SbxZn1-xO1+x/2及其壳聚糖复配物的制备和抗菌性能

采用溶胶-凝胶法制备了SbxZn1-xO1+x/2及其壳聚糖的复配物,通过X-射线衍射仪(XRD)、傅里叶变换红外光谱仪(FTIR)、扫描电子显微镜(SEM)和透射电子显微镜(TEM)等表征了样品的物相结构、组成和微观形貌。以大肠杆菌、白色念珠菌和金黄色葡萄球菌为测试菌种,研究了样品的抗菌性能。结果表明,SbxZn1-xO1+x/2的抗菌活性优于纯ZnO,其中x=0.05的样品活性最好;复配物的抗菌活性明显优于单一组分,当Sb0.05Zn0.95O1.025和壳聚糖质量比mSZ/mCS=2时,样品抗菌性能最佳。     

Nickel Oxidation State and Magnetic Properties of Hole-Doped and Reduced Nd2−xSrxNiOyCompounds

The NiK-edge XANES of reduced Nd_2−xSr_xNiO₄samples shows an increase of Ni³⁺content with Sr³⁺concentration. The appearance of mixed valence Ni²⁺/Ni³⁺produces a change in the magnetic properties of the system. The Nd³⁺sublattice orders antiferromagnetically atT_N∼13–20 K forx=0.4, 0.5, and 0.6, due to the interactions of Ni–Nd sublattices. Forx=0.8 this order begins to disappear because of the effect of the low spin state Ni³⁺created at the NiO₄planes. Additionally, the reduced family Nd_2−xSr_xNiO_y(y<4) shows the disappearance of Ni³⁺, the decrease of Ni²⁺with respect to the nonreduced form, and the appearance of Ni⁺. All the compounds of the reduced family show AF order at low temperature.     

Boron complexes of S-trityl- -cysteine and S-tritylglutathione

S-Trityl- -cysteine and S-tritylglutathione have been converted to 1,3,2-oxazaborolidine-5-ones by reaction with B-methoxydialkylborane derivatives. The synthesis of dicyclohexyl[S-trityl-(R)-cysteinato-O,N]boron (2), diisopinocampheyl[S-trityl-(R)-cysteinato-O,N]boron (3) and 9-borabicyclo[3.3.1]non-9-yl[S-tritylglutathionato-O,N]boron (5), dicyclohexyl[S-tritylglutathionato-O,N]boron (6) and diisopinocampheyl[S-tritylglutathionato-O,N]boron (7) from S-trityl- -cysteine and S-tritylglutathione, respectively, with potential application in boron neutron capture therapy is reported. The structure of 9-borabicyclo[3.3.1]non-9-yl[S-trityl-(R)-cysteinato-O,N]boron 1 has been determined by X-ray diffraction.     

镉汞四元硒化物K8Cd2.79Hg9.21Se16和Rb4Hg3.04Cd2.96Se8的溶剂热合成及表征

利用溶剂热法合成了2种含镉汞的二维(2D)四元硒化物K8Cd2.79Hg9.21Se16(1)和Rb4Hg3.04Cd2.96Se8 (2)。单晶X射线衍射分析表明,化合物1为正交晶系,空间群为Pbcn,a=1.082 71(17) nm,b=0.678 73(10) nm,c=1.415 0(2) nm,Z=1;化合物2为正交晶系,空间群为Ibam,a=0.640 72(10) nm,b=1.160 25(16) nm,c=1.452 0(2) nm,Z=2。化合物1中含有八元环Cd2Hg2Se4和六元环CdHg2Se3阴离子层(Cd2.79Hg9.21Se16)n8n-;化合物2中含有八元环Cd2(Cd/Hg)2Se4及四元环CdHgSe2和(Cd/Hg)2Se2阴离子层(Hg3.04Cd2.96Se8)n4n-。对这2种化合物进行了扫描电镜和能谱分析、粉末X射线衍射、差示扫描量热分析、固体-可见漫反射光谱和荧光性质等表征。     

Synthesis and crystal and molecular structure of CdPhen( iso -C4H9OCS2)2 and CdPhen( n -C4H9OCS2)2 mixed-ligand complexes

