AlCl3(ZnCl2,MgCl2)对Sm2O3的氯化效果及电化学行为

研究了AlCl₃(ZnCl₂、MgCl₂)对Sm₂O₃的氯化效果以及Sm₂O₃在LiCl-KCl-AlCl₃(ZnCl₂、MgCl₂)熔盐体系中的电化学行为。在LiCl-KCl-Sm₂O₃熔盐中加入AlCl₃(ZnCl₂、MgCl₂)后,ICP测量结果表明,AlCl₃体系中Sm(Ⅲ)离子的浓度最高,并且在923 K时达到最大值;固相反应表明,AlCl₃氯化Sm₂O₃生成SmCl₃,而Sm₂O₃和ZnCl₂(MgCl₂)反应生成SmOCl。电化学行为表明,AlCl₃体系中观察到了两种Al-Sm的合金峰,而ZnCl₂体系中只观察到Zn-Sm金属间化合物的形成峰,MgCl₂体系中没有形成合金。在-6.25 A·cm^-2下,W电极上恒电流电解2 h获得了Al-Li-Sm合金,经XRD分析,合金为Al₂Sm相。     

MoS2非贵金属电催化剂担载对p-InP光阴极分解水性能的影响

将MoS₂电催化剂担载在InP光阴极表面,提升了InP光阴极光电化学分解水产氢性能,确定了最优的MoS₂电催化剂担载电量为15mC·cm^-2;在担载前后,开启电势由-100mV移动至120mV;在-0.35VvsRHE时,电流密度由15mA·cm^-2提升至43mA·cm^-2。另外,通过改变入射光强和加入电子牺牲剂的方法进一步研究了MoS₂担载InP光阴极产氢反应的限制步骤为光生电子与空穴在InP表面的复合。     

Zn掺杂Co9S8纳米材料的制备及其在超级电容器和电催化析氢中的应用

采用原位溶剂热生长法设计合成了锌掺杂Co₉S₈纳米颗粒。各种表征技术和性能测试结果表明：锌掺杂Co₉S₈纳米颗粒的孔尺寸为18 nm,比表面积为23 m²·g^-1;同时微量的锌掺杂显著增强了Co₉S₈的电催化析氢（HER）活性及电容器性能。在HER性能测试中,当电流密度为10 mA·cm^-2时电位为-361 mV,电流密度最高可达38.26 mA·cm^-2,且具有优异的循环稳定性。同时在电容器性能测试中具有较高的比电容,当电流密度为1 A·g^-1时,质量比电容和面积比电容分别为235.48 F·g^-1和812.4 mF·cm^-2。     

碳布负载高致密Sn/SnBi合金的电催化CO2还原性能

通过分步电沉积法制备碳布(CC)负载高致密Sn/SnBi合金催化剂：首先在CC上电沉积致密Sn颗粒,而后利用酸性电解液部分溶解Sn为Sn²⁺离子,实现在Sn颗粒表面共沉积SnBi合金枝晶,随后经过原位化学氧化及电化学还原步骤将SnBi合金枝晶转变为SnBi合金纳米颗粒(SnBi NPs)。得益于Sn提供形核位点,SnBi枝晶在碳织物表面垂直致密生长,并通过后续氧化还原转化实现了直径约20 nm的SnBi合金颗粒在CC上致密均匀生长。CC/Sn/SnBi NPs三维电极在-1.08 V (vs RHE)下显示出较高的电催化还原CO₂活性,电流密度高达36 mA·cm^-2且甲酸盐产物选择性为94.9%。同时,在连续12 h恒电压测试中性能未发生衰减,表明电极具有良好的稳定性。     

碳布负载高致密Sn/SnBi合金的电催化CO2还原性能

通过分步电沉积法制备碳布(CC)负载高致密Sn/SnBi合金催化剂：首先在CC上电沉积致密Sn颗粒,而后利用酸性电解液部分溶解Sn为Sn²⁺离子,实现在Sn颗粒表面共沉积SnBi合金枝晶,随后经过原位化学氧化及电化学还原步骤将SnBi合金枝晶转变为SnBi合金纳米颗粒(SnBi NPs)。得益于Sn提供形核位点,SnBi枝晶在碳织物表面垂直致密生长,并通过后续氧化还原转化实现了直径约20nm的SnBi合金颗粒在CC上致密均匀生长。CC/Sn/SnBiNPs三维电极在-1.08V(vsRHE)下显示出较高的电催化还原CO₂活性,电流密度高达36mA·cm^-2且甲酸盐产物选择性为94.9%。同时,在连续12h恒电压测试中性能未发生衰减,表明电极具有良好的稳定性。     

