十二烷基苯磺酸钠-盐酸苯海索-Ru(bpy)2+3体系的电化学发光行为研究及应用

在十二烷基苯磺酸钠(SDBS)存在下,考察了盐酸苯海索(BH)-Ru(bpy)32+体系的电化学及其发光行为。结果表明,BH对Ru(bpy)32+体系的电化学发光具有增敏效应;在SDBS存在下,BH对Ru(bpy)32+体系电化学发光的增敏效应显著增强,发光强度提高约16倍。据此建立了一种高效、简便的BH电化学发光新方法。在最佳实验条件下,BH的浓度在4.0×10-7～1.0×10-4 mol/L范围内与相对发光强度呈线性关系(r=0.995 5),检出限(S/N=3)为1.11×10-9 mol/L;连续平行测定1.0×10-5 mol/L BH溶液10次,发光强度的RSD为3.2%。样品的回收率为96%～108%,RSD为4.3%。该方法样品前处理简单,具有较高的选择性和灵敏度,用于实际样品中BH的测定,结果满意。     

十二烷基磺酸钠-盐酸维拉帕米-联吡啶钌体系电化学发光及其应用

在十二烷基磺酸钠(SDS)中,考察了盐酸维拉帕米-Ru(bpy)3(2+)体系在金电极上的电化学及其发光行为.结果表明:SDS对体系的电化学反应和电化学发光强度具有显著的增敏作用.据此,建立了一种高效、简便的测定盐酸维拉帕米的电化学发光新方法.在最佳实验条件下,盐酸维拉帕米浓度在1.0×10(-4)～1.0×10(-2...     

Determination of Benzhexol Hydrochloride by Electrochemiluminescence in the Presence of Sodium Dodeeyl Benzene Sulfonate

在十二烷基苯磺酸钠(SDBS)存在下,考察了盐酸苯海索(BH)- Ru(bpy)2+3体系的电化学及其发光行为.结果表明,BH对Ru(bpy)2+3体系的电化学发光具有增敏效应;在SDBS存在下,BH对Ru(bpy)2+3体系电化学发光的增敏效应显著增强,发光强度提高约16倍.据此建立了一种高效、简便的BH电化学发光新方法.在最佳实验条件下,BH的浓度在4.0×10-7～1.0×10-4 mol/L范围内与相对发光强度呈线性关系(r=0.995 5),检出限(S/N=3)为1.11×10-9 mol/L;连续平行测定1.0×10-5 mol/L BH溶液10次,发光强度的RSD为3.29％.样品的回收率为96％～108％,RSD为4.3％.该方法样品前处理简单,具有较高的选择性和灵敏度,用于实际样品中BH的测定,结果满意.     

巯基乙酸修饰金电极电化学发光行为的研究及其对盐酸硫必利的测定

在裸金电极上制备了巯基乙酸自组装膜修饰电极(MA/SAMs-Au/CME)。基于盐酸硫必利对联吡啶钌在该电极上的电化学及其发光行为的强烈增敏作用,建立起一种直接测定盐酸硫必利电致化学发光新方法。在最佳实验条件下,盐酸硫必利在1.0×10-4～1.0×10-7mol/L与相对发光强度呈线性关系,其线性回归方程I(强度)=27.169×106c+140.26,r2=0.9959,检出限(S/N=3)为5.11×10-9mol/L。连续测定1.0×10-5mol/L盐酸硫必利10次,发光强度的RSD值为1.8%。对样品进行回收率试验,回收率在94.1%～104.9%之间,RSD为4.5%(n=5)。     

联吡啶钌体系电化学发光法测定克林霉素的研究

建立了以金电极为工作电极电致化学发光测定盐酸克林霉素的方法,并采用循环伏安和电致化学发光法,研究了体系的电化学行为和电化学发光行为.研究结果表明,在0.1 mol/L的硼酸(pH 8.0)缓冲溶液中,扫描速率为100 mV/s时,ECL的峰高与盐酸克林霉素浓度在1.0×10-5 ～1.0×10-4 mol/L和1.0×10-7 ～8.0×10-6 mol/L范围内呈线性关系,其线性回归方程分别为I(counts)=465.00×105c-133.80(r=0.996 8)和I(counts)=20.333×106c+100.25(r=0.995 9).方法的检出限为1.0×10-7 mol/L(S/N=3).连续测定2.0×10-5 mol/L的盐酸克林霉素溶液10次,发光强度值的RSD为1.74%.对样品进行加标回收率实验,回收率为93% ～102%.该方法具有较高的选择性和灵敏度,样品处理简单快速,用于盐酸克林霉素胶囊的测定,结果满意.     

