熔盐法制备氧化锆纳米棒

采用非水解溶胶-凝胶工艺合成氧化锆干凝胶粉,然后将干凝胶粉与熔盐混合制备氧化锆纳米棒。借助DTA-TG、XRD、FE-SEM、TEM等测试手段研究了氧化锆的物相转变过程,探讨了熔盐种类与用量、氟化物的添加等工艺参数对制备氧化锆纳米棒的影响。结果表明:以Na VO3为熔盐,用量为1∶1(熔盐与干凝胶的质量比),并且在添加氟化钠的条件下能够制备产率高,且沿[010]方向择优生长的单斜氧化锆纳米棒;氟离子一方面加速了熔盐中Zr4+离子的传质,促使氧化锆干凝胶粉的溶解,另一方面吸附在氧化锆的高能晶面上抑制该晶面的生长,两者的共同作用促进了大量氧化锆纳米棒的形成。     

晶种导向干凝胶法制备成型ZSM-5分子筛

在干凝胶法制备ZSM-5 分子筛的体系中添加晶种导向剂, 控制分子筛的生长, 制备了纳米沸石组装的无粘结剂成型多级孔ZSM-5 分子筛, 一步完成纳米分子筛的制备及组装成型, 即克服了传统纳米粒子难以过滤分离的问题, 同时组装所形成的多级孔有助于改善分子在催化剂内的扩散, 从而提高催化反应效率. 以硅胶、薄水铝石为原料, 四丙基氢氧化铵(TPAOH)和ZSM-5 晶种导向胶作为粘结剂, 通过混捏、挤条得到直径2 mm的条状前驱物, 随后通过干凝胶转换法制备成型分子筛. 所用晶种导向剂组成为0.35TPAOH:1SiO₂:20H₂O:4C₂H₅OH. 通过X射线衍射(XRD), 热重(TG)分析和傅里叶变换红外(FTIR)光谱等方法对分子筛晶化过程进行了表征, 结果表明晶种导向剂加入量对分子筛生长速度及多级孔结构均有影响. 当所加晶种导向剂中TPAOH与SiO₂的摩尔比为0.025时, 经过3 h晶化, 分子筛相对结晶度达到100%. 扫描电镜(SEM)结果表明, 合成的分子筛尺寸约为200 nm, 组装形成的多级孔分子筛的介孔体积为0.28 cm³·g^-1. 通过NH₃ 程序升温脱附(NH₃-TPD)考察了所得成型分子筛的酸性, 发现该分子筛酸性与市售的粉末H-ZSM-5分子筛类似.     

在一维ZnO表面可控构建Co3Mn1纳米晶及其催化CO氧化性能

利用热分解法制备了结构明确的负载型纳米晶催化剂。在纳米晶成核和生长过程中加入一维ZnO纳米棒作为晶种,调控不同组分的纳米晶在 ZnO纳米棒表面均匀生长,从而获得了结构明确的 MnO/ZnO、Co₃O₄/ZnO、Co₃Mn₁/ZnO催化剂。透射电子显微镜(TEM)与 X 射线粉末衍射(XRD)结果显示,不同组分纳米颗粒都均匀分散在 ZnO 纳米棒表面。相对于 MnO/ZnO 和Co₃O₄/ZnO催化剂,Co₃Mn₁/ZnO催化剂在CO氧化反应中具有最佳的催化性能。在200 L·g_cat^-1·h^-1的气时空速下,Co₃Mn₁/ZnO催化剂起活温度为 50 ℃,其 T100(CO 转化率达到 100% 时的温度)为 200 ℃;利用 X 射线光电子能谱(XPS)对不同催化剂进行了分析,结果显示,Co₃Mn₁/ZnO催化剂的氧空位比MnO/ZnO催化剂提高了30%以上,从而使其具有较高的CO氧化催化性能。更为重要的是,Co₃Mn₁/ZnO复合纳米晶催化剂的活化能(39.4 kJ·mol^-1)远低于其它负载型纳米晶催化剂。     

