2—溴代对苯二甲酸根桥联双核钴（Ⅱ）配合笺的合成,磁性及抗癌活性

合成了三种以２－溴代对苯二甲酸为桥联配体的新型双核钴（Ⅱ）的配合物，即［Ｃｏ２（ＢＴＰ）（ｐｈｅｎ）４］（ＣｌＯ４）２．Ｈ２Ｏ（配合物１）、［Ｃｏ２（ＢＴＰ）（Ｎｐｈｅｎ）４］（ＣｌＯ４）２．２Ｈ２Ｏ（配合物２）和［Ｃｏ２（ＢＴＰ）（Ｂｐｙ）４］ＣｌＯ４）２，２ＨＯ（配合物３）（ＢＴＰ＝２－溴代对苯二甲酸根，ｐｈｅｎ＝１，１０－菲罗啉，Ｎｐｈｅｎ＝５－硝基－１，１０－菲罗啉，Ｂｐｙ－２，２＇联吡啶     

六核配合物[Mn6O2(O2CPh)10(py)4]·MeCN的合成及结构

将［Ｍｎ３Ｏ（Ｏ２ＣＰｈ）６（ｐｙ）２（Ｈ２Ｏ）］·０．５ＭｅＣＮ、水杨醛缩邻氨基酚和三乙胺在乙腈溶液中反应，合成了六核锰配合物。经Ｘ射线单晶结构分析确定该配合物晶体的化学结构式为［Ｍｎ６Ｏ２（Ｏ２ＣＰｈ）１０（ｐｙ）４］·ＭｅＣＮ。结构中含有一个［Ｍｎ６Ｏ２］１０＋核，可看成是两个［Ｍｎ４（μ４－Ｏ）］四面体共一条边，每个四面体的中心是一个μ４－Ｏ２－离子。晶体属单斜晶系，Ｐ２１／ａ空间群，晶胞参数ａ＝２．０５７２ｎｍ，ｂ＝１．８５２０ｎｍ，ｃ＝２．５３７５ｎｍ，β＝１１１．８２°，Ｖ＝８．９７５ｎｍ３，Ｚ＝４，最终偏差因子Ｒ＝０．０６３２，Ｒｗ＝０．０５９５。     

C60哌嗪加成物的结构及光谱研究

用ＩＮＤＯ系列方法研究了Ｃ６０的哌嗪衍生物Ｃ６０Ｎ２（Ｃ２Ｈ４）２的结构。结果表明［６，６］，异构体具有Ｃ２ｖ对称性［６，５］，异构体具有Ｃｓ对称性，前者能量较低。以优化构型为基础，计算两种加成产物的ＵＶ谱，结果表明，［６，６］异构体的特征吸收与实验值相符，同时对［６，５］异构体的ＵＶ谱进行理论预测，对电子跃迁进行了理论指认，并分析了光谱红移的原因。     

2-溴代对苯二甲酸根桥联双核钴(Ⅱ)配合物的合成、磁性及抗癌活性

合成了三种以２－溴代对苯二甲酸根为桥联配体的新型双核钴（Ⅱ）的配合物，即［Ｃｏ２（ＢＴＰ）（ｐｈｅｎ）４］（ＣｌＯ４）２·Ｈ２Ｏ（配合物１）、［Ｃｏ２（ＢＴＰ）（Ｎｐｈｅｎ）４］（ＣｌＯ４）２·２Ｈ２Ｏ（配合物２）和［Ｃｏ２（ＢＴＰ）（Ｂｐｙ）４］（ＣｌＯ４）２·２Ｈ２Ｏ（配合物３）（ＢＴＰ＝２－溴代对苯二甲酸根，ｐｈｅｎ＝１，１０－菲罗啉，Ｎｐｈｅｎ＝５－硝基－１，１０－菲罗啉，Ｂｐｙ＝２，２′－联吡啶）。使用元素分析、ＩＲ、ＵＶ－Ｖｉｓ光谱和电导测定方法对该配合物进行了表征。测定了配合物的变温磁化率，并对所得数据进行了理论分析，求得了配合物１、配合物２和配合物３的自旋磁交换积分分别为：２Ｊ＝－６．５ｃｍ－１，２Ｊ＝－７．８ｃｍ－１和２Ｊ＝－８．９ｃｍ－１。对该三配合物进行了体外抗人白血病癌细胞的实验。发现该三配合物均具有一定的抑制癌细胞的活性     

