Ag3PO4/Ag2S/g-C3N4复合光催化剂的制备与性能

通过沉积法和离子交换法成功地制备了Ag_3PO_4/Ag_2S/g-C_3N_4复合型光催化剂。利用X射线多晶粉末衍射仪(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、X射线光电子能谱(XPS)、N_2吸附-脱附等温线、紫外-可见漫反射光谱、荧光光谱等手段对样品进行了表征。通过降解罗丹明B考察其可见光催化活性及稳定性,研究了硫化钠与磷酸银物质的量的比值(n_(Na_2S)/n_(Ag_3PO_4))、g-C_3N_4添加量对所制备复合光催化材料性能的影响,同时对光催化机理进行了探讨。结果表明,随着n_(Na2S)/n_(Ag3PO4)的增加,所得复合催化材料活性先增加后降低;当n_(Na2S)/n_(Ag_3PO_4)为1.5%、g-C_3N_4与Ag_3PO_4的质量比为3∶7时制备的催化剂ASC1.5的光催化活性最好,在可见光照射下,40 min内可将罗丹明B完全降解,且5次循环使用后仍保持较高的催化活性。和Ag_3PO_4相比,Ag_3PO_4/Ag_2S/g-C_3N_4复合型光催化材料的活性与稳定性都得到明显提高,这主要归因于复合催化剂比表面积和孔结构的增加,载流子分离效率的提高。光催化机理研究表明,空穴(h~+)、超氧阴离子自由基(·O~(2-))和羟基自由基(·OH)都是光催化过程中的主要活性物种。三者作用大小依次为:h~+·O~(2-)·OH。     

Syntheses, structures, and properties of Ag4(Mo2O5)(SeO4)2(SeO3) and Ag2(MoO3)3SeO3

Ag₄(Mo₂O₅)(SeO₄)₂(SeO₃) has been synthesized by reacting AgNO₃, MoO₃, and selenic acid under mild hydrothermal conditions. The structure of this compound consists of cis-MoO₂²⁺ molybdenyl units that are bridged to neighboring molybdenyl moieties by selenate anions and by a bridging oxo anion. These dimeric units are joined by selenite anions to yield zigzag one-dimensional chains that extended down the c-axis. Individual chains are polar with the C₂ distortion of the Mo(VI) octahedra aligning on one side of each chain. However, the overall structure is centrosymmetric because neighboring chains have opposite alignment of the C₂ distortion. Upon heating Ag₄(Mo₂O₅)(SeO₄)₂(SeO₃) looses SeO₂ in two distinct steps to yield Ag₂MoO₄. Crystallographic data: (193 K; MoKα, λ=0.71073 Å): orthorhombic, space group Pbcm, a=5.6557(3), b=15.8904(7), c=15.7938(7) Å, V=1419.41(12), Z=4, R(F)=2.72% for 121 parameters with 1829 reflections with I>2σ(I). Ag₂(MoO₃)₃SeO₃ was synthesized by reacting AgNO₃ with MoO₃, SeO₂, and HF under hydrothermal conditions. The structure of Ag₂(MoO₃)₃SeO₃ consists of three crystallographically unique Mo(VI) centers that are in 2+2+2 coordination environments with two long, two intermediate, and two short bonds. These MoO₆ units are connected to form a molybdenyl ribbon that extends along the c-axis. These ribbons are further connected together through tridentate selenite anions to form two-dimensional layers in the [bc] plane. Crystallographic data: (193 K; MoKα, λ=0.71073 Å): monoclinic, space group P2₁/n, a=7.7034(5), b=11.1485(8), c=12.7500(9) Å, β=105.018(1) V=1002.7(2), Z=4, R(F)=3.45% for 164 parameters with 2454 reflections with I>2σ(I). Ag₂(MoO₃)₃SeO₃ decomposes to Ag₂Mo₃O₁₀ on heating above 550 °C.     

