二氧化钛系列光催化剂的拉曼光谱

采用溶胶-凝胶法制备了TiO₂粉体和薄膜光催化剂.使用FT-Raman光谱和激光共聚焦拉曼光谱研究了粉体和薄膜的拉曼光谱,探讨了热处理条件、Fe³⁺掺杂和以硅胶为载体的薄膜化所引起的TiO₂结构变化.结果表明,TiO₂在350℃存在由无定形向锐钛矿相的转变,600℃下存在锐钛矿相向金红石相的转变,750℃下完全转变为金红石相;掺杂会引起TiO₂的晶格畸变,导致拉曼谱峰宽化;以硅胶为载体的TiO₂负载薄膜的部分拉曼谱峰与粉体相比,有一定的位移和宽化.     

纳米金属微粒M-Al2O3介孔复合薄膜的光谱特性

用电化学方法合成了纳米金属微粒M(M=Au,Ag,Cu,Co,Ni,CuAg)-Al₂O₃介孔复合薄膜,并研究了其在近紫外至可见光波范围的光谱特性.研究结果表明,复合薄膜的光吸收峰位置与纳米金属微粒和Al₂O₃介孔薄膜的介电常数有关,且随着膜层中纳米金属微粒复合量的增加,大幅度向红外波段移动;通过共沉积的方法形成的合金微粒复合膜也能使吸收边发生移动.同时还发现Ag-Al₂O₃,Au-Al₂O₃介孔复合薄膜分别在波长为360,500nm处存在等离子体共振吸收峰.     

衬底温度对强流脉冲离子束烧蚀沉积类金刚石薄膜化学结构的影响

采用强流脉冲离子束(High-intensitypulsedionbeam,HIPIB)烧蚀技术在Si(100)基体上沉积类金刚石(Diamond-likecarbon,DLC)薄膜,衬底温度的变化范围为298～673K.利用Raman光谱和X射线光电子谱(XPS)对DLC薄膜的化学结合状态与衬底温度之间关系进行研究.薄膜XPS的C1s谱的解谱分析得出薄膜中含有sp³C(结合能为285.5eV)和sp²C(结合能为284.7eV)成分,根据解谱结果评价薄膜中sp³C含量.根据XPS分析可知,衬底温度低于473K时,sp³C的含量大约为40%左右;随着沉积薄膜时衬底温度的提高,sp³C的含量降低,由298K时的42.5%降到673K时的8.1%,从573K开始发生sp³C向sp²C转变.Raman光谱表明,随着衬底温度的提高,Raman谱中G峰的峰位靠近石墨峰位,G峰的半峰宽降低,D峰与G峰的强度比I_D/I_G增大,说明薄膜中的sp³C的含量随衬底温度增加而减少.     

气液界面法组装的Ni3(HITP)2电致变色薄膜及其性能

由于缺乏可控的成膜技术,三亚苯类金属有机框架(MOFs)材料的应用受到了限制。我们在气液界面组装了不同厚度的Ni₃(HITP)₂薄膜(HITP^3-=2,3,6,7,10,11-六亚氨基三亚苯),并将制备的薄膜转移到导电玻璃表面。利用X射线衍射(XRD)、场发射透射电子显微镜(FETEM)、场发射扫描电镜(FESEM)、X射线光电子能谱(XPS)和拉曼光谱对样品的晶体结构、微观形貌和元素组成进行表征,采用紫外可见分光光度计以及电化学工作站对Ni₃(HITP)₂薄膜的电化学和电致变色性能进行了研究和表征。结果表明,得益于Ni₃(HITP)₂电致变色薄膜的多孔结构和与电解液良好的接触,所得薄膜电极N-20具有较短的着色响应时间/褪色响应时间(0.6/0.7 s),且着色效率可达530 cm²·C^-1;而N-50具有较大的光调制范围(740 nm,70%)。     

