Phase equilibria and glass formation in the As2S3-TlAs2S2Se2 section of the As2S3-As2Se3-TlS system

Alloys in the As₂S₃-TlAs₂S₂Se₂ section of the As₂S₃-As₂Se₃-TlS ternary system were studied and a phase diagram was constructed using physicochemical methods (differential thermal analysis, microstructural analysis, X-ray powder diffraction, also microhardness and density measurements). The diagram in the As₂S₃-TlAs₂S₂Se₂ section is a non-quasi-binary diagonal section of the As₂S₃-As₂Se₃-TlSe quasi-ternary system. It was found that all the alloys in the section under ordinary conditions are obtained in the vitreous state. At low As₂S₃ concentrations in the section, solid solutions form up to 2.5 mol %, and at low TlAs₂S₂Se₂ concentrations, their extent is 3 mol %.     

Interactions of Cr2S3 with GeS2 and Cu2GeS3

The interactions in the GeS₂-Cr₂S₃ and Cu₂GeS₃-Cr₂S₃ sections were studied by differential thermal analysis and X-ray powder diffraction. The GeS₂-Cr₂S₃ section was shown to be quasi-binary, with a degenerate eutectic; no ternary compound was formed. In the Cu₂GeS₃-Cr₂S₃ section, a quaternary phase of variable composition having a homogeneity range of 69–75 mol % Cr₂S₃ crystallized in the cubic system. The samples of this composition are spin glasses with freezing temperatures of 20–25 K.     

Phase diagram of the In3As2Se6-In3As2S3Se3 system

The In₃As₂Se₆-In₃As₂S₃Se₃ system has been investigated by methods of physicochemical analysis (DTA, X-ray powder diffraction, MSA) and by microhardness and density measurements. The phase diagram of the system, which is the quasi-binary section of the As-In-S-Se quaternary system, has been constructed. The region of the In₃As₂Se₆-based solid solutions is extended to 7 mol %, and the In ₃As₂S₃Se₃-based region to 15 mol %. A new quaternary compound In₆As₄S₃Se₉ is found in the system. Original Russian Text ? I.I. Aliev, R.S. Magammedragimova, A.A. Farzaliev, Dzh. Veliev, 2009, published in Zhurnal Neorganicheskoi Khimii, 2009, Vol. 54, No. 4, pp. 691–694.     

Mo¨ssbauer studies of thiospinels. IV. The system FeCr2S4-Fe3S4

Spinel compounds of the composition Fe_1+xCr_2?xS₄, with 0 ≦ x ≦ 0.5, have been prepared in polycrystalline form. The ionic distribution Fe²⁺[Cr³⁺_2?xFe³⁺_x]S^2?₄ is derived from both X-ray and ⁵⁷Fe Mo¨ssbauer data. Room temperature Mo¨ssbauer spectra show the typical behavior of tetrahedral-site Fe²⁺ surrounded by different octahedral-site neighbors. Octahedral-site Fe³⁺ absorbs as a doublet with Δ ≈ 0.5 mm/s. Samples of overall composition FeCr₂S₄ consist mainly of a spinel Fe²⁺[Cr³⁺_2?yFe³⁺_y]S^2?₄, y ≈ 0.02.     

Phase diagram of the Pb5Sb4S11-Pb2SnSb2S6 system

The Pb₅Sb₄S₁₁-Pb₂SnSb₂S₆ system was studied by a number of physicochemical methods, and its phase diagram was constructed. It was found that the system under investigation is a quasi-binary eutectic type section of the SnS-PbS-Sb₂S₃ ternary system. The coordinates of the eutectic are found to be 33 mol % Pb₅Sb₄S₁₁ and 750 K. Regions of solid solutions based on Pb₅Sb₄S₁₁ (6 mol % Pb₂SnSb₂S₆) and Pb₂SnSb₂S₆ (4 mol % Pb₅Sb₄S₁₁) were determined.     

The phase relationship among compounds Ba1+xFe2S4

The dependence of composition of the phases Ba_1+xFe₂S₄ on sulfur vapor pressure and starting composition was investigated at 650, 747, and 800°C. The infinitely adaptive series Ba_1+xFe₂S₄ spans the compositions 0.072 ≤ x ≤ 0.142. The value of x decreases as the sulfur vapor pressure increases at a given temperature. Varying the ratio of $\text{Ba}\text{Fe}$ in the starting mixture has no effect on the Ba_1+xFe₂S₄-sulfur fugacity relationship. The phase BaFe₂S₄ is not part of the infinitely adaptive series.     