Mixed-ligand complexes CdPhen(i-BuOCS₂)₂ (I) and CdPhen(n-BuOCS₂)₂ (II) have been synthesized. Their structures were solved using X-ray diffraction data (X8 APEX diffractometer, MoK _α radiation, 1641 and 2497 F _hkl , R = 0.0359 and 0.0389). Crystals I are orthorhombic with unit cell parameters a = 6.5883(3) Å, b = 19.7123(10) Å, c = 20.1936(11) Å, V = 2622.6(2) ų; Z = 4, space group Pbcn; crystals II are monoclinic, a = 6.5845(2) Å, b = 19.1522(6) Å, c = 20.7091(7) Å, β = 97.106(1), V = 2591.5(1) ų, Z = 4, space group C2/c. The structures consist of discrete mononuclear molecules in which the coordination polyhedron of the Cd atom is a distorted N₂S₄ octahedron. Molecular packing and interactions in the structures are discussed. Original Russian Text Copyright ? 2007 by R. F. Klevtsova, T. G. Leonova, L. A. Glinskaya, and S. V. Larionov __________ Translated from Zhurnal Strukturnoi Khimii, Vol. 48, No. 2, pp. 274–281, March–April, 2007.     

Crystal and molecular structures of Ni[(iso-C4H9)2PS2]2 and Pd[(iso-C4H9)2PS2]2 chelates

Crystal structures of chelate compounds Ni[(iso-C₄H₉)₂PS₂]₂ (I) and Pd[(iso-C₄H₉)₂PS₂]₂ (II) have been determined by X-ray diffraction: diffractometer X8-APEX, MoK _α∔ -radiation, 1048 F _hkl , R = 0.0544 for I and CAD-4 diffractometer, MoK _α∔ -radiation, 1283 F _hkl , R = 0.0347 for II. The crystals are rhombic: a = 12.921(5) Å, b = 17.094(5) Å, c = 22.971(5) Å; V = 5074(3) ų, Z = 8, calc = 1.250 g/cm³, space group Pbca for I and a = 13.312(3) Å, b = 16.130(7) Å, c = 23.171(5) Å; V = 4975(3) ų, Z = 8, ρ_calc = 1. 208 g/cm³, space group Pbca for II. The structures of I and II are formed by discrete mononuclear molecules. Coordination cores MS₄ (M = Ni, Pd) approach planar square configurations. Original Russian Text Copyright ? 2005 by L. A. Glinskaya, T. G. Leonova, T. E. Kokina, R. F. Klevtsova, and S. V. Larionov __________ Translated from Zhurnal Strukturnoi Khimii, Vol. 46, No. 4, pp. 715–720, July–August, 2005.     

Synthesis and characterization of the La1−xSrxFeO3−δ system and the fluorinated phases La1−xSrxFeO3−xFx

The oxyfluorides La_1−xSr_xFeO_3−xF_x have been prepared by fluorination of the precursor oxides La_1−xSr_xFeO_3−δ via a low temperature route using poly(vinylidene fluoride) (PVDF). The structures of the oxides and oxyfluorides were investigated in detail by the Rietveld analysis of powder diffraction data. The oxyfluorides crystallize in the space group Pnma for 0<x≤0.9 (SrFeO₂F itself is cubic, space group Pm-3m) and show a sort of two-step structural distortion for decreasing x. Furthermore, a structural comparison of the oxyfluorides with the oxides is given, revealing an increase of the volume per La_1−xSr_xFeX₃ unit during fluorination, of which the magnitude highly depends on the value of x.     

Electronic structure of magnetic semiconductors Cd1 ? xMnxGeAs2 and Cu1 ? xMnxGaTe2

The band structures of pure semiconductors CdGeAs₂ and CuGaTe₂, as well as magnetic semiconductors Cd_{1 − x} Mn _x GeAs₂ and Cu_{1 − x} Mn _x GaTe₂ (x = 0.0625), have been calculated by the density functional theory method. In both compounds, the Mn3d orbitals form a narrow band near the Fermi level. In the case of Cd_{1 − x} Mn _x GeAs₂, the Mn3d orbitals are slightly involved in chemical bonding. In the case of Cu_{1 − x} Mn _x GaTe₂, the same orbitals are considerably involved in chemical bonding. The relationship of these results with the properties of the compounds and ferromagnetism models is discussed. Original Russian Text ? S.V. Murashov, V.G. Yarzhemsky, V.I. Nefedov, E.N. Murav’ev, 2007, published in Zhurnal Neorganicheskoi Khimii, 2007, Vol. 52, No. 8, pp. 1327–1331.     

