间甲基苯甲醚分子旋转异构体的质量分辨阈值电离光谱

间甲基苯甲醚分子有顺式和反式两个转动异构体.利用单光共振双光子电离技术和质量分辨阈值电离技术,研究了间甲基苯甲醚分子顺反异构体的基态到第一电子激发态(S1←S0)的跃迁和阈值电离.得到顺式、反式间甲基苯甲醚分子S1态的激发能(E1)分别为(36049±2)和(36117±2)cm-1,绝热电离能(Ip)分别为(64859±5)和(65110±5)cm-1.结合从头算法和密度泛函理论的量子化学计算,解释了顺式、反式间甲基苯甲醚分子E1和Ip存在差异的原因,并且对S1态和离子基态D0态出现的谱峰进行了标识.间甲基苯甲醚分子顺反异构体在S1态和D0态的活性振动主要是甲基转动、面内环的运动和与取代基相关的弯曲振动.间甲基苯甲醚分子的S1态振动光谱、D0态离子光谱以及理论计算均表明这两个转动异构体在D0态的几何构型与S1态的中性几何构型相比有较大改变,取代基与取代基、取代基与苯环间的相互作用强度高低次序为:S0S1D0.     

对一个大单轴磁各向异性镍(Ⅱ)配合物中的磁跃迁的直接观察

最近Ruamps和同事发现三角双锥构型的Ni（Ⅱ）配合物[Ni（Me₆tren）Cl]ClO₄（1，Me₆tren=tris（2-（dimethylamino）ethyl）amine）具有大的单轴磁各向异性（J.Am.Chem.Soc.，2013，135：3017-3026）。他们利用HF-EPR研究获得横向零场分裂（ZFS）参数E=1.56（5）cm^-1但未能确定轴向零场分裂参数D。在本工作中，我们利用0~17.5 T和5 K的变磁场远红外光谱（FIRMS）来检测自旋基态S=1中的M_S=±1和M_S=0态之间的磁跃迁。在FIRMS中直接观察到Zeeman分裂态之间的跃迁，得出轴向ZFS参数D=-110.7（3）cm^-1。我们对1的晶体结构进行了Hirshfeld表面分析，揭示了1分子中的阳离子与阴离子之间以及分子之间的相互作用。     

飞秒时间分辨的光电子影像对3-甲基吡啶分子超快动力学研究

利用飞秒时间分辨的光电子影像技术结合时间分辨的质谱技术,研究了3-甲基吡啶分子激发态的超快过程. 实时观察到了3-甲基吡啶分子S₂态向S₁态高振动能级的超快内转换过程,该内转换的时间大约为910fs. 二次布居的S₁态主要通过内转换衰减到基态S₀,该内转换的时间尺度为2.77 ps. 光电子能谱分布和光电子角分布显示,S₂态和S₁态在电离的过程中跟3p里德堡态发生偶然共振. 本次实验中还用400 nm两个光子吸收的方法布居了3-甲基吡啶的3s 里德堡态. 研究表明,3s 里德堡态的寿命为62 fs,并主要通过内转换快速衰减到基态.     

4-硝基咪唑A-带激发态结构动力学

通过共振拉曼光谱实验和量子化学计算的方法研究了4-硝基咪唑(4NI)A-带激发态衰变动力学. 对4NI的振动光谱、紫外电子吸收光谱、荧光光谱和共振拉曼光谱进行了指认. 在全活化空间自洽场法(CASSCF)/6-31G(d)计算水平下获得了单重激发态S₁(n_Oπ^*)和S₂(ππ^*)和势能面交叉点S₁(n_Oπ^*)/S₂(ππ^*)的优化几何结构和能量, 分析了A-带共振拉曼光谱的强度模式特征, 获得了短时结构动力学, 并结合全活化空间自洽场法(CASSCF)理论计算结果确定了4NI 在S₂(ππ^*)态衰变通道主要是S_{2, FC}→S_{2, min}(ππ^*)→S₀辐射弛豫.     