一种在室温合成具有宽带隙CdS的简单方法

采用简单的磁控溅射方法, 在室温合成了CdS多晶薄膜. 在溅射CdS多晶薄膜过程中, 分别在Ar 气中通入0%、0.88%、1.78%、2.58%和3.40% (体积分数, φ)的O₂, 得到不同O含量的CdS多晶薄膜. 通过X射线衍射仪、拉曼光谱仪、扫描电子显微镜、X射线光电子能谱仪、紫外-可见光谱仪对得到的CdS多晶薄膜进行表征.分析结果表明: O的掺入能得到结合更加致密, 晶粒尺寸更小的CdS多晶薄膜; 与溅射气体中没有O₂时制备的CdS多晶薄膜的光学带隙(2.48 eV)相比, 当溅射气体中O₂的含量为0.88%和1.78% (φ)时, 制备得到的CdS多晶薄膜具有更大的光学带隙, 分别为2.60和2.65 eV; 而当溅射气体中O₂的含量为2.58%和3.40% (φ)时, 得到的CdS光学带隙分别为2.50 和2.49 eV, 与没有掺杂O的CdS的光学带隙(2.48 eV)相当; 当溅射气体中O₂的含量为0.88% (φ)时, 制备的CdS多晶薄膜具有最好的结晶质量. 通过磁控溅射方法, 在溅射气体中O₂含量为0.88% (φ)条件下制备的CdS多晶薄膜表面沉积了CdTe 多晶薄膜并在CdCl₂气氛中进行了高温退火处理, 对退火前后的CdTe多晶薄膜进行了表征. 表征结果显示: CdS中掺入O能得到结合更紧密、退火后晶粒尺寸更大的CdTe多晶薄膜. 通过磁控溅射方法, 在CdS制备过程中于Ar 中掺入O₂, 在室温就能得到具有更大光学带隙的CdS多晶薄膜, 该方法是一种简单和有效的方法, 非常适用于大规模工业化生产.     

木质纤维类生活垃圾热解过程矿物质和碳结构的演化规律

使用水平管式炉,在不同热解温度(500~1 000 ℃)条件下对废纸屑和樟树叶两种木质纤维类生活垃圾进行了热解实验,分别采用X射线衍射(XRD)和拉曼光谱研究了样品所含矿物质和碳结构随热解温度的变化。结果表明,废纸屑和樟树叶含有的主要矿物分别为方解石和草酸钙,在500 ℃之前草酸钙全部转化为方解石,焦样中的方解石在800 ℃以后逐渐分解并形成生石灰。拉曼光谱对生活垃圾焦的碳结构变化非常敏感,低温热解时生活垃圾的大分子结构发生缩合和解聚,产生了孤立sp²碳原子,导致峰参数D1峰半高宽和峰面积比值I_D1/I_G逐渐增大;高温热解时晶体sp²碳原子增多,导致D1峰半高宽和I_D1/I_G逐渐减小。焦样的碳结构有序度随热解温度升高先降低后提高。     

ZnO薄膜的XPS价带谱研究

用MOCVD方法在Al₂O₃衬底c面生长ZnO薄膜,用XPS对薄膜进行了测量.结果显示,与O_1s和Zn_2p态相比,Zn_3d态有更大的化学位移,可用于更有效地分析ZnO薄膜变化;随着Zn_3d+Zn_4s态和Zn_3d态电子与O_2p态电子耦合的增强,Zn_3d态电子的结合能变大;二乙基锌(DEZn)源温是影响ZnO成键的重要因素.     

WO3/PANI核壳结构反蛋白石薄膜的电致变色性能

采用连续离子层吸附法在反蛋白石结构三氧化钨(IO-WO₃)薄膜表面引入导电聚合物聚苯胺(PANI)层, 制备了独特的WO₃/PANI核壳结构反蛋白石薄膜(IO-WO₃/PANI). 探究了IO-WO₃/PANI薄膜的形貌、 组成和电化学行为. 结果表明, 当电位扫描范围为-0.6~1.0 V时, IO-WO₃/PANI复合膜在不同电压状态下会呈现出4种不同的颜色, 分别为蓝色(1.0 V)、 绿色(0.2 V)、 浅绿色(0 V)和蓝紫色(-0.6 V). 与IO-WO₃薄膜相比, IO-WO₃/PANI复合膜的电致变色性能显著提高, 其着色与退色响应时间分别为3.8和6.14 s, 变色效率(CE)值为201.1 cm²/C. 电致变色性能的改善主要归因于WO₃与PANI形成给体-受体体系和核壳反蛋白石等级孔结构, 使得离子快速扩散, 并为电荷转移反应提供更大的表面积. 研究结果表明, IO-WO₃/PANI核壳结构反蛋白石薄膜是一种潜在的多色电致变色材料, 具有广阔的应用前景.     

