超低密度SiO2气凝胶的制备及成型研究

 以正硅酸乙酯(TEOS)为硅源，采用酸碱二步催化溶胶-凝胶法，结合超临界干燥技术制备了超低密度SiO₂气凝胶,最低密度为3.4 mg/cm³；进一步结合成型工艺，在解决了模具设计和脱模技术后制备了具有不同密度的柱状和微型套筒样品，密度10～50 mg/cm³。研究了水、催化剂、稀释剂对二步溶胶-凝胶过程的影响，获得了制备低密度SiO₂气凝胶的最佳条件。利用扫描电镜、孔径分布及比表面积测试仪等对SiO₂气凝胶微结构进行了研究。结果表明，获得的超低密度SiO₂气凝胶具有较好的纳米网络，平均孔径18.9 nm，还具有高比表面积898 9 m²/g。     

碳气凝胶薄片的制备及表面密度致密层去除工艺

 研究了不同密度和厚度的碳气凝胶薄片的制备及其表面致密层去除工艺。在以间苯二酚、甲醛为原料制备有机及碳气凝胶块体材料的基础上，结合自制活动式微模具成型工艺，制备了厚度在80~350 μm，密度在50~600 mg·cm^-3范围内变化的碳气凝胶薄片。采用场发射扫描电镜、X射线相衬成像和表面轮廓仪-台阶仪等手段对其表面和内部微观结构进行了表征。测试结果表明，碳气凝胶薄片与块体的内部结构相同，但薄片表面存在一层和内部结构截然不同的致密层。采用不同粗糙程度的材料对薄片进行了表面微处理，成功去除该致密“皮”层。     

用SCLC法研究低k多孔SiO2:F薄膜的隙态密度

用溶胶-凝胶法制备了低k多孔SiO₂:F薄膜，用空间电荷限制电流法(SCLC)研究了多孔SiO₂:F薄膜中的隙态密度以及掺F量对隙态密度的影响，得到了平衡费米能级附近的隙态密度约为7×10¹⁵cm^-3·eV^-1，以及带隙中隙态随能量的分布. 并对造成隙态的主要原因也进行了讨论.     

碳气凝胶/聚苯乙烯双介质柱状靶的研制

 介绍了碳气凝胶/聚苯乙烯（CRF/CH）双介质柱状靶的制备方法。使用溶胶-凝胶法和微模具原位成型法制备了直径为820 μm的间苯二酚-甲醛（RF）气凝胶微柱,在氮气保护下进行高温碳化后得到直径为730 μm、密度为250 mg·cm^-3的CRF微柱;采用浸渍提拉法在CRF微柱柱面镀制一层厚度为26 μm 的CH薄膜, 形成CRF/CH双介质结构;采用机械微切割技术制备了长度为1 mm, 内径为730 μm,壁厚为26 μm的CRF/CH双介质柱状靶。实验研究了RF,CRF气凝胶微柱的制备工艺、微观形貌及CRF微柱轴向和径向的密度均匀性,探讨了影响CH薄膜厚度的主要因素,并对CH薄膜的表面形貌和两种材料之间的界面进行了表征。     

Nd掺杂对Bi4Ti3O12铁电薄膜的微结构和铁电性能的影响

利用溶胶-凝胶法在Pt/Ti/SiO₂/Si(100)衬底上制备了Nd掺杂Bi₄Ti₃O₁₂(Bi_4-xNd_xTi₃O₁₂, x=0.00,0.30,0.45,0.75,0.85,1.00,1.50)铁电薄膜样品.研究了Nd掺杂对Bi₄Ti₃O₁₂薄膜的微结构和铁电性能的影响.研究结果表明:Nd掺杂未改变Bi₄Ti₃O₁₂薄膜的基本晶体结构.在掺杂量x<0.45时,Nd³⁺只取代类钙钛矿层中的A位Bi³⁺.当x=0.45时,样品剩余极化强度达最大值,在270kV·cm^-1的电场下为32.7μC·cm^-2.掺杂量进一步增加时,结构无序度开始明显增大,Nd³⁺开始进入(Bi₂O₂)²⁺层,削弱其绝缘层和空间电荷库的作用,导致材料剩余极化逐渐下降.当掺杂量x达到1.50时,掺杂离子最终破坏(Bi₂O₂)²⁺层的结构,材料发生铁电-顺电相变.     