负载钨催化剂的载体效应及其表面酸性

运用BET、XRD、FT-Raman以及微量吸附量热等手段对由浸渍三种晶型氧化锆及其前体氢氧化锆制备的负载钨催化剂的结构及其表面酸性进行了研究。结果表明起始原料和制备条件对氧化锆的结构有显著影响。浸渍在氢氧化锆上的钨物种会使氢氧化锆转变为四方晶型氧化锆。但浸渍于氧化锆上的钨物种使氧化锆发生晶型转变相对较难。负载钨催化剂表面强酸位的形成与载体晶型、表面钨物种WO_x以及WO_x与载体氧化锆之间的相互作用有关。催化剂上的强酸位可因残留的Na⁺离子所毒化或阻抑。少量Y³⁺离子对表面酸性则无明显影响。     

Yb3+/Tm3+共掺杂的钨酸镉纳米晶发光性能的研究

本文采用水热法制备了稀土离子Yb³⁺/Tm³⁺共掺杂的钨酸镉纳米晶。运用X-射线粉末衍射、场发射环境扫描电子显微镜和光谱分析对制备的样品的结构和发光性能进行了表征。根据XRD图谱可知, 钨酸镉为单斜晶系, 晶粒平均尺寸在28 nm左右。从ESEM图片可明显看出, 钨酸镉呈纳米棒结构, 直径在30 nm左右, 长径比在5~8之间。利用980 nm半导体激光器激发钨酸镉纳米晶得到样品的发射光谱, 存在一个较强的蓝光发射, 发光峰位于481 nm,对应于Tm³⁺的¹G₄→³H₆能级的跃迁, 分析了Tm³⁺/Yb³⁺离子共掺体系的发光机制。讨论了发光强度随稀土离子浓度的变化, 当Tm³⁺离子的掺杂浓度在2%, Yb³⁺/Tm³⁺物质的量浓度比为10:1时钨酸镉纳米晶的发光强度最强。根据泵浦功率与发光强度之间的关系, 可知处于481 nm的蓝光发射属于三光子过程, 由发光强度与掺杂浓度之间的双对数衰减曲线可知, 引起蓝光发射源于Tm³⁺的电偶极跃迁。     

CaTiO3纳米粉体溶胶-凝胶法合成、表征及介电特性

采用无机盐溶胶-凝胶法制备了CaTiO₃纳米粉体，采用TG-DTA、XRD、TEM等技术进行了表征，并探讨了CaTiO₃纳米粉体烧结特性及介电效应。结果表明，干凝胶800 ℃低温煅烧可获得粒径分布较窄、平均粒径为60～70 nm的单相CaTiO₃纳米粉。纳米CaTiO₃粉具有较大的比表面积，使作为粉体烧结驱动力的表面能剧增，促使CaTiO₃在1 200 ℃实现致密烧结，比固相法制备的微米粉烧结降低100～200 ℃，且具有较宽的烧结温区。与微米级粉体烧结体介电特性相比，纳米粉具有更高的Q_f值。纳米CaTiO₃粉制备的陶瓷在1 250 ℃烧结2 h，获得优良的介电性能：ε_r=172，Q_f=4 239 GHz，τ_f=+7.68 × 10^-4 ℃^-1。     

共沉淀-熔盐法制备BaMoO4∶Eu3+及其发光性能研究

以KCl-NaCl为熔盐,采用共沉淀前躯体-熔盐辅助焙烧法合成了红色发光材料BaMoO₄∶Eu³⁺。运用X射线粉末衍射(XRD)、扫描电子显微镜(SEM)及荧光光谱(PL)等测试手段,研究了熔盐辅助焙烧温度对粉体相结构、形貌和发光性能的影响,并对比了直接采用共沉淀法合成BaMoO₄∶Eu³⁺的结构与发光性能。结果表明：采用两种方法制备的BaMoO₄∶Eu³⁺均是纯相,粒径随温度升高而增大。当KCl-NaCl复合熔盐焙烧温度大于700 ℃,BaMoO₄晶粒在熔盐中实现了(111)面取向生长,得到均一的尖晶石型BaMoO₄∶Eu³⁺微晶。光谱研究表明：共沉淀前躯体-熔盐辅助焙烧法合成样品在615 nm处的Eu³⁺的⁵D₀-⁷F₂发射明显得到加强,样品发出明亮的红色发射光。     

