单分散SiO2微球的制备及疏水改性研究

采用改进的凝胶-溶胶法制备了200~800 nm的单分散SiO2微球,并通过真空冷冻干燥法得到不易团聚的单分散SiO2粉体,采用乙醇超临界方法对制备的SiO2微球进行疏水改性.通过扫描电镜和氮吸附-脱附分析仪对SiO2微球的表面形貌、粒径以及孔径分布进行表征;用傅里叶红外变换测试和测量接触角对疏水改性的SiO2微球进行分析.结果表明SiO2微球粒径随二次加入TEOS体积增加呈先增大后减小.经过乙醇超临界处理,SiO2微球表面成功接枝上了疏水烷基,微球尺寸越小,疏水性越好,其接触角高达149°,单次SiO2微球处理量对结果无明显影响.采用本方法可以单次处理12 g以上的SiO2微球,接触角均在140°左右,可充分满足实验室使用需求.经过真空冷冻技术和乙醇超临界技术得到疏水单分散SiO2微球粉体,具有不易团聚及单分散性良好的优点,能够作为胶体晶体原料和三维有序材料(3-DOM)模板剂进行广泛应用.     

SiO2双尺寸光子晶体的自组装及稳定性探索

采用St?ber法制备不同尺寸SiO2胶体球,利用多次垂直沉积法制备SiO2双尺寸光子晶体.通过场发射扫描电子显微镜(FE-SEM)对所得双尺寸光子晶体的形貌和排列方式进行表征.对双尺寸光子晶体的生长过程进行探讨,研究界面作用力及胶体球间相互作用力对制备稳定结构的影响.研究结果表明,SiO2双尺寸光子晶体具有更加有序稳定的结构.胶体球间的相互作用力随胶体球粒径增大而增大,大粒径胶体球更有利于形成稳定的结构.     

不同膜厚对SiO2光子晶体形貌及光学性能的影响

利用改良的St6ber法制成了粒径均一的SiO2胶体颗粒,胶体微球颗粒平均粒径为200 nm.保持SiO2悬浮液体积分数相同,对双基片自组装垂直沉积进行改造,改变夹层厚度,沉积得到厚度不同的SiO2光子晶体薄膜.利用扫描电子显微镜观察了膜厚不同的SiO2光子晶体薄膜样品的表面以及断面微观形貌,测试了样品的光反射性能,此外还讨论了光子晶体薄膜厚度对样品表面的形貌以及样品光反射性能带来的影响.     

化学还原法向二氧化硅人工欧泊中填充Se

本文提出了一种新的调节人工欧泊晶体的光学带隙的方法.采用改进的溶剂蒸发法将单分散SiO2微球组装成在红外光区具有光子带隙的人工欧泊,采用化学还原法向欧泊中填充高折射率材料Se,改变其光学带隙特性.采用扫描电子显微镜(SEM)、X射线衍射和可见-近红外光谱仪(VIS-NIR)等对Se-SiO2三维光子晶体的形貌、结构和光学性能进行了观察测试.研究结果表明Se以纳米晶粒的形式均匀地包覆在SiO2微球表面,与相同晶格周期的SiO2光子晶体相比,Se-SiO2光子晶体的带隙发生明显的红移.     

双尺寸胶体晶体的制备及其结构表征

采用垂直沉积法制备了双尺寸胶体晶体结构,并实现多种双尺寸SiO2胶体晶体结构的自组装.通过场发射扫描电子显微镜(FE-SEM)对胶体晶体的结构及排列方式进行测试分析.对双尺寸胶体晶体的生长过程进行探讨,研究大小胶体球的粒径比及体积比对结构的影响规律.研究结果表明大小球粒径比过小时,双尺寸胶体晶体排列结构有序性差.增大大胶体球的粒径时,合成相同双尺寸胶体晶体结构所对应的大小胶体球体积比增大.     