固定Ionic liquid/Silica sol/Nafion膜中的联吡啶钌电化学发光行为的研究及应用

制备了Ionic liquid/Silica sol/Nafion-联吡啶钌复合物膜修饰金电极。采用循环伏安(CV)和电致化学发光(ECL)法,考察了联吡啶钌和左氧氟沙星在此修饰电极上的电化学及其发光行为。结果表明,此修饰电极表现出很好的电化学活性和电化学发光响应。基于左氧氟沙星对固定化联吡啶钌在0.1 mol/L磷酸盐缓冲液中的弱电化学发光信号有较强的增敏作用,建立了电化学发光检测盐酸左氧氟沙星的新方法。在最佳实验条件下,左氧氟沙星浓度在1.0×10-7～1.0×10-4mol/L范围内与相对发光强度呈线性关系(r2=0.998 4),检出限(S/N=3)为1.59×10-9mol/L。连续平行测定2.2×10-5mol/L的左氧氟沙星溶液10次,发光强度的相对标准偏差(RSD)为3.6%。对样品进行回收率试验,回收率在95.6%～103.5%之间,RSD(n=5)为3.0%。该方法具有较高的选择性和灵敏度,样品处理简单快速,用于盐酸左氧氟沙星的测定,结果满意。     

Silica sol/Nano-Au/PVA/L-cysteine修饰金电极电致化学发光测定甲氧氯普胺的研究

在甲氧氯普胺对联吡啶钌具有较好电化学发光增敏效果的基础上,制备出Silica sol/Nano-Au/PVA/L-cysteine修饰金电极,并通过电致化学发光法,考察了联吡啶钌及联吡啶钌-甲氧氯普胺体系在此电极上的电化学及电化学发光行为。该修饰电极对联吡啶钌-甲氧氯普胺体系有良好的电致化学发光响应特性;在最优条件下,在1.0×10-7~1.0×10-4mol/L范围内甲氧氯普胺浓度与其对应的电化学发光强度值线性关系良好,检出限(S/N=3)为1.40×10-9mol/L;通过平行测定1.0×10-5mol/L甲氧氯普胺溶液8次,发光强度值相对偏差(RSD)为1.8%,样品回收率在98.3%~104.4%之间,RSD为2.3%(n=5)。     

Nano-Au/Silica sol/PVP修饰金电极上电化学发光测定盐酸硫必利

采用溶胶-凝胶法制备了Nano-Au/Silica sol/PVP修饰金电极,并基于盐酸硫必利对联吡啶钌(Ru(bpy)2+3)在该修饰电极上弱电化学发光具有较强的增敏作用,建立了电化学发光检测盐酸硫必利的新方法。在最佳实验条件下,盐酸硫必利浓度在1.0×10-7~1.0×0-4 mol/L范围内与相对发光强度呈线性关系(r2=0.9978),检出限(S/N=3)为6.7×10-10 mol/L。连续平行测定1.0×10-5 mol/L盐酸硫必利溶液10次,发光强度的相对标准偏差(RSD)为1.78%。对样品进行回收率试验,其回收率在97.7%~103.9%之间,RSD为2.62%。该方法具有较高的选择性和灵敏度,样品处理简单快速,用于盐酸硫必利的测定,结果满意。     

固定丝素蛋白膜中的联吡啶钌电化学发光行为的研究与应用

基于苯海拉明对联吡啶钌(Ru(bpy)2+3)的电化学发光的增敏作用和丝素蛋白-联吡啶钌复合膜修饰玻碳电极稳定好的特点,建立了一种以丝素蛋白多孔膜-联吡啶钌复合物修饰的玻碳电极电化学发光检测苯海拉明的新方法.结果表明,该修饰电极具有很好的电化学活性和电化学发光(ECL)响应.在最佳实验条件下,苯海拉明浓度在1.0×10-4～1.0×10-7 mol/L范围内与其相对发光强度呈良好的线性关系(r=0.9989); 检出限为2.3×10-7 mol/L(S/N=3).连续平行测定3.78×10-5 mol/L苯海拉明5次,发光强度的RSD为1.76%. 用于实际样品中苯海拉明的测定,结果满意.     

卤素离子-富马酸酮替芬-联吡啶钌体系电化学发光的研究及应用

在卤素离子存在下,考察了富马酸酮替芬-Ru(bpy)32+体系在金电极上的电化学及其发光行为。结果表明:Br-对富马酸酮替芬-Ru(bpy)32+体系在金电极上发光行为具有显著的促进和增敏作用。据此,建立了一种高效、简便的富马酸酮替芬检测的新方法。在最佳实验条件下,富马酸酮替芬在1.0×10-4～1.0×10-7mol/L浓度范围内与相对发光强度呈线性关系,回归方程为I(counts)=1.73×108c+188.15(R2=0.9989),检出限(S/N=3)为4.29×10-8mol/L,连续平行测定富马酸酮替芬溶液(1×10-5mol/L)6次,发光强度的RSD为4.7%。回收率在99.5%～105.0%之间,RSD为2.3%(n=5)。该方法用于实际样品的测定,结果满意。     

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).     

