C12A7-O-纳米材料的制备及抗菌活性

利用溶胶-凝胶法制备了C12A7-O-{[Ca24Al28O64]4+·4(O-)}纳米材料. 采用X射线衍射、电子顺磁共振及透射电子显微镜等手段对制备的材料进行了表征. 结果表明, 在最佳焙烧条件(1150 ℃, 6 h)下制备的材料平均粒径为74 nm, 并具有晶胞参数为(1.199±0.004) nm的C12A7(Ca12Al14O33)笼状结构, 材料内包含浓度高达1.2×1020 cm-3的氧负离子(O-). 初步研究结果表明, 合成的C12A7-O-纳米材料具有良好的广谱抗菌作用.     

溶胶-凝胶法制备多孔晶体材料C12A7-Cl-

利用溶胶-凝胶法制备了多孔晶体材料C12A7-Cl- (Ca12Al14O32Cl2), 制备凝胶的原料是四水合硝酸钙、九水合硝酸铝、氯化钙、尿素和乙二醇. 混合溶液经过搅拌2-3 h形成溶胶, 再经350 ℃热处理后形成凝胶体, 最终在流动氩气气氛中1000 ℃烧结后得到材料. 用X射线衍射, 场发射扫描电子显微镜, 热重分析, 电子顺磁共振和离子色谱等方法表征合成的C12A7-Cl-多孔晶体材料. 结果表明, 利用溶胶-凝胶法成功地生成了C12A7 结构, 氯负离子是材料中存储的主要负离子. 此外, 从C12A7-Cl-晶体材料表面发射的氯负离子也被飞行时间质谱观测到. 上述结果说明溶胶-凝胶法可被用于制备C12A7-Cl-晶体材料.     

M2+(M=Cu、Cd、Ag、Fe)掺杂氧化锌纳米粉晶的抗菌性能

采用柠檬酸溶胶-凝胶法制备了ZnO及M²⁺掺杂ZnO纳米粉晶(M=Cu、Cd、Ag、Fe),用现代测试技术表征了样品的组成、结构和形貌,以大肠杆菌(Escherichia coli)、金黄色葡萄球菌(Staphylococcus aureus)和白色念珠菌(Candida albicans)为测试菌株,用抑菌圈、最小抑菌浓度和最小杀菌浓度等方法研究了样品在日光照射下的抗菌活性。结果表明,与母体ZnO相比,Cu、Ag、Cd掺杂样品的抗菌性能明显地增强,这可能是由于掺杂金属离子置换Zn²⁺生成了晶格缺陷和电荷缺陷,阻止了光生电子和光生空穴对的复合从而增强了光催化活性和抗菌活性。     

掺杂Cs元素的微孔晶体材料C12A7的表征及负离子发射特性

利用浸渍CsI的方法在微孔晶体材料12CaO·7Al₂O₃ (C12A7)表面掺杂Cs元素并对其进行场发射扫描电镜、透射电子显微镜、X射线衍射以及电子顺磁共振的表征. 场发射扫描电镜以及透射电子显微镜的结果均证实CsI沉积在C12A7的表面; X射线衍射证明C12A7的结构并没有被破坏; 电子顺磁共振谱说明了浸渍后C12A7中的O^-和O₂^-浓度也无明显变化. 将浸渍后的同原始的C12A7进行比较发现, 掺杂样品在结构和存储特性上均无明显变化. 此外, 对该材料的发射性能与温度和引出场的关系也进行了研究与分析. 结果表明: 浸渍CsI至C12A7表面不仅降低了氧负离子的发射温度, 还大幅增强了发射强度; 氧负离子发射增强的主要原因归结于浸渍CsI后其表观活化能的降低.     

