间苯二酚-甲醛气凝胶空心微球制备技术

 采用微流体注射成型技术,以邻苯二甲酸二丁酯为内外油相,间苯二酚/甲醛(RF)溶液为水相,经过溶胶-凝胶、溶剂交换、超临界干燥等过程制备出了RF气凝胶空心微球。分别采用红外光谱、光学显微镜、X光显微分析、透射电镜(TEM)、N­₂吸附-脱附,对RF空心微球成分、形貌、孔径、直径分布等进行表征。结果表明：RF为单层空心微球,具有典型的气凝胶多孔结构,由粒径为10 nm左右、且粒度分布较为均匀的纳米粒子构成,平均孔径为20 nm左右,球形度和同心度大于95%,微球直径分布在550～750 mm,最大可达到800 mm,达到了快点火靶的基本要求。     

间苯二酚-甲醛凝胶自发成膜技术研究

 以间苯二酚和甲醛为原料,对水相溶胶-凝胶聚合自发成膜技术获得间苯二酚-甲醛(RF)凝胶薄膜进行了研究。主要研究了溶胶-凝胶过程中冰醋酸（HAC）含量和反应温度对凝胶过程的影响,分析了RF有机凝胶自发成膜的形成机理。IR和SEM分析表明,所得到的凝胶膜具有典型的RF有机气凝胶结构,薄膜厚度大约为50 μm,膜由直径10 μm左右的粒子组成,没有观察到明显的孔洞结构。分析认为,在间苯二酚和甲醛占总溶液的质量分数为67％左右及控制pH值在一定的酸性范围,RF凝胶自发成膜过程和机理可以用RF凝胶的收缩机理加以解释,RF自发膜的表面形貌及形成机理与均匀泡沫的连续相分离机理类似。     

间苯二酚-甲醛凝胶自发成膜技术研究

以间苯二酚和甲醛为原料,对水相溶胶-凝胶聚合自发成膜技术获得间苯二酚-甲醛(RF)凝胶薄膜进行了研究。主要研究了溶胶-凝胶过程中冰醋酸（HAC）含量和反应温度对凝胶过程的影响,分析了RF有机凝胶自发成膜的形成机理。IR和SEM分析表明,所得到的凝胶膜具有典型的RF有机气凝胶结构,薄膜厚度大约为50 μm,膜由直径10 μm左右的粒子组成,没有观察到明显的孔洞结构。分析认为,在间苯二酚和甲醛占总溶液的质量分数为67％左右及控制pH值在一定的酸性范围,RF凝胶自发成膜过程和机理可以用RF凝胶的收缩机理加以解释,RF自发膜的表面形貌及形成机理与均匀泡沫的连续相分离机理类似。     

高密度间苯二酚-甲醛碳气凝胶ICF靶的制备与吸附性能研究

以间苯二酚和甲醛为前驱体,通过改进传统制备技术解决了高密度间苯二酚-甲醛(CRF)碳气凝胶制备过程中的龟裂问题,制备出了符合ICF实验需要的高密度CRF碳气凝胶材料。分别对CRF碳气凝胶的元素组成和物相组成进行了鉴定,采用自动吸附仪考察了CRF碳气凝胶对N2和H2的吸附性能。结果表明：该碳气凝胶是一种由C元素组成的类似石墨结构的非晶固态材料,结构均匀性好,具有良好的机械加工性能,比表面积达676 m2·g-1,平均孔径为7.16 nm;氢吸附质量分数达2.28%,相应体积密度为17.83 kg·m-3。     

高密度间苯二酚-甲醛碳气凝胶ICF靶的制备与吸附性能研究

 以间苯二酚和甲醛为前驱体,通过改进传统制备技术解决了高密度间苯二酚-甲醛(CRF)碳气凝胶制备过程中的龟裂问题,制备出了符合ICF实验需要的高密度CRF碳气凝胶材料。分别对CRF碳气凝胶的元素组成和物相组成进行了鉴定,采用自动吸附仪考察了CRF碳气凝胶对N₂和H₂的吸附性能。结果表明：该碳气凝胶是一种由C元素组成的类似石墨结构的非晶固态材料,结构均匀性好,具有良好的机械加工性能,比表面积达676 m²·g^-1,平均孔径为7.16 nm;氢吸附质量分数达2.28%,相应体积密度为17.83 kg·m^-3。     