对苯二酚-甲醛碳气凝胶的制备

 溶胶-凝胶法制备了高HC比（10~40，对苯二酚与催化剂(Na₂CO_{3/sub>)的物质的量之比）的对苯二酚-甲醛有机气凝胶，并经高温碳化处理得到其碳气凝胶。借助有机气凝胶的红外光谱研究了其化学结构，说明其网孔结构形成的可能性；研究了有机气凝胶的扫描电镜图像、比表面积及孔径分布等，并得到碳化前后的一些对比数据：有机气凝胶颗粒大小30~50 nm，碳化后约为10 nm，比表面积从341.77 m²/g增大到452.75 m²/g，密度从0.170 8 g/cm^{3/sup>增大到0.335 6 g/cm3/sup>。}}     

种子法制备金掺杂二氧化硅气凝胶

 采用羟胺种子法合成了金掺杂二氧化硅气凝胶。采用紫外 可见光分光光度计研究了还原过程中体系的变化情况。使用透射电镜（TEM）研究了气凝胶的微观结构，气凝胶的比表面积和孔径分布由BET-BJH方法测试。结果表明通过种子法可以制备金掺杂质量分数0.01%~1.00%，密度25～50 mg／cm³，比表面积达800 m²/g以上的SiO₂气凝胶样品。     

块状Ta2O5-TiO2复合气凝胶的制备与表征

 以乙醇钽、钛酸丁酯为原料，以乙醇为溶剂，通过溶胶-凝胶法及超临界干燥成功制备了Ta₂O₅-TiO₂复合气凝胶。用场发射扫描电镜（SEM）、透射电镜（TEM）、扫描电镜模式下的电子能谱仪（EDS）以及比表面积吸附仪（BET）对其进行表征。结果表明:该气凝胶是由粒径在nm量级的Ti和Ta的羟基氧化物胶体颗粒堆积而成的低密度、高比表积的多孔网络结构材料，孔径分布主要集中在5~15 nm，比表面积为492.9 m²/g，密度为90 mg/cm³左右。     

SiO2分子的基态(X1A1)结构与分析势能函数

应用群论及原子分子反应静力学方法推导了SiO₂分子的电子态及其离解极限，采用B3P86方法，在6-311G^**水平上,优化出SiO₂基态分子稳定构型为单重态的C_2V构型，其平衡核间距R_e=R_Si—O=0.1587 nm,∠OSiO＝111.2°,能量为-440.4392 a.u..同时计算出基态的简正振动频率:对称伸缩振动频率ν(B₂)=945.4cm^-1，弯曲振动频率ν(A₁)=273.5 cm^-1和反对称伸缩振动频率ν(A₁)=1362.9cm^-1.在此基础上，使用多体项展式理论方法，导出了基态SiO₂分子的全空间解析势能函数，该势能函数准确再现了SiO₂(C_2V)平衡结构.     

改性SiO2气凝胶制备及其在ICF实验中的应用

 以正硅酸乙酯（TEOS）为前驱体，采用酸碱两步催化法制备了SiO₂醇凝胶。醇凝胶分别经过TEOS母液、甲基三乙氧基硅烷（MTEOS）处理后，以六甲基二硅胺烷（HMDSA）为疏水改性试剂，制备了改性SiO₂醇凝胶，醇凝胶经溶剂交换后以CO₂作为干燥介质，采用超临界干燥法制备了密度在30～100 mg/cm³的SiO₂气凝胶。用傅里叶变换红外光谱仪（FTIR）对疏水性SiO₂气凝胶进行了研究。研究结果表明,经过改性的气凝胶在潮湿环境中具有极好的尺寸稳定性和疏水性。采用精密车床加工得到了满足惯性约束聚变（ICF）物理试验要求的微柱。     

ICF分解实验用双介质调制靶的研制

为了研究惯性约束聚变(ICF)实验用靶丸不同密度界面的流体力学不稳定性增长,设计并制备了聚苯乙烯(CH)/碳气凝胶(CRF),CRF/硅气凝胶(SiO2)和CH/Al三种双介质调制靶。采用溶胶-凝胶工艺制备了密度分别为250和800mg/cm3的CRF气凝胶薄片;采用激光微加工工艺分别在两种不同密度的CRF薄片和工业用纯Al箔上引入调制图形;采用旋涂工艺在Al箔和CRF薄片(250mg/cm3)的调制表面制备一层CH薄膜,得到CH/Al和CH/CRF双介质调制靶,采用溶胶-凝胶工艺在CRF薄片(800mg/cm3)表面制备一层低密度SiO2气凝胶,得到CRF/SiO2双介质调制靶。采用电子天平、扫描电子显微镜、工具显微镜和台阶仪对所制备的CH/CRF,CRF/SiO2和CH/Al三种双介质调制靶进行靶参数测量。结果表明:三种双介质调制靶层与层之间结合紧密,界面清晰,调制图形为正弦,靶参数测量准确。     

X-ray spectroscopic observations of a superdense plasma in nanoparticles irradiated by superintense femtosecond laser radiation

The interaction of femtosecond laser pulses with SiO₂ aerogel targets has been analyzed by x-ray spectroscopic methods. The use of an aerogel target with transparent grains makes it possible to considerably reduce the requirements on laser-pulse contrasts for which heating occurs without the formation of a preplasma. A nanoplasma with a density sevenfold higher than the solid-state density has been detected.     