Unique {H(SiR(3))(2)}, (H(2)SiR(3)), H(HSiR(3)), and (H(2))SiR(3) ligand sets supported by the {Fe(Cp)(L)} platform (L=CO, PR(3))

This work deals with the type and incidence of nonclassical Si--H and H--H interactions in a family of silylhydride complexes [Fe(Cp)(OC)(SiMe(n)Cl(3-n))H(X)] (X=SiMe(n)Cl(3-n), H, Me, n=0-3) and [Fe(Cp)(Me(3)P)(SiMe(n)Cl(3-n))(2)H] (n=0-3). DFT calculations complemented by atom-in-molecule analysis and calculations of NMR hydrogen-silicon coupling constants revealed a surprising diversity of nonclassical Si--H and H--H interligand interactions. The compounds [Fe(Cp)(L)(SiMe(n)Cl(3-n))(2)H] (L=CO, PMe(3); n=0-3) exhibit an unusual distortion from the ideal piano-stool geometry in that the silyl ligands are strongly shifted toward the hydride and there is a strong trend towards flattening of the {FeSi(2)H} fragment. Such a distortion leads to short Si--H contacts (range 2.030-2.075 A) and large Mayer bond orders. A novel feature of these extended Si--H interactions is that they are rather insensitive towards the substitution at the silicon atom and the orientation of the silyl ligand relatively the Fe--H bond. NMR spectroscopy and bonding features of the related complexes [Fe(Cp)(OC)(SiMe(n)Cl(3-n))H(Me)] (n=0-3) allow for their rationalization as usual eta(2)-Si--H silane sigma-complexes. The series of "dihydride" complexes [Fe(Cp)(OC)(SiMe(n)Cl(3-n))H(2)] (n=0-3) is different from the previous two families in that the type of interligand interactions strongly depends on the substitution on silicon. They can be classified either as usual dihydrogen complexes, for example, [Fe(Cp)(OC)(SiMe(2)Cl)(eta(2)-H(2))], or as compounds with nonclassical H--Si interactions, for example, [Fe(Cp)(OC)(H)(2)(SiMe(3))] (16). These nonclassical interligand interactions are characterized by increased negative J(H,Si) (e.g. -27.5 Hz) and increased J(H,H) (e.g. 67.7 Hz).     

A crossed molecular beam study on the formation of hexenediynyl radicals (H(2)CCCCCCH; C(6)H(3) (X(2)A')) via reactions of tricarbon molecules, C(3)(X(1)Sigma(g)(+)), with allene (H(2)CCCH(2); X(1)A(1)) and methylacetylene (CH(3)CCH; X(1)A(1))

Crossed molecular beams experiments have been utilized to investigate the reaction dynamics between two closed shell species, i.e. the reactions of tricarbon molecules, C(3)(X(1)Sigma(g)(+)), with allene (H(2)CCCH(2); X(1)A(1)), and with methylacetylene (CH(3)CCH; X(1)A(1)). Our investigations indicated that both these reactions featured characteristic threshold energies of 40-50 kJ mol(-1). The reaction dynamics are indirect and suggested the reactions proceeded via an initial addition of the tricarbon molecule to the unsaturated hydrocarbon molecules forming initially cyclic reaction intermediates of the generic formula C(6)H(4). The cyclic intermediates isomerize to yield eventually the acyclic isomers CH(3)CCCCCH (methylacetylene reaction) and H(2)CCCCCCH(2) (allene reaction). Both structures decompose via atomic hydrogen elimination to form the 1-hexene-3,4-diynyl-2 radical (C(6)H(3); H(2)CCCCCCH). Future flame studies utilizing the Advanced Light Source should therefore investigate the existence of 1-hexene-3,4-diynyl-2 radicals in high temperature methylacetylene and allene flames. Since the corresponding C(3)H(3), C(4)H(3), and C(5)H(3) radicals have been identified via their ionization potentials in combustion flames, the existence of the C(6)H(3) isomer 1-hexene-3,4-diynyl-2 can be predicted as well.     

Hexaaquacobalt(II) bis(hypophosphite) and hexaaquacobalt(II)/nickel(II) bis(hypophosphite)

The title compounds, hexa­aqua­cobalt(II) bis­(hypophosphite), [Co(H₂O)₆](H₂­PO₂)₂, and hexa­aqua­cobalt(II)/nickel(II) bis(hypophosphite), [Co_0.5Ni_0.5(H₂O)₆](H₂PO₂)₂, are shown to adopt the same structure as hexa­aqua­magnesium(II) bis­(hypophosphite). The packing of the Co(Ni) and P atoms is the same as in the structure of CaF₂. The Co^II(Ni^II) atoms have a pseudo‐face‐centred cubic cell, with a = b～ 10.3 Å, and the P atoms occupy the tetrahedral cavities. The central metal cation has a slightly distorted octahedral coordination sphere. The geometry of the hypophosphite anion in the structure is very close to ideal, with point symmetry mm2. Each O atom of the hypophosphite anion is hydrogen bonded to three water mol­ecules from different cation complexes, and each H atom of the hypophosphite anion is surrounded by three water mol­ecules from further different cation complexes.     

