与DNA形成电子激发态复合物的水溶铜卟啉Cu（NEAE）的共振拉曼研究

本文用４００ｎｍ和４４５ｎｍ脉冲激光激发测量了不同功率条件下的水溶酮卟啉Ｃｕ（ＮＥＡＥ）（４－Ｎ－乙酸酯基－吡啶基铜卟啉）及其与小牛胸腺脱氧核糖核酸（ＤＮＡ）复合物的共振拉曼光谱。结果表明，Ｃｕ（ＮＥＡＥ）与ＤＮＡ形成了电子激发态复合物。首次观察到激发态铜卟啉除拉曼谱带Ⅵ（～１３７０ｃｍ＾－１）和Ⅷ（～１５７０ｃｍ＾－１）外Ⅶ带（～１４７０ｃｍ＾－１）也出现代表激发态复合物形成的额外峰。激发态复合     

四氧杂卟啉二价正离子共振拉曼光谱的TDDFT计算研究

采用DFT/TDDFF计算和极化率的态求和方法研究了四氧杂卟啉二价正离子(TOP²⁺)B态(S₂态)激发的共振拉曼(RR)光谱, 计算模型同时处理了A项和B项对拉曼极化率的贡献.用PBE1PBE、B3LYP、Cam-B3LYP、B3LYP-D3四种交换-相关泛函计算得到的RR光谱总体上相似,其中PBE1PBE和B3LYP 给出的RR 强度与实验吻合得更好一些. 对于全对称振动(A_1g),其拉曼谱带相对强度的理论计算结果与实验一致;TDDFF计算表明： 相对于基态,TOP²⁺的B态沿υ2、υ6、υ7、υ8简正模式有较大的无量纲位移, 导致相应的RR带有较大的强度. 非全对称的B_1g和B_2g 模式通过B项机理增强,其强度比A_1g模式小1～2个量级,与实验结果定性符合. 与实验相比,υ10模式(B_1g)RR强度的理论值过小,而υ11模式(B_1g)的理论值偏大;这可能是由于TOP²⁺的B-态(S₂态)具有Jahn-Teller效应.     

硫脲21A激发态扭曲几何结构的共振拉曼光谱和理论研究

获得了硫脲在水和乙腈溶液中A吸收带的共振拉曼光谱,通过B3LYP/6-311++G(3df,3pd)和RCIS/6-311++G(3df,3pd)分别对硫脲的电子跃迁和2¹A 激发态鞍点结构进行了研究．对共振拉曼光谱进行了归属,并通过含时波包理论对吸收光谱和共振拉曼光谱进行拟合,结果表明硫脲动态结构特征主要沿着：C=S伸缩振动ν₆(|△|=0.95)、H₅N₃H₆+H₈N₄H₇弯曲振动ν₅(|△|=0.19)、NCN对称伸缩振动+C=S伸缩振动+N₃H₆+H₈N₄弯曲振动ν₄(|△|=0.18)．ν₁₅倍频2ν₁₅和4ν₁₅强度主要归因于ν₁₅激发态频率的改变而不是简正模位移量的变化．对S=CN₂面外变形振动ν₁₅倍频出现的机理进行了探究,结果表明Franck-Condon区域势能面鞍点是标准A项共振拉曼散射里的二次声子机制的驱动力,导致碳原子中心的锥形化,并使硫脲在2¹A激发态发生几何结构扭曲.     

过渡金属Mn（Ⅲ）,Fe（Ⅲ）,Rh（Ⅱ）和Pd（Ⅱ）卟啉配合物的共振拉…

讨论了金属离子Ｍｎ（Ⅲ），Ｆｅ（Ⅲ），Ｒｈ（Ⅲ）和Ｐｄ（Ⅱ）原卟啉Ⅸ－二甲酯（ＰＰ）和四苯基卟啉（ＴＰＰ）配合物及Ｐｄ（Ⅱ）间氯四苯基卟啉（ＴＰＰｍ－ｃｌ）配合物的共振拉曼光谱。利用金属离子外层ｄ电子与卟啉环的作用，解释了配合物结构灵敏带的变化规律，同时讨论了不同卟啉及卟啉环上取代基团对结构灵敏带的影响。     

