球形微粒Co3O4电极催化氧化硫离子

尝试用氨蒸发诱导合成方法在石墨小片上生长球形Co₃O₄微粒, 并用其制备电极且进行S^2-的电化学氧化研究. 用极化曲线、恒电位技术等电化学方法考察了Co₃O₄电极对S^2-的电化学氧化的催化性能, 发现Co₃O₄电极对电化学氧化S^2-具有优异的催化性能, 极大地促进了-0.40 V 附近S^2-向含硫的酸根离子和低级多硫离子的转变, 电流密度最大可以达到580 mA·cm^-2. 恒电位极化表明电极的电催化稳定性良好; 电化学阻抗谱(EIS)测试显示Co₃O₄在碱性S^2-电解液中的电荷转移电阻很小, 这从电化学动力学角度解释了它对S^2-具有良好的催化性能.     

N′-乙基-N-哌嗪基二硫代氨基甲酸铜(Ⅱ)配合物Cu(S2CNC4H8NC2H5)2的晶体结构及谱学研究

合成了标题化合物Cu(S₂CNC₄H₈NC₂H₅)₂,得到深棕色柱状晶体。晶体属三斜晶系,空间群为P1。中心Cu(Ⅱ)离子分别与来 自2个N′-乙基-N-哌嗪基二硫代氨基甲酸的4个硫原子配位,形成略微扭曲的平面四方配位构型。4个Cu-S键的键长范围0.220 10(11)～0.220 34(13) nm;Cu-S键的FT-Raman伸缩振动峰在134.921 cm^-1;ESR谱表明Cu(Ⅱ)离子处于对称中心;其局部配位构型属于D_2h群;热分析表明标题化合物在753.15 ℃时分解为金属Cu。     

CexPr1-xO2-δ复合氧化物的XRD和Raman表征

A series of Ce_xPr_1-xO_2-δ mixed oxides were synthesized by sol-gel method and characterized by Raman and XRD techniques. When x value was changed from 1.0 to 0.5, only a cubic phase CeO₂ was observed. The samples were very well crystallized on decreasing x from 0.50 to 0.99. For Ce_xPr_1-xO_2-δ samples 465 cm^-1 and 1 150 cm^-1 Raman peaks are attributed to the Raman active F_2g mode of CeO₂. The broad peak at about 570 cm^-1 in the region of 0.3 ≤x≤ 0.99 can be linked to lattice defects resulting in oxygen vacancies. The new band at about 195 cm^-1 may be attributed to the asymmetric vibration caused by the formation of oxygen vacancies. Calcination temperatures had great effect on the peak intensity for CeO₂ but less effect on Ce_0.8Pr_0.2O_2-δ in Raman spectra. It might be due to the transformation of the colors for the mixed oxides, the insertion of Pr atom into the ceria lattice could enhance the sintering resistance and thermal stability of the mixed oxides.     

多孔纳米Ce-M-O (M＝Pr, La)粉末的微波诱导燃烧合成及其表征

使用Ce(NO₃)₃•6H₂O, Pr(NO₃)₃•6H₂O, La(NO₃)₃•6H₂O, 尿素为原料, 利用微波引诱燃烧法合成了多孔纳米Ce-M-O (M＝Pr, La)固溶体. 使用XRD, X光电子能谱仪(XPS), Raman光谱仪, 红外光谱仪(FT-IR), 透射电镜(TEM), 场发射扫描电镜(FE-SEM)等仪器对纳米粉体进行了表征. XRD分析显示Ce-M-O粉体的粒径在20～50 nm之间, 且所有样品均具有萤石结构. XPS证明在Ce-Pr-O固溶体中Pr以＋3和＋4两种形式存在. Raman光谱表明随着M^3＋的掺杂, 在CeO₂晶格中产生氧缺陷, 且缺陷浓度随掺杂量增加不断提高. 红外光谱证明Ce—O键的吸收峰在1400 cm^－1左右, 且由于M^3＋的掺杂在2346 cm^－1的吸收峰消失. TEM照片说明样品具有类盘状的网络纳米微晶结构. 扫描图像说明产物具有多孔的外貌特征, 且孔径分布在2～40 nm之间.     