Phosphine-boranes as bidentate ligands: formation of [8,8-eta(2)-(eta(2)-(BH(3)).dppm)-nido-8,7-RhSB(9)H(10)] and [9,9-eta(2)-(eta(2)-(BH(3)).dppm)-nido-9,7,8-RhC(2)B(8)H(11)] from [8,8-(eta(2)-dppm)-8-(eta(1)-dppm)-nido-8,7-RhSB(9)H(10)] and [9,9-(eta(2)-dppm)-9-(eta(1)-dppm)-nido-9,7,8-RhC(2)B(8)H(11)], respectively

The two clusters [8,8-(eta(2)-dppm)-8-(eta(1)-dppm)-nido-8,7-RhSB(9)H(10)] (1) and [9,9-(eta(2)-dppm)-9-(eta(1)-dppm)-nido-9,7,8-RhC(2)B(8)H(11)] (2) (dppm = PPh(2)CH(2)PPh(2)), both of which contain pendant PPh(2) groups, react with BH(3).thf to afford the species [8,8-eta(2)-(eta(2)-(BH(3)).dppm)-nido-8,7-RhSB(9)H(10)] (3) and [9,9-eta(2)-(eta(2)-(BH(3)).dppm))-nido-9,7,8-RhC(2)B(8)H(11)] (4), respectively. These two species are very similar in that they both contain the bidentate ligand [(BH(3)).dppm], which coordinates to the Rh center via a PPh(2) group and also via a eta(2)-BH(3) group. Thus, the B atom in the BH(3) group is four-coordinate, bonded to Rh by two bridging hydrogen atoms, to a terminal H atom, and to a PPh(2) group. At room temperature, the BH(3) group is fluxional; the two bridging H atoms and the terminal H atom are equivalent on the NMR time scale. The motion is arrested at low temperature with DeltaG++ = ca. 37 and 42 kJ mol(-1), respectively, for 3 and 4. Both species are characterized completely by NMR and mass spectral measurements as well as by elemental analysis and single-crystal structure determinations.     

New layered materials: syntheses, structures, and optical properties of K(2)TiCu(2)S(4), Rb(2)TiCu(2)S(4), Rb(2)TiaAg(2)S(4), Cs(2)TiAg(2)sS(4), and Cs(2)TiCu(2)Se(4)

The new compounds K(2)TiCu(2)S(4), Rb(2)TiCu(2)S(4), Rb(2)TiAg(2)S(4), Cs(2)TiAg(2)S(4), and Cs(2)TiCu(2)Se(4) have been synthesized by the reactions of A(2)Q(3) (A = K, Rb, Cs; Q = S, Se) with Ti, M (M = Cu or Ag), and Q at 823 K. The compounds Rb(2)TiCu(2)S(4), Cs(2)TiAg(2)S(4), and Cs(2)TiCu(2)Se(4) are isostructural. They crystallize with two formula units in space group P4(2)/mcm of the tetragonal system in cells of dimensions a = 5.6046(4) A, c = 13.154(1) A for Rb(2)TiCu(2)S(4), a =6.024(1) A, c = 13.566(4) A for Cs(2)TiAg(2)S(4), and a =5.852(2) A, c =14.234(5) A for Cs(2)TiCu(2)Se(4) at 153 K. Their structure is closely related to that of Cs(2)ZrAg(2)Te(4) and comprises [TiM(2)Q(4)(2)(-)] layers, which are separated by alkali metal atoms. The [TiM(2)Q(4)(2)(-)] layer is anti-fluorite-like with both Ti and M atoms tetrahedrally coordinated to Q atoms. Tetrahedral coordination of Ti(4+) is rare in the solid state. On the basis of unit cell and space group determinations, the compounds K(2)TiCu(2)S(4) and Rb(2)TiAg(2)S(4) are isostructural with the above compounds. The band gaps of K(2)TiCu(2)S(4), Rb(2)TiCu(2)S(4), Rb(2)TiAg(2)S(4), and Cs(2)TiAg(2)S(4) are 2.04, 2.19, 2.33, and 2.44 eV, respectively, as derived from optical measurements. From band-structure calculations, the optical absorption for an A(2)TiM(2)Q(4) compound is assigned to a transition from an M d and Q p valence band (HOMO) to a Ti 3d conduction band.