柠檬酸络合法制备La2CuO4纳米晶

以硝酸镧和硝酸铜为起始原料,柠檬酸为络合剂,采用溶胶-凝胶法制备了La₂CuO₄纳米晶。通过X射线衍射、场发射扫描电子显微镜、透射电子显微镜研究了柠檬酸的加入量对La₂CuO₄纳米粉体相组成、显微结构的影响,并采用Kissinger方法研究了La₂CuO₄纳米晶的合成活化能。结果表明：600 ℃煅烧保温2 h后,可获得单一物相的La₂CuO₄,晶粒为类钙钛矿型结构,晶粒尺寸为60~80 nm,分布集中;在制备过程中提高柠檬酸的加入量能够降低La₂CuO₄晶体的合成活化能,当柠檬酸与溶液中阳离子(La³⁺和Cu²⁺)的物质的量的比由1∶1增加至1.5∶1时,La₂CuO₄纳米晶的合成活化能由147.0 kJ·mol^-1降低到133.4 kJ·mol^-1。     

高质量NaNdF4六方棱柱纳米棒的水热形貌控制合成及发光性质

采用水热法在温和的条件下合成了具有规则外形的六方棱柱状NaNdF₄纳米棒。X射线衍射（XRD）分析表明：产物为纯六方相NaNdF₄,场发射扫描电镜（SEM）分析表明产物形貌为棱柱状纳米棒,长约为550nm,棒的端部呈规则六边形,边长约为85nm。高分辨透射电子显微镜（HRTEM）和选区电子衍射（SD）显示所得样品为良好的单晶。NaNdF₄晶体的生长动力学过程表明：螯合剂（EDTA-Na₂）与稀土金属离子间的螯合作用受pH值影响,导致成核速度变化,进而影响NaNdF₄纳米晶的最终尺寸和形貌。室温下的NaNdF₄纳米棒的发光峰位于红外光范围（λ=892,1058,和1342nm）,其最强发射峰位于1058nm,对应于Nd³⁺的⁴F_3/2→⁴I_11/2f-f跃迁。     

水热-微波法合成纳米晶长余辉发光材料Y2O2S∶Eu3+，Mg，Ti

采用新型水热-微波法合成了纳米晶长余辉发光材料Y₂O₂S∶Eu³⁺,Mg,Ti。通过XRD、TEM、荧光光谱对其进行表征。X射线衍射测试表明所制备的Y₂O₂S∶Eu³⁺,Mg,Ti纳米发光材料为单相,六方晶。透射电子显微镜(TEM)测试表明所制备的Y₂O₂S∶Eu³⁺,Mg,Ti纳米发光材料粒径小,分布集中。激发和发射光谱测试表明Eu³⁺离子能有效地掺入硫氧化钇基质中,并具有良好的发光性能。余辉光谱测试表明其余辉颜色为红色,具有良好的余辉效果。     

Mg二次电池正极材料Cu2Mo6S8的合成与表征

采用CuS.H2O、MoS2、Mo为原料,用熔盐法(KCl为熔盐)合成了谢弗雷尔相的Cu2Mo6S8正极材料,并用XRD,SEM,循环伏安测试,充放电测试对材料的结构和电化学性能进行研究。XRD结果表明本Cu2Mo6S8正极材料属于R3空间群,具有良好的晶型。电化学测试表明,当材料在电压0.2～2 V范围内进行充放电时,其放电比容量在90 mAh.g-1左右,循环稳定性和可逆性均良好。该材料的充放电曲线中在1.2 V和1.9 V分别有还原峰,0.7 V和1.0 V分别有氧化峰,与伏安曲线相对应。     

Zirconia‐based Aerogels via Hydrolysis of Salts and Alkoxides: The Influence of the Synthesis Procedures on the Properties of the Aerogels