A study of the faradaic impedance of lead in 5 M H2SO4 in the anodic region

The faradaic impedance of Pb/PbSO₄·H₂SO₄ (5 M) and Pb/PbO₂ · PbSO₄, H₂SO₄ (5 M) as well as a system which probably corresponds to Pb/PbO · PbSO₄, H₂SO₄ (5 M) have been investigated using a Schering bridge. The effect of incorporation of 2% and 6% of antimony in the lead was also studied. The results show that in addition to charge transfer and Warburg impedances, crystallisation, nucleation and adsorption impedances are also present.     

Infrared spectra of Ag2BrNO3 and Ag2ClNO3

The infrared spectra of Ag₂BrNO₃ and Ag₂ClNO₃ are reported. Vibration assignments are proposed on the basis of the group theoretical analysis and D_2h symmetry. Factor group, site and TO-LO splittings are observed. The internal and external mode frequencies are correlated with those of AgNO₃ and KNO₃(II).     

The phase diagram of the system La2(SO4)3Ag2SO4

The phase diagram of the system La₂(SO₄)₃Ag₂SO₄ was studied by DTA, XRD, SEM, and optical methods. One double salt is formed at 67 mole% La₂(SO₄)₃ and this melts incongruently at 876±6°C. A eutectic is formed at 8 mole% La₂(SO₄)₃ and at a temperature of 618±3°C. Suppression of decomposition was effected by the sealed tube method, but some reference is made to experiments conducted with a flowing atmosphere of SO₃, SO₂ and O₂.     

The electrical conductivity of single crystals of Ag2HgI4

Electrical conductivity measurements are reported for single crystal samples of Ag₂HgI₄ in the temperature range between ?17°C and 72°C. The results are interpreted in terms of two distinct regions of linear log conductivity versus reciprocal temperature behavior for β-Ag₂HgI₄, a phase transition region, and an α-Ag₂HgI₄ region. The data reaffirm the anomalously high pre-exponential and activation energy terms in the conductivity equation for α-Ag₂HgI₄ as compared with other AgI-type conductors. Thermo-emf measurements on polycrystalline Ag₂HgI₄ samples are also reported.     

Phase formation in the Ag2MoO4-CuO-MoO3 system and the crystal structure of the new double molybdate Ag2Cu2(MoO4)3

Subsolidus phase relations in the Ag₂MoO₄-CuO-MoO₃ oxide-salt ternary system were determined. T-x diagram was plotted for the Ag₂MoO₄-CuMoO₄ quasi-binary join. Double molybdate Ag₂Cu₂(MoO₄)₃ was found to exist on this join. This compound is a superstructure derived from orthorhombic Li₃Fe(MoO₄)₃. Its structure was solved in terms of a subcell (a = 5.0749(3), b = 11.300(2), c = 18.127(3) ?, space group Pnma, Z = 4, R = 0.0678). In the true unit cell, the parameter a is tripled; suggested space group is P2₁2₁2₁. A characteristic feature of the Ag₂Cu₂(MoO₄)₃ structure is infinite columns (extended along axis a) of face-sharing oxygen octahedra, in which disordered silver atoms are located (Ag(21), Ag(22), and Ag(23)) with various degrees of irregularity of their octahedral coordination and a strong anisotropy of thermal vibrations. Distorted CuO₆ octahedra form zigzag ribbons extended in the same direction. MoO₄ tetrahedra, which are arranged according to the pseudo-hexagonal law, link the aforementioned major structural elements into a three-dimensional framework. Trigonal-prismatic voids of the framework are occupied by silver atoms Ag (1). Presumably, the disorder of the silver ions in octahedral columns can be responsible for the increased ion conductivity of silver copper molybdate. A partial order of the same ions is the most likely reason for the appearance of superstructure with the tripled unit cell volume. Original Russian Text ? G.D. Tsyrenova, S.F. Solodovnikov, E.T. Pavlova, E.G. Khaikina, Z.A. Solodovnikova, 2009, published in Zhurnal Neorganicheskoi Khimii, 2009, Vol. 54, No. 5, pp. 802–809.     