固体电解质La2-xCaxMo1.7W0.3O9-δ(0≤x≤0.2)的合成、表征及电性能

在氧离子导体La₂Mo_1.7W_0.3O₉的基础上，采用固相法合成了La位掺杂的Ca系列新型氧化物La_2-xCa_xMo_1.7W_0.3O_9-δ(0≤x≤0.2)。通过XRD、Raman和XPS等手段对化合物结构进行表征，交流阻抗谱测试其电性能。结果表明：掺杂离子Ca²⁺的半径小于基质离子La³⁺的半径导致晶格收缩；Ca的掺杂在La₂Mo_1.7W_0.3O₉自身内置氧空位的基础上增加了额外的氧空位，提高了氧离子导体的电导率，550 ℃电导率由0.79 × 10^-4 S·cm^-1 (x=0.0)增加到1.5 × 10^-4 S·cm^-1 (x=0.16，0.2)，电导率增加89.9%。     

基于二茂铁羧酸配体的镉配合物的合成及结构研究

以二茂铁甲酸根FcCOO^-(Fc=(η⁵-C₅H₅)Fe(η⁵-C₅H₄))为主要配体，合成了3个新的配合物[Na₂Cd( μ₃-η²-FcCOO^-)₂(μ₂-η²-FcCOO^-)₂(CH₃OH)₂]_n (1)、[Cd(phen)(FcCOO^-)(η²-FcCOO)(H₂O)](phen=邻菲咯啉) (2)、[Cd(Det)(η²-FcCOO^-)(FcCOO^-)](H₂O)₂(Det=二乙撑三胺) (3)。测定了配合物的晶体结构。配合物1为单斜晶系，C2/c空间群，二茂铁甲酸根采用μ₃-η²-FcCOO^-和μ₂-η²-FcCOO^-的配位方式将Cd²⁺和Na⁺连接成一维无限链状结构。配合物2和3均为单核结构，单斜晶系，P2₁/c空间群，二茂铁甲酸根都采用 FcCOO^-和η²-FcCOO^-的方式配位。2中phen以双齿螯合形式配位，水分子参与配位，中心镉离子配位数为6。3中Det以三齿螯合形式配位，中心镉离子配位数也为6，但水分子未参与配位。     

Ti-MWW分子筛正弦孔道内骨架钛物种的结构和红外振动光谱的理论计算

应用密度泛函理论计算,研究了Ti-MWW分子筛10元环正弦孔道内骨架钛物种的结构和振动光谱。计算采用基于36T簇模型的B3LYP/6-31G(d,p)方法,确定了[Ti(OSi)₄]物种优先落位于T3位,在924~987cm^-1区域内存在3个振动峰,都属于以Ti为正四面体中心分布的4个Ti-O-Si键的协同伸缩振动,其中958cm^-1的振动强度较大,属于[Ti(OSi)₄]的特征频率。T2和T8位上钛物种不出现该特征峰。Ti(Ⅳ)中心上吸附一个水分子形成五配位配合物,其特征振动频率没有变化。[Ti(OSi)₄]物种进一步水解形成[Ti(OSi)₃OH]物种,其Ti-O-Si的特征振动蓝移到969cm^-1。此外,还考察了Ti-MWW分子筛中可能存在的骨架硼以及羟基巢的结构和振动光谱,计算频率与已有文献数据相符。     

1R，3S-1，2，2-三甲基-1，3-环戊二胺为配体的铂(Ⅱ) 配合物的合成、表征和抗肿瘤活性

本文合成了9种含有由天然D(+)-樟脑衍生的1R，3S-1，2，2-三甲基-1，3-环戊二胺(A)为配体的铂(Ⅱ)配合物[Pt(Ⅱ)AX]{其中，X=(CH₂)₃C(COO^-)₂(1，1-环丁烷二羧酸根)，2CH₃OCH₂COO^-，2CH₃CH₂OCH₂COO^-，2CH₃(CH₂)₃OCH₂COO^-，[OCH(CH₃)COO]^2-(乳酸根)，(OCH₂COO)^2-(乙醇酸根)，2CH₃OCH₂CH₂OCH₂COO^-，2CH₃CH₂OCH₂CH₂OCH₂COO^-和2CH₃(CH₂)₃OCH₂CH₂OCH₂COO^-}。通过元素分析、热重分析、红外光谱、¹H核磁共振谱和电喷雾质谱等对配合物进行了表征。体外生物活性测试表明，部分配合物对A549人肺癌细胞和HCT-116人结肠癌细胞具有较强的抗肿瘤活性。     

室温离子液体FeCl3-BPC体系的研究

利用差示扫描量热法(DSC)建立了无水三氯化铁和氯化正丁基吡啶(BPC)二元体系相图. 依据相图, FeCl₃和BPC形成室温离子液体的窗口是x＝0.26～0.58; 室温离子液体的深度是80 ℃. 利用UHF/6-31G^*对FeCl₃, FeCl₄^－, Fe₂Cl₇^－等配合物的几何结构、键长、能量和Raman频率进行优化, 从头算和Raman光谱证实了相图中FeCl₃摩尔分数x＝0.50处有稳定化合物存在, FeCl₄^－是主要阴离子; x＝0.67处, FeCl₄^－, Fe₂Cl₇^－是主要阴离子.     