Al掺杂对尖晶石型LiMn2O4结构及循环性能的影响

用柠檬酸作为螯和物的载体,采用溶胶-凝胶法合成了A l3 掺杂的锂离子电池正极材料L iA lxMn2-xO4。XRD,SEM研究表明,于800℃煅烧可获得单一尖晶石结构的物相;随着A l3 掺入量的增加,L iA lxMn2-xO4的晶格常数变小,晶格更趋于完整,有利于抑制因锂的反复脱嵌而造成的结构破坏。x=0.05时,首次放电容量为103.8 mAh.g-1,25次循环后放电容量还有100.6 mAh.g-1,容量衰减仅为3.08%。     

低温区CsI掺杂的12CaO·7Al2O3型发射材料负离子的发射特性

本文利用潮湿浸渍法将碘化铯(CsI)掺杂至12CaO·7Al2O3(C12A7)型负离子存储发射材料的表面并对其的结构与存储特性进行了X射线衍射和电子顺磁共振的表征,与此同时还对该材料的发射特性、离子发射分支比以及温度对发射强度的影响等方面进行了研究和分析。将实验和表征结果与未掺杂的C12A7进行对比后发现,C12A7表面上CsI的掺入很大程度上改善了该材料的发射特性。掺杂CsI后,在800 V·cm-1的引出场下,发射温度由570℃降低至470℃,与此同时,在同样的发射条件下,其发射强度也明显增强。低温区(<500℃)氧负离子O-的发射纯度接近100%。以上结果表明掺杂CsI至C12A7表面是一种在低温下获得氧负离子O-源的有效途径。     

钼掺杂Li3V2（PO4）3/C正极材料的制备及其电化学性能研究

以Li2CO3、NH4H2PO4、V2O5和MoO3为原料,柠檬酸为络合剂和碳源,采用溶胶-凝胶法制备了锂离子正极材料Li3MoxV2-x(PO4)3/C(x=0.01,0.02,0.03).X射线衍射(XRD)表明,合成的材料具有单一的单斜晶系结构,空间群为P21/n.扫描电镜(SEM)显示Li3Mo0.02V1.98(PO4)3/C具有均一的表面形貌.恒流充放电测试表明,当x=0.02时,掺杂后的Li3Mo0.02V1.98(PO4)3具有最佳的电化学性能.在1C倍率下,3.0～4.3 V电位区间,Li3Mo0.02V1.98(PO4)3/C的首次放电比容量达到122.3 mAh.g-1,循环50周之后,容量没有衰减的迹象;而当x=0、0.01和0.03时,首次放电比容量仅分别为117.1、115.1和116.0 mAh.g-1.在3C和5C倍率下,样品Li3Mo0.02V1.98(PO4)3/C仍能保持优异的循环稳定性.     

过渡金属离子掺杂Zn3(OH)2V2O7·2H2O的合成及其光催化性质

利用水热法合成了3d过渡金属离子掺杂Zn3(OH)2V2O7·2H2O的微米花结构,其分子式可表达为Zn3-3xM3x(OH)2V2O7·2H2O(其中M=Cu,Co,Ni,Mn;0.001≤x≤0.20)。应用XRD、SEM、TEM、UV-Vis DRS、EDX和BET等分析测试技术对产物进行了表征。结构和形貌分析结果显示过渡金属离子掺杂后产物仍保持Zn3(OH)2V2O7·2H2O的六方晶体结构,微米花由主晶面为(0001)的纳米片组装而成。紫外-可见漫反射光谱显示过渡金属离子掺杂后带边吸收红移,其中以Cu的掺杂产物Zn3-3xCu3x(OH)2V2O7·2H2O最为明显,带边吸收扩展到可见光区。首次对Zn3(OH)2V2O7·2H2O及其不同金属离子掺杂产物Zn3-3xM3x(OH)2V2O7·2H2O进行了可见光催化降解有机污染物的研究,结果显示与其它产物相比掺0.1at%Cu的Zn2.997Cu0.003(OH)2V2O7·2H2O对亚甲基蓝(MB)的可见光催化降解效果最好。对掺杂离子种类、掺杂离子浓度对产物可见光催化性质的影响也进行了考察。     