激光拉曼光谱研究NiMoP浸渍液活性组分的结构 Ⅱ.不同有机添加剂的影响

采用激光拉曼光谱（LRS）技术对添加有乙二醇和柠檬酸的NiMoP浸渍液和用该浸渍液制备的NiMoP/Al₂O₃催化剂进行了表征,研究了乙二醇和柠檬酸含量对NiMoP浸渍液及浸渍过程中活性相组成、结构的影响。结果表明,乙二醇使NiMoP(0.063)浸渍液中H_{x\[PMo11O39\]⁽7-x)- 或Hx\[PMo9O31\]⁽3-x)-及Hx\[PMo12O40\]⁽3-x)- 杂多阴离子结构转化成Hx\[P2Mo5O23\]⁽6-x)- 结构,而柠檬酸能保持NiMoP(0.063)浸渍液中Hx\[P2Mo5O23\]⁽6-x)-、Hx\[PMo11O39\]⁽7-x)- 或Hx\[PMo9O31\]⁽3-x)-及Hx\[PMo12O40\]⁽3-x)-杂多阴离子结构共存,但导致Hx\[P2Mo5O23\]⁽6-x)-含量降低,Hx\[PMo12O40\]⁽3-x)-含量升高。相对乙二醇而言,柠檬酸有机添加剂能够更有效地阻止浸渍过程中各杂多阴离子结构在载体氧化铝孔道中的分解。}     

钠和钾离子对磷酸二氢根拉曼光谱的影响

磷酸二氢根(H₂PO^-₄)溶液在生物缓冲、分子识别、晶体生长等方面有着重要的研究价值。 本文以KH₂PO₄(KDP)和NaH₂PO₄(NaDP)溶液为研究对象,利用原位微区拉曼光谱研究钠离子和钾离子对H₂PO^-₄溶液团簇聚合及化学键振动的影响,讨论单价阳离子(K⁺,Na⁺)的差异、溶液浓度对H₂PO^-₄拉曼位移变化和成核诱导时间的影响。 结果表明,拉曼位移变化、成核诱导时间随阳离子溶液电负性的增加、浓度的降低而增大。 在拉曼光谱中观察到P(OH)₂和PO₂振动峰在成核过程中发生偏移,表明由氢键作用导致的团簇构型逐渐稳定,化学键逐渐增强,深化溶液结晶过程中对溶液结构和化学键的理解。     

An ab initio close-coupling calculation of the lower vibrational energies of the HCl dimer

We have previously determined an analytical ab initio six-dimensional potential energy surface for the HCl dimer, and in the present paper we use this potential, with the HCl bond lengths held fixed, in a full (four-dimensional) close-coupling calculation to determine the energies of the lowest 24 vibrational states. These vibrational states involve the intermolecular stretch ν₄, the trans-bend tunneling vibration ν₅, and the torsion ν₆. The highest of the 24 levels is the (ν₄ν₅ν₆)=(111) state, for which we calculate an energy of 200 cm⁻¹ above the (000) state. As well as determining tunneling energies up to 5ν₅=183 cm⁻¹, we determine ν₄=49 cm⁻¹, 2ν₄=93 cm⁻¹, 3ν₄=134 cm⁻¹, 4ν₄=172 cm⁻¹, ν₆=137 cm⁻¹ and ν₄+ν₆=178 cm⁻¹, together with tunneling energies in all these states. Making allowance for the HCl stretching zero-point energy we determine the dissociation energy D₀ as 390 cm⁻¹ on this analytical surface. We determine that below 300 cm⁻¹ there are 72 vibrational (J=K=0) states, and below dissociation there are 162 vibrational (J=K=0) states, for this potential surface.     