Structural and magnetic properties of the solid solution () YMn1−x(Cu3/4Mo1/4)xO3

Recently, the ferroelectromagnet YMnO₃ has been the focus of interest because it exhibits both antiferromagnetism (Néel temperature 80 K) and ferroelectricity (Curie temperature 914 K). There have been no reports of complete YMn_1−xM_xO₃ solid solutions in which substitution of the foreign M cation preserves the hexagonal P6₃cm structure. In contrast there exist several homeotypic phases with the general formula, Ln_1+nCu_nMO_3+3n (n=1 (M=Ti), 2 (M=V) and 3 (M=Mo); Ln: lanthanide). Several YMn_1−x(Cu_3/4Mo_1/4)_xO₃ compounds have been synthesized. The solid solution, from YMnO₃ (x=0) to YCu_3/4Mo_1/4O₃ (x=1) has been characterized by X-ray diffraction and transmission electron microscopy study. For 0<x<0.9, the compounds are found to crystallize in the non-centrosymmetric structure, space group P6₃cm, of YMnO₃. The Mn-free end member, x=1, crystallizes in a complex multiple cell, the superstructure being associated to Cu³⁺/Mo⁶⁺ cationic ordering. Dilution of the Mn³⁺ magnetic array by the paramagnetic (Cu²⁺) and diamagnetic (Mo⁶⁺) cations is found to decrease the antiferromagnetic ordering temperature and it becomes undetectable for x0.5 compositions.     

Synthesis, Crystal Structure, and Magnetic Properties of Quasi-One-Dimensional Oxides Ca3CuMnO6 and Ca3Co1+xMn1−xO6

Synthesis conditions, crystal structures, and magnetic properties of quasi-one-dimensional complex oxides Ca₃CuMnO₆ (space group P-1, z=4, triclinic cell) and Ca₃Co_1+xMn_1−xO₆ with x=0, 0.25, 1.0 (structural type K₄CdCl₆, space group R-3c, z=6) are presented. The crystal structures of Ca₃CoMnO₆ and Ca₃CuMnO₆ were refined using neutron and combined X-ray and neutron diffraction analysis, respectively. The interatomic distances in oxygen polyhedra were found. In contrast to ferromagnetic Ca₃Co₂O₆ (T_c=24 K), manganese-containing phases Ca₃Co_1+xMn_1−xO₆ are characterized by antiferromagnetic interactions with Neel temperatures 18 K (x=0.25) and 13 K (x=0). For Ca₃CuMnO₆T_N was established to be 6 K.     

Carbometallic derivatives of hydroborons C2h and D5d: A list of substitution isomers

The problem of determining the number and type of X-substituted (where X represents certain substituents) carbometallic derivatives of hydroborons [Co(C₂B₉H₁₁)₂]⁻ C _2h and [Co(C₅B₆H₁₁)₂]⁻ D _5d (from apexes) was solved on the basis of G. Pólya’s theorem by means of combinatory analysis. The formulae of symmetry Z and generating functions of the number of achiral substitution isomers were determined. The family distributions of isomers (depending on the type and number of substituents) and the sites of possible substitution depending on the number m were determined. Mono and di-X-substituted isomers of [Co(C₅B₆H₁₁)₂]⁻ C _2h , as well as mono and di-X-substituted isomers of [Co(C₅B₆H₁₁)₂]⁻ D _5d , were identified. The procedure for plotting an additive model of calculating the properties of isomers of apical substitution of [Co(C₅B₆H₁₁)₂]⁻ D _5d was described on the basis of splitting of polygonal numbers (K ₃, K _TE, K ₅, and so on) of Pascal triangle, upon use of which there is no randomization in the choice of parameters of calculation model. The additive schemes containing 7 and 25 parameters for the calculation of properties of X-substituted carbometallic derivative of hydroboron [Co(C₅B₆H₁₁)₂]⁻ D _5d to various approximations were obtained.     

Models of p-T-x1-x2 diagrams for ternary systems with vapor-liquid equilibria and continuous solutions in subcritical and supercritical regions

We consider model p-T-x ₁-x ₂ diagrams for ternary systems with continuous solutions in subcritical and supercritical vapor-liquid regions. Phase equilibria are analyzed with the parameters of state of the system varying as dependent on components’ volatilities. The methodology is described, and sample constructions of isobaric-isothermal diagrams and polythermal sections are made proceeding from p-T and T-x ₁-x ₂ projections of the four-dimensional diagram.     

