平面四配位和五配位的B6S5团簇

采用B3LYP/def2-TZVP优化和在耦合簇方法(CCSD)单点水平下, 将$B_{6}S^{n}_{5}$ (n=0, +1, +2)作为基础结构研究证实了S原子对于形成B平面多配位结构具有良好的作用. 研究发现, $B_{6}S^{n}_{5}$ (n=0, +1, +2) 3种价态下最稳定和次稳定结构均为纯平面结构, 仅在不同电子数下两者的能量次序发生改变. 中性的B₆S₅因满足18电子规则其最稳定结构具有D_5h对称性, 且中心B为平面五配位. 在$B_{6}S^{+}_{5}$和$B_{6}S^{2+}_{5}$中, 其17电子和16电子时的最稳定结构中的所有B均为平面四配位. 18电子的B₆S₅更为稳定.     

Crystal and Molecular Structure of 4-Hydroxy-3-Methoxy-4-N-Methylstilbazonium Iodide C_(15) H_(16) NO_2 +·I~-CrystalandMolecularS

１　ＩＮＴＲＯＤＵＣＴＩＯＮＲｅｓｅａｒｃｈｏｎＳＨＧｅｆｆｅｃｔｈａｓｂｅｅｎｏｎａｒｅｍａｒｋａｂｌｅｐｏｓｉｔｉｏｎｉｎｏｒｇａｎｉｃｎｏｎｌｉｎｅａｒｏｐｔｉｃａｌ（ＮＬＯ）ｍａｔｅｒｉａｌｓｆｉｅｌｄ．Ｔｈｅｃｏｎｊｕｇａｔｅｄｄｅｌｏｃａｌｉｚｅｄπｅｌｅｃｔｒｏｎｓｐｏｓｓｉｂｌｙｒｅｓｕｌｔｉｎｔｈｅｓｅｃｏｎｄ－ｏｒｄｅｒＮＬＯｐｒｏｐｅｒｔｙｏｆｏｒｇａｎｉｃｃｏｍｐｏｕｎｄｓ,ｓｏａｎｕｍｂｅｒｏｆｎｉｔｒｏａｎｉｌｉｎｅｄｅｒｉｖａｔｉｖｅｓ,ｓｕｃｈａｓ２－ｍｅｔｈｙｌ…     

Das erste Alkali-Erdalkalimetall-Oxoniccolat(II,III): NaBa2Ni22+Ni3+O6

The First Alkalinc Alkaline Earth Oxoniccolate(II,III): NaBa₂Ni₂²⁺Ni³⁺O₆ Single crystals of NaBa₂Ni₂²⁺Ni³⁺O₆ were prepared by solid state reaction. X-ray investigations led to orthorhombic symmetry, space group D-Fmmm; a = 8.310; b = 11.220; c = 14.397 Å; Z = 8. Na⁺ is coordinated by six O^2? in form of a trigonal prism and the two Ba²⁺ point positions show different coordination numbers C.N. = 6 + 4 and 8. The Ni²⁺ /Ni³⁺ ions are in square planar polygons, six of them are forming a so far unknown closed macro polyhedra.     

Growth and Crystal Structure of YbAl3（BO3）4

1 INTRODUCTION With the development of high power InGaAs laser diode (LD) as pump sources, the Yb3+-doped laser crystals have received much attention. Due to the simple energy level structure of the Yb3+ ions, the Yb3+-doped laser crystals have no concentration quenching, and have high quantum efficiency and low quantum defects even at high doping concentration of the Yb3+ ions[1, 2]. Therefore, the Yb3+-doped crystals are good candidates of media in the LD-pumped solid-state laser,…     

Synthesis and Crystal Structure of [2-dapp]2[Zn（dmit）2] （2-dapp = 2-（4-Dimethylaminophenyl）ethyl-l-methylpyridinium, dmit = 1,3-Dithiole-2-thione-4,5-dithiolato）

1 INTRODUCTION The transition metal complexes with dmit ligand together with their derivatives have received signi- ficant attention due to their metallic-like electronic properties[1～8]. More recently, our researches show that they may be the new kind…     