Ag1/8Pr5/8MoO4: An incommensurately modulated scheelite-type structure

The crystal structure of a complex molybdenum oxide Ag_1/8Pr_5/8MoO₄ is reported. The Ag_1/8Pr_5/8MoO₄ sub-structure can be described on the base of the scheelite (CaWO₄) structure. Transmission electron microscopy reveals that the real structure is better described in a (3+1)D formalism. According to electron diffraction study the new scheelite-type complex oxide Ag_1/8Pr_5/8MoO₄ crystallizes in the B2/b(αβ0)00 (3+1)D superspace group with unit cell parameters , , and γ≈135° (Z=4) and modulation vector q=0.56a^*+0.59b^*. The structure of Ag_1/8Pr_5/8MoO₄ is refined from X-ray powder data in the scheelite setting I2/b(αβ0) with , , q=1.14690(14)a^*+0.58921(12)b^* with fixed γ=90° angle (R_p=0.033, R=0.033, R_m=0.029, R₁=0.047, S=1.36). Displacement modulations apply for all atoms. The occupancy modulation shows that one-fourth of the Ag/Pr atoms are absent. The structure can be considered as a crystallographic shear structure with incommensurate ordering of vacancies and displacement modulations for all atoms. The arrangement of Ag/Pr atoms and vacancies is at the origin of the incommensurate modulation in the cation-deficient Ag_1/8Pr_5/8MoO₄ phase.     

Preparation and visible-light photocatalytic activity of Ag3VO4 powders

Monoclinic structure Ag₃VO₄ was prepared by precipitation method and evaluated for the decolorization of azodye acid red B (ARB) under visible light irradiation (λ>420 nm). The Ag₃VO₄ prepared in the excess vanadium or silver exhibited higher visible-light-driven activity than the sample prepared in a stoichiometric ratio. X-ray diffraction and UV-vis diffuse reflectance measurements indicated that the excess vanadium or silver in the preparation increased the crystallinity and absorbance in visible light region, resulting in an increase in the photocatalytic efficiency. Furthermore, the activity of the Ag₃VO₄ was increased by 3.8 times when a NiO was loaded. It was due to the formation of a short-circuited microphotoelectrochemical cell on the surface of NiO/Ag₃VO₄, enhancing the separation of photogenerated electron-hole pairs, which was proved by ESR studies.     

S-scheme Porous g-C3N4/Ag2MoO4 Heterojunction Composite for CO2 Photoreduction

Utilizing solar energy to achieve artificial photosynthesis of chemical fuel is prevalent in tackling excessive CO₂ emission and fossil fuel depletion. Grievous charge recombination and weak redox capability aggravate the CO₂ photoreduction performance. Engineering tailored morphology and constructing matched heterostructure are two significant schemes to ameliorate the CO₂ photoconversion efficiency of g-C₃N₄-based composite. Herein, a nove...     

可见光响应的Co3(PO4)2/Ag3PO4纳米复合光催化剂的制备及表征

采用简单的化学偏聚法合成出Ag₃PO₄纳米颗粒、磷酸钴（Co₃（PO₄）₂,CoP）纳米片以及它们两者的纳米复合结构（CoP/Ag₃PO₄）,同时还比较了它们的可见光催化活性. 采用场发射扫描电镜（FESEM）、X 射线衍射（XRD）、紫外-可见（UV-Vis）吸收光谱以及光致发光谱等手段对其形貌、结构、光学以及可见光催化性能等进行表征. 结果表明,CoP/Ag₃PO₄复合纳米结构的可见光降解甲基橙（MO）的速率和循环稳定性均明显优于其它两种物质. 这表明CoP应该起着共催化剂的作用,它能够抑制光生电子与空穴之间的复合,并且提供大量高活性的光生空穴. 此外,我们还发现CoP/Ag₃PO₄降解另一种阳离子型染料——罗丹明B（RhB）的能力则远不如纯Ag₃PO₄,这可能是与光催化剂的表面性质发生改变有关,造成更低的RhB吸附能力. 本文提供了一种廉价制备高效可见光催化剂的新方法.     

The stereospecific synthesis of leukotriene A4 (LTA4), 5-epi-LTA4, 6-epi-LTA4 and 5-epi,6-epi-LTA4

The stereospecific syntheses of the four isomers of 6-formyl-5,6-epoxy hexanoic acid methyl ester $\text{8}$, $\text{15}$, $\text{23}$ and $\text{30}$ from Z-deoxy-D-ribose have allowed the preparation of methyl esters of LTA₄, $\text{1}$, and its three unnatural isomers.     