钠离子电池Na2MnSiO4正极材料的合成、结构及其电化学性能研究

首次采用溶胶-凝胶法制备Na₂MnSiO₄/C纳米复合正极材料. X射线衍射（XRD）和Rietveld结构精修结果表明,合成的Na₂MnSiO₄材料为单斜晶系、Pn空间群. 红外光谱（FTIR）结果证实材料中不含有Na₂SiO₃和SiO₂等杂质. 电化学测试结果表明,该材料在1 mol·L^-1 NaClO₄/PC电解液中,电流密度为14 mA·g^-1、电压范围为1.5 ~4.2 V（vs. Na⁺/Na）测试条件下,其首次可逆放电比容量高达113 mAh·g^-1.     

微孔晶体材料C12A7-Cl-的表面氯负离子发射性能和机理

利用飞行时间质谱(TOF-MS)观测到氯负离子从合成的微孔晶体材料C12A7-Cl-(11CaO·7Al2O3·CaCl2)表面发射出来, 详细研究了C12A7-Cl-的发射特性, 包括发射强度分支比、温度效应、电场效应和表观活化能. 在我们的检测范围内从C12A7-Cl-表面发射的离子中绝大部分是氯负离子(最大强度分支比为98%), 此外还有弱的氧负离子和电子发射. 各种离子的绝对发射电流强度都随着表面温度升高或引出电场强度的增加而显著增强, 随着引出电场强度从200增加到1200 V·cm-1, 氯负离子发射的表观活化能从180.9 kJ·mol-1减小到110.0 kJ·mol-1. 氯负离子和C12A7-Cl-表面之间的结合能大约是228 kJ·mol-1. 研究了氯负离子的发射稳定性, 并且应用一种电化学注入法, 以获得持续的氯负离子发射. 基于上述实验还讨论了氯负离子的形成和发射机理. 目前的方法可望被用于发展氯负离子储存/发生器.     

Thermal decomposition mechanisms of MgCl2·6H2O and MgCl2·H2O

The thermal decomposition mechanisms and the intermediate morphology of MgCl₂·6H₂O and MgCl₂·H₂O were studied using integrated thermal analysis, X-ray diffraction, scanning electron microscope and chemical analysis. The results showed that there were six steps in the thermal decomposition of MgCl₂·6H₂O: producing MgCl₂·4H₂O at 69 °C, MgCl₂·2H₂O at 129 °C, MgCl₂·nH₂O (1 ≤ n ≤ 2) and MgOHCl at 167 °C, the conversion of MgCl₂·nH₂O (1 ≤ n ≤ 2) to Mg(OH)Cl·0.3H₂O by simultaneous dehydration and hydrolysis at 203 °C, the dehydration of Mg(OH)Cl·0.3H₂O to MgOHCl at 235 °C, and finally the direct conversion of MgOHCl to the cylindrical particles of MgO at 415 °C. To restrain the sample hydrolysis and to obtain MgCl₂·H₂O, MgCl₂·6H₂O was first calcined in HCl atmosphere until 203 °C when MgCl₂·H₂O was obtained; HCl gas was then turned off and the calcination process continued, producing Mg₃Cl₂(OH)₄·2H₂O calcined at 203 °C, Mg₃(OH)₄Cl₂ at 220 °C and MgO at 360 °C. The temperature of producing MgO from calcination of MgCl₂·H₂O was lower (360 °C) than that from MgCl₂·6H₂O (415 °C) because of its more reactive intermediate products: the irregular shape and tiny needle-like Mg₃Cl₂(OH)₄·2H₂O particles and the uneven surface porous Mg₃(OH)₄Cl₂ particles. The MgO particles obtained at 360 °C had a flake structure.     