AgIn5S8/碳量子点/ZnIn2S4的多途径电子迁移与光催化性能

首先,借助碳量子点（CQDs）的上转换光致发光（UCPL）特性对ZnIn₂S₄进行了表面改性,再结合离子交换法制备了复合材料AgIn₅S₈/CQDs/ZnIn₂S₄。采用X射线衍射（XRD）、X射线光电子能谱（XPS）、紫外可见漫反射吸收光谱（UV-Vis DRS）、扫描电镜（SEM）、透射电镜（TEM）、氮气吸附-脱附、光致发光（PL）和电化学阻抗（EIS）等测试手段对复合材料的组成、结构、形貌以及表面物理化学性质等进行了表征。结果表明,该复合材料中不同组分间的协同作用导致其呈现宽光谱响应（250~800 nm）。与对比体系相比,复合材料AgIn₅S₈/CQDs/ZnIn₂S₄表现出明显增强的光电流密度,更小的电荷转移阻抗,较长的光生载流子寿命。以甲基橙为模型分子,在不同光源作用下进行的光催化活性研究结果显示,AgIn₅S₈/CQDs/ZnIn₂S₄呈现增强的光催化降解活性。同时,该复合材料在光解水性能研究中不仅表现较高的光解水制氢速率（312.09 μmol·h^-1·g^-1）,而且呈现良好的稳定性。     

含吡咯环的缩氨基硫脲席夫碱镍、铜配合物的晶体结构及与DNA的相互作用

合成并通过单晶衍射、元素分析及红外光谱表征了配合物[Ni（L¹）₂]·2DMF （1）,[Cu（L¹）₂]·THF·0.25MeOH·2.25H₂O（2）, [Ni（L²）₂]·2MeOH（3）和[Cu（L²）₂]·2EtOH （4）的结构（HL¹：5-甲酰基-3,4-二甲基-吡咯-2-甲酸乙酯缩硫代氨基脲,HL²：5-甲酰基-2,4-二甲基-吡咯-3-甲酸乙酯缩4-异丙基氨基硫脲）。单晶衍射结果表明,除溶剂分子不同外,配合物1~4的结构相似。每个配合物的中心金属离子分别与来自2个阴离子L^-配体的N₂S₂电子供体配位,采取扭曲的平面正方形配位构型。荧光光谱结果表明,配合物与DNA的相互作用强于其配体。     

含吡咯环的缩氨基硫脲席夫碱镍、铜配合物的晶体结构及与DNA的相互作用

合成并通过单晶衍射、元素分析及红外光谱表征了配合物[Ni（L¹）₂]·2DMF（1）,[Cu（L¹）₂]·THF·0.25MeOH·2.25H₂O（2）,[Ni（L²）₂]·2MeOH（3）和[Cu（L²）₂]·2EtOH（4）的结构（HL¹：5-甲酰基-3,4-二甲基-吡咯-2-甲酸乙酯缩硫代氨基脲,HL²：5-甲酰基-2,4-二甲基-吡咯-3-甲酸乙酯缩4-异丙基氨基硫脲）。单晶衍射结果表明,除溶剂分子不同外,配合物1~4的结构相似。每个配合物的中心金属离子分别与来自2个阴离子L-配体的N₂S₂电子供体配位,采取扭曲的平面正方形配位构型。荧光光谱结果表明,配合物与DNA的相互作用强于其配体。     

非血红素铁超氧化物活化丙烯分子多态反应机理的理论研究

采用密度泛函DFT-B3LYP理论对非血红素铁超氧化物活化丙烯分子多态反应机理进行了探讨. 研究结果表明氢原子抽取过程遵守单态反应机制,主要在基态高自旋七重态势能面进行,且具有较低活化能（ΔG^≠=65.6 kJ·mol^-1）,非血红素铁超氧化物可以作为有效氧化剂抽取氢原子。单态反应机制可能归因于近来建议的交换-加强反应原则（EER,铁中心具有较大交换稳定作用）。对于O-O键的活化,在CASSCF（10,8）/6-31+G（d）//TZVP水平下,势能面交叉区内,高自旋七重态（S₁）和五重态（Q₀）的自旋-轨道耦合（SOC）常数分别为2.26和2.19 cm^-1。轨道分析表明两条发生翻转自旋轨道具有相同空间组成（π_sub^*）,SOC禁阻,因此通过SOC作用反应体系不可能有效地从七重态（S=3）势能面系间穿越到五重态（S=2）势能面,系间穿越可能发生在反应最后的退出阶段。     

非血红素铁超氧化物活化丙烯分子多态反应机理的理论研究

采用密度泛函DFT-B3LYP理论对非血红素铁超氧化物活化丙烯分子多态反应机理进行了探讨.研究结果表明氢原子抽取过程遵守单态反应机制,主要在基态高自旋七重态势能面进行,且具有较低活化能（ΔG^≠=65.6 kJ·mol^-1）,非血红素铁超氧化物可以作为有效氧化剂抽取氢原子。单态反应机制可能归因于近来建议的交换-加强反应原则（EER,铁中心具有较大交换稳定作用）。对于O-O键的活化,在CASSCF（10,8）/6-31+G（d）//TZVP水平下,势能面交叉区内,高自旋七重态（S₁）和五重态（Q₀）的自旋-轨道耦合（SOC）常数分别为2.26和2.19 cm^-1。轨道分析表明两条发生翻转自旋轨道具有相同空间组成（π_sub^*）,SOC禁阻,因此通过SOC作用反应体系不可能有效地从七重态（S=3）势能面系间穿越到五重态（S=2）势能面,系间穿越可能发生在反应最后的退出阶段。     

