四—（对—磺基苯基）卟啉二酸（H4^2＋TSPP）分子聚集体的共？…

研究了四－（对－磺基苯基）卟啉二酸的Ｊ－聚集体共振喇曼光谱,用氘代法考察了各喇曼谱带的同位素位移。指认３条低波数喇曼带为分子聚集体的晶格模,喇曼光谱退偏比测量表明,聚集体中Ｈ４＾２＋ＴＳＰＰ的对称性较分子态降低。Ｈ４＾２＋ＴＳＰＰ在聚集体中以这面对面方式排列。     

四-(对-磺基苯基)卟啉二酸(H2+4TSPP)分子聚集体的共振喇曼光谱研究

研究了四-(对-磺基苯基)卟啉二酸(H2+4TSPP)的J-聚集体共振喇曼光谱,用氘代法考察了各喇曼谱带的同位素位移.指认3条低波数喇曼带为分子聚集体的晶格模.喇曼光谱退偏比测量表明,聚集体中H2+4TSPP的对称性较分子态降低.比较游离碱H2TSPP和分子态H2+4TSPP共振喇曼光谱讨论了聚集体中H2+4TSPP的结构变化.H2+4TSPP在聚集体中以接近面对面方式排列.     

金属卟啉－甲基紫精二连体配合物的合成及其光化学行为

本文合成了四（对－氯代甲基）苯基－甲基紫精卟啉及其Ｚｎ、Ｃｏ、Ｍｎ配合物，用元素分析、红外光谱和紫外可见光谱进行了表征．研究了它们的光化学性质．结果表明．在ＴＥＯＡ中光照使Ｍ·ＴＣＭＰＰ—ｍｖ￣２＋发生了分子内从卟啉到甲基紫精的电子迁移反应．在ＺｎＴＣＭＰＰ－ｍｖ￣２＋／ＴＥＯＡ／ＤＭＳＯ—Ｈ２Ｏ体系中可发生光敏化还原ｍｖ２＋反应，生成较稳定的ｍｖ＋．在Ｍｎ（Ⅲ）ＴＣＭＰＰ－ｍｖ２＋／ＣＨ３ＯＨ／Ｈ２Ｏ体系中可发生光助氧化甲醇反应，并检出了氧化产物甲醛．     

金属卟啉－甲基紫精二连体配合物的合成及其光化学行为

本文合成了四（对－氯代甲基）苯基－甲基紫精卟啉及其Ｚｎ，Ｃｏ，Ｍｎ配合物，用元素分析、红外光谱和紫外可见光谱进行了表征。研究了它们的光化学性质。结果表明，在ＴＥＯＡ中光照使Ｍ。ＴＣＭＰＰ－ｍｖ＾２＋发生了分子内从卟啉到甲基紫精的电子迁移反应。在ＺｎＴＣＭＰＰ－ｍｖ＾２＋／ＴＥＯＡ／ＤＭＳＯ－Ｈ２Ｏ体系中可发生光敏化还原ｍｖ＾２＋反应，生成较稳定的ｍｖ＾＋。在Ｍｎ（Ⅲ）ＴＣＭＰＰ－ＭＶ＾２＋／ＣＨ３     

卟啉试剂光度法间接测定硫离子的研究（1）

本文以ＴＰＰＳ４、Ｔ（４－ＭＯＰ）ＰＳ４和Ｔ（４－ＭＰ）ＰＳ４为例，研究了Ａｇ·ｐｈｅｎ·ＰＰ光度法间接测定废水中痕量硫离子的有关条件。同时用上述三种卟啉试剂试验了Ｃｕ￣（２＋）、Ｈｇ￣（２＋）、Ｃｄ￣（２＋）、Ｐｂ￣（２＋）等软酸和交界酸间接测定Ｓ￣（２－）的可能性，结果表明，Ｈｇ－ＰＰ也可用于间接测定Ｓ（２－）。最后，对Ｈ＿２Ｓ的吸收液进行了筛选。     