蓝色聚苯乙烯胶体晶体膜的制备及其呈色机理研究

以粒径为340±10 nm的单分散聚苯乙烯微球为原料,采用垂直沉积法制备了蓝色聚苯乙烯胶体晶体膜.通过研究不同组装容积对聚苯乙烯胶体晶体膜的微观形貌和宏观呈色性能的影响规律,探索制备大面积蓝色聚苯乙烯胶体晶体膜的方法.结果表明,当聚苯乙烯乳液浓度为0.1wt;,干燥温度为40℃,自组装容积为50 mL时,所得聚苯乙烯胶体晶体膜呈现高质量的密排六方结构,宏观上呈现均匀明亮的蓝色,该蓝色具有一定的角度依赖性.研究发现,采用该方法制备聚苯乙烯胶体晶体膜时,在基片上和玻璃器皿壁上同时进行着垂直自组装.同时,在玻璃器皿底部也进行着蒸发自组装,形成了较大面积的蓝色聚苯乙烯胶体晶体膜,有望为制备大面积聚苯乙烯胶体晶体膜提供新的方法.     

单分散二氧化硅微球的制备及表面化学修饰

采用St(o)ber法在醇-水混合体系中,以正硅酸乙酯(TEOS)作为硅源,在氨水催化作用下制备SiO2纳米微球,分析了不同浓度的氨水、TEOS、乙醇和温度对SiO2微球形貌及粒径的影响,并利用透射电镜对其形貌和粒径进行表征.最后引入具有疏水基团的十六烷基三甲氧基硅烷对SiO2微球表面进行修饰,并采用FT-IR和测量接触角对修饰的SiO2微球进行分析.结果表明:SiO2微球粒径随氨水浓度的增加而增大;随TEOS、乙醇浓度和温度的升高先增大后减小;并通过FT-IR和测量接触角证明疏水基团成功接枝到SiO2微球表面.     

SiO2-BaTiO3异质双尺寸超材料结构的制备

采用垂直沉积法自组装制备了SiO2胶体晶体模板,并结合Pechini溶胶-凝胶法实现多种SiO2-BaTiO3异质双尺寸超材料结构的制备.通过X射线衍射分析仪(XRD)和场发射扫描电子显微镜(FE-SEM)对所得粉体和光子晶体的晶型、形貌及排列方式进行测试分析.对比钛酸钡粉体,对SiO2-BaTiO3异质超材料的结构进行探讨,研究不同pH值对钛酸钡粉体的形貌和粒径的影响,进而研究不同凝胶对异质超材料结构的影响.研究结果表明异质结构中胶体晶体模板的排列更加紧密有序,缺陷减少,纳米颗粒的粒径与原钛酸钡粉体的粒径基本一致,利用不同凝胶可获得LS2、LS4、LS6型结构及层-层复合结构.     

SiO2粉体制备及其与Ag2S复合工艺研究

采用改性Stober法来可控制备SiO2粉体,并探究了不同沉淀剂对SiO2粉体形貌及粒径大小的影响.分别采用水热法、溶剂热法和沉淀法来制备SiO2/Ag2S复合粉体,并使用XRD、SEM-EDS、NanoMeasure等手段对制备出的各种粉体的物相、成分、形貌和粒径分布等进行表征与分析.结果表明,以正硅酸乙酯(TEOS)为硅源,氨水为沉淀剂时,添加适量聚丙烯酸酯乳液可有效控制SiO2微球的粒径;以碳酸钠水溶液为沉淀剂时,能得到线状SiO2粉体.在140 ℃下水热处理6 h得到的SiO2/Ag2S粉体的复合效果较好;常温下,通过热处理共沉淀出的SiO2/Ag2S粉体具有操作简便、反应条件易控制、复合效果较好等优点.     

纳米结构四氧化三铁空心微球的合成及磁性研究

用乙二醇为溶剂,三氯化铁和尿素为起始反应试剂,通过水热反应合成了Fe3O4空心微球.用X射线衍射仪(XRD)、透射电子显微镜(TEM)和扫描电子显微镜(SEM)表征样品的结构和形貌,结果表明,所制备的单分散Fe3O4空心微球为立方单晶结构,其直径约400 nm,是由纳米颗粒组装而成.用振动样品磁强计(VSM)测量了Fe3O4空心微球的室温磁性,发现其表现为铁磁性.     

