和性能

用脉冲激光沉积(pulsed laser deposition,PLD)法在玻璃基片上沉积了组分为80GeS2-15Ga2S3-5CdS的硫系非晶薄膜,利用x射线衍射、分光光度计、扫描电镜、场发射扫描电镜、Raman光谱等研究了薄膜的性能和结构.对薄膜进行紫外脉冲激光极化,采用Maker条纹法测试薄膜的二阶非线性光学效应(second harmonic generation,SHG).结果表明:获得的硫系GeS2-Ga2S3-CdS非晶薄膜表面光滑平整、厚度约为8000m、透过率高达78%,与靶材相比,薄膜中的缺陷较多.在紫外脉冲激光极化的薄膜中观察到了明显的SHG,强度约为参考石英单晶的两倍.     

Properties and Microstructure of GeS_2-Ga_2S_3-CdS Glasses

1Introduction OsterbergUetal[1]firstlydetectedtheSecond Har monicGeneration(SHG)bythelaser inducedmethodin GeO2SiO2glassfiber,andMyersRAetal[2]observed SHGeffectinSiO2bulkglassesafterpolarizationwitha strongelectronicfield.Sincethenthescholarsalloverthe w…     

PLD preparation of GeS6 amorphous film and investigation on its photo-induced darkening phenomenon

GeS6 chalcogenide amorphous fi lm was deposited on glass substrate via PLD（pulsed laser deposition） technique. The performance and structure of the fi lm was characterized by XRD（X-ray diffraction）, SEM（Scanning Electron Microscopy）, EDS（Energy Dispersive Spectroscopy）, optical transmission spectra, and Raman spectra, etc. The GeS6 amorphous fi lm was irradiated by 532 nm linearly polarized light, and its photoinduced darkening was investigated. The results showed that the GeS6 chalcogenide amorphous fi lm was smooth and compact with uniform thickness and combined with the substrate fi rmly, and its chemical composition was in consistency with the bulky target. When laser energy was fi xed, the transparence of the fi lm declined with the increase of the laser irradiation time. Obvious photo-induced darkening and relaxation phenomenon of the fi lm after laser irradiation were observed in this investigation.