Cu（Ⅱ）NEAE和Cu（Ⅱ）NACN的NIR FT－SERS光谱研究

用沉积银胶的银镜作活性载体，获得了中位－四－（４－Ｎ－乙氧羧甲基吡啶）卟啉络铜（Ⅱ）（Ｃｕ（Ⅱ）ＮＥＡＥ）、中位－四－（４－Ｎ－氰甲基吡啶）卟啉络酮（Ⅱ）（Ｃｕ（Ⅱ）ＮＡＣＮ）的近红外富里叶变换－表面增强喇曼光谱（ＮＩＲＦＴＳＥＲＳ），对其谱峰位移作了归属，并与它们的可见激光表面增强共振喇曼光谱（ＳＥＲＲＳ）作了比较。     

液芯光纤预共振和共振喇曼光谱及其应用

在液芯光纤内产生预共振和共振喇曼效应，可大度提高喇曼光谱强度，用波长远离样品吸收峰的激光激发观察到了α－甲基吡啶的预共振喇曼光谱。用长１．１ｍ，内径２００μｍ的液芯光纤，波长５１４．５ｎｍ，功率０．８０Ｗ激光激发获得了β－胡萝卜素在ＣＳ２中的共振喇曼光谱，其浓度为２×１０＾－８ｍｏｌ／Ｌ，比普通方法的样品的浓度低２－３个数量级。     

钢铁表面W—S簇合物彩色钝化膜的组成和结构

通过（ＮＨ４）２ＷＳ４溶液浸渍，在钢铁表面获得了具有良好装饰效果和耐蚀性能的彩色Ｗ－Ｓ簇合物膜．ＦＴ－ＩＲ、Ｆ－ＩＲ、ＦＴ－Ｒａｍａｎ、ＸＰＳ和ＡＥＳ分析结果表明，簇合物膜中存在Ｗ—Ｓ—Ｆｅ、端基Ｗ—Ｓ和端基Ｗ—Ｏ键，膜层由Ｗ、Ｓ、Ｆｅ、Ｏ元素组成，膜外层各元素价态分别为＋６、＋６（＋４）、＋３、－２，膜内层其价态则分别为＋６（＋４）、－２、＋２、－２．膜为多分子层结构，从ＡＥＳ深度分布曲线的组成恒定区求得了元素的相对原子分数和膜层厚度．反应时间越长，膜越厚．在２５０℃空气中加热２ｈ后膜层所含元素种类和价态不变，但各元素的分布和膜的结构发生了变化     

杂多阴离子的有机金属化学(Ⅲ)──缺位Keggin阴离子PW_9O_(34)~(9-)的酯基锡杂多配合物的合成及性质

利用酯基锡与缺位Ｋｅｇｇｉｎ结构杂多阴离子ＰＷ９Ｏ９－３４反应，合成了６种新的杂多阴离子有机金属配合物Ｍ９［（Ｒ′ＯＯＣＣＨＲ″ＣＨ２ＳｎＯＨ２）３（ＰＷ９Ｏ３４）２］·ｘＨ２Ｏ（Ｍ＝（ＣＨ３）４Ｎ＋，Ｋ＋；Ｒ′＝ＣＨ３＿，ＣＨ３ＣＨ２＿；Ｒ″＝Ｈ，ＣＨ３＿），通过元素分析、ＩＲ光谱、紫外电子光谱、１ＨＮＭＲ、３１ＰＮＭＰ、１８３ＷＮＭＲ和ＴＧＡ－ＤＳＣ热分析等测试手段对标题配合物进行了表征和性质研究，确定该系列配合物为Ａ－β－ＰＷ９型夹心配合物结构．     

镧系元素的中性络合固-液萃取分离研究(Ⅱ)--TOPO-NaClO4-石蜡体系

本文以正三辛基氧膦为萃取剂,以熔融石蜡为稀释剂,研究了ＨＣｌＯ４－ＮａＣｌＯ４介质中Ｌａ＾３＋、Ｎｄ＾３＋、Ｓｍ＾３＋、Ｄｙ＾３＋Ｙｂ＾３＋的固－－液萃取行为及萃取反应热力学性能。斜率比法给出萃合物组成为Ｌｎ（ＴＯＰＯ）２（ＯＨ）（ＣｌＯ４）２。测定了萃取反应势力学参数、平衡常数及半萃取ｐＨ值。     