共振拉曼光谱研究卟啉二酸H4^2＋TSPP的J—聚集

用共振拉曼光谱和ＵＶ－Ｖｉｓ吸收光谱考察了离子强度对四－（对－磺酸基）苯基卟啉二酸（Ｈ４＾２＋ＴＳＰＰ）聚集体形成的影响,实验表明加入少量的ＮａＣｌＯ４有助于聚集体的形成,而ＮａＣｌＯ４的浓度过高则倾向于形成单体。ＮａＣｌＯ４的加入不改变聚集体中分子的才排列方式,但高浓度的ＮａＣｌＯ４可能在聚集体中引入某种缺陷,使激发态发生局域化。我们还得到了具有宏观尺寸的纤维状Ｈ４＾２＋ＴＳＰＰ沉淀,并研究了其     

分子费米共振拉曼光谱强度分析

测量了CCl₄和CS₂分子的Raman光谱。用Bertran理论和群论等相关理论对其光谱强度进行了分析,获得了发生费米共振分子的拉曼光谱强度的特殊规律： (1)发生费米共振的基频和倍频(和频)间发生能量转移,两光谱强度大小相互接近,当发生费米共振的基频和倍频(和频)间距离很小时,两发生费米共振的光谱强度相等(R=1);(2)能出现倍频光谱强度高于其基频光谱强度;(3)也会观测到费米共振光谱,而观测不到参与费米共振的和频中的基频光谱。此研究对化学、材料科学中的分子结构、材料成分等研究中的谱线认证、归属有很好的参考价值。     

四氯化碳费米共振的拉曼光谱研究

费米共振现象是一种广泛存在于分子振动光谱中的现象,特别是结构比较复杂的多原子分子.在多原子分子中当振动倍频或组合频位于某一基频附近,由于发生振动耦合,会出现两个新峰,峰的位置向两侧发生移动,二者谱线强度发生变化,把这种现象称为费米共振.费米共振现象不仅存在于红外光谱中,也存在于拉曼光谱中.文章中测量了CCl4的拉曼光谱,利用所得到的谱线峰位和用Originpro7.5软件程序获得积分强度,用费米共振的相关理论计算了C-Cl的a1对称伸缩振动频率v1与C-Cl2的f对称弯曲振动频率v4的组合频(v1 v4)与(某一未知基频)C-Cl的f对称伸缩振动频率v03的费米共振特征参数,进而计算出了耦合系数W和这一未知基频v03.该文对理解费米共振,了解分子振动频率,研究分子结构有很重要的参考价值.     

共振拉曼光谱研究卟啉二酸H_4~(2+)TSPP的J-聚焦

用共振拉曼光谱和ＵＶ Ｖｉｓ吸收光谱考察了离子强度对四一（对一磺酸基）苯基卟啉二酸（Ｈ２＋４ＴＳＰＰ）Ｊ 聚集体形成的影响。实验表明加入少量的ＮａＣｌＯ４有助于聚集体的形成,而Ｎａ ＣｌＯ４的浓度过高则倾向于形成单体。ＮａＣｌＯ４的加入不改变聚集体中分子的构型和排列方式,但高浓度的ＮａＣｌＯ４可能在聚集体中引入某种缺陷,使激子态发生局域化。我们还得到了具有宏观尺寸的纤维状Ｈ２＋４ＴＳＰＰ沉淀,并研究了其固体显微拉曼谱。     

中位-四(4-N甲氧羰甲基吡啶)卟啉锌的表面增强拉曼光谱研究

我们研究了水溶性的中位一四(4-N甲氧羰甲基吡啶)卟啉及其锌配合物的共振拉曼光谱和表面增强拉曼光谱。对其拉曼特征频率作了经验式的归属,同时还研究了溶液酸度对它的表面增强拉曼光谱的影响,并对其表面增强机理进行了初步探讨。     

Infrared and Raman Spectra of Sulfur-Nitride Complexes of Nickel(II) and Palladium(II)

Abstract

The infrared and Raman spectra of trans-Ni(S₂N₂CH₃)₂ and Pd(S₃N)₂ were measured from 4000-200 cm^?1. The absorption bands were assigned by comparison to the sulfur nitride complexes of nickel(II), palladium(II) and platinum(II). Normal coordinate analyses on these complexes were carried on these data using molecular parameters taken from X-ray data. To aid in band assignments, isotope shift data on trans-⁶²Ni(S₂N₂CH₃)₂ have also been carried out.     