Infrared laser magnetic resonance spectroscopy of OD at 118.8, 96.5 and 215.4μ m

Zeeman spectral data are presented for the ²Π_3/2: J = _7/2 → J= _9/2,²Π_3/2: J= _7/2→²Π_1/2:J= _5/2 and²Π_3/2 J= _3/2→ J = _5/2 transitions in OD. Data for the ²Π_3/2. J=3/2→ J= 5/2 and ²Π_3/2 J= _5/2 → ²Π_l/2 : J= _3/2 transitions in OH, taken under similar conditions, are included.     

The tungsten-tungsten triple bond---18. Bridging and terminal allyl ligands in complexes of the formula W2(R)2(NMe2)4, where R = C3H5 and C4H7

The reaction between RMgCl (two equivalents) and 1,2-W₂Cl₂(NMe₂)₄ in hydrocarbon solvents affords the compounds W₂R₂(NMe₂)₄, where R = allyl and 1− and 2-methyl-allyl. In the solid state the molecular structure of W₂(C₃H₅)₂(NMe₂)₄ has C₂ symmetry with bridging allyl ligands and terminal W---NMe₂ ligands. The W---W distance 2.480(1) Å and the C---C distances, 1.47(1) Å, imply an extensive mixing of the allyl π-MOs with the WW π-MOs, and this is supported by an MO calculation on the molecule W₂(C₃H₅)₂(NH₂)₄ employing the method of Fenske and Hall. The most notable interaction is the ability of the (WW)⁶⁺ centre to donate to the allyl π^*-MO (π₃). This interaction is largely responsible for the long W---W distance, as well as the long C---C distances, in the allyl ligand. The structure of the 2-methyl-allyl derivative W₂(C₄H₇)₂(NMe₂)₄ in the solid state reveals a gauche-W₂C₂N₄ core with W---W = 2.286(1) Å and W---C = 2.18(1) Å, typical of WW and W---C triple and single bonds, respectively. In solution (toluene-d₈) ¹H and ¹³C NMR spectra over a temperature range −80°C to +60°C indicate that both anti- and gauche- W₂C₂N₄ rotamers are present for the 2-methyl-allyl derivative. In addition, there is a facile fluxional process that equilibrates both ends of the 2-methyl-allyl ligand on the NMR time-scale. This process leads to a coalescence at 100°C and is believed to take place via an η³-bound intermediate. The 1-methyl-allyl derivative also binds in an η¹ fashion in solution and temperature-dependent rotations about the W---N, W---C and C=C bonds are frozen out at low temperatures. The spectra of the allyl compound W₂(C₃H₅)₂(NMe₂)₄ revealed the presence of two isomers in solution—one of which can be readily reconciled with the presence of the bridging isomer found in the solid state while the other is proposed to be W₂(η³-C₃H₅)₂(NMe₂)₄. The compound W₂R₂(NMe₂)₄ where R = 2,4-dimethyl- pentadiene was similarly prepared and displayed dynamic NMR behaviour explainable in terms of facile η¹ = η³ interconversions.     

Synthesis of Re-Ru heterobimetallic polyhydride complexes. Study of the influence of ligands bonded to the monometallic precursors on the nature of the isolated binuclear complexes

The reaction of K[H₆ReL₂] with [RuHCl(CO)(PPh₃)_3−x {P(OPrⁱ}₃)_x](L₂ = (PMePh₂)₂, dppe, (AsPh₃)₂, or (PPh₃)₂; x = 0, 1 or 2) leads to [L₂(CO)HRe(μ-H)₃RuH(PPh₃)_2−y{P(OPrⁱ)₃}_y] (x = 0 or 1, Y = 0; X = 2, Y = 1(L₂ = PPh₃)) in a first step. Under the reaction conditions most of these complexes react rapidly with the liberated phosphine giving [L₂(CO)Re(μ-H)₃Ru(PPh₃)_3−y- {P(OPrⁱ)₃}_y] (L₂ = (PMePh₂)₂ or dppe, Y = 0; L₂ = (PPh₃)₂, Y = 1) as the only iso complexes. The structure of [(PMePh₂)₂(CO)Re(μ-H)₃Ru(PPh₃)₃] has been establishedby X-ray structure analysis. The complex [(PPh₃)₂(CO)Re(μ-H)₃Ru(PPh₃)₂(P(OPrⁱ)₃)] reacts with molecular hydrogen under pressure to generate [L₂(CO)HRe(μ-H)₃RuH(PPh₃)(P(OPrⁱ)₃) as the sole product.     