四-(对-磺基苯基)卟啉二酸(H2+4TSPP) 分子聚集体的共振喇曼光谱研究

研究了四-(对-磺基苯基)卟啉二酸(H     

四-（4-吡啶基）卟啉二酸聚集体的共振拉曼光谱

研究了近激子吸收带激发下四-（4-吡啶基）卟啉二酸（H8TPyP^6＋）聚集体的共振拉曼光谱。测量了H8TPyP^6＋单体和聚集体的紫外可见吸收谱和共振光散射光谱．在氘代位移的基础上结合相关体系振动光谱研究,对测得的H8TPyP^6＋单体和聚集体的拉曼谱带进行了指认．聚集体的形成导致H8TPyP^6＋的卟啉环CC／CN面内伸缩振动向低波数方向位移2-6cm^-1,而卟啉环鞍形面外振动带向高波数方向位移12cm^-1．基于拉曼谱带的强度和频率变化分析了聚集引起的H8TPyP^6＋分了内结构变化和分子间氢键作用．     

卟啉H2TSPP和Ag(II)TSPP吸附在均分散Fe3O4胶体上的拉曼光谱

Surface Enhanced Raman Scattering (SERS) of tetrasodium meso-tetrakis (4-sulfonatophenyl) porphine (H2TSPP) and silver tetraphenylporphyrin (Ag(Ⅱ)TSPP) adsorbed spontaneously on uniform Fe3O4 colloids are recorded. The enhancement of Raman bands is approximately 30. An analysis of the SERS spectrum shows that on the Fe3O4 surface H2TSPP takes its diacid form H42+TSPP.     

Counterion-dependent excitonic spectra of tetra(p-carboxyphenyl)porphyrin aggregates in acidic aqueous solution

Aggregates of the diacid form of tetra(p-carboxyphenyl)porphyrin (TCPP) are found to be stabilized in aqueous solution at low pH in the presence of poly(vinyl alcohol). At pH values in the range from about 1 to 4, a split Soret band is observed which is independent of counterion and tentatively assigned to a dimer species. As the pH is made lower than 1, the spectra evolve to reveal the presence of porphyrin aggregates. As in the case of the well-known aggregates of the related tetra(p-sulfonatophenyl)porphyrin (TSPP) diacid, the concentration of spectroscopically distinguishable aggregates increases with increasing ionic strength or decreasing pH. Unlike aggregates of TSPP, however, TCPP aggregates below pH 1 have visible absorption spectra which depend on the counterion, which is Cl(-) or NO(3)(-) in this study. In this work, we present visible absorption, light-scattering, and resonance Raman spectra of TCPP diacid in its monomer, dimer, and aggregated forms and attempt to understand the structural basis for counterion-dependent structure and excitonic coupling in the aggregates. Evidence is presented for intercalation of inorganic counterions between porphyrin molecules in the aggregate, an effect which to our knowledge has not been previously reported.     

Surface-enhanced Raman scattering of TSPP,Ag(II)TSPP,and Pb(II)TSPP adsorbed on AgI and AGCl colloids

Surface-enhanced Raman scattering (SERS) was measured for meso-tetrakis(4-sulfonatophenyl)porphine (TSPP) and its metal derivatives Ag(II)TSPP and Pb(II)TSPP adsorbed on AgI colloids, and for TSPP adsorbed on AgCl colloids. The experiments show that TSPP molecules adsorbed on AgI colloids undergo a silver incorporation, while TSPP adsorbed on AgCl colloids are converted into the porphyrin diacid H₄TSPP²⁺ and the metalloporphyrin Ag(II)TSPP. The concentration dependences of SERS spectra for TSPP adsorbed on the two substrates are quite different.     