STUDY ON TETRANUCLEAR TRANSITION METAL CLUSTER WITH μ_3-O BRIDGES I . SYNTHESIS AND CRYSTAL STRUCTURE OF [Fe_4O_2(O_2CCH_3)_7(2,2''''-bipy)_2]Cl

INTRODUCTION.The first tetranuelear oxo一bridged manganese eomplex eon-taining〔Mn4OZ〕“+eore was reported on its synthesis,strueture and magnetie proper-ties in 1 987〔‘〕,representing the best available model for the photosynthetie water oxi-dation eentre.In order to find out the relationship of aetivity with eonfiguration ofthis kind of eomplexes,a series of dual oxo一bridged tetranuelear eomplexes have beensynthesized in our laboratory〔2〕.In this paper the aeetato一bridged tetran…     

La3Ni2O6: a new double T'-type nickelate with infinite Ni1+/2+O2 layers

New mixed-valent, Ni1+/Ni2+, metastable nickelate, La3Ni2O6, was synthesized by low-temperature reduction of La3Ni2O7 with CaH2. The crystal structure of La3Ni2O6 (space group: I4/mmm, a = 3.9686(1) A and c = 19.3154(6) A) was determined from powder neutron diffraction data by Rietveld analysis. The structure can be described as an intergrowth of LaO2 fluorite and double infinite layer (LaNiO2)2 blocks and represents the n = 2 homologue of the T'-type series Lan+1NinO2n+2. Such double T'-type structural arrangement has never been observed before. The 3d9/3d8 electronic configuration of Ni1+/Ni2+ and the presence of NiO2 infinite layers resemble electronic and structural features of the superconducting cuprates. X-ray absorption spectroscopy supports the 1+/2+ oxidation state and planar coordination of Ni in agreement with the structure determination.     

Das erste Erdalkalimetall-Mercurato(II)-Palladat(II,IV): Ba2Hg3Pd52+ Pd24+ O14

On the First Alkaline Earth Mercurato(II)-Palladate(II, IV): Ba₂Hg₃Pd₅²⁺Pd₂⁴⁺O₁₄ Single crystals of Ba₂Hg₃Pd₇O₁₄ were prepared by oxygen high-pressure technique (3900 bar) and investigated by X-ray technique. It crystallizes with monoclinic symmetry, space group C–C2/m; Z = 2 (a = 10.583; b = 6,207; c = 10.919 Å, β = 90.56°). The Hg²⁺ ions show partially dumb-bell like and one sided 3 fold coordination respectively. Pd⁴⁺ /Pd²⁺ show an octahedric or square planar surrounding.     

Das erste Alkali-Erdalkali-Oxocuprat(II,III): NaBa2Cu22+Cu3+O6

The first Alkaline Alkaline-Earth Oxocuprate (II, III): NaBa₂Cu₂²⁺Cu³⁺O₆ The compound NaBa₂Cu₃O₆ was prepared by heating of Na₂O₂, BaO₂, Cu₂O in closed Ag-tubes. X-ray single crystal investigations led to orthorhombic symmetry, space group D-Fmmm; a = 8.4229; b = 11.4418; c = 14.4063 Å; Z = 8. Cu²⁺ and Cu³⁺ show square planar polygones of four and Na⁺ trigonal prisms of six O^2?. The two barium point positions show coordination numbers C.N. = 8 and 6 + 4. The crystal structure is discussed.     

Crystal and Molecular Structure of 4-Hydroxy-3-Methoxy-4-N-Methylstilbazonium Iodide C15H16NO2+·I-

The crystal structure of the title compound C15H16NO2+ · I-(Mr=369. 19) has been determined by single crystal X-ray diffraction analysis. The crystal belongs to tbe monoclinic system with space group P21/c, a=8. 957(1), b=21. 8117(2), c=7. 8760(10)A , β=103.94(1)°, V=1493.8(3)A3, Z=4, Dc=1. 642g cm3,μ=2. 141mm-1, F(000)=728, final R=0. 0264, and Rw=0. 0644(I＞2σ(I)) for 2938 independent reflections. The results show that in the crystal structure of the title compound the planar cations have two configurations, and these cations are anti-parallelly packed through the strong π…π interaction.     