温和条件下CO2为原料电合成碳酸二甲酯

常温常压下, 研究了以CO₂和甲醇为原料电合成碳酸二甲酯的反应. 在四乙基溴化铵为支持电解质的乙腈溶液中, 通过恒电流电解得到了唯一的产物碳酸二甲酯. 为了优化电解条件, 分别考察了工作电极、电流密度、支持电解质、通电量以及电解前后加入甲醇顺序的不同等因素对该反应的影响. 以铜为工作电极, 石墨为对电极, 在17 mA•cm^－2的电流密度下恒电流电解, 当通过2 F•mol^－1的电量后, 碳酸二甲酯的产率可达74%, 大大高于文献报道值.     

二硫化钴多孔风叶结构助力肼辅助高效电解产氢

以泡沫镍(NF)为基底,采用一步水热法制备了主晶相为CoS₂、夹杂少量NiO相、具有三维多孔风叶结构的CoS₂/NF电极材料。当溶液中钴硫物质的量之比为 1∶5 时,在 140 ℃下保温 18 h,获得了由 10 nm 厚度的纳米片构成的三维风叶结构的晶态CoS₂/NF电催化剂。CoS₂/NF在肼氧化及析氢反应中均表现出优异的催化性能,在水合肼碱性介质中,获得-10 mA·cm^-2的析氢电流密度时,需要的过电势仅为83 mV,获得50 mA·cm^-2的氧化电流密度时,需要的肼氧化电位仅为51 mV(vs RHE);在水合肼辅助电解水双功能电解槽中,获得100 mA·cm^-2的电流密度时,需要的分解槽压仅为0.550 V,远低于其在同条件下全水分解的2.075 V,大幅减小了电能消耗,极大地提高了电解水产氢效率。无论在三电极体系还是双电极体系,CoS₂/NF均表现出优异的长效稳定性及耐用性。分析认为,电极表面多孔风叶结构的形成,使其电化学活性面积增加了24倍,为催化反应的发生提供了海量的活性位点及物质传递通道。CoS₂及NiO相的形成,在一定程度上协同改善了本征析氢活性。CoS₂/NF的组成、结构特性共用造就了其优异催化性能,其中结构优势起主导作用。通过机理研究,提出了CoS₂/NF在析氢及肼氧化过程中的反应路径。     

CoFeOx/MoO2准平行纳米阵列电极的析氢性能

利用CoFe层状双金属氢氧化物(CoFe LDH)准平行纳米片阵列作为载体前驱体,通过原位负载及煅烧方式,实现了含有氧空位的 MoO₂纳米颗粒在纳米片阵列表面的生长。电化学研究结果表明,所得 CoFeO_x/MoO₂纳米阵列电极具有高析氢反应(HER)催化活性。该电极在10和1 000 mA·cm^-2时的HER过电位分别为40和217 mV。在50 mA·cm^-2的电流密度下,该电极可以稳定运行125 h。     

Co金属有机骨架模板制备NiCo水滑石/泡沫镍复合材料及电容性能

通过两步法先在泡沫镍(nickel foam,NF)上原位生长Co金属有机骨架(Co metal-organic framework,Co-MOF)纳米片阵列,再浸入不同浓度Ni²⁺离子溶液刻蚀Co-MOF纳米片,在NF表面得到NiCo水滑石(NiCo layered double hydroxide,NiCo-LDH)。NiCo-LDH/NF继承了Co-MOF纳米片结构形成一级纳米片阵列,并在一级纳米片表面形成次级纳米片褶皱。在2 mmol Ni(NO₃)₂·6H₂O溶液中刻蚀得到的NiCo-LDH/NF表现出高容量、高倍率性能,在电流密度为5 mA·cm^-2时比电容为7 764.5 mF·cm^-2,电流密度为20 mA·cm^-2时比电容为6 098.2 mF·cm^-2,容量保持率为78.5%,在20 A·g^-1电流密度下经过5 000次长循环后,容量保持率为85.9%。与活性炭组装的混合电容器达到38.9 Wh·kg^-1的最大能量密度和8 000.0 W·kg^-1的最大功率密度。     