Reactions of tetrakis(trifluoromethyl) diphosphine and bis(trifluoromethyl) phosphine with ruthenium carbonyl clusters; X-ray structure of tetraruthenium carbonyl cluster derivatives

Reaction of [Ru₃(CO)₁₂ with (CF₃)₂P---P(CF₃)₂ in p-xylene at 140°C yielded the compounds [Ru₄(CO)₁₃{μ-P(CF₃)₂}₂] (1), [Ru₄(CO)₁₄{μ-P(CF₃)₂}₂] (2) and [Ru₄(CO)₁₁{μ-P(CF₃)₂}₄] (3). Reaction with [(μ-H)₄Ru₄(CO)₁₂] under similar conditions yielded [(μ-H)₃Ru₄(CO)₁₂{μ-P(CF₃)₂}] (4). All four compounds have been characterised by X-ray crystallography. The fluxional behaviour of the hydrides in 4 has also been studied by variable-temperature NMR spectroscopy. Compounds 1, 2 and 4 were also obtained from the reactions of Ru₃(CO)₁₂ with (CF₃)₂PH in dichloromethane at 80°C.     

Study of the N2 bΠu state via 1 + 1 multiphoton ionization

Medium-resolution spectra of the N₂ b¹Π_u-X¹Σ_g⁺ band system were recorded by 1 + 1 multiphoton ionization. In the spectra we found different linewidths for transitions to different vibrational levels in the b ¹Π_u state: Δν₀ = 0.50 ± 0.05 cm⁻¹, Δν₁ = 0.28 ± 0.02 cm⁻¹, Δν₂ = 0.65 ± 0.06 cm⁻¹, Δν₃ = 3.2 ± 0.5 cm⁻¹, Δν₄ = 0.60 ± 0.07 cm⁻¹, and Δν₅ = 0.28 ± 0.02 cm⁻¹. From these linewidths, predissociation lifetimes τ_ν were obtained: τ₀ = 16 ± 3 ps, τ₁ > 150 ps, τ₂ = 10 ± 2 ps, τ₃ = 1.6 ± 0.3 ps, τ₄ = 9 ± 2 ps, and τ₅ > 150 ps. Band origins and rotational constants for the b ¹Π_uν = 0 and 1 levels were determined for the ¹⁴N₂ and ¹⁴N¹⁵N molecules.     

Organometallic complexes for nonlinear optics: Part 32: Synthesis, optical spectroscopy and theoretical studies of some osmium alkynyl complexes

The complexes trans-[Os(CCPh)Cl(dppe)₂] (1), trans-[Os(4-CCC₆H₄CCPh)Cl(dppe)₂] (2), and 1,3,5-{trans-[OsCl(dppe)₂(4-CCC₆H₄CC)]}₃C₆H₃ (3) have been prepared. Cyclic voltammetric studies reveal a quasi-reversible oxidation process for each complex at 0.36–0.39 V (with respect to the ferrocene/ferrocenium couple at 0.56 V), assigned to the Os^II/III couple. In situ oxidation of 1–3 using an optically transparent thin-layer electrochemical (OTTLE) cell affords the UV–Vis–NIR spectra of the corresponding cationic complexes 1⁺–3⁺; a low-energy band is observed in the near-IR region (11 000–14 000 cm⁻¹) in each case, in contrast to the neutral complexes 1–3 which are optically transparent below 20 000 cm⁻¹. Density functional theory calculations on the model compounds trans-[Os(CCPh)Cl(PH₃)₄] and trans-[Os(4-CCC₆H₄CCPh)Cl(PH₃)₄] have been used to rationalize the observed optical spectra and suggest that the low-energy bands in the spectra of the cationic complexes can be assigned to transitions involving orbitals delocalized over the metal, chloro and alkynyl ligands. These intense bands have potential utility in switching nonlinear optical response, of interest in optical technology.     