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>。}}     

间苯三酚-甲醛气凝胶及其碳气凝胶的制备与表征

以间苯三酚(P)和甲醛(F)为原料,经溶胶-凝胶、溶剂交换、超临界干燥和碳化等过程制备出了间苯三酚-甲醛气凝胶(PF)及其碳气凝胶(CPF)。测试结果表明气凝胶具有比较高的比表面积、是一种连续nm级3维网络结构的多孔材料;碳化后密度和平均孔径增大,比表面积基本无变化,且仍然维持气凝胶的网络结构。催化剂摩尔比决定气凝胶的微观结构,反应物质量分数控制着气凝胶密度。通过优化制备条件,可以制备出能满足惯性约束聚变(ICF)靶需要的不同结构和不同密度的气凝胶。     

间苯三酚-甲醛气凝胶及其碳气凝胶的制备与表征

 以间苯三酚(P)和甲醛(F)为原料,经溶胶-凝胶、溶剂交换、超临界干燥和碳化等过程制备出了间苯三酚-甲醛气凝胶(PF)及其碳气凝胶(CPF)。测试结果表明气凝胶具有比较高的比表面积、是一种连续nm级3维网络结构的多孔材料;碳化后密度和平均孔径增大,比表面积基本无变化,且仍然维持气凝胶的网络结构。催化剂摩尔比决定气凝胶的微观结构,反应物质量分数控制着气凝胶密度。通过优化制备条件,可以制备出能满足惯性约束聚变(ICF)靶需要的不同结构和不同密度的气凝胶。     

无催化法制备低密度三聚氰胺-甲醛气凝胶

以三聚氰胺和多聚甲醛为原料,二甲基亚砜为溶剂制备三聚氰胺-甲醛(MF)气凝胶,湿凝胶经超临界干燥,制备出密度最低可达70 kg/m3的MF气凝胶。采用红外吸收光谱、场发射扫描电镜、N2吸附-脱吸附分析和热失重分析表征了MF气凝胶的组成、微结构以及热性能。结果表明:以二甲基亚砜为溶剂制备的MF气凝胶,虽然其微观结构较以水为溶剂的气凝胶差,比表面积及孔径分布均一性均降低,但是其热稳定性有所提高。     

催化剂对三聚氰胺-甲醛有机气凝胶的影响

采用溶胶-凝胶法制备出一系列不同催化剂种类和浓度的三聚氰胺-甲醛(MF)有机气凝胶模板,通过傅里叶变换红外光谱仪、热分析仪、N2吸附等测试手段对其分子结构、热稳定性、孔结构进行了表征。测试结果表明：催化剂种类和浓度变化不影响模板的分子结构和热性能;各模板热解程度均达97%;相比NaOH和NaHCO3为催化剂制备的模板,Na2CO3为催化剂时,制备的模板更优,比表面积和孔容较大,孔分布范围较宽; 当三聚氰胺与催化剂的浓度比为500时,比表面积达到最大。     

低频用周期性结构管道的研究

在扬声器单元的一侧耦合管道是解决声短路,实现低频下潜的有效方法。本文研究了一种周期性结构管道,对其低频辐射特性进行理论分析,提出了使用周期性结构管道代替传统均匀管道以缩短长度。在实际的扬声器单元上分别耦合传统的均匀管道和周期性结构管道,实验结果与理论计算基本吻合。结果表明,为实现相同的低频下潜,合理的周期性结构可以有效地缩短管道长度,从而具有更高的实用价值。     

The geometry and electronic structure of Aristolochic acid: possible implications for a frozen resonance