Bi2S3/CdSe共修饰TiO2纳米管膜的构建及其光电化学阴极保护效应

为获得良好光电化学性能的TiO₂半导体复合膜,采用Bi₂S₃和CdSe对TiO₂纳米管膜进行共修饰。以阳极氧化法在Ti表面先制备TiO₂纳米管膜,再通过恒电流电沉积和连续离子层吸附反应在纳米管表面依次沉积CdSe和Bi₂S₃,构建了具有级联能带结构的Bi₂S₃/CdSe共修饰的TiO₂纳米管复合膜。结果表明,Bi₂S₃/CdSe/TiO₂纳米管复合膜对可见光吸收显著增强,光电化学性能大幅度提高。白光照射下,复合膜的光电流密度为670 μA·cm^-2,达到了纯TiO₂纳米管膜的17.6倍。Bi₂S₃/CdSe/TiO₂复合膜作为光阳极可使0.5 mol·L^-1 NaCl溶液中的403不锈钢的电位相对于腐蚀电位下降690 mV,显示出良好的光电化学阴极保护效应。     

Li_(1.3)Ti_(1.7)Al_(0.3)(PO_4)_3,Na_(1.3)Ti_(1.7)Al_(0.3)(PO_4)_3的离子交换研究

研究了在不同温度下的NaNO3和AgNO3水溶液中Li1.3Ti1.7Al0.3(PO4)3和Na1.3Ti1.7Al0.3(PO4)3离子交换行为.实验表明Li1.3Ti1.7Al0.3(PO4)3和Na1.3Ti1.7Al0.3(PO4)3均显示出了高选择性与Na+和Ag+进行离子交换的特征,且对Ag+的选择性高于Na+.升高温度可显著提高Ag/Li和Ag/Na的交换反应速度.     

Crystal growth, structure determination, and optical properties of new potassium-rare-earth silicates K3RESi2O7 (RE=Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu)

Single crystals of K₃RESi₂O₇ (RE=Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu) were grown from a potassium fluoride flux. Two different structure types were found for this series. Silicates containing the larger rare earths, RE=Gd, Tb, Dy, Ho, Er, Tm, Yb crystallize in a structure K₃RESi₂O₇ that contains the rare-earth cation in both a slightly distorted octahedral and an ideal trigonal prismatic coordination environment, while in K₃LuSi₂O₇, containing the smallest of the rare earths, lutetium is found solely in an octahedral coordination environment. The structure of K₃LuSi₂O₇ crystallizes in space group P6₃/mmc with a=5.71160(10) Å and c=13.8883(6) Å. The structures containing the remaining rare earths crystallize in the space group P6₃/mcm with the lattice parameters of a=9.9359(2) Å, c=14.4295(4) Å, (K₃GdSi₂O₇); a=9.88730(10) Å, c=14.3856(3) Å, (K₃TbSi₂O₇); a=9.8673(2) Å, c=14.3572(4) Å, (K₃DySi₂O₇); a=9.8408(3) Å, c=14.3206(6) Å, (K₃HoSi₂O₇); a=9.82120(10) Å, c=14.2986(2) Å, (K₃ErSi₂O₇); a=9.80200(10) Å, c=14.2863(4) Å, (K₃TmSi₂O₇); a=9.78190(10) Å, c=14.2401(3) Å, (K₃YbSi₂O₇). The optical properties of the silicates were investigated and K₃TbSi₂O₇ was found to fluoresce in the visible.     

B2O3-Bi2O3-ZnO-Al2O3玻璃助烧剂对BaTiO3陶瓷烧结条件、晶体结构和介电性能的影响

通过调节B₂O₃-Bi₂O₃-ZnO-Al₂O₃(BBZA)玻璃的添加量研究其对钛酸钡(BaTiO₃)陶瓷烧结条件、晶体结构和介电性能的影响。结果表明：添加适量的BBZA玻璃能够有效地将BaTiO₃陶瓷烧结温度由1 350℃降至950℃,并使其致密化。同时,添加BBZA玻璃后,BaTiO₃的晶体结构随着烧结温度的升高而发生转变(立方相→四方相)。另外,BBZA玻璃的引入使BaTiO₃陶瓷的居里峰得到了有效的抑制和拓宽。陶瓷微观形貌显示,玻璃相均匀分布在BaTiO₃晶粒表面。优化的BaTiO₃陶瓷制备条件如下：BBZA添加量(质量分数)为2.0%,烧结温度为950℃。在该条件下制备的BaTiO₃陶瓷介电常数达到1 364,介电损耗低至1.2%。     

Metal-organic deposition of YBa2Cu3Ox and Bi2Sr2Ca1Cu2Ox films on various substrates starting from different fluorine-free metallorganic compounds