有机磺酸根阴离子调控的[Co (pytpy)2]2+自旋交叉化合物

本文报道了2例由有机磺酸根阴离子调控的单核钴(Ⅱ)配合物[Co(pytpy)₂](2-NH₂-1-NS)₂·MeOH·H₂O (1)和[Co(pytpy)₂](4-NH₂-1-NS)₂·H₂O (2)的合成、晶体结构和磁性,其中pytpy=4''-(4-吡啶基)-2,2''∶6'',2″-三联吡啶,2-NH₂-1-NS^-=2-氨基-1-萘磺酸根离子,4-NH₂-1-NS^-=4-氨基-1-萘磺酸根离子。单晶X射线衍射分析表明,这2例配合物均由[Co(pytpy)₂]²⁺阳离子、有机磺酸根阴离子和结晶溶剂分子组成。其中,阴离子2-NH₂-1-NS^-和4-NH₂-1-NS^-仅在磺酸根和氨基的相对位置上有所不同。有趣的是,具有处于邻位的磺酸根和氨基的2-NH₂-1-NS^-阴离子与[Co(pytpy)₂]²⁺阳离子和溶剂分子形成氢键,而具有处于对位的磺酸根和氨基的4-NH₂-1-NS^-阴离子之间通过氢键形成了二维层状结构。磁测量表明配合物1和2的磁性有很大的不同：配合物1具有可逆的渐变型自旋交叉行为,而化合物2则保持在高自旋态。     

Ein- und zweikernige MoII-Phthalocyaninate(2–): Darstellung und Eigenschaften von Bis(cyano)phthalocyaninato(2–)molybdat(II) und Bis(phthalocyaninato(2–)molybdän(II))

Mono- and Dinuclear Mo^II Phthalocyaninates(2–): Syntheses and Properties of Bis(cyano)phthalocyaninato(2–)molybdate(II) and Bis(phthalocyaninato(2–)molybdenum(II)) Blue diamagnetic bis(phthalocyaninato(2–)molybdenum(II)) is synthezied by reduction of oxophthalocyaninato(2–)molybdenum(IV) with boiling triphenylphosphine. The Mo–Mo stretching vibration ist observed in the resonance Raman spectrum at 374 cm^–1. It is chemically inert and dissolves in conc. sulfuric acid without decomposition. It reacts with molten tetra(n-butyl)ammonium cyanide to yield redbrown paramagnetic bis[tetra(n-butyl)ammonium] biscyanophthalocyaninato(2–)molybdate(II) (μ_eff = 3.15 μ_B; S = 1). The complex salt is very instable and demetallizes in solution. In the extraordinary UV-VIS-NIR spectrum an intense trip-triplet transition at 7780 cm^–1 together with a very structured B region between 14000 and 21000 cm^–1 of comparable absorbance is observed.     

Comparative study of the synthesis of layered transition metal molybdates

Mixed metal oxides (MMOs) prepared by the mild thermal decomposition of layered double hydroxides (LDHs) differ in their reactivity on exposure to aqueous molybdate containing solutions. In this study, we investigate the reactivity of some T-Al containing MMOs (T=Co, Ni, Cu or Zn) towards the formation of layered transition metal molybdates (LTMs) possessing the general formula AT₂(OH)(MoO₄)₂·H₂O, where A=NH₄⁺, Na⁺ or K⁺. The phase selectivity of the reaction was studied with respect to the source of molybdate, the ratio of T to Mo and the reaction pH. LTMs were obtained on reaction of Cu-Al and Zn-Al containing MMOs with aqueous solutions of ammonium heptamolybdate. Rehydration of these oxides in the presence of sodium or potassium molybdate yielded a rehydrated LDH phase as the only crystalline product. The LTM products obtained by the rehydration of MMO precursors were compared with LTMs prepared by direct precipitation from the metal salts in order to study the influence of preparative route on their chemical and physical properties. Differences were noted in the composition, morphology and thermal properties of the resulting products.     

Tetraammonium Diglycinyl‐octamolybdate(VI) Dihydrate, (NH4)4[(NH3CH2CO)2(Mo8O28)] · 2 H2O

The reaction of ammonium heptamolybdate with hydrazine sulfate in an aqueous solution of glycine at room temperature yielded colorless crystals of (NH₄)₄[(NH₃CH₂CO)₂(Mo₈O₂₈)] · 2 H₂O. The crystal is monoclinic, space group C2/c (no. 15), a = 17.234 Å, b = 10.6892 Å, c = 18.598 Å, β = 108.280°, V = 3253.2 ų, Z = 4. The crystal structure contains ammonium cations and isolated octamolybdate(4–) anions, [(NH₃CH₂CO)₂(Mo₈O₂₈)]^4–, with two zwitterionic glycine molecules as ligands.     