Molecular mutagens and carcinogens are structures which carry chemical and electronic properties that disturb and interact with the genomic machinery. Principally, a rule of thumb for carcinogens is that carcinogens are expected to introduce covalent irreversible bonding to one or several types of DNA bases, causing errors in the reading frame for the polymerases. 8‐methoxy‐6‐nitrophenanthro[3,4‐d][1,3]dioxole‐5‐carboxylic acid, better known as Aristolochic acid (AA1) is a recognized carcinogen which causes urotherial cancer and is found in certain plants. Its structure is particularly interesting given that it is closely related to phenanthrene in its polycyclic arrangement, and has four functional groups, a carboxyl‐, a nitro‐, a methoxy‐ and a dioxolane group. In this work, the structure of AA1 has been resolved at the MPWPW91 density functional theory method in combination with Aug‐cc‐pVDZ basis sets. A geometry analysis shows that in AA1 the carboxyl group's torsion is caused by steric strain from the nitro group, which elevates the molecular plane of the first phenanthrene ring with 0.1Å. The wavefunction analysis of AA1 shows that the ring deformation enhances a double π‐bond localization in the first ring, adjacent to the dioxalane group, and results in a decrease of ring aromaticity and induces a potentially frozen resonance. Intermolecular and intramolecular interactions were characterized by atoms in molecules and reduced density gradient analysis. This study brings novel information on the geometry and electronic structure of AA1, which are important for the further knowledge of its transformation in vivo and in situ. Copyright © 2013 John Wiley & Sons, Ltd.     

DATB和TATB的特殊稳定性分析

利用HONDO程序包,采用从头算法,计算了TNA、DATB和TATB的分子结构和分子内各原子上的净电荷.根据分子结构和各原子上的净电荷,深入分析了DATB和TATB的特殊稳定性.     

立方相Ag3PO4(111)面原子几何及弛豫结构的第一性原理计算

采用平面波超软赝势方法研究了立方相Ag3PO4(111)面的表面能和表面原子弛豫结构.首先对Ag3PO4(111)面的八种不同原子终止结构的体系总能量进行计算,结果表明B种表面模型被证实为最稳定的(111)面原子几何结构.针对该表面结构,探讨了表面能和原子弛豫与模型中原子层数和真空厚度的关系,当原子层数为24层,真空厚度为0.6 nm时,表面能收敛于1.41 J/m2(LDA-CAPZ)和1.39 J/m2(GGA-PBE).表面原子弛豫后,表面两个三配位的Ag原子均向里移动,超过0.06 nm,而表面次层的O原子则均向外移动约0.0042 nm,导致弛豫后暴露在最表面的是O原子,同时表面原子的核外电子向表面内部发生转移,结构趋于稳定.这些结果为进一步深入研究Ag3PO4表面的光催化活性起源提供理论支持.     

Optimized geometry and electronic structure of graphyne-like silicyne nanoribbons

Silicyne, a silicon allotrope, which is closely related to silicene and has graphyne-like structure, is theoretically investigated in this work. Its optimized geometry and electronic band structure are calculated by means of the first-principles frozen-core projector-augmented wave method implemented in the Vienna ab initio simulation package (VASP). We find that the lattice parameter is 9.5, the silicon chain between hexagons is composed of disilynic linkages (-Si≡Si-) rather than cumulative linkages (=Si=Si=), and the binding energy is 3.41 eV per atom. The band structure is calculated by adopting the generalized gradient approximation and hybrid functionals. The band gap produced by the HSE06 functional is 0.73 eV, which is nearly triple that by the generalized gradient approximation of Perdew-Burke-Ernzerhof functional.     

