多吡唑烷配体与（CH3CN）2Mo（Cl）（CO）3（GeCl3）取代反应？…

通过多吡啶烷配体与（ＣＨ３ＣＮ）２Ｍｏ（Ｃｌ）（ＣＯ）３（ＧｅＣｌ３）中乙腈配体的取代反应,合成了含多吡唑烷配体的Ｍｏ－Ｇｅ双核金属化合物。多吡唑烷配体环上３,５位取代基的立体位阻以及４位取供基的电子效应均影响其配侠能力。通过元素分析,＾１Ｈ ＮＭＲ,ＩＲ和ＭＳ谱表征了所有新化合物的分子结构。     

17α-羟化酶/C17,20-裂解酶(P45017α)抑制剂17-(取代吡唑、异唑基)雄烯衍生物的合成

在17-(3-吡唑基)和17-(5-异唑基)雄甾-4,16-二烯-3-酮的吡唑基的5-位和异唑基的3-位引入取代基, 设计并合成了11个17-(取代的吡唑基、异唑基)雄烯衍生物, 化合物的结构经1H NMR, IR, 元素分析或质谱确证.     

有机锡修饰的双吡唑甲烷及其与W(CO)5THF的反应

通过双吡唑甲基锂(LiCHPz₂)与有机锡卤化物(R₃SnX)的反应合成了一系列有机锡修饰的双吡唑甲烷配体(R₃SnCHPz₂).由于锡上取代基的不同,这些配体与W(CO)₅THF反应时表现出了不同的反应方式.三芳基锡修饰的双吡唑甲烷与W(CO)₅THF反应发生Sn-C(sp₃)键对W(0)中心的氧化加成;而三苄基锡修饰的双吡唑甲烷与其反应时仅给出羰基取代产物[Bz₃SnCHPz₂W(CO)₄].另外,二苯基苄基锡以及三(2-苯基-2-甲基丙基)锡修饰的双吡唑甲烷配体类似的反应导致配体的分解,产生单吡唑配体取代的羰基钨衍生物[W(CO)₅PzH]以及脱有机锡的双吡唑甲烷四羰基钨衍生物[CH₂Pz₂W(CO)₄].     

17α-羟化酶/C_(17,20)-裂解酶(P450_(17α))抑制剂17-(取代吡唑、异噁唑基)雄烯衍生物的合成

在 1 7-( 3 -吡唑基 )和 1 7-( 5 -异噁唑基 )雄甾 -4 ,1 6-二烯 -3 -酮的吡唑基的 5 -位和异唑基的 3 -位引入取代基 ,设计并合成了 1 1个 1 7-(取代的吡唑基、异唑基 )雄烯衍生物 ,化合物的结构经 1H NMR,IR,元素分析或质谱确证     

双吡唑烷ⅥB金属羰基配合物的取代基效应与电化学性质研究

对双吡唑烷ⅥB金属羰基配合物的电化学特性进行了系统研究，结果表明，吡唑环上的取代基极大的影响双吡唑烷ⅥB金属羰基配合物金属中心的峰电位E1／2。给电子代取代基增强配体的配位能力且使金属中心的E1／2减小，而吸电子取代基减弱配体的配位能力使金属中心的E1／2增大。     

磷光配合物(L)Re(CO)3Cl(L=α,α-diamine)的电化学性质和电子能级

通过循环伏安法对磷光发光材料(L)Re(CO)3Cl(L=α,α-diamine)系列配合物的电化学性质进行了研究.结合电子吸收、荧光光谱和量子化学计算确定了其能级结构,考察了二胺配体的取代基修饰对能级结构影响的规律.(L)Re(CO)3Cl系列配合物表现为单一的氧化(正电位方向)和多步还原(负电位方向)过程,分别反映了Re—Cl的杂化轨道组成的HOMO能级和二胺配体的π*轨道组成的LUMO能级的结构.与光谱数据比较发现,(L)Re(CO)3Cl配合物电化学数据主要反映的是三重态电子能级结构.     