Syntheses and structures of N-phenylmaleimidetriazoles and by-products

The syntheses, properties, and structures of N-phenylmaleimidetriazole derivatives are described. Intermediates and by-products are also discussed. 1b. a = 43.997(7) Å, 5.7610(9) Å, 8.245(1) Å, = 99.339(4), C₂/c; 2a. a = 13.646(4) Å, b = 7.744(2) Å, c = 10.612(3) Å, = 91.979(6), P2₁/c. 3a. a = 22.245(1) Å, b = 22.245(1) Å, 10.010(1) Å, P42/n. 3a. a = 11.727(2) Å, b = 14.075(3) Å, c = 16.080(3) Å, = 105.859(3), = 105.331(3), = 98.187(3), P-1. 3b. a = 8.561(3) Å, b = 14.755(5) Å, c = 22.771(7) Å, = 97.006(5), P2₁/c. 3c. a = 10.500(2) Å, b = 12.189(2) Å, c = 13.040(2) Å, = 109.091(3), = 106.089(3), = 101.022(3), P-1. 8a. a = 16.389(8) Å, b = 5.749(3) Å, c = 19.316(3) Å, = 97.467(9), P2₁/n. 8b. a = 5.822(2) Å, b = 10.114(3) Å, c = 16.705(4) Å, = 84.681(5), = 82.840(5), = 75.769(4), P-1. 9b. a = 11.251(1) Å, 13.335(3) Å, 13.376(3) Å, = 102.456(4), P2₁/n. 9c. a = 15.836(3) Å, b = 8.236(2) Å, c = 5.447(3) Å, = 92.551(3), P2₁/c. 10a. a = 13.177(2) Å, b = 14.597(2) Å, c = 5.5505(8) Å, = 110.979(2), Cc. 11a. a = 14.720(2) Å, b = 13.995(2) Å, c = 38.245(6) Å, = 94.430(3), P2₁/n. 12b. a = 15.067(5) Å, b = 20.378(6) Å, c = 8.669(5) Å, = 99.16(4), = 99.32(3), = 105.23(3), P-1. 13b. a = 8.2824(6) Å, b = 10.5245(7) Å, c = 15.518(1) Å, = 92.305(1), = 100.473(1), = 100.124(1), P-1. 15a. a = 15.357(3) Å, b = 7.778(2) Å, c = 22.957(2) Å, Pbca. 16b. a = 18.0384(4) Å, b = 12.474(3) Å, c = 20.078(5) Å, Pbca.     

Sol-gel synthesis and characterization of adsorbent and photoluminescent nanocomposites of starch and silica

Using sol-gel method, mesoporous and photoluminescent silica nanocomposites of soluble starch have been synthesized and characterized. Different ratios of H₂O, TEOS and EtOH were used at fixed template (soluble starch) and catalyst (NH₄OH) concentrations to obtain materials of different performances in terms of heavy metal binding from a solution which has been monitored using Cd(II) as representative divalent heavy metal ion. Optimum material was obtained when H₂O, TEOS and EtOH were used in 14:1:2 ratio. This sample was not only an efficient metal ion adsorbent but also had an intense luminescence in ultra-violet region and potentially may be used in silicon-based UV-emitting devices. Metal binding by the material was further enhanced after calcination (at 800 °C in air) while its luminescence had a multipeak profile in UV-visible region. In a batch adsorption study, calcined hybrid composite (0.25 g/L) could remove 98.5% Cd(II) from 100 mg/L Cd(II) solution in 2 h. The chemical, structural and textural characteristics of the synthesized materials have been investigated using Fourier Transform Infrared Spectroscopy (FTIR), X-rays Diffraction (XRD), Thermal Analysis (TGA/DTA), Photoluminescence (PL), Brunauer-Emmett-Teller Analysis (BET) and Scanning Electron Microscopy (SEM).     

晶体中负离子配位多面体结晶方位、形变与晶体压电、铁电性

本文研究了压电、铁电晶体中负离子配位多面体的结晶方位与形变,提出了压电晶体中同一种负离子配位多面体的结晶方位是一致的.在铁电晶体中,负离子配位多面体发生形变,伴随着晶体发生顺电-铁电相变,并从这一基本过程出发,对铁电体相变的形成机理进行了讨论.     

Biocrystallization in Bacterial and Fungal Cells and Spores

A series of X-ray diffraction experiments were performed for the first time to study stress-induced biocrystallization (structural response to stress) in the bacteria E. coli, the spore-forming bacteria Bacillus cereus, and in cells and spores of the mycelial fungus Umbelopsis ramanniana. High-intensity areas with spacings of 90 and 44 Å are indicative of a periodically ordered arrangement (most likely nanocrystalline) of the bacterial nucleoid. For the starved bacteria Bacillus cereus, a peak at a spacing of 45 Å is also assigned to nanocrystalline complexes of DNA with the Dps protein. The spores of the fungus Umbelopsis ramanniana VKM F-582, as well as the spores of Bacillus cereus, form ordered arrays of DNA molecules with DNA-condensing acid-soluble proteins SASPs. Starved dehydrated mycelial cells of the fungus Umbelopsis ramanniana form ordered structures with spacings from 27 to 55 Å. A series of peaks reflect the formation of a number of ordered protein arrays, apparently with DNA, with continuously varying characteristic interplanar spacings.     