FeS2(100)表面原子几何与电子结构的理论研究

采用密度泛函理论研究了FeS2(100)表面原子几何与电子结构.理论计算结果表明:FeS2(100)表面无弛豫、无重构,是体相原子几何的自然终止.与体相电子结构相比,FeS2(100)表面电子特性明显不同,禁带中央产生新的表面态,且表面态局域性强,主要由Fe原子的3d分波贡献.配位场理论定性分析表明:FeS2(100)完整晶面表面态产生机制是Fe原子的配位数减少、局部对称性下降所致 关键词： 密度泛函理论 表面电子结构 FeS2     

几何结构对Na8团簇熔化过程的影响

运用距离相关紧密结合的分子动力学模型,对金属原子团簇Na8的两种不同的异构体进行了数值模拟.根据零温下基态结构中不同原子到质心的不同距离,把Na8的两种异构体分为多个子系统.分别提取各个子系统在不同温度下的围绕质心的径向分布、无单位键长涨落、平均位移、扩散系数,发现尽管两个异构体的基态能量很接近,但他们的稳定性、熔化过程的热力学性质等有着很大的差别,这也反映了它们在几何结构上的差别.     

The hierarchical porous structure of carbon aerogels as matrix in cathode materials for Li-S batteries

For Li-S batteries, commercial application was hindered by the insulating nature of S and the solubility of polysulfide. Porous carbon materials had proven themselves to be an ideal immobilizer host for S impregnation. Herein, carbon aerogels (CAs) with tunable pore microstructure were synthesized from resorcinol-formaldehyde reaction with increasing catalyst concentration and pyrolysis under high temperature. The results demonstrated that the catalyst concentration played a key role in tuning the porous microstructure of the CAs. In addition, potassium hydroxide (KOH) was introduced to activate the obtained CAs. The activated carbon aerogels (A-CAs) with hierarchical porous structure exhibited the highest specific surface area (1837.4 m² g^?1) and the largest total pore volume (2.276 cm³ g^?1), which combined the advantages of both mesoporous and microporous. The effects of porous microstructure, specific surface area, and pore volume of the CAs and A-CAs on S incorporation were studied. The S/A-CAs exhibited significantly improved reversible capacity (1260 mAh g^?1 at a rate of 0.1 C), enhanced high-rate property, and excellent cycling performance (229 mAh g^?1 after 500 cycles at 1 C) as a cathode for Li-S batteries.     

Band structure of the quasi two-dimensional purple molybdenum bronze

The molybdenum purple bronze KMo₆O₁₇ is quasi two-dimensional (2D) metallic oxide that shows a Peierls transition towards a metallic charge density wave state. Since this specific transition is directly related to the electron properties of the normal state, we have investigated the electronic structure of this bronze at room temperature. The shape of the Mo_K1s absorption edge reveals the presence of distorted MoO₆ octahedra in the crystallographic structure. Photoemission experiments evidence a large conduction band, with a bandwidth of 800 meV and confirm the metallic character of this bronze. A wide depleted zone separates the conduction band from the valence band that exhibits a fourfold structure, directly connected to the octahedral symmetry of the Mo sites. The band structure is determined by ARUPS in two main directions of the (0 0 1) Brillouin zone. It exhibits some unpredicted features but corroborates the earlier theoretical band structure and Fermi surface. It confirms the hidden one-dimensionality of KMo₆O₁₇ that has been proposed to explain the origin of the Peierls transition in this 2D compound.     

The properties of halo structure for 17B

The total reaction cross section (1724 ± 93 mb) of ¹⁷B at the energy of 43.7 A MeV on C target has been measured by using the transmission method at the Radioactive Ion Beam Line in Lanzhou (RIBLL). Assuming ¹⁷B consists of a core ¹⁵B plus two halo neutrons, the total cross section of ¹⁷B on C target was calculated with the zero-range Glauber model, where double Gaussian density distributions and Gaussian plus HO density distributions were used. It can fit the experimental data very well. The characteristic of halo structure for ¹⁷B was found with a large diffusion of the neutrons density distribution. Supported by the National Natural Science Foundation of China (Grant Nos. 10475098, 10605033 and 10221003), the Chinese Academy of Sciences (Grant Nos. CXTD-J2005-1 and KJCX2-SW-N18), and Hundred Talent Project of CAS (Grant No. 0501080BR0)