含不同芳香取代基的肼基二硫代甲酸甲酯-Ga3+配合物的合成及抑菌活性

设计合成了4种含不同芳香取代基团的肼基二硫代甲酸甲酯配体（2-乙酰基吡啶肼基二硫代甲酸甲酯（L¹-H）、2-甲酰基吡啶肼基二硫代甲酸甲酯（L²-H）、2-甲酰基噻吩肼基二硫代甲酸甲酯（L³-H）、2-甲酰基水杨醛肼基二硫代甲酸甲酯（L⁴-H））的镓配合物,对它们的抑菌活性进行了测试,并讨论了配体分子中不同芳香取代基对配合物抑菌活性的影响。在模拟生理条件下,L与Ga³⁺生成较稳定的单核配合物[Ga（L¹）₂]NO₃（1）、[Ga（L²）₂]NO₃（2）、[Ga（L³）₂]NO₃（3）、[Ga（L⁴）₂]NO₃（4）,各配合物对金黄色葡萄球菌和大肠杆菌表现出比Ga（NO₃）₃·9H₂O强的抑制活性,抑制金黄色葡萄球菌的能力高于大肠杆菌,其中,1和2的活性比相应配体高,其余2个配合物与其配体之间无明显活性差异。L¹和L²分子中吡啶基的较强吸电子效应可能是1和2具有较强抑菌活性的主要原因。4种配合物抑制黑曲霉生长的活性同样高于Ga（NO₃）₃·9H₂O,其中3最强,并显著高于L³,其余配合物与相应配体间无活性差异。     

Mass-analyzed Threshold Ionization Spectroscopy of Rotamers of p-ethoxyphenol Cations and Configuration Effect

Two-color resonant two-photon mass-analyzed threshold ionization （MATI） spectroscopy was used to record the vibrationally resolved cation spectra of the selected rotamers of p- ethoxyphenol. The adiabatic ionization energies of the trans and cis rotamers are determined to be 61565±5 and 61670±5 cm^-1, which are less than that of p-methoxyphenol by 645 and 643 cm^-1, respectively. Analysis on the MATI spectra of the selected rotamers of p-ethoxyphenol cation shows that the relative orientation of the ethoxy group has little effect on the in-plane ring vibrations. The low-frequency OC2H5 bending vibrations appear to be active for both forms of the cation.     

2, 5-二氟苯酚分子之旋转异构物的质量分辨阈值电离光谱

利用共振双光子电离(R²PI)技术和质量分辨阈值电离(MATI)技术来研究2, 5-二氟苯酚分子。实验所测得的顺式、反式2, 5-二氟苯酚分子电子激发能E₁分别为36448和36743 cm^-1,绝热电离能分别为71164和71476 cm^-1。这两个顺反转动同素异构分子在电子激发S₁态与离子D₀态活性振动主要是由于面内环变形和与取代基相关的弯曲振动。分析2, 5-二氟苯酚分子的振动光谱、D₀态离子光谱以及理论计算均表明这两个转动异构体在D₀态的几何构型与S₁态的中性几何构型相当相似。     

Molecular Structure, Vibrational Spectrum and Ionization Energy of m-Dimethoxybenzene

The optimized molecular geometries of the three rotamers of m-dimethoxybenzene in the ground So and electronically excited Sl states were predicted by ab initio and density functional theory （DFF） calculations. Their vibrational spectra in the St state were studied by one color resonant two photon ionization （1C-R2PI） method, and their ionization energies were measured by two color resonant two photon ionization （2C-R2PI） experiment. The optimized molecular geometries showed that the total energy of conformer a was the lowest in the So state. Most of the active vibrations assigned from the 1C-R2PI spectrum were found to be of the in-plane ring modes. The ionization energies （IE） of conformers a, b and c were determined to be 63521, 64487 and 63755 cm^-1, respectively.     

Rotamers of m-cresol cation studied by mass-analyzed threshold ionization spectroscopy

We have applied two-color resonant two-photon mass-analyzed threshold ionization technique to record the vibrational spectra of the selected rotamers of m-cresol. The adiabatic ionization energies of cis and trans m-cresol are determined to be 66,933+/-5 and 67,084+/-5 cm(-1), respectively. Frequencies of the in-plane ring vibrations 6a, 1, and 9b are measured to be 528, 720, 1167 cm(-1) for the cis and 520, 698, and 1153 cm(-1) for the trans m-cresol cation. This indicates that different orientation of the OH group with respect to the CH(3) group slightly influences these ring vibrations.     