Formation of a shock wave in aerogel irradiated with a high-current pulsed electron beam

The propagation of pressure jumps excited by a high-current pulsed electron beam in SiO₂ aerogels with density ranging from 0.025 to 0.25 g/cm³ is investigated using a laser differential interferometer and optical methods. Spallation on the back side of the aerogel targets is observed and the velocity of the spallation fragments is measured. The expansion velocity of the aerogel in the direction of the electron beam is determined. The parameters of the shock adiabat are established in a wide range of aerogel porosities. The depth of the energy-deposition zone of the electron beam is determined experimentally as a function of the aerogel density in the range from 0.015 to 0.25 g/cm³. A model describing highly porous materials which reflects the fractal properties of highly porous aerogels is developed on the basis of the experimental data. Numerical calculations of the observed phenomena are performed. Zh. Tekh. Fiz. 69, 18–25 (December 1999)     

Nuclear fusion induced by a super-intense ultrashort laser pulse in a deuterated glass aerogel

A SiO₂ aerogel with absorbed deuterium is proposed as a target for the fusion reaction d + d → He³ + n induced by a superintense ultrashort laser pulse. The multiple inner ionization of oxygen and silicon atoms in the aerogel skeleton occurs in the superintense laser field. All the formed free electrons are heated and removed from the aerogel skeleton by the laser field at the front edge of the laser pulse. The subsequent Coulomb explosion of the deuterated charged aerogel skeleton propels the deuterium ions up to kinetic energies of ten keV and higher. The neutron yield is estimated at up to 10⁵ neutrons per laser pulse for ～200–500 ps if the peak intensity is 10¹⁸ W/cm² and the pulse duration is 35 fs.     

TiO2和SiO2薄膜应力的产生机理及实验探索

对最常用的TiO₂和SiO₂薄膜应力, 包括应力模型、应力测试方法和不同实验条件下的应力测试结果作了研究.基于曲率法模型，对TiO₂和SiO₂单层膜和多层膜进行了实验测试，得到了一些有价值的结果，特别是离子辅助淀积和基板温度等工艺参数对薄膜应力的影响.提出了薄膜聚集密度是应力的重要因素，低聚集密度产生张应力，而高聚集密度产生压应力.在多层膜中通过调节工艺参数，适当地控制张应力或压应力，可使累积应力趋向于零. 关键词： 薄膜应力 离子辅助淀积 聚集密度     

Studies on the performances of silica aerogel electrodes for the application of supercapacitor

Silica aerogel (SiO₂ aerogel) was prepared by sol–gel method from tetraethyl orthosilicate hydrolyzation and has been characterized by scanning electron microscopy and N₂ adsorption for its surface structure, surface area, and pore-size distribution. Constant current charge–discharge technique, cyclic voltammetry, and electrochemical impedance spectrum were employed for its specific capacitance and equivalent series resistance. The results showed that the maximum specific capacitance of SiO₂ aerogel electrode in 1 M Et₄NBF₄/PC electrolyte was 62.5 F g⁻¹. In addition, the SiO₂ aerogel capacitor exhibits excellent long-term stability with no significant degradation after 500 charging and discharging cycles. Therefore, the application of high surface area SiO₂ aerogel as electrodes in supercapacitor devices is promising.     

Electrical and optical properties of Si-doped indium tin oxides as transparent electrode and anti-reflection coating for solar cells

We have studied the electrical and optical properties of Si-doped indium tin oxides (ITSOs) as transparent electrodes and anti-reflection coatings for Si-based solar cells. The ITSO thin films were obtained by co-sputtering of ITO and SiO₂ targets under target power control. The resistivity of the ITSO thin films deposited at 0.625 in terms of power ratio (ITO/SiO₂) were 391 Ωcm. In this condition, the ITSO thin films showed very high resistivity compared to sputted pure ITO thin films (1.08 × 10⁻³ Ωcm). However, refractive index of ITSO thin films deposited at the same condition at 500 nm is somewhat lowered to 1.97 compared to ITO thin films (2.06). The fabricated graded refractive index AR coatings using ITO, ITSO, and SiO₂ thin films kept over 80% of transmittance regardless of their thickness varing from 97 nm to 1196 nm because of their low extinction coefficient. As the AR coating with graded refractive indices using ITO, ITSO, and SiO₂ layers was applied to general silicon-based solar cell, the current level increased nearly twice more than that of bare silicon solar cell without AR coating.     

Evolution of the glow of an aerogel irradiated with a high-power pulse electron beam

The evolution of the glow of the energy-release zone in porous transparent aerogel, with a density of 0.03–0.25 g/cm³, which is irradiated by a high-power pulse electron beam, is studied experimentally. In addition to a fast (τ≤τ_beam) and a luminescent (τ≈10⁻⁶ s) glow components, a slow glow component (τ≈2×10⁻⁵ s) has been revealed. The appearance of this slow component is associated with an aerogel rarefaction wave and its destruction (cracking) arising after its isochoric bulk heating by electron radiation, which may occur due to an electrostatic field induced under irradiation. The discovered glow is utilized to visually determine the current position of the rarefaction wave front. The sound velocity measured as a function of the density of SiO₂ aerogels with porosities of 10–100 allowed us to experimentally determine the percolation parameter of the aerogel equation of state.