YBa₂Cu₃O_x (Y-123) and Bi₂Sr₂Ca₁Cu₂O_x (Bi-2212) films on various substrates have been prepared by Metal-Organic Deposition starting from different metallorganic fluorine-free compounds and using a very simple instrumentation. The processing conditions include a rapid pyrolysis step in air and an annealing step in oxygen for Y-123 and in air for Bi-2212. The films obtained have been characterized by X-ray diffraction (XRD) and the formation of a superconducting phase of Y-123 or Bi-2212 was confirmed measuring the critical temperature (T _c) with Ac-susceptibility and resistive measurements. Microstructure and final cationic ratios have been studied by scanning electron microscopy (SEM) and energy dispersive spectroscopy (EDS).     

Decomposition of P2S2N4(Si(CH3)3)4A12C14 as Studied by FT-Raman and Quantum Chemistry Means

The dimeric title compound decomposes upon heating to give the monomer and desulphurized monomer as shown by FT-Raman and quantum chemical means.     

Near infrared study of aqueous rare-earth ethylsulfates

The near infrared spectra of aqueous solutions of the ethylsulfates of La, Nd, Gd, Tb, Er, Yb, Lu, Y, and Na have been determined from about 0.2 mol-dm^–3 to nearly saturation. The extinction coefficients of water have been calculated taking into account the absorption of ethylslfate anions determined in separate experiments. Their values appeared to be nearly the same as that of pure water. The relative contents of free OH groups in 0.5 and 0.7M solutions have been estimated from the absorbances at 1160 nm. They were lower in solutions of the heavy rare-earth ethylsulfates (Tb, Er, Yb, Lu) than in equimolar solutions of the lighter ones (La, Nd), confirming our previous view that secondary hydration of the heavy trivalent rare-earth cations is distinctly stronger than that of the lighter ones. A comparison of the spectra of these aqueous ethylsulfates with those of perchlorates shows that the structure-breaking ability of the C₂H₅SO ₄ ^– ion is much smaller than that of perchlorate anion.     

电感耦合等离子体光谱法(ICP-AES)测定银精矿中铜、铅、锌、砷、镉、钙、镁、锰含量

针对银精矿样品复杂,难消解的特点,研究了不同酸溶法和碱熔法对样品的消解情况,建立了硝酸,盐酸,氢氟酸,高氯酸消解银精矿的方法。根据元素灵敏度和抗干扰性,选定各元素的测定波长。通过酸溶样和碱熔样测定结果比对,验证了方法准确性。建立了四酸消解-电感耦合等离子体光谱法测定银精矿中铜、铅、锌、砷、镉、钙、镁、锰含量的方法,元素的线性相关系数均在0.9999以上。通过共存元素干扰实验,确定了银精矿中高含量元素(铜、铅、锌、铁、锑、铋等)对测定元素结果没有影响。方法检出限：Cu 0.0063 mg/L, Pb 0.0159 mg/L ,Zn 0.0090 mg/L,As 0.0192 mg/L, Cd 0.0093 mg/L ,Ca 0.0084 mg/L, Mg 0.0075 mg/L, Mn 0.0081 mg/L。测定下限：Cu 0.0105mg/L,Pb 0.0265 mg/L, Zn 0.0150 mg/L, As 0.0320 mg/L, Cd 0.0155 mg/L, Ca 0.0140 mg/L, Mg 0.0125 mg/L,Mn 0.0135 mg/L。3个样品的相对标准偏差在0.87%~3.56%之间,加标回收率在95.00%~103.56%之间。方法流程短,操作简单,快速,灵敏度和再现性高,结果准确可靠,可以满足银精矿中铜、铅、锌、砷、镉、钙、镁、锰含量的测定。     

Structural studies of five layer Aurivillius oxides: A2Bi4Ti5O18 (A=Ca, Sr, Ba and Pb)