Preparation and characterization of PbSe nanopowder and quasi-ceramics

By means of the reduction of Pb(II) and Se(IV) with hydrazine, oval monodispersed PbSe nanoparticles characterized by sizes ～100 nm and the cubic symmetry were obtained. Their compaction and sintering into quasi-ceramic state were performed. The samples were investigated by means of scanning electron microscopy, X-ray diffraction and FTIR spectroscopy. The results obtained are discussed.     

Simulation and Experiment in X-ray Topography and Diffractometry

X-ray double crystal topography and high resolution diffractometry reveal very small deformations of the crystal lattice. However, this information can be directly obtained from the topographs or diffractometer curves only if certain conditions are fulfilled. Generally a deformation model has to be used, that is compared to the measurements by simulation calculations based on the dynamical diffraction theory. Trial and error allow to adapt the parameters of the model. An example illustrates that with a few parameters an automatic fit is possible.     

Melting and short-range order in liquids and glasses

A theory is proposed to explain two-dimensional melting based on the gauge-invariant Lagrangian with spontaneous breaking (Higgs mechanism) or the SU(2) gauge field to U(1) symmetry. The first-order phase transition in two-dimensional melting may be strongly related to the asymptotic freedom-like interaction of the SU(2) gauge field in the case when the distance between each excited disk is shorter than a critical length, 2/ boxv;mboxv, near the melting temperature.     

Structural and spectral studies of N-trans-cinnamylidene-m-toluidine and N-trans-cinnamylidene-m-chloroaniline

N-trans-cinnamylidene-m-toluidine (1) C₁₆H₁₅N, and N-trans-cinnamylidene-m-chloroaniline (2) C₁₅H₁₂NCl form isomorphous crystals which are monoclinic, space group P2_l/c, with unit cell dimensionsa=5.967(2),b=13.793(3),c=15.048(5) Å, =91.97(3)° anda=5.868(2),b=13.788(4),c=15.191(4) Å, =91.87(3)°, respectively. The single-crystal X-ray structure determinations of the title compounds revealtrans structures. Ring (A) C_10–15 and ring (B) C_1–6, are practically planar in both structures with dihedral angels of 61.3(3) and 63.6(2)°, respectively.¹H nmr, u.v. and i.r. spectra are also reported.     

Chemistry and Electrocrystallization of Organic Metals and Superconductors

Abstract

Considerable variation in the conditions of electrochemical crystal growth of TMTSF₂X (i.e., constant current versus constant potential, ambient versus inert atmosphere, etc.) and in the purity of the constituents (donor, electrolyte, solvent) does not significantly affect the unusual low-temperature properties of this class of materials. Our results suggest that the electrocrystallization procedure may be self-purifying by selecting for conducting crystal phases with constituents having specific oxidation potentials and solubility properties. However, doping solutions with structurally and chemically similar constituents (i.e., TMTTF, and IO^? ₄ in CIO^? ₄) leads to their incorporation in the crystal structure where they have a profound effect. Several mole percent of these dopants suppress superconductivity in the PF^? ₆ and CIO^? ₄ salts, and increase and broaden the metal-insulator phase transition.     

Hydrothermal Synthesis and Morphology of Thomsonite and Edingtonite

The hydrothermal treatment of different glasses of the composition 2 Na₂O–8 CaO–10 Al₂O₃– 20 SiO₂ and 2 BaO–2 Al₂O₃–6 SiO₂ at one kilobar pressure in a temperature-range between 80 °C and 230 °C lead to the formation of the zeolite-minerals thomsonite (orthorhombic symmetry space-group Pbmn, a = 13.05 Å, b = 13.09 Å and c = 13.22 Å), and edingtonite (orthorhombic symmetry, space-group: P2,2,2, a = 9.55 Å, b = 9.67 Å and c = 6.52 Å). Under the chosen hydrothermal conditions both mineral phases are formed in the whole temperature interval.