Electrochemical processes of meso-tetrakis (4-sulfonatophenyl) porphine at a silver electrode studied by surface-enhanced resonance raman spectroscopy

The potential dependence of surface-enhanced resonance Roman spectra of meso-tetrakis (4-sulfonatophenyl) porphine (TSPP) in 0.05 M H₂SO₄ reveals two electrochemical processes at a silver electrode surface. One which begins around ?0.3 V is interpreted as dissociation of aggregated TSPP to monomers. The other which occurs near ?0.4 V is ascribed to a partial Ag incorporation of TSPP molecules.     

Raman and infrared spectral study of meso-sulfonatophenyl substituted porphyrins (TPPSn,n = 1, 2A, 2O, 3, 4)

Raman and IR spectra of the free base p-sulfonatophenyl and phenyl meso-substituted porphyrins [5,10,15,20-tetrakis(4-sulfonatophenyl)porphyrin (TPPS4); 5,10,15-tris(4-sulfonatophenyl)-20-phenyl-porphyrin (TPPS3); 5,10-bis(4-sulfonatophenyl)-15,20-diphenylporphyrin (TPPS2A); 5,15-bis(4-sulfonatophenyl)-10,20-diphenylporphyrin (TPPS2O); and 5-(4-sulfonatophenyl)-10, 15,20-trisphenylporphyrin (TPPS1)] and their N-diprotonated derivatives (porphyrin diacids) were studied. The Raman spectra of the deuterated analogues of these porphyrins, in which the central hydrogen atoms were substituted with deuterium, were also measured. The observed vibrational bands were assigned on the basis of the deuteration shifts and compared with the structural analogues of these compounds. In IR spectra of the free-base porphyrins, the p-sulfonation of phenyl groups results in evident alteration for the phenyl modes and the porphyrin skeleton modes that are strongly coupled with phenyl vibrations. While the p-sulfonation of phenyl groups causes only slight changes for the high-frequency Raman bands (> 850 cm(-1)), dramatic shifts and band splitting were observed in the low-frequency region (< 500 cm(-1)) of Raman spectra. The observed differences of low-frequency Raman spectra were attributed to the alteration of the structure of the porphyrin ring, especially the CalphaCmCalpha bond-angles, by different meso-sulfonatophenyl substitutions. In addition, different packing style of TPPSn molecules in the aggregates is also responsible for the alteration of the vibrational spectra of the aggregated TPPSn.     

A PORPHYRIN-DNA EXCIPLEX: RESONANCE RAMAN SPECTRA OF ELECTRONICALLY EXCITED Cu(TMpy-P4) BOUND TO POLY(dA-dT)-POLY(dA-dT)

The resonance Raman spectra of water-soluble porphyrins, Cu(TMpy-P4) and Ni(TMpy-P4), and their mixtures with DNA, Poly(dG-dC).Poly(dG-dC), and Poly(dA-dT).Poly(dA-dT) were measured using 426 nm pulsed laser excitation (and 556 nm for some applications). At high laser power, the solution of Cu(TMpy-P4) mixed with DNA or Poly(dA-dT).Poly(dA-dT) exhibits new bands at 1550 and 1349 cm-1 that are not observed for Cu(TMpy-P4) alone or for Cu(TMpy-P4) mixed with Poly(dG-dC).Poly(dG-dC). These extra bands do not appear when the resonance Raman spectra are measured by a cw laser or by a pulsed laser with low power. Similar mixtures of M(TMpy-P4) (where M = Ni, Zn, Co, Mn, and H2) with these nucleic acids exhibit no such bands even by high power pulsed laser excitation. We attribute the new resonance Raman bands to an electronically excited Cu(TMpy-P4), stabilized by forming an exciplex with the A-T site of the nucleic acid. The minimum lifetime value of such an exciplex was estimated to be on the order of 10 ps.     