Synthesis, structure and hydrogenation catalytic activity of [Ru3(μ3,η-ampy)(μ,η:η-PhC=CHPh)(CO)6(PPh3) (Hampy = 2-amino-6-methylpyridine)

The compound [RU₃(μ₃,η²- -ampy)(μ₃η¹:η²-PhC=CHPh)(CO)₆(PPh₃)₂] (1) (ampy = 2-amino-6-methylpyridinate) has been prepared by reaction of [RU₃(η-H)(μ₃,η²- ampy) (μ,η¹:η²-PhC=CHPh)(CO)₇(PPh₃)] with triphenylphosphine at room temperature. However, the reaction of [RU₃(μ-H)(μ₃, η² -ampy)(CO)₇(PPh₃)₂] with diphenylacetylene requires a higher temperature (110°C) and does not give complex 1 but the phenyl derivative [RU₃(μ₃,η²-ampy)(μ,η ¹:η² -PhC=CHPh)(μ,-PPh₂)(Ph)(CO)₅(PPh₃)] (2). The thermolysis of complex 1 (110°C) also gives complex 2 quantitatively. Both 1 and 2 have been characterized by0 X-ray diffraction methods. Complex 1 is a catalyst precursor for the homogeneous hydrogenation of diphenylacetylene to a mixture of cis- and trans -stilbene under mild conditions (80°C, 1 atm. of H₂), although progressive deactivation of the catalytic species is observed. The dihydride [RU₃(μ-H)₂(μ ₃,η²-ampy)(μ,η¹:η²- PhC=CHPh)(CO)₅(PPh₃)₂] (3), which has been characterized spectroscopically, is an intermediate in the catalytic hydrogenation reaction.     

Electrochemical behaviour of some polyoxo clusters

We describe the redox behaviour in non-aqueous solvents of some cyclopentadienyl(oxo)titanium derivatives. The derivative [Ti₄{η⁵-C₅H₄(SiMe₃)}₄(μ-O)₆] shows an electrochemically and chemically reversible le reduction process, followed by a multi-electron, chemically complicated reduction at a fairly cathodic potential. On the basis of the overall electrochemical features and the comparison with the redox behaviour of the quasi-planar compound [[Ti{η⁵-C₅H₄(SiMe₃)}Cl(μ-O)]₄] we propose an EECCEE mechanism for the first derivative, where the second electron-transfer induces a cascade of chemical reactions giving rise to irreversible cluster breakdown. The electrochemically induced fragmentation can be viewed as a retrosynthetic pathway. The heterometallic derivative [{Ti(η⁵-C₅H₄Me)₂(μ₂-MoO₄)₂}₂] shows two consecutive reduction processes; the first is chemically reversible, and the second quasi-reversible. The molybdate bridges apparently increase the stability of the electrogenerated anions. However none of these poly-oxo clusters can be considered as good models of electron ‘sinks’.     

Two Pentavanadate-based Organic-inorganic Materials with Third-order NLO Properties

Two isolated organic-inorganic pentavanadate-based hybrids,[H2N(CH3)2]6.34[V^V(μ3-O)4V4^IVO5(SO4)4]·(SO4)0.67·(DMF)·[HN(CH3)2]1.66(1)and [(HN)2(CH2)2(CH3)4][V^V(μ3-O)4V4^IVO5(SO4)4][H2N(CH3)2]3@(DMF)@ [HN(CH3)2]0.5(2)(DMF=N,N-dimethylformamide)have been synthesized under solvothermal conditions and structurally characterized.In compound 1,three adjacent basic units form a triangle type cluster.The symmetric double-layer exists in compound 2.The study of the third-order nonlinear optical(NLO)properties for the two compounds demonstrates that the two-photon absorption(TPA)cross-section σ values of compounds 1 and 2 are 1372 and 1228 GM,respectively,indicating that both compounds may have potential application in optical field.