Critical covalence and superconductivity in Ln2−xCexCuO4

The variations of superconductive properties with x of the n-type Ln_2−xCe_xCuO₄ (Ln = La_0.5Nd_0.5, Nd, or Gd) systems have been investigated. As the size of Ln³⁺ decreases, (i) the solubility limit x of Ce decreases, (ii) the value of x at which a transition from antiferromagnetic semiconductor to superconductor occurs increases, and (iii) the width Δx of the superconductive region decreases. The decreasing solubility of Ce with decreasing size of Ln³⁺ is due to decreasing tensile strain in the CuO₂ sheets. The progressive shift of the semiconductor to superconductor transition to higher x values with decreasing size of Ln³⁺ is explained on the basis of increasing electrostatic Madelung energy E_M caused by decreasing Cu---O bond length. A larger E_M means a larger charge transfer gap Δ and a smaller covalent-mixing parameter λ and bandwidth W; so a decreasing size of Ln³⁺ necessitates a higher level of Ce-doping in order to achieve a critical covalence essential for superconductivity to occur.     

Approximate formulae for calculation of the integral òT0Tmexp(-E/RT)dT

Summary In this paper two approximate formulae have been developed for calculation of the integral ò^T₀T^mexp(-E/RT)dT by using integration-by-parts approaches. They are in the following forms: I(m,T) = (RT^m+2)/(E+(m+2)RT)exp(-E/RT) I(m,T) = (RT^m+2)/(E+(m+2)(0.00099441E+0.93695599RT)exp(-E/RT) The validity of the two formulae has been confirmed and their accuracies have been tested with data from numerical calculating. In contrast to existing other integral methods, both the present approaches are simply used, accurate, and can be used for arbitrary values of m.     

用于NO_x低温下吸附还原的CoO_x/CeO_2二元氧化物的制备

研究了以多孔二氧化硅微球和活性炭为载体制备NOx吸附/还原催化剂的方法,摸索了最佳Ce/Co物质的量的比例。采用低温氮吸附方法测定了样品的BET比表面和孔容,利用XRD方法表征了样品中所掺杂的金属元素的晶型。研究发现:当nCe/nCo=75/25时,材料获得最佳NOx吸附能力,当以多孔二氧化硅微球作载体时,材料对于NOx的吸附主要来自CoOx和CeO2的二元氧化物;当以活性炭作为载体时,活性炭参与了NOx的吸附,因此其吸附容量大大提高。对NOx的吸附机理进行了探讨,并研究了样品的NH3还原性质。     

Triethylantimony(V) complexes with bidentate O,N-, O,O- and tridentate O,N,O′-coordinating o-iminoquinonato/o-quinonato ligands: Synthesis, structure and some properties

The novel triethylantimony(v) o-amidophenolato (AP-R)SbEt₃ (R = i-Pr, 1; R = Me, 2) and catecholato (3,6-DBCat)SbEt₃ (3) complexes have been synthesized and characterized by IR, NMR spectroscopy (AP-R is 4,6-di-tert-butyl-N-(2,6-dialkylphenyl)-o-amidophenolate, alkyl = isopropyl (1) or methyl (2); 3,6-DBCat is 3,6-di-tert-butyl-catecholate). Complexes 1–3 have been obtained by the oxidative addition of corresponding o-iminobenzoquinones or o-benzoquinones to Et₃Sb. The addition of 4,6-di-tert-butyl-N-(3,5-di-tert-butyl-2-hydroxyphenyl)-o-iminobenzoquinone to Et₃Sb at low temperature gives hexacoordinate [(AP-AP)H]SbEt₃ (4) which decomposes slowly in vacuum with the liberation of ethane yielding pentacoordinate complex [(AP-AP)]SbEt₂ (5). [(AP-AP)H]²⁻ is O,N,O′-tridentate amino-bis-(3,5-di-tert-butyl-phenolate-2-yl) dianion and [(AP-AP)]³⁻ is amido-bis-(3,5-di-tert-butyl-phenolate-2-yl) trianion. The decomposition of 4–5 accelerates in the presence of air. o-Amidophenolates 1 and 2 bind molecular oxygen to give spiroendoperoxides Et₃Sb[L-iPr]O₂ (6) or Et₃Sb[L-Me]O₂ (7) containing trioxastibolane rings. This reaction proceeds slowly and reaches the equilibrium at 15–20% conversion five times more than for (AP-R)SbPh₃ analogues. Molecular structures of 1 and 5 were determined by X-ray analysis.     