室温下制备Cu7S4和Ag2S的球形空心纳米粒子

以Cu₂O和Ag₂O纳米粒子为前驱体,利用Kirkendall效应,在室温条件下制备出Cu₇S₄和Ag₂S的球形空心纳米粒子。用X-射线衍射(XRD)、透射电镜(TEM)、扫描电镜(SEM)等测试手段对产物进行了表征。结果表明,粒子的空心化程度取决于反应物的物质的量之比;空心粒子的形貌与前驱体粒子的形貌很相似。研究了这种反应的机理,并对这两种氧化物发生这类反应的难易程度作了理论探讨。     

Ag2S/Ag3PO4/Ni复合薄膜的制备及其光催化性能

采用电化学方法制备Ag₂S/Ag₃PO₄/Ni复合薄膜,以扫描电子显微镜（SEM）、X射线衍射（XRD）、紫外-可见漫反射光谱（UV-Vis DRS）对薄膜的表面形貌、晶相结构、光谱特性及能带结构进行了表征,以罗丹明B为模拟污染物对薄膜的光催化活性和稳定性进行了测定,采用向溶液中加入活性物种捕获剂的方法对薄膜的光催化机理进行了探索。结果表明：最佳工艺制备的Ag₂S/Ag₃PO₄/Ni是由均匀的球形纳米颗粒构成的薄膜,其光催化活性明显优于纯Ag₃PO₄/Ni薄膜和纯Ag₂S/Ni薄膜,且在保持薄膜光催化活性基本不变的前提下可循环使用6次。提出了可见光下Ag₂S/Ag₃PO₄/Ni复合薄膜光催化降解罗丹明B的反应机理。     

Synthesis and properties of pyrazine-pillared Ag3Mo2O4F7 and AgReO4 layered phases

The new pyrazine-pillared solids, AgReO₄(C₄H₄N₂) (I) and Ag₃Mo₂O₄F₇(C₄H₄N₂)₃ (C₄H₄N₂=pyrazine, pyz) (II), were synthesized by hydrothermal methods at 150 °C and characterized using single crystal X-ray diffraction (I—P2₁/c, No. 14, Z=4, a=7.2238(6) Å, b=7.4940(7) Å, c=15.451(1) Å, β=92.296(4)°; II—P2/n, No. 13, Z=2, a=7.6465(9) Å, b=7.1888(5) Å, c=19.142(2) Å, β=100.284(8)°), thermogravimetric analysis, UV-Vis diffuse reflectance, and photoluminescence measurements. Individual Ag(pyz) chains in I are bonded to three perrhenate ReO₄^- tetrahedra per layer, while each layer in II contains sets of three edge-shared Ag(pyz) chains (π-π stacked) that are edge-shared to four Mo₂O₄F₇^3- dimers. A relatively small interlayer spacing results from the short length of the pyrazine pillars, and which can be removed at just slightly above their preparation temperature, at >150-175 °C, to produce crystalline AgReO₄ for I, and Ag₂MoO₄ and an unidentified product for II. Both pillared solids exhibit strong orange-yellow photoemission, at 575 nm for I and 560 nm for II, arising from electronic excitations across (charge transfer) band gaps of 2.91 and 2.76 eV in each, respectively. Their structures and properties are analyzed with respect to parent ‘organic free’ silver perrhenate and molybdate solids which manifest similar photoemissions, as well as to the calculated electronic band structures.     

Ag2S/Ag3PO4/Ni复合薄膜的制备及其光催化性能

采用电化学方法制备Ag_2S/Ag_3PO_4/Ni复合薄膜,以扫描电子显微镜(SEM)、X射线衍射(XRD)、紫外-可见漫反射光谱(UVVis DRS)对薄膜的表面形貌、晶相结构、光谱特性及能带结构进行了表征,以罗丹明B为模拟污染物对薄膜的光催化活性和稳定性进行了测定,采用向溶液中加入活性物种捕获剂的方法对薄膜的光催化机理进行了探索。结果表明:最佳工艺制备的Ag_2S/Ag_3PO_4/Ni是由均匀的球形纳米颗粒构成的薄膜,其光催化活性明显优于纯Ag_3PO_4/Ni薄膜和纯Ag_2S/Ni薄膜,且在保持薄膜光催化活性基本不变的前提下可循环使用6次。提出了可见光下Ag_2S/Ag_3PO_4/Ni复合薄膜光催化降解罗丹明B的反应机理。     