Na2MoO4·2H2O晶体及其熔体结构的温致拉曼光谱

利用原位高温拉曼光谱技术对Na_2MoO_4·2H_2O(NMHO)晶体的脱水、相变以及熔融过程中微结构变化和分子振动特性进行了研究。结果显示在363 K,正交NMHO晶体脱水形成对称性更高的立方α-NMO(Na_2MoO_4)晶体;随着温度升高至熔点,α-NMO晶体经历了如下相变:α→β→γ→δ,分析了相变过程中温度对孤立的[MoO_4]_(2-)中Mo-O键的对称伸缩振动波数的作用,进而获得其平均键长以及对称性的变化过程;结合密度泛函理论对已知晶型的NMHO,α-NMO及γ-NMO晶体进行了拉曼光谱的计算模拟,并对其振动模式进行了归属;采用量子化学从头计算方法研究了NMO熔体中[MoO_4]~(2-)的团簇类型。     

The crystal structure determinations and refinements of K2S2O7, KNaS2O7 and Na2S2O7 from X-ray powder and single crystal diffraction data

The crystal structures of K₂S₂O₇, KNaS₂O₇ and Na₂S₂O₇ have been solved and/or refined from X-ray synchrotron powder diffraction data and conventional single-crystal data. K₂S₂O₇: From powder diffraction data, monoclinic C2/c, Z=4, a=12.3653(2), b=7.3122(1), , β=93.0792(7)°, R_Bragg=0.096. KNaS₂O₇: From powder diffraction data; triclinic , Z=2, a=5.90476(9), b=7.2008(1), , α=101.7074(9), β=90.6960(7), γ=94.2403(9)°, R_Bragg=0.075. Na₂S₂O₇: From single-crystal data; triclinic , Z=2, a=6.7702(9), b=6.7975(10), , α=116.779(2), β=96.089(3), γ=84.000(3)°, R_F=0.033. The disulphate anions are essentially eclipsed. All three structures can be described as dichromate-like, where the alkali cations coordinate oxygens of the isolated disulphate groups in three-dimensional networks. The K-O and Na-O coordinations were determined from electron density topology and coordination geometry. The three structures have a cation-disulphate chain in common. In K₂S₂O₇ and Na₂S₂O₇ the neighbouring chains are antiparallel, while in KNaS₂O₇ the chains are parallel. The differences between the K₂S₂O₇ and Na₂S₂O₇ structures, with double-, respectively single-sided chain connections and straight, respectively, corrugated structural layers can be understood in terms of the differences in size and coordinating ability of the cations.     

硼砂水溶液的低温热容及热化学性质研究

利用精密绝热量热仪测定了0.03355mol·kg-1的硼砂水溶液在78～351K温区的热容,从实验热容测定结果得到了该水溶液的凝固点为272.905K。用最小二乘法将实验热容值对温度进行拟合,建立了该溶液的热容随温度变化的多项式方程。根据热力学函数关系式,用此多项式方程进行数值积分,获得了以298.15K为基准的该溶液在80～350K温区每隔5K的热力学函数值,并计算出摩尔熔化焓和熔化熵分别为4.536kJ·mol-1和16.22J·K-1·mol-1。根据溶液凝固点降低值,计算出了该溶液的活度为0.99763。     

CO2在Na2Cr2O7溶液中的平衡溶解度模型

为研究重铬酸钠(Na₂Cr₂O₇)对CO₂溶解的影响, 本文在带有搅拌的气液相高压平衡釜内, 采用静态法测定了温度在313.2-333.2 K, 压力在0.1-1.9 MPa 范围内, 重铬酸钠浓度分别为0、0.361、0.650、0.901 mol·kg^-1 时, CO₂ 在Na₂Cr₂O₇溶液中的溶解度. 结果表明: (1) Na₂Cr₂O₇对CO₂ 的溶解有盐析效应; (2) CO₂ 在Na₂Cr₂O₇溶液中的溶解符合亨利定律, 并且CO₂溶解度是温度和Na₂Cr₂O₇浓度的函数, 且用改进的Setschenow方程和Peng-Robinson-Pitzer (PR-Pitzer)方程拟合了在此温度、压力及重铬酸钠浓度范围内的实验数据, 拟合效果较好, 并且其平均相对误差分别为4.24%和3.32%.     