新型六核钼原子簇化合物{[Mo3（μ3—S）（μ—S2）2（dtp）3]—（μ3—S）（η…

［Ｍｏ３（μ３－Ｏ）（μ－Ｓ）３（μ－ＯＡｃ（ｄｔｐ）３（ｐｙ）］和［Ｍｏ３（μ－Ｓ）３（μ－ＯＡｃ（ｄｔｐ）３－（ｐｙ）］（ｄｔｐ＝Ｓ２Ｐ（ＯＣ２Ｈ５）２＾－）族合物分别与金属化合物ＢｉＩ３和ＳｂＢｒ３进行原子簇反应均能获得意外产物｛［Ｍｏ３（μ３－Ｓ）（μ－Ｓ２）２（ｄｔｐ）３］（μ３－Ｓ）（η＾３－Ｓ２）［Ｍｏ２（μ３－Ｓ）（μ－Ｓ）３（μ－ＯＡｃ）（ｄｔｐ）２］｝六核钼簇。其结构实际上是由     

17电子钒开环夹心羰基配合物的合成及XRD,IR,EPR研究

以４种甲基取代戊二烯基为配体合成了４个过渡金属钒开环夹心羰基配合物［２，４－（ＣＨ３）２Ｃ５Ｈ５］２ＶＣＯ（Ｉ），［２，３－（ＣＨ３）２Ｃ５Ｈ５］ＶＣＯ（Ⅱ），［２－ＣＨ３Ｃ５Ｈ６］２ＶＣＯ（Ⅲ）和［３－ＣＨ３Ｃ５Ｈ６］２ＶＣＯ（Ⅳ），其中Ⅱ，Ⅲ，Ⅳ为新配合物，用Ｘ射线单晶衍射，ＩＲ，ＥＰＲ法对所合成配合物进行了结构表征，发现Ｉ具有两种晶相。     

Synthesis and Crystal Structure of Pyridine－2－thiolato－Molybdenum Complex［Et_4N］［Mo（CO_4）（pyS）］

ＳｙｎｔｈｅｓｉｓａｎｄＣｒｙｓｔａｌＳｔｒｕｃｔｕｒｅｏｆＰｙｒｉｄｉｎｅ－２－ｔｈｉｏｌａｔｏ－ＭｏｌｙｂｄｅｎｕｍＣｏｍｐｌｅｘ［Ｅｔ_４Ｎ］［Ｍｏ（ＣＯ_４）（ｐｙＳ）］ＹｕＰｅｉ－Ｈｕａ；ＨｕａｎｇＬｉａｎｇ－Ｒｅｎ；ＺｈｕａｎｇＢｏ－Ｔａｏ...     

TiO2纳米粒子膜表面性质的研究

ＴｉＯ_２纳米粒子膜在光催化降解大气和水中的污染物［１］、光电转换［２］、光致变色［３］等方面有广阔的应用前景,近年来受到了科学界的高度重视．研究表明,膜的表面性质对如上应用有着重要影响．本文采用等离子体化学气相沉积法（ＰＥＣＶＤ法）［４］制备了ＴｉＯ２的纳米粒子膜,分别采用ＴｉＣｌ４等离子体或Ｏ２等离子体处理膜表面,获得两种不同表面性质的ＴｉＯ２纳米粒子膜;并利用表面光电压谱（ＳＰＳ）和电场诱导表面光电压谱（ＥＦＩＳＰＳ）技术对膜的表面性质进行具体分析,探讨了其在光催化领域的可能应用．１实验部…     

As-V-O簇合物对乙苯选择氧化反应的催化活性

通过水热方法合成了簇合物［Ｎ（ＣＨ３）４］４［Ａｓ８Ｖ１４Ｏ４２（８Ｈ２Ｏ）］及其相近的同多及杂多钒氧簇Ｋ６Ｖ１０Ｏ２８·９Ｈ２Ｏ，ＮａＫＶ２Ｏ６，（Ｈ２Ｅｎ）０．５Ｖ２Ｏ５，（Ｈ２Ｅｎ）３（ＶＯ）９（ＰＯ４）８，Ｎａ３ＶＯ（ＨＰＯ４）（ＰＯ４）·Ｈ２Ｏ．运用ＸＲＤ和ＩＲ等手段表征了［Ｎ（ＣＨ３）４］４［Ａｓ８Ｖ１４Ｏ４２（８Ｈ２Ｏ）］的结构．该类化合物对于催化乙苯过氧化氢选择氧化制苯乙酮具有较高的催化活性．通过比较含钒与不含钒化合物的活性情况，讨论了催化氧化的活性中心．     

双核铁原子簇体系的CI计算

用ＩＮＤＯ／ＣＩ方法研究了含有Ｆｅ－Ｆｅ键的原子簇体系［Ｆｅ２Ｓ２Ｘ４］＾２－（Ｘ＝Ｃｌ，Ｂｒ，Ｉ）的电子光谱及电子结构，对于这些多谱带体系，谱带波数计算值与实验值符合，在谱带的指认分析中，发现了πｄ＾１→πｄ等新的跃迁方式，对跃迁方式作了解释和分类，并讨论了谱带的电荷转移性质，此外，还对体系的化学键等性质进行了分析。     

CH自由基多光子电离新观测到3个nd Rydberg态

(2+1) resonant multiphoton ionization of photolytically produced CH radical yields previously unobserved bands arising from two-photon transition to Rydberg states. Analysing of the spectrum of CH+, three new states are identified. They are 8 d, 9 d and 10 d Rydberg states, respectively.     