4-苯基-2-对甲氧基苯基-1,5-苯并硫氮杂卓-α,α-二甲基-β-内酰胺的合成及晶体结构

合成了标题化合物并测定了其晶体结构。该化合物的化学式为C26H25NO2S, Mr = 415.53。晶体为三斜晶系,P 空间群,晶胞参数为:a = 9.299(3), b = 10.134(3), c = 12.455(4) ? a = 98.457(5), b = 106.143(5), g = 103.843(5), V = 1065.7(6) 3, Z = 2, Dc = 1.295 g/cm3, F(000) = 440, m = 0.175 mm-1, R = 0.0406, wR = 0.1064。晶体结构显示,化合物中七员环呈类椅式构象,b-内酰胺环近似梯形。     

Crystal Structure of 1-Methyl-5-phenylhydantoin

1　INTRODUCTIONInourinvestigationofhemithioacetals,wediscoveredthatα-benzoylhemithioac-etalisquitestableandhastwoelectrophilicsitesthatcanreactwithalkylureastoformahydantoinring[1].Althoughthehydantoinringitselfdoesnotpresentanymedicinalactivity,somedisubstitutedhydantoinshavebeenwidelyusedasmedicineforitsregulareffectonthebioelectricactivityofthenervoussystem.Inordertoim-proveandexpandtheactivityaswellastopreventsideeffects,variouskindsofhy-dantoinderivativeshavebeenpreparedandtested[2].…     

Zur Kristallstruktur von Cu2M(BO3)O2 (M = Fe3+, Ga3+)

The Crystal Structure of Cu₂M(BO₃)O₂ (M = Fe³⁺, Ga³⁺) Single Crystals of the compounds Cu₂M(BO₃)O₂ (M = Fe³⁺ (I), Ga³⁺ (II)) were obtained by a B₂O₃ flux-technique. They crystallize in a monoclinic distorted variant of a Ludwigite structure with a partly ordered metal distribution. X-ray investigations on single crystals led to the space group C–P2₁/c (No. 14); I: a = 3.108(1); b = 12.003(1); c = 9.459(3) Å; b? = 96.66(3)°; Z = 4 and II: a = 3.1146(2); b = 11.921(3); c = 9.477(2) Å; b? = 97.91(2)°; Z = 4. All metal-sites are distorted octahedraly coordinated by oxygen-ions. The structure contains isolated planar BO₃-units and oxygen which is not coordinated to boron.     

CRYSTAL STRUCTURE OF CK(C_(12)H_(24)O_6)]_2Pd(SCN)_4(H_2O)

<正> [K(C_12H_24O_6)]_2Pd(SCN)_4(H_2O),MT=963.59,monoclinic, P21/n,a= 11. 075(1),b= 12. 231(1),c= 15. 863(2) A ,β=93. 25(1)°,V=2145. 3A3,Z=2, Dc=1. 492gcm-3,λ(MoKa) = 0. 71073A μ=8. 64cm-1,F(000) = 996,final R=0. 045 for 1835 observable reflections. The Pd2+ ion coordinates with four S atoms from SCN- groups forming a regular square planar configuration. The K+ ion is surrounded by six ether oxygen atoms,one O atom from water molecule coordinated to two K+ions and one N atom from SCN- group to form a distorted hexagonal bipyramid. Two K atoms are linked with one Pd atom by two bridging SCN- groups forming a chain molecular array in the crystal.     

Structure of Non-stoichiometric Sr6Gd0.61Sc1.39（BO3）6 Crystal

1 INTRODUCTION With the increasing interest in diode-pumped solid state lasers, researches on more efficient new materials for diode pumping become more important. The double borates are a type of excellent laser gain media, for example, Nd3 -doped RAl…     

Isolierte quadratische Koordination von Pt2+ in BaNd2PtO5

Isolated Square-Planar Coordinated Pt²⁺ Inside of BaNd₂PtO₅ Single crystals of the hitherto unknown compound BaNd₂PtO₅ were prepared and examined by X-ray technique. The compound crystallizes with tetragonal symmetry D? P4 b2; a = 6.7569(6) and c = 5.9119(13) Å; Z = 2. The structure is discussed in respect of the isolated square-planare coordination of Pt²⁺ ions and its relation with other planar coordinated platinum of oxocompounds.     