3-(3-吲哚基)-5-吡唑甲酰胺的合成及抑菌活性

本文以3-乙酰吲哚、草酸二乙酯、水合肼等为原料,经缩合、环化、水解反应制备3-(3-吲哚基)吡唑-5-甲酸,后者再与苄胺或2-苯乙胺在EDC-BTOH催化下合成了一系列N-取代苄基-3-(3-吲哚基)吡唑-5-甲酰胺和N-(2-取代苯基乙基)-3-(3-吲哚基)吡唑-5-甲酰胺。采用平板计数法测试了化合物对大肠杆菌和金黄色葡萄球菌的抑制活性,结果表明,在浓度为80 μg/mL时部分化合物有较高的抑菌活性。     

3-取代苄氧基-6-(取代-1H-吡唑-1-基)哒嗪的合成与生物活性

3-氯-6-肼基哒嗪分别与乙酰丙酮和3-二甲胺基丙烯醛反应, 合成了中间体3-氯-6-(3,5-二甲基-1H-吡唑-1-基)哒嗪(2)和3-氯-6-(1H-吡唑-1-基)哒嗪(4), 它们与多种取代苄醇反应, 得到了一系列未见报道的3-取代苄氧基-6-(取代-1H-吡唑-1-基)哒嗪, 其结构均经1H NMR, IR和元素分析确证. 初步的生物活性测试结果表明, 所合成的化合物对油菜和稗草均具有一定的抑制作用.     

4-酰基-双(1,3-二苯基-5-吡唑啉酮)铽(Ⅲ)配合物的合成及荧光性质

合成了3种4-酰基-双(1,3-二苯基-5-吡唑啉酮),1,5-双(1,3-二苯基-5-吡唑啉酮-4-基)-1,5-戊二酮;1,6-双(1,3-二苯基-5-吡唑啉酮-4-基)-1,6-己二酮和1,10-双(1,3-二苯基-5-吡唑啉酮-4-基)-1,10-癸二酮,通过元素分析、红外光谱和核磁共振氢谱对产物组成进行了表征.合成了它们的Tb(Ⅲ)二元和三元[1,10-二氮杂菲(Phen) 或2,2-联吡啶(Dipy)]配合物,测定了配合物的荧光光谱,对其荧光性质进行了研究.结果表明,配合物发射Tb(Ⅲ)的特征荧光,4-酰基-双(1,3-二苯基-5-吡唑啉酮)配体的三重态能级与Tb(Ⅲ)的最低激发态(5D4)能级匹配较好;配合物荧光强度随4-酰基-双(1,3-二苯基-5-吡唑啉酮)配体2个吡唑环间碳链的增长而减弱;第2配体Phen 和Dipy具有荧光增强作用,且前者优于后者.     

3-(吲哚-3-基)-5-吡唑甲酰胺衍生物的合成及抑菌活性

本文以3-乙酰吲哚、草酸二乙酯、水合肼等为原料,经缩合、环化、水解反应制备3-(吲哚-3-基)吡唑-5-甲酸,后者再与苄胺或2-苯乙胺在EDC-BTOH催化下合成了一系列N-取代苄基-3-(吲哚-3-基)吡唑-5-甲酰胺和N-(2-取代苯基乙基)-3-(吲哚-3-基)吡唑-5-甲酰胺。采用平板计数法测试了化合物对大肠杆菌和金黄色葡萄球菌的抑制活性,结果表明,在浓度为80μg/m L时部分化合物有较高的抑菌活性。     

LiMn3(SeO3)2(HSeO3)6

The title compound, lithium trimanganese bis­[trioxo­selenate(IV)] hexa­kis[hydrogentrioxoselenate(IV)], is built up from a vertex‐sharing network of distorted Mn^IIIO₆ octa­hedra, SeO₃ and HSeO₃ pyramids and unusual Li(OH)₆ octa­hedra, resulting in a dense three‐dimensional structure. Mn, Li and one Se atom have site symmetries of , , and 3, respectively. An O—H⋯O hydrogen bond helps to establish the crystal packing.     

Spectroscopic properties of Er(3+)/Yb(3+) co-doped Bi(2)O(3)-B(2)O(3)-GeO(2) glasses

Er(3+)/Yb(3+) co-doped 60Bi(2)O(3)-(40 - x)B(2)O(3)-xGeO(2) (BBG; x=0, 5, 10, 15 mol%) glasses that are suitable for fiber lasers, amplifiers have been fabricated and characterized. The absorption spectra, emission spectra, and lifetime of the (4)I(13/2) level and quantum efficiency of Er(3+):(4)I(13/2) --> (4)I(15/2) transition were measured and calculated. With the substitution of GeO(2) for B(2)O(3), both Delta lambda(eff) and sigma(e) decrease from 75 to 71 nm and 9.88 to 8.12 x 10(-21) cm(2), respectively. The measured lifetime of the (4)I(13/2) level and quantum efficiency of Er(3+):(4)I(13/2) --> (4)I(15/2) transition increase from 1.18 to 1.5 ms and 36.2% to 43.2%, respectively. The emission spectra of Er(3+):(4)I(13/2) --> (4)I(15/2) transition was also analyzed using a peak-fit routine, and an equivalent four-level system was proposed to estimate the stark splitting for the (4)I(15/2) and (4)I(13/2) levels of Er(3+) in the BBG glasses. The results indicate that the (4)I(13/2) --> (4)I(15/2) emission of Er(3+) can be exhibit a considerable broadening due to a significant enhance the peak A, and D emission.     