This contribution aims at evaluating different synthesis procedures leading to zirconia‐based aerogels. A series of undoped and yttrium‐doped zirconia aerogels have been prepared via hydrolysis and condensation reaction of different alkoxy‐ and different inorganic salt‐based precursors followed by supercritical drying. Well‐established but deleterious zirconium n‐propoxide (TPOZ) or zirconium n‐butoxide (TBOZ) were used as metal precursors in combination with acids like nitric acid and acetic acid as auxiliary agent for the generation of non‐yttrium stabilized zirconia aerogels. Yttrium‐stabilized zirconia aerogels as well as pure zirconia aerogels were obtained by the salt route starting from ZrCl₄ and crosslinking agents like propylene oxide or acetylacetone. The characteristics of the products were analyzed by nitrogen adsorption measurements, electron microscopy, and X‐ray scattering. It turned out that with respect to all relevant properties of the aerogels as well as the practicability of the synthesis procedures, approaches based on inexpensive non‐toxic salt precursors are the methods of choice. The salt‐based approaches allow not only for low‐cost, easy‐to‐handle synthesis procedures with realizable gelation times of less than 60 seconds, but also delivered the products with the highest surface area (449 m² g^?1 for ZrCl₄) within this series of syntheses.     

Potentiometric determination of ultratrace amounts of fluoride enriched by zirconia in a flow system

A satisfactory method was described for separation and preconcentration of ultratrace amounts of fluoride ions enriched by zirconia (ZrO₂) as an inorganic ion exchanger. Fluoride ions can be adsorbed rapidly and selectively on zirconia from an acidic solution (pH 4.8) then reversibly desorbed by increasing pH up to 13. A flow system consisting of a column packed with zirconia impregnated on cellulose fibers and an ion-selective electrode was used for the determination of fluoride. The RSD was found to be 1.6% and the detection limit defined by S/N = 3 was 3 × 10⁻⁹ mol L⁻¹. The interference effects of various ions, such as nitrate, sulfate, halides, alkaline, and alkaline earth ions, which may be found in the environmental water, were studied, and it was found that they were tolerated even at high concentrations. The method was applied to determine fluoride in drinking water, which contains ultratrace amounts of fluoride. The concentration of fluoride was found to be 42 μg L⁻¹, which is confirmed by spiking 2 μmol fluoride to the drinking water with a recovery of 99%. Published in Russian in Zhurnal Analiticheskoi Khimii, 2006, Vol. 61, No. 2, pp. 179–183. The text was submitted by the authors in English.     

Rod-like polyelectrolyte adsorption onto charged surfaces in monovalent and divalent salt solutions

We analyze the adsorption of strongly charged polyelectrolytes onto weakly charged surfaces in divalent salt solutions. We include short-range attractions between the monomers and the surface and between condensed ions and monomers, as well correlations among the condensed ions. Our results are compared with the adsorption in monovalent salt solutions. Different surface charge densities (σ), and divalent (m) and monovalent (s) salt concentrations are considered. When the Wigner-Seitz cells diameter (2R) is larger than the length of the rod, the maximum amount of adsorption scales like n_max ∼ σ^4/3 in both monovalent and divalent solutions. For homogeneously charged surfaces, the maximum adsorption occurs at s* ∼ σ² when s* > ϕ, where ϕ is the monomer concentration, the counterpart for divalent salt solution, m* roughly scales as σ^2.2 when m* > ϕ. The effective surface charge density has a maximum absolute value at m′ < m*. A discrete surface charge distribution and short-range attractions between monomers and surface charge groups can greatly enhance surface charge inversion especially for high salt concentration. The critical salt concentration for adsorption in divalent salt solution roughly scales as m_c ∼ bσ^1.9, where b is the distance between two neighboring charged monomers. © 2004 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 42: 3642–3653, 2004     

Preparation and Magnetic Property of La0.7Sr0.3MnO3 Nanorod by Combination Sol-Gel with Molten Salt

La0.7Sr0.3MnO3（LSMO） nanorods were synthesized by a method combining sol-gel with molten salts at 950 ℃ for 10 h, which employed KCl＋NaCl（mass ratio 4：1） as eutectic molten salts. The morphologies and magnetic properties of the resulting LSMO nanorods were investigated by X-ray diffraction（XRD）, scanning electron microscopy（SEM）, transmission electron microscopy（TEM）, and vibrating sample magnetometer（VSM） measurements. It was found that the obtained perovskite manganite LSMO was a uniform nanorod with a diameter of about 50 nm and a length of longer than 500 rim. The Curie temperature（To） of the LSMO nanorod used here was 262 K, much lower than that of bulky single crystal LSMO（360 K）. The low Curie temperature might be a result of the great disorder near the grain boundary, which could be observed clearly from the TEM picture.     