Laser Flash Photolysis on Electron Transfer Reactions between 1,8-Dihydroxyanthraquinone with Adenine and Cytosine

Electron transfer （ET） reactions between 1,8-dihydroxyanthraquinone （DHAQ） and two DNA bases, adenine （A） and cytosine （C）, have been investigated in CH3CN/H20 solution with nanosecond time-resolved laser flash photolysis. After irradiation at 355 nm, the triplet DHAQ is produced via intersystem crossing and reacts with two nucleobases. ET processes for both reactions have been definitely identified, in which two bases play a significant role of electron donor. Based on the measured decay dynamics of various intermediates and the corresponding quenching rates, an initial ET process followed by a secondary proton-transfer reaction is suggested for both the overall reactions. By plotting the observed quenching rate against the concentration of two DNA bases, the bimolecular quenching rate constants are determined as 9.0-10s L/（mol.s） for the 3DHAQ＊＋C reaction and 3.3x10^8 L/（mol.s） for the 3DHAQ＊＋A reaction, respectively.     

Investigation of the Interaction between Isoflavonoids and Bovine Serum Albumin by Fluorescence Spectroscopy

The interactions of bovine serum albumin （BSA） with three structurally related isoflavonoids, genistein, puerarin and daidzein, were studied under physiological conditions by fluorescence spectroscopic technique. The quenching mechanism of these compounds with BSA was suggested as static quenching and the binding constants were determined at different temperatures based on the fluorescence quenching results. The transfer efficiency of energy and distance between the acceptor and BSA were investigated on the basis of the mechanism of the Forster energy transference. According to the thermodynamic parameters it has been suggested that the acting force be mainly hydrophobic force. The comparison of binding potency of the three isoflavonoids to BSA showed that the substitution by 5-OH and 8-Glc could enhance the binding affinity. All these obtained in the work can make us better understand the mode of the action and pharmacological activities of the isoflavonoids.     

Theoretical Investigation on Interaction between Guanine and Luteolin

The interacting patterns of the luteolin and guanine have been investigated by using the density functional theory B3LYP method with 6-31＋G＊ basis set. Eighteen stable structures for the luteolin-guanine complexes have been found respectively. The results indicate that the complexes are mainly stabilized by the hydrogen bonding interactions. Meanwhile, both the number and strength of hydrogen bond play important roles in determining the stability of the complexes which can form two or more hydrogen bonds. Theories of atoms in molecules and natural bond orbital have also been utilized to investigate the hydrogen bonds involved in all the systems. The interaction energies of all the complexes which were corrected by basis set superposition error are 6.04-56.94 kJ/mol. The calculation results indicate that there are strong hydrogen bonding interactions in the luteolin-guanine complexes. We compared the interaction between luteolin and four bases of DNA, and found luteolin-thymine was the strongest and luteolin-adenine was the weakest. The interaction between luteolin and DNA bases are all stronger than luteolin-water.     

Fe48Co52 Alloy Nanowire Arrays： Effects of Magnetic Field Annealing

The effects of magnetic field annealing on the properties of Fe48Co52 alloy nanowire arrays with various interwire distances （Di=30-60 nm） and wire diameters （Dw=22-46 nm） were investigated in detail. It was found that the array＇s best annealing temperature and crys- talline structure did not show any apparent dependence on the treatment of applying a 3 kOe magnetic field along the wire during the annealing process. For arrays with small Dw or with large Di, the treatment of magnetic field annealing also had no obvious influence on their magnetic performances. However, such a magnetic field annealing constrained the shift of the easy magnetization direction and improved the coercivity and the squareness obviously for arrays with large Dw or with small Di. The difference in the intensity of the effective anisotropic field within the arrays was believed to be responsible for this different variation of the array＇s magnetic properties after magnetic field annealing.