Electronic and Resonance Raman Spectra of a Multibridged Iron Porphyrin

Abstract

Reported are the electronic and resonance Raman (rR) spectra of a multibridged iron porphyrin derived from meso-tetra(4-pyridil)porphynate iron(II) by complexing the pyridine residues with [Ru^II(edta)]^2- ions. The polymetallated system exhibits the characteristic Soret band at 428 nm (log ε = 5.2) and a shoulder around 465 nm (4.6). The rR enhancement of the porphyrin vibrational modes is similar to those previously reported for typical porphyrins; however, an additional feature appears around 465 nm, associated with the selective enhancement of some pyridine vibrational modes. Based on the rR excitation profiles the absorption band at 465 nm was assigned to a Ru^II-to-pyridine dπ→Pπ? charge-transfer transition.     

Raman Scattering Intensities of the NO2 Symmetric Stretching Vibration Band of Some Aromatic Nitrocompounds (II)

The Raman scattering intensities of the NO₂ symmetric stretching vibration band were investigated experimentally for some para and meta substituted nitrobenzenes. The excitation profiles obtained with the six excitation wavelengths from 457.9 to 514.5 nm were presented. The results were examined in terms of the Albrecht-Hutley's theory, and the electronic states involved in the preresonance Raman intensity enhancement were suggested.     

蛋白质结构和功能的紫外共振喇曼光谱研究

紫外共振喇曼光谱技术是研究复杂大分子结构的有力工具。结合作者在美国Pittsburgh University期间所做的工作，介绍了用紫外共振喇曼光谱研究肽和蛋白质结构与功能的现状和进展，N-methylacetamide和glycyglycine水溶液光化学异构过程的紫外共振喇曼光谱研究，简述了紫外共振喇曼光谱实验技术要点。本文还跟踪国际最新研究成果，介绍了利用紫外共振喇曼光谱技术研究蛋白质的折叠和去折叠过程。     

Infrared Spectra of the Copper(II), Nickel(II) and Palladium(II) Complexes of 4-amino-3-pentene-2-one

Abstract

The infrared spectra of the metal complexes of 4-amino-3-pentene-2-one were measured from 4000 - 20 cm^?1. The absorption bands were assigned by comparison to other similar molecules: The Cu(II) complex of 4-methylamino-3-pentene-2-one, and complexes of acetylacetone. Force constants for the molecules were calculated using the A_xsm matrix method. The spectra were measured at 298^oK and 77^oK.     

Resonance Raman spectroscopy and theoretical study on the photodissociation dynamics of diuron in S2 state

Resonance Raman spectra (RRs) and quantum chemical calculations were used to investigate the photodissociation dynamics of diuron in S₂ state. The RRs indicate that the photorelaxation dynamics for the S₀ → S₂ excited state is predominantly along nine motions: the ring C = C stretch vibration ν₁₂ (1593 cm⁻¹), Ph–N–H wag ν₁₄ (1517 cm⁻¹), CO–N(CH₃)₂ stretch ν₂₃ (1365 cm⁻¹)_, CCH wag in plane/ring C = C stretch ν₂₄ (1297 cm⁻¹)_, ring CH rock in plane/ring deformation ν₂₇ (1233 cm⁻¹), CCH wag in plane ν₂₉ (1151 cm⁻¹), Ph–Cl (para) stretch ν₃₅ (1028 cm⁻¹), Ph–N–H wag ν₃₇ (913 cm⁻¹) and ring breath ν₄₄ (685 cm⁻¹). Dissociation by Ph–Cl (para) cleavage at S₂ state directly or relaxation to T₂ state by internal conversion (S₂ → S₁) and intersystem crossing (S₁/T₂) is expected by ~250 nm irradiation based on the RRS, complete active space self‐consistent field, configuration interaction singles and time‐dependent density functional theory calculations. Copyright © 2012 John Wiley & Sons, Ltd.