Vibrational Spectra and Quantum Calculations of Ethylbenzene

Normal vibrations of ethylbenzene in the first excited state have been studied using resonant two-photon ionization spectroscopy. The band origin of ethylbenzene of S₁←S₀ transition appeared at 37586 cm^-1. A vibrational spectrum of 2000 cm^-1 above the band origin in the first excited state has been obtained. Several chain torsions and normal vibrations are obtained in the spectrum. The energies of the first excited state are calculated by the time-dependent density function theory and configuration interaction singles (CIS) methods with various basis sets. The optimized structures and vibrational frequencies of the S₀ and S₁ states are calculated using Hartree-Fock and CIS methods with 6-311++G(2d,2p) basis set. The calculated geometric structures in the S₀ and S₁ states are gauche conformations that the symmetric plane of ethyl group is perpendicular to the ring plane. All the observed spectral bands have been successfully assigned with the help of our calculations.     

Vibrational Spectrum of o‐Dimethoxybenzene in the S1 and D0 States

The optimized molecular geometries of o‐dimethoxybenzene (ODMB) in the S₀ state were predicted by ab initio and density functional theory calculations. Its vibrational spectra in the S₁ and D₀ states were studied by one color resonant two photon ionization (1C‐R2PI) and mass analyzed threshold ionization (MATI) experiments. The results indicated that trans rotamer was most stable. Only one rotamer of ODMB was detected by the 1C‐R2PI spectra, and its band origin was (35750±2) cm^?1, its ionization energy was (61617±5) cm^?1. Most of the observed vibrations in the D₀ state resulted from the in‐plane ring and substituent sensitive modes.     

Assignment of the first photoelectron band of the CH<Subscript>3</Subscript>CHCl radical using ab initio quantum mechanical calculations

HeI photoelectron spectra have been recorded for the reaction of atomic fluorine with ethyl chloride at different reaction times. A structured band associated with a short-lived primary reaction product has been recorded with adiabatic and vertical ionization energies of (7.84±0.02) and (8.18±0.02) eV respectively. An average vibrational separation of (680±30) cm^–1was observed in this band. Comparison between the experimental vertical and adiabatic ionization energies and ionization energies computed for CH₃CHCl (X²A) and CH₂CH₂Cl (X²A) at different levels of theory led to the assignment of the observed first photoelectron band to the ionization of CH₃CHCl (X²A). The observed vibrational structure was assigned to excitation of the C–Cl stretching mode in CH₃CHCl⁺(X¹A).Proceedings of the 11th International Congress of Quantum Chemistry satellite meeting in honor of Jean-Louis Rivail     

Rotational isomers of several aromatic molecules studied by supersonic jet spectroscopy

The electronic spectra of m—substituted phenols and β-naphthol in supersonic free jets have been investigated. All the molecules studies exhibit two strong features in the fluorescence excitation spectra, which are due to two rotational isomers in which the hydrogen atom of the OH group is in cis and trans configurations with respect to the m—substituent. The difference between the S₁ — S₀ excitation energies of the two isomers is in the range from 100 to 300 cm^?1. This large difference indicates the potentiality of electronic spectroscopy in the discrimination of the rotational isomers. The dispersed fluorescence spectra of the molecules as well as the electronic spectra of the hydrogen—bonded complexes provide definite evidences for the existence of the two isomers     

1-萘酚的紫外共振双光子电离光谱

利用脉冲分子束技术, 在305-322 nm范围内研究了1-萘酚(1NP)的共振双光子电离(R2PI)光谱. 1NP分子存在cis和trans两种旋转异构体, 但实验中仅观测到trans异构体的电子振动跃迁光谱, 其S1←S0跃迁的(0-0)带头出现在317.90 nm(即31456 cm-1)位置. 利用光谱选律及ab initio和密度泛函(DFT)计算, 对trans异构体在S1态的振动模进行标识, 得出主要对应于对称性为a'的平面内振动模. 计算显示, cis异构体在电子基态S0的能量较trans异构体高出439 cm-1, 而第一激发能却比trans异构体的低1216 cm-1, 与之相应的实验值分别是220和274 cm-1. 计算数值与实验结果在能量变化趋势上完全一致. 共振双光子电离谱中没有观测到cis异构体的光谱信号, 其原因可归结为分子束的有效冷却效应使得处于基态的cis异构体的布居数密度相对trans异构体极低, 导致cis光谱信号太小而未能被探测到.