Interactions in the Quinary System H2O-Y(NO3)3-La(NO3)3-Pr(NO3)3-Nd(NO3)3 to Very High Concentrations

Isopiestic measurements have been carried out for the quinary system H₂O-Y(NO₃)₃-La(NO₃)₃-Pr(NO₃)₃-Nd(NO₃)₃ at 298.15 K to near saturation. The measurements can be represented within experimental uncertainty over the full concentration range by a modified Pitzer ion-interaction model extending to the C ⁽³⁾ term. In addition, the system obeys the Zdanovskii–Stokes–Robinson model or partial ideal solution model within the accuracy of the isopiestic measurements, indicating zero interchange energy between the unlike salts, which is consistent with the nature of trivalent rare-earth elements.     

Schwingungsspektren und Kraftkonstanten der Übergangsreihen OP(N(CH3)2)3 – OP(CH3)3 und SP(N(CH3)2)3 – SP(CH3)3

Vibrational Spectra and Force Constants of the Series OP(N(CH₃)₂)₃ – OP(CH₃)₃ and SP(N(CH₃)₂)₃ – SP(CH₃)₃ The vibrational spectra (IR and Raman) of the compounds of the title series are recorded and assigned to the normal vibrations. By a simplified force field the valence force constants are calculated and discussed. The results are compared with those of the NMR spectroscopy.     

Bis(trifluoroacetyl) peroxide, CF(3)C(O)OOC(O)CF(3)

Pure, highly explosive CF(3)C(O)OOC(O)CF(3) is prepared for the first time by low-temperature reaction between CF(3)C(O)Cl and Na(2)O(2). At room temperature CF(3)C(O)OOC(O)CF(3) is stable for days in the liquid or gaseous state. The melting point is -37.5 degrees C, and the boiling point is extrapolated to 44 degrees C from the vapor pressure curve log p = -1875/T + 8.92 (p/mbar, T/K). Above room temperature the first-order unimolecular decay into C(2)F(6) + CO(2) occurs with an activation energy of 129 kJ mol(-1). CF(3)C(O)OOC(O)CF(3) is a clean source for CF(3) radicals as demonstrated by matrix-isolation experiments. The pure compound is characterized by NMR, vibrational, and UV spectroscopy. The geometric structure is determined by gas electron diffraction and quantum chemical calculations (HF, B3PW91, B3LYP, and MP2 with 6-31G basis sets). The molecule possesses syn-syn conformation (both C=O bonds synperiplanar to the O-O bond) with O-O = 1.426(10) A and dihedral angle phi(C-O-O-C) = 86.5(32) degrees. The density functional calculations reproduce the experimental structure very well.     

Hyperfine structures of the 2 (3)Sigma(g) (+), 3 (3)Sigma(g) (+), and 4 (3)Sigma(g) (+) states of Na(2)

The hyperfine structures of the 2 (3)Sigma(g) (+), 3 (3)Sigma(g) (+), and 4 (3)Sigma(g) (+) states of Na(2) have been resolved with sub-Doppler continuous wave perturbation facilitated optical-optical double resonance spectroscopy via A (1)Sigma(u) (+) approximately b (3)Pi(u) mixed intermediate levels. The hyperfine patterns of these three states are similar. The hyperfine splittings of the low rotational levels are all very close to the case b(betaS) limit. As the rotational quantum number increases, the hyperfine splittings become more complicated and the coupling cases become intermediate between cases b(betaS) and b(beta J) due to spin-rotation interaction. We present a detailed analysis of the hyperfine structures of these three (3)Sigma(g) (+) states, employing both case b(betaS) and b(beta J) coupling basis sets. The results show that the hyperfine splittings of the (3)Sigma(g) (+) states are mainly due to the Fermi-contact interaction. The Fermi contact constants for the two d sigma Rydberg states, the 2 (3)Sigma(g) (+) and 4 (3)Sigma(g) (+), are 245+/-5 MHz and 225+/-5 MHz, respectively, while the Fermi contact constant of the s sigma 3 (3)Sigma(g) (+) Rydberg state is 210+/-5 MHz. The diagonal spin-spin and spin-rotation constants, and nuclear spin-electronic spin dipolar interaction parameters of the 3 (3)Sigma(g) (+) and 4 (3)Sigma(g) (+) states are also obtained.     