Electrical resistivity of cubanite: CuFe2S3

The electrical resistivity of a single crystal of cubanite, CuFe₂S₃, has been determined from 4.2 to 340 K. Definite semiconducting behavior is observed, showing that the rapid electron exchange between Fe²⁺ and Fe³⁺ in Cu¹⁺Fe²⁺Fe³⁺S₃ is confined to the edge-shared pairs of iron-sulfur tetrahedra.     

介孔调控Co9S8/Ni3S2复合电极材料及电催化析氢性能

利用快速凝固结合化学脱铝模板法制备前驱体纳米多孔Ni-Co合金,再经气相沉积硫和热氢还原制备纳米多孔Co₉S₈/Ni₃S₂复合电极材料。研究表明,通过气相沉积,硫原子与Ni-Co合金原位生成CoS₂/NiS₂复合相,再经过热氢还原后,形成硫原子比例较低的Co₉S₈/Ni₃S₂复合相。该热氢还原过程不仅提高了Co₉S₈/Ni₃S₂各元素周围的电子密度,而且在其表面调制出有介孔结构的异质界面,进而提高其电子传输能力并增大活性比表面积。相比于其他同条件下制备的Ni、Co硫化物,Co₉S₈/Ni₃S₂拥有更佳的析氢反应（HER）活性,在50 mA·cm^-2的电流密度下,Co₉S₈/Ni₃S₂的HER过电位为234 mV,Tafel斜率为106 mV·dec^-1,经稳定性测试后,电压变化仅为14 mV。     

泡沫镍负载Fe2O3@Ni3S2纳米线网状结构电极的制备及其电催化析氧性能

通过两步水热法制备泡沫镍(NF)负载Fe_2O_3纳米粒子@Ni_3S_2纳米线网状结构电极(Fe_2O_3@Ni_3S_2/NF)。运用X射线衍射(XRD)、X射线光电子能谱(XPS)、透射电子显微镜(TEM)、N_2吸附-脱附测试等方法对电极材料的物相和微观结构特征等进行了表征。水热条件下原位表面化学刻蚀生成的Ni_3S_2纳米线与三维多孔NF基体间拥有强结合力和低界面电阻,Fe_2O_3粒子均匀分布在纳米线的表面。在1 mol·L~(-1)的KOH溶液中,运用线性扫描伏安测试(LSV)、计时电位法、电化学交流阻抗测试(EIS)等对电极的电催化析氧(OER)性能进行了测试。结果表明:在100 mA·cm~(-2)的超高电流密度下,Fe_2O_3@Ni_3S_2/NF电极的OER过电势仅为223 mV,比Ni_3S_2/NF材料的过电势降低了285 mV;经过10 h计时电位测试,性能保持率高达80%。     

Structure de La2Fe2S5 et de La2Fe1.87S5

The compound La₂Fe₂S₅ is orthorhombic. Cell parameters are: a = 3.997(2)Å; b = 16.485(5)Å; c = 11.394(4)Å. Space group is Cmc2₁ (Z = 4. In the cell, chains of polyedra comprised of sulfur atoms tetrahedrally or octahedrally coordinating centrally located iron atoms give a monodimensional character to the structure. This one is refined to R = 0.037. To complete the study of these chains, in the La₂Fe_2?xS₅ system, vacancies are introduced on iron atom sites. The ordered compound, La₂Fe_1.87S₅, having such vacancies, is an orthorhombic superstructure of the stoechiometric compound. Cell parameters are: a = 3.9996(5)Å; b = 49.508(3)Å; c = 11.308(3)Å. Space group is Cmc2₁ and Z = 12. The structure is refined to R = 0.068. Only two iron atom sites have vacancies. One is tetrahedral, the other octahedral. In this last case the chain deformations are the more important. The chain becomes a sort of tunnel made of atoms of sulfur, with in its center the short iron-iron separation of 2.82 Å.     