CH自由基多光子电离新观测到3个ndRydberg态

由于CH自由基在星际空间、燃烧过程和有机化学反应中大量存在,而且CH自由基是量子化学计算中的模型分子,是人们研究的主要目标之一．几十年来,人们对它进行了大量研究．Herzberg等t‘’利用闪光光解研究了CH自由基紫外及真空紫外区域的发射谱,除了标识一些价键态外,还观察到了一些Rydberg态的发射．此后,Chupka等［’－‘］通过光解乙烯酮产生CH自由基,利用共振增强多光子电离光谱和光电子谱研究了CH在50000－75000cm－‘范围的价键态和Rydberg态．最近,理论计算表明l’I,CH的Rydberg态受排斥态的作用而发生预离解,但预离…     

Experimental and Theoretical Investigation of the 3sp(d) Rydberg States of Fenchone by Polarized Laser Resonance-Enhanced-Multiphoton-Ionization and Fourier Transform VUV Absorption Spectroscopy

The VUV absorption spectrum of fenchone is re-examined using synchrotron radiation Fourier transform spectrometry, revealing new vibrational structure. Picosecond laser (2+1) resonance enhanced multiphoton ionization (REMPI) spectroscopy complements this, providing an alternative view of the 3spd Rydberg excitation region. These spectra display broadly similar appearance, with minor differences that are largely explained by referring to calculated one- and two-photon electronic excitation cross-sections. Both show good agreement with Franck-Condon simulations of the relevant vibrational structures. Parent ion REMPI ionization yields with both femtosecond and picosecond excitation laser pulses are studied as a function of laser polarization and intensity, the latter providing insight into the relative two-photon excitation and one-photon ionization rates. The experimental circular-linear dichroism observed in the parent ion yields varies strongly between the 3s and 3p Rydberg states, in good overall agreement with the calculated two-photon excitation circular-linear dichroism, while corroborating other evidence that the 3p_z sub-state plays no more than a very minor role in the (2+1) REMPI spectrum. Vibrationally resolved photoelectron spectra are recorded with picosecond pulse duration (2+1) REMPI at selected intermediate vibrational excitations. The 3s intermediate state displays a very strong Δv=0 propensity on ionization, but the 3p intermediate evidences more complex vibronic dynamics, and we infer some 3p→3s internal conversion prior to ionization.     

Investigation of the electronic vibrational structure of furan by REMPI

Resonance-enhanced multiphoton ionization (REMPI) has been applied to detect the hot bands as well as the cold bands of the 1a2-->-->3dxy(1A1) Rydberg transition of furan (jet-cooled, mass-analyzed). Based on the unambiguous assignment of the hot bands, a complete vibronic analysis is given for the cold bands of this transition (up to 4600 cm(-1) above the origin). This analysis can be used for the interpretation of the vibrational structure in the X 2A2 photoelectron band. The energy ordering of the five 3d Rydberg states is 1A2 approximately 2A2相似文献   

Vibronic spectra of the allyl radical at 6-8 eV with resonance-enhanced multiphoton ionization technique

The allyl radical was produced in molecular beam by pyrolysis of allyl iodide. The vi-bronic spectra from ground state to six new electronic states of the allyl radical at 6-8 eV, π→3dxz, π→3dxy, and π→ns (n=4, 6, 7, 8) were observed firstly with the aid of time-of-flight mass spectros-copy and resonance-enhanced multiphoton ionization technique. Vibrational progression of v7 (C3 bend) with gross spacing of about 430 cm-1 was observed in ns Rydberg states. The adiabatic ionization potential of the allyl radical was obtained to be (65641 ± 20) cm-1 ((8.138± 0.002) eV) by fitting the term values of ns (n=4,6,7,8) Rydberg states with Rydberg formula.     