不同形貌InxGa1-xN纳米材料的制备及发光性能研究

采用常压化学气相沉积法(APCVD),分别以金属镓(Ga),铟(In)和氨气(NH3)为镓源,铟源和氮源,在Si衬底上利用催化剂Au成功合成了不同形貌的InxGa1-xN纳米材料。利用X射线衍射仪(XRD)、扫描电子显微镜(SEM),X射线光电子能谱(XPS)和光致发光谱(PL)对比研究了InxGa1-xN(x=0,0.25)纳米材料在形貌,化学成分,晶体结构以及发光特性的变化。分析结果表明:当没有催化剂时,所生成的InxGa1-xN样品形貌由片状结构自组装成花状结构,而在催化剂Au的作用下,生成的InxGa1-xN纳米晶的形貌变为以纳米线为轴在其上生长的片状的"塔"状结构;虽然在催化剂Au的作用下生成的InxGa1-xN(x=0.25)形貌发生了很大变化,但晶体结构未发生改变,均为六方纤锌矿结构;PL分析结果显示InxGa1-xN纳米结构的发光性能随着In含量的增加,发光谱的强度增加且同时出现了蓝光区,在催化剂Au的作用下生成的InxGa1-xN的发光强度最强。最后对不同形貌InxGa1-xN其生长机理做简单分析。     

Isotachophoretic determination of mobility and pKa by means of computer simulation : V. Evaluation of mo and pKa of twenty-eight dipeptides and assessment of separability

Isotachophoretic qualitative indices, R_E, for twenty-eight dipeptides were measured in the range pH 7.4–9.6. The absolute mobility, m_o, and pK_a values were evaluated by the use of the least-squares method, utilizing a simulation of the isotachophoretic steady state. The m_o values were newly evaluated and the pK_a values were in good agreement with literature values. By comparison of the evaluated m_o and pK_a values of the dipeptides with those of the constituent amino acids, simple relationships were found which may be used to estimate the m_o and pK_a values of other dipeptides. The separability of the dipeptides was also evaluated by considering the differences between their simulated effective mobilities. It is concluded that isotachophoresis is very convenient for the separation of dipeptides and their constituent amino acids.     

Preparation and Structure of Cerium Titanates Ce2TiO5, Ce2TiO7, and Ce4Ti9O24

Compounds Ce₂TiO₅, Ce₂Ti₂O₇, and Ce₄Ti₉O₂₄ were prepared by heating appropriate mixtures of solids containing Ce⁴⁺ and Ti³⁺ or Ti which were placed in a platinum-silica-ampoule combination at T = 1250°C (3d) under vacuum. The new compounds were characterized by powder patterns. We obtained Ce₂TiO₅ which is isotypic to La₂TiO₅ and crystallizes in the Y₂TiO₅-type (space group Pnma) with a = 10.877(6) Å, b = 3.893(1) Å, c = 11.389(8) Å, Z = 4. Ce₂Ti₂O₇ is isotypic to La₂Ti₂O₇ and crystallizes in the monoclinic Ca₂Nb₂O₇ type (space group P 2₁) with a = 7.776(6) Å, b = 5.515(4) Å, c = 12.999(6) Å, β = 98.36(5), Z = 4. The compound Ce₄Ti₉O₂₄ crystallizes orthorhombic with a = 14.082(4) Å, b = 35.419(8) Å, c = 14.516(4) Å, Z = 16. The new cerium titanate Ce₄Ti₉O₂₄ is isotypic to Nd₄Ti₉O₂₄ (space group Fddd (No. 70)) which represents a novel type of structure.     

The structure Tl3SbS3, Tl3SbSe3, Tl3SbS3−xSex, and Tl3SbyAs1−ySe3

The space group symmetry and crystal structure of Tl₃SbS_3−xSe_x compounds in the composition range 0 < x < 3 have been determined by a combination of powder X-ray diffraction, electron diffraction, and high-resolution electron microscopy. The incongruently melting compound Tl₃SbSe₃ has been shown to crystallize in cubic space group P2₁3 with a = 9.435Å in a structure related to that of Langbeinite. The convergent beam electron diffraction pattern of Tl₃SbS₃ is in accord with the space group R3m determined by X-ray diffraction. The cubic Langbeinite-type structure is found for Tl₃SbS_3−xSe_x for 0.5 < x < 3 and for Tl₃Sb_yAs_1−ySe₃ for 0.077 < y < 1.0. A five-component compound Tl₃Sb_0.5As_0.5Se_1.5S_1.5 was also found to be cubic.