Tl2S-Sb2S3-Bi2S3 quasi-ternary system

The Tl₂S-Sb₂S₃-Bi₂S₃ quasi-ternary system (system A) was studied using DTA, X- ray powder diffraction, microstructure examination, and microhardness measurements. TlSbS₂-Tl₄Bi₂S₅(TlBiS₂, Bi₂S₃), Sb₂S₃-TlBiS₂, Tl₃SbS₃-TlBiS₂(Bi₂S₃), and [TlSb_0.5Bi_0.5S₂]-Tl₂S isopleths; isothermal sections at 500 K; and liquidus surface projection of system A were constructed. Characteristic features of the title system are extensive fields of solid solutions extended along the TlSbS₂-TlBiS₂ quasi-binary section and a continuous solubility belt 1–2 mol % wide extended along the Sb₂S₃-Bi₂S₃ binary subsystem. Primary separation fields of phases and the types and coordinates of invariant and monovariant equilibria in system A were determined.     

Phases in the Ba3Fe1+xS5 series: The structure of β-Ba9Fe4S15 and its low-temperature α polymorph

The crystal structure of β-Ba₉Fe₄S₁₅ shows that it is a phase in the infinitely adaptive series of compounds Ba₃Fe_1+xS₅, 0 ? x ? 1. The material is synthesized by reacting a slightly sulfur-rich mixture at 900°C in a sealed quartz ampoule. Lattice constants are a = 25.212(3), Å, b = 9.594(1), Å, c = 12.575(1), Å, Pnma, z = 4. Three thousand thirty-three structure amplitudes were refined to R = 0.049. BaS₆ trigonal prisms share triangular faces to form infinite columns; the columns in turn share edges and create nearly hexagonal enclosures. Within these rings are additional Ba and S and tetrahedral interstices are created which can be occupied by Fe. The variation of the Fe occupancy from ring to ring gives rise to phases in which one dimension is an integral multiple of the 8.5-Å repeat observed in one end member of the series, Ba₃FeS₅. The other end member is Ba₃Fe₂S₅. At temperatures below 900°C a polymorphic phase is formed. Its lattice constants are a = b = 9.634(1), Å, c = 34.311(3)Å, $\text{I4}{}_1\text{a}\text{, z = 4}$. One thousand five hundred eighty-three structure amplitudes were refined to R = 0.0483. Trigonal prisms and bisdisphenoids articulate to form a complex three-dimensional structure. Two of the S atoms in the structure have statistical site occupancies.     

Interaction in the Ga2S3-Y2O2S system

The phase diagram of the Ga₂S₃-Y₂O₂S system has been investigated by differential thermal, X-ray powder diffraction, microstructural, and thermodynamic analyses. It has been established that the system is eutectic, and solubility at 295 K from the Ga₂S₃ side reaches 3 mol % Y₂O₂S. The coordinates of the eutectic point are 14 mol % Y₂O₂S and 1320 K.     

Insights into photoluminescence property and photocatalytic activity of cubic and rhombohedral ZnIn2S4

Cubic and rhombohedral ZnIn₂S₄ were synthesized by thermal sulfidation of Zn-In mixed oxide precursor in H₂S atmosphere at different temperatures. Cubic ZnIn₂S₄ was obtained when Zn-In mixed oxide precursor was sulfurized at 400 °C. With sulfidation temperature increasing from 400 to 800 °C, the crystal phase of ZnIn₂S₄ gradually turned from cubic to rhombohedral, which was demonstrated by different analysis techniques such as XRD, Raman, SEM, etc. UV-vis absorption spectra indicated that cubic ZnIn₂S₄ displayed better light absorption property than rhombohedral ZnIn₂S₄, with band gaps calculated to be 2.0 and 2.5 eV, respectively. However, under visible light irradiation, rhombohedral ZnIn₂S₄ photocatalyzed H₂ evolution from aqueous sodium sulfite/sulfide solution efficiently, whereas cubic ZnIn₂S₄ was not active for this reaction. The photoluminescence property revealed the different dynamics of photogenerated carriers, which made a predominant contribution to the increasing photocatalytic performances of ZnIn₂S₄ with crystal phase turning from cubic to rhombohedral.     

Mo¨ssbauer studies of thiospinels. III. The system FeCr2S4 -FeIn2S4

Polycrystalline samples of spinel compounds FeCr_2?xIn_xS₄ have been obtained in the range 0 ≦ x ≦ 2. The nonlinear changes of the cell parameters are explained by the nonlinear behavior of the inversion parameter λ according to the ionic distribution Fe²⁺_1?λIn³⁺_λ[Cr³⁺_2?xFe²⁺_λIn³⁺_x?λ]S^2?₄. Room temperature⁵⁷Fe-Mo¨ssbauer spectra exhibit two sets of absorptions for tetrahedrally and octahedrally coordinated Fe, respectively, each consisting of several overlapping doublets of similar isomer shifts but varying quadrupole splittings. The partial intensity of octahedral-site Fe is in agreement with λ. The spectra can be understood by accounting for the influence of variable octahedral-site neighbors on tetrahedral-site iron.     