Two-colour bound—free—bound spectroscopy of the [E1/2]c6S Rydberg states of CH3I and CD3I

In this resonantly enhanced multiphoton ionization (REMPI) experiment, an extended vibrational progression in the CI stretching mode (v₃) of methyl iodide (-h₃ and -d₃) is observed in the 1 + 1′ excitation of the [1/2] 6s; 0 Rydberg state when the pump photon wavelength lies in the bound → free absorption continuum. This is in contrast with one-colour coherent (non-resonant) two-photon excitation, where the v₃ mode is not excited. By working at several different fixed probe wavelengths and scanning the pump frequency, the relative contributions from the three intermediate repulsive states can be explored through changes in the relative strengths of the Ω = 0 and 1 components of the final Rydberg states. Extensive predissociation in the Rydberg states curtails the vibrational progression.     

3s Rydberg and cationic States of pyrazine studied by photoelectron spectroscopy

We have studied 3s(n-1 and pi-1) Rydberg states and D0(n-1) and D1(pi-1) cationic states of pyrazine [1,4-diazabenzene] by picosecond (2 + 1) resonance-enhanced multiphoton ionization (REMPI), (2 + 1) REMPI photoelectron imaging, He(I) ultraviolet photoelectron spectroscopy (UPS), and vacuum ultraviolet pulsed field ionization photoelectron spectroscopy (VUV-PFI-PE). The new He(I) photoelectron spectrum of pyrazine in a supersonic jet revealed a considerably finer vibrational structure than a previous photoelectron spectrum of pyrazine vapor. We performed Franck-Condon analysis on the observed photoelectron and REMPI spectra in combination with ab initio density functional theory and molecular orbital calculations to determine the equilibrium geometries in the D0 and 3s(n-1) states. The equilibrium geometries were found to differ slightly between the D0 and 3s states, indicating the influence of a Rydberg electron on the molecular structure. The locations of the D1-D0 and 3s(pi-1)-3s(n-1) conical intersections were estimated. From the line width in the D1 <-- S0 spectrum, we estimated the lifetime of D1 to be 12 fs for pyrazine and 15 fs for fully deuterated pyrazine. A similar lifetime was estimated for the 3s(pi-1) state of pyrazine by REMPI spectroscopy. The vibrational feature of D1 observed in the VUV-PFI-PE measurement differed dramatically from that in the UPS spectrum, which suggests that the high-n Rydberg (ZEKE) states converging to the D1 vibronic state are short-lived due to electronic autoionization to the D0 continuum.     

丁酮分子的共振增强多光子电离解离研究

利用可调谐染料激光研究了丁酮分子的共振增强多光子电离解离过程,发现在428～448nm激光波段丁酮分子发生的是经4p和4dRydberg态的(3+1)多光子过程。此外,我们还用“梯开关”模型对丁酮母体离子的解离机理和各碎片来源作了详细的分析,分析认为在丁酮母体离子的解离过程中存在H原子重排与电荷的重新分布现象。     

Observation of a New 2§ Excited Electronic State of SF by Resonance-Enhanced Multiphoton Ionization Spectroscopy

The (2+1) resonance-enhanced multiphoton ionization (REMPI) spectrum of SF has been obtained in the single-photon wavelength region of 307-321 nm. Five vibronic bands were observed and assigned to the two-photon transitions from the ground state to a 2§ Rydberg state. The term value Te, vibrational frequency, and the rotational constant of the 2§ Rydberg state were determined. Another 2P state was observed near 312 nm.     

Photofragmentations, state interactions, and energetics of Rydberg and ion-pair states: two-dimensional resonance enhanced multiphoton ionization of HBr via singlet-, triplet-, Ω = 0 and 2 states

Mass spectra were recorded for one-colour resonance enhanced multiphoton ionization (REMPI) of H(i)Br (i = 79, 81) for the two-photon resonance excitation region 79,040-80,300 cm(-1) to obtain two-dimensional REMPI data. The data were analysed in terms of rotational line positions, intensities, and line-widths. Quantitative analysis of the data relevant to near-resonance interactions between the F(1)Δ(2)(v' = 1) and V(1)Σ(+)(v' = m + 7) states gives interaction strengths, fractional state mixing, and parameters relevant to dissociation of the F state. Qualitative analysis further reveals the nature of state interactions between ion-pair states and the E(1)Σ(+) (v' = 1) and H(1)Σ(+)(v' = 0) Rydberg states in terms of relative strengths and J' dependences. Large variety in line-widths, depending on electronic states and J' quantum numbers, is indicative of number of different predissociation channels. The relationship between line-widths, line-shifts, and signal intensities reveals dissociation mechanisms involving ion-pair to Rydberg state interactions prior to direct or indirect predissociations of Rydberg states. Quantum interference effects are found to be important. Moreover, observed bromine atom (2 + 1) REMPI signals support the importance of Rydberg state predissociation channels. A band system, not previously observed in REMPI, was observed and assigned to the k(3)Π(0)(v' = 0) ←← X transition with band origin 80,038 cm(-1) and rotational parameter B(v('))=7.238 cm(-1).