SnO2 纳米棒的氧化还原特性

 利用室温固相反应在 NaCl-KCl 熔盐介质中, 通过焙烧含 SnO2 纳米颗粒前驱体合成了 SnO2 纳米棒, 并采用 X 射线衍射、扫描电镜、透射电镜、选区电子衍射和 X 射线光电子能谱对 SnO2 纳米棒进行了表征. 结果表明, SnO2 纳米棒是表面光滑、结晶完整的金红石结构单晶体, 直径为 10~20 nm, 长度为几百纳米到几个微米. 程序升温还原结果表明, SnO2 纳米棒具有较好的氧化还原性能和催化活性. 探讨了 SnO2 纳米棒的氧化还原机理.     

K3TaF8 from laboratory X‐ray powder data

The crystal structure of tripotassium octafluoridotantalate, K₃TaF₈, determined from laboratory powder diffraction data by the simulated annealing method and refined by total energy minimization in the solid state, is built from discrete potassium cations, fluoride anions and monocapped trigonal–prismatic [TaF₇]²⁻ ions. All six atoms in the asymmetric unit are in special positions of the P6₃mc space group: the Ta and one F atom in the 2b (3m) sites, the K and two F atoms in the 6c (m) sites, and one F atom in the 2a (3m) site. The structure consists of face‐sharing K₆ octahedra with a fluoride anion at the center of each octahedron, forming chains of composition [FK₃]²⁺ running along [001] with isolated [TaF₇]²⁻ trigonal prisms in between. The structure of the title compound is different from the reported structure of Na₃TaF₈ and represents a new structure type.     

Characterization of an exception to the ‘even‐electron rule’ upon low‐energy collision induced decomposition in negative ion electrospray tandem mass spectrometry

Electrospray‐generated precursor ions usually follow the ‘even‐electron rule’ and yield ‘closed shell’ fragment ions. We characterize an exception to the ‘even‐electron rule.’ In negative ion electrospray mass spectrometry (ES‐MS), 2‐(ethoxymethoxy)‐3‐hydroxyphenol (2‐hydroxyl protected pyrogallol) easily formed a deprotonated molecular ion (M‐H)^? at m/z 183. Upon low‐energy collision induced decomposition (CID), the m/z 183 precursor yielded a radical ion at m/z 124 as the base peak. The radical anion at m/z 124 was still the major fragment at all tested collision energies between 0 and 50 eV (E_lab). Supported by computational studies, the appearance of the radical anion at m/z 124 as the major product ion can be attributed to the combination of a low reverse activation barrier and resonance stabilization of the product ions. Furthermore, our data lead to the proposal of a novel alternative radical formation pathway in the protection group removal of pyrogallol. Copyright © 2009 John Wiley & Sons, Ltd.     

Loss of CO from the molecular ions of o-, m- and p-anisoyl fluorides,CH3OC6H4COF,with fluorine atom migration

Loss of CO from the molecular ions ([CH₃OC₆H₄COF]⁺˙) of o-, m- and p-anisoyl fluorides has been investigated by mass-analysed ion kinetic energy (MIKE) spectrometry. This reaction involves fluorine atom migration from the carbonyl group to the benzene ring. In the cases of o- and p-anisoyl fluorides, the fluorine atom migrates via a three-membered transition state to form the molecular ions ([CH₃OC₆H₄F]⁺˙) of o- and p-fluoroanisoles, respectively. On the other hand, in the case of m-anisoyl fluoride, the fluorine atom migrates from the carbonyl group to the benzene ring via a three- or four-membered transition state.