Na(110)和Na2O(111)表面弛豫的研究

We have studied the relaxation of Na(110) and Na_2O(111) surfaces with LEED, and found that the best agreement between theory and experiment in such a structure, the surface layer distance d=0.291±0.01 nm (contracted 0.34%±0.01 nm) [for Na(110)]; and the three atomic surface layer distances d_1=0.117±0.01 nm (expanded 4.63%±0.01 nm), d_2=0.161±0.01 nm(expanded 0.063%±0.01 nm) and d_3=0.086±0.01 nm (expanded 0.75%±0.01 nm) [for Na_2O(111)].     

Crystal chemistry of Co-doped Zn7Sb2O12

Zn₇Sb₂O₁₂ forms a full range of Co-containing α solid solutions, Zn_7−xCo_xSb₂O₁₂, with an inverse-spinel structure at high temperature. At low temperatures for x<2, the solid solutions transform into the low temperature β-polymorph. For x=0, the β→α transition occurs at 1225±25 °C; the transition temperature decreases with increasing x. At high x and low temperatures, α solid solutions are formed but are non-stoichiometric; the (Zn+Co):Sb ratio is >7:2 and the compensation for the deficiency in Sb is attributed to the partial oxidation of Co²⁺ to Co³⁺. From Rietveld refinements using ND data, Co occupies both octahedral and tetrahedral sites at intermediate values of x, but an octahedral preference attributed to crystal field stabilisation, causes the lattice parameter plot to deviate negatively from the Vegard's law. Sub-solidus compatibility relations in the ternary system ZnO-Sb₂O₅-CoO have been determined at 1100 °C for the compositions containing ?50% Sb₂O₅.     

焦磷酸钠对液相碳化法制备纳米碳酸钙形貌的影响

利用液相碳化法制备了不同形态的纳米碳酸钙颗粒，用TEM、XRD和IR等手段分析表征了纳米碳酸钙的形态和结构，研究了焦磷酸钠对液相碳化法制备纳米碳酸钙合成过程及颗粒形态结构的影响规律。结果表明反应温度是影响纳米碳酸钙形态的关键因素，温度升高时纳米碳酸钙由立方形转变为纺锤形。焦磷酸钠能够促进碳酸钙的晶体成核，抑制晶体生长，在碳化温度大30 ℃时生成链状和棒状的纳米碳酸钙。另外，还分析了链状和棒状纳米碳酸钙的形成机理。     

Structure and magnetism of NaRu2O4 and Na2.7Ru4O9

The structures of NaRu₂O₄ and Na_2.7Ru₄O₉ are refined using neutron diffraction. NaRu₂O₄ is a stoichiometric compound consisting of double chains of edge sharing RuO₆ octahedra. Na_2.7Ru₄O₉ is a non-stoichiometric compound with partial occupancy of the Na sublattice. The structure is a mixture of single, double and triple chains of edge-shared RuO₆ octahedra. NaRu₂O₄ displays temperature independent paramagnetism with . Na_2.7Ru₄O₉ is paramagnetic, χ₀= with and a Curie constant of 0.0119 emu/mol Oe K. Specific heat measurements reveal a small upturn at low temperatures, similar to the upturn observed in La₄Ru₆O₁₉. The electronic contribution to the specific heat (γ) for Na_2.7Ru₄O₉ was determined to be15 mJ/mole_Ru K².     

Pulse radiolysis study of trapped electron in MgSO4.7H2O single crystal

The single crystal of MgSO₄.7H₂O is very interesting to study the structure and kinetics of trapped electron in solids, because the hydrated salt has many H₂O molecules in the crystal lattice like water. The pulse radiolysis study of the trapped electrons in MgSO₄.7H₂O single crystal was carried out based on an electron linear accelerator. Two optical absorption peaks of the trapped electron in MgSO₄.7H₂O single crystal were observed: one is at the wavelength of 600 nm with a short lifetime of 81.4 ns; another is at 400 nm with a long lifetime of 1.06 μs. The kinetics of the trapped electron in the crystal was also compared with that in the aqueous solution.