Li(VO2)3(TeO3)2

The title compound, lithium tris[dioxidovanadium(V)] bis[trioxidotellurium(IV)], contains chains of edge‐sharing distorted VO₆ octahedra. The pyramidal TeO₃ groups crosslink the chains into sheets. Finally, an Li⁺ cation adopting an unusual capped trigonal–bipyramidal LiO₆ geometry bridges the layers to complete a three‐dimensional structure.     

Syntheses and structures of the infinite chain compounds Cs(4)Ti(3)Se(13), Rb(4)Ti(3)S(14), Cs(4)Ti(3)S(14), Rb(4)Hf(3)S(14), Rb(4)Zr(3)Se(14), Cs(4)Zr(3)Se(14), and Cs(4)Hf(3)Se(14)

The alkali metal/group 4 metal/polychalcogenides Cs(4)Ti(3)Se(13), Rb(4)Ti(3)S(14), Cs(4)Ti(3)S(14), Rb(4)Hf(3)S(14), Rb(4)Zr(3)Se(14), Cs(4)Zr(3)Se(14), and Cs(4)Hf(3)Se(14) have been synthesized by means of the reactive flux method at 823 or 873 K. Cs(4)Ti(3)Se(13) crystallizes in a new structure type in space group C(2)(2)-P2(1) with eight formula units in a monoclinic cell at T = 153 K of dimensions a = 10.2524(6) A, b = 32.468(2) A, c = 14.6747(8) A, beta = 100.008(1) degrees. Cs(4)Ti(3)Se(13) is composed of four independent one-dimensional [Ti(3)Se(13)(4-)] chains separated by Cs(+) cations. These chains adopt hexagonal closest packing along the [100] direction. The [Ti(3)Se(13)(4-)] chains are built from the face- and edge-sharing of pentagonal pyramids and pentagonal bipyramids. Formal oxidation states cannot be assigned in Cs(4)Ti(3)Se(13). The compounds Rb(4)Ti(3)S(14), Cs(4)Ti(3)S(14), Rb(4)Hf(3)S(14), Rb(4)Zr(3)Se(14), Cs(4)Zr(3)Se(14), and Cs(4)Hf(3)Se(14) crystallize in the K(4)Ti(3)S(14) structure type with four formula units in space group C(2)(h)()(6)-C2/c of the monoclinic system at T = 153 K in cells of dimensions a = 21.085(1) A, b = 8.1169(5) A, c = 13.1992(8) A, beta = 112.835(1) degrees for Rb(4)Ti(3)S(14);a = 21.329(3) A, b = 8.415(1) A, c = 13.678(2) A, beta = 113.801(2) degrees for Cs(4)Ti(3)S(14); a = 21.643(2) A, b = 8.1848(8) A, c = 13.331(1) A, beta = 111.762(2) degrees for Rb(4)Hf(3)S(14); a = 22.605(7) A, b = 8.552(3) A, c = 13.880(4) A, beta = 110.919(9) degrees for Rb(4)Zr(3)Se(14); a = 22.826(5) A, b = 8.841(2) A, c = 14.278(3) A, beta = 111.456(4) degrees for Cs(4)Zr(3)Se(14); and a = 22.758(5) A, b = 8.844(2) A, c = 14.276(3) A, beta = 111.88(3) degrees for Cs(4)Hf(3)Se(14). These A(4)M(3)Q(14) compounds (A = alkali metal; M = group 4 metal; Q = chalcogen) contain hexagonally closest-packed [M(3)Q(14)(4-)] chains that run in the [101] direction and are separated by A(+) cations. Each [M(3)Q(14)(4-)] chain is built from a [M(3)Q(14)] unit that consists of two MQ(7) pentagonal bipyramids or one distorted MQ(8) bicapped octahedron bonded together by edge- or face-sharing. Each [M(3)Q(14)] unit contains six Q(2)(2-) dimers, with Q-Q distances in the normal single-bond range 2.0616(9)-2.095(2) A for S-S and 2.367(1)-2.391(2) A for Se-Se. The A(4)M(3)Q(14) compounds can be formulated as (A(+))(4)(M(4+))(3)(Q(2)(2-))(6)(Q(2-))(2).