Raman Combinations and Stretching Overtones from Water, Heavy Water, and NaCl in Water at Shifts to ca. 7000 cm−1

Photographic Raman spectra were obtained at shifts to ca. 7000 cm^–1 for pure water and for a saturated aqueous solution of NaCl using argon ion laser excitation. Raman spectra were also obtained photoelectrically for H₂O and D₂O between ca. 2500 and ca. 7000 cm^–1 using 248-nm excimer laser excitation and boxcar detection. Overtone and combination assignments are presented for H₂O and D₂O. The first IR OH-stretching overtone from water occurs 215 cm^–1 above the first Raman OH-stretching overtone because the IR overtones are dominated by asymmetric stretching. The second OH-stretching Raman overtone from water is estimated to occur near 10,020 ± 20 cm^–1, with 9950 cm^–1 as a lower limit.     

Reaction of Hg2+ Insertion into Cysteine Pairs Within Bovine Insulin Crystals Followed via Raman Spectroscopy

Chemical modifications of protein crystals may be achieved via soaking of reactants from their precipitating solution, through the solvent channel, into the protein matrix. We describe a Raman microscopy approach to follow mercury insertion into cysteine pairs within protein single crystals, via soaking in an aqueous Hg²⁺ solution. The method has been developed using bovine insulin as the model system. Applying an efficient mercuration protocol, consisting of a first step of disulphide bridge TCEP-induced reduction within the crystal, followed by overnight reaction with a HgCl₂ solution, we obtained Hg-derivative crystals. Raman spectra collected on these derivative crystals, kept in the mother liquor, reveal a characteristic Raman band at 335 cm^?1, which has been assigned to a –S–Hg–S– bridge. The analysis provides Raman-based markers of mercury binding to cysteines, and thus of mercury intoxication.     

Vibrational spectra of molten and aqueous NaClO3 and KClO3

Raman spectra of molten NaClO₃ and KClO₃ and of aqueous solutions of these salts were measured over the frequency interval from 50 to 1200 cm⁻¹|. Infrared emission spectra of the molten chlorates and of chlorate-nitrate mixtures were recorded, and absorption spectra of aqueous sodium and potassium chlorate also were determined. The ν₃(e) and ν₄(e) modes of ClO⁻₃ were split in the molten salt and aqueous solution spectra, and a single, weak band was observed between ca. 80 and 200 cm⁻ in the Raman spectra of molten NaClO₃ and KClO₃.     

X–ray Single Crystal Structure and Raman Spectrum of Ammonium Hexafluoroarsenate

The structure of ammonium hexafluoroarsenate, NH₄AsF₆, has been determined by X‐ray diffraction using a single crystal grown from saturated solution in anhydrous HF. NH₄AsF₆ crystallizes rhombohedral with the KOsF₆ structure type, with a = 7.459(3) Å, c = 7.543(3) Å (at 200 K), Z = 3, space group (No. 148). No phase transition was observed in the 100 K–296 K temperature range. The structure is dominated by regular AsF₆ octahedra and disordered NH₄⁺ cations. Raman spectrum of a single crystal of NH₄AsF₆ shows the bands at 372 cm^?1, 572 cm^?1, 687 cm^?1 (AsF₆^?) and at 3240 cm^?1 and 3360 cm^?1 (NH₄⁺).     

Raman Study of the Pulsed Discharge Effect on Molecular Relaxation in Aqueous Sodium Nitrate

The high-voltage pulsed electric discharge effect (HPED activation) on the Raman spectra of a saturated aqueous solution of sodium nitrate (NaNO₃/H₂O) in the region of the totally symmetric vibration ₁(A) of the NO _- ³ anion has been studied. The temperature dependences of the width and frequency of the corresponding spectral line are examined.     

Characterization of silica-supported molybdenum catalysts by ESR, XPS and thiophene hydrodesulfurization

Two Mo/SiO₂ samples have been prepared by impregnation of silica gel with aqueous solution of molybdophosphoric heteropoly acid or ammonium heptamolybdate. The catalysts were studied by ESR and IR spectroscopy, X-ray diffraction, and XPS. Their activity was measured in the reaction of thiophene hydrodesulfurization. The silica-supported P–Mo heteropoly acid, with a preserved Keggin structure of the heteropoly anion and sulfided by H₂S, exhibited two times higher steady conversion in comparison with ammonium heptamolybdate supported on silica at pH=11 and calcined and sulfided at 500°C.     

Raman spectra of single crystal Li2SeO4

The room temperature polarized Raman spectra of single crystal Li₂SeO₄ are assigned using a factor group analysis. The internal optic modes of the selenate ion are responsible for Raman bands from 920 to 440 cm⁻¹, the translational optic modes of the lithium occur in the interval from 444 to 290 cm⁻¹ and the external optic modes of the selenate ion are found between 210 and 70 cm⁻¹. The symmetry-based assignments of these bands are discussed.