Ag3PO4的可见光光催化性能及机理分析

采用沉淀置换法制备了可见光光催化剂Ag3PO4,利用XRD、UV-Vis及XPS等对其进行了结构特性分析,以水中微污染有机物的降解评价了Ag3PO4的光催化活性,并通过活性物种及能带结构的分析对催化剂的光催化机理进行了推测。结果表明,Ag3PO4的带隙能约为1.9 eV、催化剂表面存在的Ag+可捕获光生e-、催化剂的价带电位较低,这有利于Ag3PO4在可见光照射下产生的e--h+的分离及活性物种.OH的形成。经60 min可见光光催化反应,15 mg.L-1的甲基橙和腐殖酸的降解率分别达97%和82%,比同等条件下TiO2-P25的降解率还高40%和25%,光催化剂Ag3PO4的用量为0.6 g.L-1。     

沉积Pt对Ag2CO3纳米晶的物理化学性质和光催化性能影响

采用NaBH_4还原法合成了系列Pt沉积的Ag_2CO_3复合光催化剂。通过在可见光照射下降解甲基橙研究沉积不同含量的Pt对Ag_2CO_3光催化性能的影响。应用X射线粉末衍射(XRD)、扫描电子显微镜(SEM)、透射电镜(TEM)、光电子能谱(XPS)、傅立叶变换红外光谱(FT-IR)、光致发光光谱(PL)、紫外可见漫反射吸收光谱(DRS)、光电流(PC)和N_2物理吸附等研究了沉积Pt纳米颗粒对Ag_2CO_3纳米晶的物理化学性质的影响。结果表明,沉积质量分数为0.1%～0.5%的Pt,可使Ag_2CO_3的活性提升3倍以上,同时光催化剂的稳定性得到极大改善。Pt/Ag_2CO_3光催化性能大幅提升的主要原因是,沉积少量的Pt可以增强Ag_2CO_3对可见光的吸收,同时增大Ag_2CO_3的比表面积和表面羟基的数量;另外,沉积在Ag_2CO_3表面的Pt粒子可以承担电子俘获中心的作用,使Ag_2CO_3中光激发产生的电子(e~-)有效地转移到Pt上,加速光生电子-空穴对的分离速率,产生更多的光催化活性自由基,在提升光催化活性的同时,减少Ag_2CO_3中的Ag~+被光生电子(e~-)还原的几率,增强Ag_2CO_3的抗光腐蚀能力。     

Trapping phosphate anions inside the [Ag4I] framework: Structure, bonding, and properties of Ag4I(PO4)

Orange-red Ag₄I(PO₄) crystallizes in the monoclinic system, space group P2₁/m (No. 11), with the unit cell dimensions a=9.0874(6) Å, b=6.8809(5) Å, c=11.1260(7) Å, β=109.450(1)°, and Z=4. The crystal structure is fully ordered; it comprises the silver-iodine three-dimensional positively charged framework hosting the tetrahedral PO₄³⁻ guest anions. The framework features high coordination numbers for iodine and manifold Ag-Ag bonds ranging from 3.01 to 3.46 Å. The Ag-Ag interaction is bonding, it involves silver 4d and 5s orbitals lying, together with the orbitals of iodine, just below the Fermi level. Though the orbitals of silver and iodine define the conducting properties of the title compound, the interaction between the framework and the guest anions is also important and is responsive to the number of the silver atoms surrounding the PO₄³⁻ tetrahedra. Ag₄I(PO₄) melts incongruently at 591 K and produces a mixture of the silver phosphate and an amorphous phase upon cooling. Pure Ag₄I(PO₄) is a poor conductor with a room temperature conductivity of 3×10⁻⁶ S m⁻¹. The discrepancies between the properties observed here and those reported previously in the literature are discussed.