The room temperature structures of the five layer Aurivillius phases A₂Bi₄Ti₅O₁₈ (A=Ca, Sr, Ba and Pb) have been refined from powder neutron diffraction data using the Rietveld method. The structures consist of [Bi₂O₂]²⁺ layers interleaved with perovskite-like [A₂Bi₂Ti₅O₁₆]²⁻ blocks. The structures were refined in the orthorhombic space group B2eb (SG. No. 41), Z=4, and the unit cell parameters of the oxides are a=5.4251(2), b=5.4034(1), c=48.486(1); a=5.4650(2), b=5.4625(3), c=48.852(1); a=5.4988(3), b=5.4980(4), c=50.352(1); a=5.4701(2), b=5.4577(2), c=49.643(1) for A=Ca, Sr, Ba and Pb, respectively. The structural features of the compounds were found similar to n=2-4 layers bismuth oxides. The strain caused by mismatch of cell parameter requirements for the [Bi₂O₂]²⁺ layers and perovskite-like [A₂Bi₂Ti₅O₁₆]²⁻ blocks were relieved by tilting of the TiO₆ octahedra. Variable temperature synchrotron X-ray studies for Ca and Pb compounds showed that the orthorhombic structure persisted up to 675 and 475 K, respectively. Raman spectra of the compounds are also presented.     

The crystal chemistry of Bi6TP2O15+x, T=Fe, Ni, Zn: Isomorphism and polymorphism, structural relationship to Bi6TiP2O16

The crystal structures of compounds with nominal compositions Bi₆FeP₂O_15+x (I), Bi₆NiP₂O_15+x (II) and Bi₆ZnP₂O_15+x (III) were determined from single-crystal X-ray diffraction data. They are monoclinic, space group I2, Z=2. The lattice parameters for (I) are a=11.2644(7), b=5.4380(3), c=11.1440(5) Å, β=96.154(4)°; for (II) a=11.259(7), b=5.461(4), c=11.109(7) Å, β=96.65(1)°; for (III) a=19.7271(5), b=5.4376(2), c=16.9730(6) Å, β=131.932(1)°. Least squares refinements on F² converged for (I) to R1=0.0554, wR₂=0.1408; for (II) R₁=0.0647, wR₂=0.1697; for (III) R₁=0.0385, wR₂=0.1023. The crystals are complexly twinned by 2-fold rotation about , by inversion and by mirror reflection. The structures consist of edge-sharing articulations of OBi₄ tetrahedra forming layers in the a-c plane that then continue by edge-sharing parallel to the b-axis. The three-dimensional networks are bridged by Fe and Ni octahedra in (I) and (II) and by Zn trigonal bipyramids in (III) as well as by oxygen atoms of the PO₄ moieties. Bi also randomly occupies the octahedral sites. Oxygen vacancies exist in the structures of the three compounds due to required charge balances and they occur in the octahedral coordination polyhedron of the transition metal. In compound (III), no positional disorder in atomic sites is present. The Bi-O coordination polyhedra are trigonal prisms with one, two or three faces capped. Magnetic susceptibility data for compound (I) were obtained between 4.2 and 350 K. Between 4.2 and 250 K it is paramagnetic, μ_eff=6.1 μ_B; a magnetic transition occurs above 250 K.     

Structure Study of Bi2.5Na0.5Ta2O9 and Bi2.5Nam−1.5NbmO3m+3 (m=2-4) by Neutron Powder Diffraction and Electron Microscopy

The crystal structures of Bi_2.5Na_0.5Ta₂O₉ and Bi_2.5Na_m-1.5Nb_mO_3m+3 (m=3,4) have been investigated by the Rietveld analysis of their neutron powder diffraction patterns (λ=1.470 Å). These compounds belong to the Aurivillius phase family and are built up by (Bi₂O₂)²⁺ fluorite layers and (A_m-1B_mO_3m+1)^2- (m=2-4) pseudo-perovskite slabs. Bi_2.5Na_0.5Ta₂O₉ (m=2) and Bi_2.5Na_2.5Nb₄O₁₅ (m=4) crystallize in the orthorhombic space group A2₁am, Z=4, with lattice constants of a=5.4763(4), b=5.4478(4), c=24.9710 (15) and a=5.5095(5), b=5.4783(5), c=40.553(3) Å, respectively. Bi_2.5Na_1.5Nb₃O₁₂ (m=3) has been refined in the orthorhombic space group B2cb, Z=4, with the unit-cell parameters a=5.5024(7), b=5.4622(7), and c=32.735(4) Å. In comparison with its isostructural Nb analogue, the structure of Bi_2.5Na_0.5Ta₂O₉ is less distorted and bond valence sum calculations indicate that the Ta-O bonds are somewhat stronger than the Nb-O bonds. The cell parameters a and b increase with increasing m for the compounds Bi_2.5Na_m-1.5Nb_mO_3m+3 (m=2-4), causing a greater strain in the structure. Electron microscopy studies verify that the intergrowth of mixed perovskite layers, caused by stacking faults, also increases with increasing m.