Perfluoroterephthalate bridged complexes with M-M quadruple bonds: ((t)BuCO(2))(3)M(2)(mu-O(2)CC(6)F(4)CO(2))M(2)(O(2)C(t)Bu)(3), where M = Mo or W. Studies of solid-state,molecular, and electronic structure and correlations with electronic and Raman spectral data

The compounds [((t)BuCO(2))(3)M(2)(mu-O(2)CC(6)F(4)CO(2))M(2)(O(2)C(t)Bu)(3)], M(4)PFT, where M = Mo or W, are shown by model fitting of the powder X-ray diffraction data to have an infinite "twisted" structure involving M.O intermolecular interactions in the solid state. The dihedral angle between the M(2) units of each molecule is 54 degrees. Electronic structure calculations employing density functional theory (Gaussian 98 and ADF2000.01, gradient corrected and time dependent) on the model compounds (HCO(2))(3)M(2)(mu-O(2)CC(6)F(4)CO(2))M(2)(O(2)CH)(3), where M = Mo or W, reveal that in the gas phase the model compounds adopt planar D(2)(h) ground-state structures wherein M(2) delta to bridge pi back-bonding is maximized. The calculations predict relatively small HOMO-LUMO gaps of 1.53 eV for M = Mo and 1.22 eV for M = W for this planar structure and that, when the "conjugation" is removed by rotation of the plane of the C(6)F(4) ring to become orthogonal to the M(4) plane, this energy gap is nearly doubled to 2.57 eV for M = Mo and 2.18 eV for M = W. The Raman and resonance Raman spectra of solid M(4)PFT and of Mo(4)PFT in THF solution are dominated by bands assigned to the bridging perfluoroterephthalate (pft) group. The intensities of certain Raman bands of solid W(4)PFT are strongly enhanced on changing the excitation line from 476.5 nm (off resonance) to 676.5 nm, which is on resonance with the W(2) delta --> CO(2) (pft) pi transition at ca. 650 nm. The resonance enhanced bands are delta(s)(CO(2)) (pft) at 518 cm(-)(1) and its first overtone at 1035 cm(-)(1), consistent with the structural change to W(4)PFT expected on excitation from the ground to this pi excited state. The electronic transitions for solid Mo(4)PFT (lowest at 410 nm) were not accessible with the available excitation lines (457.9-676.5 nm), and no resonance Raman spectra of this compound could be obtained. For Mo(4)PFT in THF solution, it is the band at 399 cm(-)(1) assigned to nu(MoMo) which is the most enhanced on approach to resonance with the electronic band at 470 nm; combination bands involving the C(6)F(4) ring-stretching mode, 8a, are also enhanced.     

Molecular spectroscopy of uranium(IV) bis(ketimido) complexes. rare observation of resonance-enhanced raman scattering from organoactinide complexes and evidence for broken-symmetry excited states

Electronic absorption and resonance-enhanced Raman spectra for ketimido (azavinylidene) complexes of tetravalent uranium, (C(5)Me(5))(2)U[-N=C(Ph)(R)](2) (R = Ph, Me, and CH(2)Ph), have been recorded. The absorption spectra exhibit four broad bands between 13 000 and 24 000 cm(-1). The highest-energy band is assigned to the ketimido-localized p( perpendicular)(N)-->pi(N=C) transition based on comparison to the spectra of (C(5)H(5))(2)Zr[-N=CPh(2)](2) and (C(5)Me(5))(2)Th[-N=CPh(2)](2). Upon excitation into any of these four absorption bands, the (C(5)Me(5))(2)U[-N=C(Ph)(R)](2) complexes exhibit resonance enhancement for several Raman bands attributable to vibrations of the ketimido ligands. Raman bands for both the symmetric and nominally asymmetric N=C stretching bands are resonantly enhanced upon excitation into the p( perpendicular)(N)-->pi(N=C) absorption bands, indicating that the excited state is localized on a single ketimido ligand. Raman excitation profiles for (C(5)Me(5))(2)U[-N=CPh(2)](2) confirm that at least one of the lower-energy electronic absorption bands (E(max) approximately 16300 cm(-1)) is a charge-transfer transition between the U(IV) center and the ketimido ligand(s). The observations of both charge-transfer transitions and resonance enhancement of Raman vibrational bands are exceedingly rare for tetravalent actinide complexes and reflect the strong bonding interactions between the uranium 5f/6d orbitals and those on the ketimido ligands.