镁二次电池正极材料纳米Fe3S4的电化学性能

首次将尖晶石相的纳米Fe₃S₄材料用作镁二次电池的正极材料。采用水热法一步合成了具有纳米结构的Fe₃S₄材料, 并采用XRD、SEM测试手段对产物的物相、形貌进行了表征。实验结果表明, 在160 ℃能够合成纯相的Fe₃S₄材料, 该材料具有银耳状纳米结构。电化学测试结果显示, 水热法合成的纳米Fe₃S₄材料能够在镁二次电池体系中进行有效的可逆充放电, 放电平台电压为0.9 V, 首次放电容量高达267 mAh·g^-1, 50次循环后衰减至110 mAh·g^-1。电化学交流阻抗测试结果表明镁离子能够在Fe₃S₄晶格中扩散。     

镁二次电池正极材料纳米Fe3S4的电化学性能研究

首次将尖晶石相的纳米Fe₃S₄材料用作镁二次电池的正极材料。采用水热法一步合成了具有纳米结构的Fe₃S₄材料, 并采用XRD、SEM测试手段对产物的物相、形貌进行了表征。实验结果表明, 在160 ℃能够合成纯相的Fe₃S₄材料, 该材料具有银耳状纳米结构。电化学测试结果显示, 水热法合成的纳米Fe₃S₄材料能够在镁二次电池体系中进行有效的可逆充放电, 放电平台电压为0.9 V, 首次放电容量高达267 mAh· g^-1, 50次循环后衰减至110 mAh· g^-1。电化学交流阻抗测试结果表明镁离子能够在Fe₃S₄晶格中扩散。     

The role of pyrrhotite (Fe7S8) and the sample texture in the hydrothermal transformation of pentlandite ((Fe,Ni)9S8) to violarite ((Ni,Fe)3S4)

The catalytic role of pyrrhotite (Fe₇S₈) in the reaction kinetics of the hydrothermal transformation of pentlandite ((Fe,Ni)₉S₈) to violarite ((FeNi₂S₄) was found to depend on the physical form of pyrrhotite. Pyrrhotite in fine scale intergrown with pentlandite boosts the reaction, whereas in a mechanical mixture of pyrrhotite and pentlandite, it plays the opposite role. This phenomenon was interpreted as result of dissolution of pyrrhotite under reaction conditions.     

Crystal structures of V3S4 and V5S8

Crystal structures of the ordered phases of V₃S₄ and V₅S₈ were refined with single crystal data. Both are monoclinic. Chemical compositions, space groups and lattice constants are as follows: VS_1.47, $\text{I2}\text{m}$ (No. 12), a = 5.831(1), b = 3.267(1), c = 11.317(2)Å, β = 91.78(1)° and VS_1.64, $\text{F}\text{2}\text{m}$ (No. 12), a = 11.396(11), b = 6.645(7), c = 11.293(4), Å, β = 91.45(6)°. In both structures, short metal-metal bonds were found between the layers as well as within them. In comparison with the structure of Fe₇S₈, the stability of NiAs-type structure was discussed based on the detailed metal-sulfur distances.     

The phase study of the TlVS system and the properties of TlV6S8 and TlV5S8 phases

The ternary phase diagram of the TlVS system was investigated using samples quenched from 400°C, especially in the neighborhood of TlV₆S₈ and TlV₅S₈ phases. The TlV₆S₈ phase (Tl_xV₆S_y) exists between 0.75 < x < 1.00 and 7.55 < y < 7.90, and the TlV₅S₈ phase (Tl_x′V₅S_y′) between 0.70 < x′ < 1.00 and 7.54 < y′ < 7.98. A new ternary phase with the nominal composition of TlV₂S₄ was found in addition to the three known ternary phases. The entirely deintercalated V₆S_7.8 with the framework structure was obtained by using 1 N AlCl₃ + 0.01 N FeCl₃ aqueous solution, while the lower phase limit of the TlV₅S₈ phase was Tl_0.33V₅S₈ consistent with the earlier work. The electrical resistivity and the magnetic susceptibility measurements show that these compounds are expected to be weakly magnetic itinerant-electron systems.