有机亚碘酰化合物的研究(Ⅲ)——不同取代基对取代亚碘酰苯中亚碘酰基IO的红外吸收波数■_(IO)的相关分析

本文研究了不同取代亚碘酰苯的IO基红外特征吸收峰■和■_s,分别为亚碘酰化合物聚合态结构中的反对称振动和对称振动。它们与取代基常数σ_I、σ_R~O、E_s间都存在着线性关系。     

N-甲基吡咯-2-甲醛激发态结构动力学及其溶剂效应的共振拉曼光谱和密度泛函理论研究

获取了覆盖N-甲基吡咯-2-甲醛(NMPCA)A-带和B-带电子吸收共7个激发波长的共振拉曼光谱,并结合含时密度泛函理论(TD-DFT)方法研究了的A-带和B-带电子激发和Franck-Condon区域结构动力学.TD-B3LYP/6-311++G(d,p)计算表明:A-带和B-带电子吸收的跃迁主体为π→π*.共振拉曼光谱可以指认为,11-13振动模式(A-带激发)或者7-11振动模式(B-带激发)的基频、倍频和组合频,其中C=O伸缩振动(ν7)、环的变形振动+N1-C6伸缩振动(ν17)、环的变形振动(ν21)和C6-N1-C2/C2-C3-C4不对称伸缩振动(ν14)占据了绝大部分.这表明NMPCA的Sπ激发态结构动力学主要沿C=O伸缩振动、环的变形振动和环上N1-C6伸缩振动等反应坐标展开.在同一溶剂的共振拉曼光谱中随激发波长由长变短,ν7与ν14的强度比呈现出由强变弱再变强的现象,这种变化规律被认为与Franck-Condon区域Sn/Sπ态混合或势能面交叉有关.溶剂对Sn/Sπ态混合或势能面交叉具有调控作用.     

特定条件下的定向ZnO纳米棒的制备及表征

采用改进的溶胶凝胶和化学溶液生长两步法, 并控制特定条件在镀银载玻片上制备出定向ZnO纳米棒. 利用X射线衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)、选区电子衍射(SAED)、能谱(EDS)及傅里叶红外吸收光谱(FTIR)对纳米棒的表面形貌、结构、组分进行分析. XRD和SEM结果表明该ZnO纳米棒具有六角纤锌矿结构, 结晶质量良好, 垂直衬底生长. TEM和SAED结果表明该ZnO纳米棒形状规则, 为单晶结构. FTIR谱中的位于418 和541 cm^－1的吸收峰对应于棒状ZnO结构的伸缩振动吸收峰, 1384 和1636 cm^－1对应于六方纤锌矿ZnO晶体的Zn—O伸缩振动吸收峰. 利用负离子配位四面体生长理论初步解释ZnO纳米棒的生长过程.     

金属羰基化合物氧原子转移反应——在PhIO存在下Cr(CO)6的CO取代反应动力学与机理的研究

亚碘酰苯作为氧原子转移试剂越来越引起人们的注意。Patton曾在PhIO存在的条件下合成了〔η~5-C_5(CH_3)_5ReCONOPPh_3〕BF_4,指出PhIO可能氧化消除了一个羰基。但有关PhIO与金属羰基化合物反应的动力学研究未见报道。为了解其反应性质,我们对在PhIO存在下Cr(CO)_6的取代反应进行了研究。     

水／AOT／正庚烷微乳体系中磺酸根水化作用的FT—IR研究

运用傅立叶变换红外光谱（FT－IR）对水／琥珀酸（乙基已基）磺酸钠（AOT）／正庚烷微乳体系中磺酸根的水化作用进行了研究．由于微乳体系中水分子与表面活性剂分子的相互作用，S＝O对称伸缩振动的红外吸收峰向低频方向移动．体系中的加水量W0（水与AOT的摩尔比）由0.5增大至25时，磺酸根对称伸缩振动的红外吸收峰由1051．39cm－1向低频移动至1046．15cm－1．同时，由于Na 的不对称作用，AOT分子中磺酸根反对称伸缩振动分裂成两个吸收峰，分别位于正215cm-1及1245cm－1附近，两个劈裂峰的距离及各自的峰面积均随体系中加水量的变化而变化，应用二阶导数、傅立叶退卷积及曲线拟会等分辨率增强技术可更清楚地反映出这个二重峰的变化情况．固体AOT分子中碳酸根反对称伸缩振动分裂的两个峰之间频率的差值约为42cm－1，形成微乳液以后，这两个峰的差值变小，W0为20时，这两个峰频率的差值逐渐减小到29cm-1，这些变化与磺酸根的水化程度直接相关     

模拟细胞色素P-450的仿生氧化反应的研究 I:氯合5,10,15,20-四苯基卟吩合铁(III)催化下不同亚碘酰芳烃及其衍生物的结构对环己烷充氧化反应的影响

在氯合5,10,15,20-四苯基卟吩合铁(III)[TPPFe(III)Cl]催化下, 带有不同取代基的亚碘酰苯和亚碘酰苯的衍生物作充氧化剂对环己烷进行了仿生单充氧化反应的研究.取代亚碘酰苯中对位取代基的电子效应和间位取代基的电子及立体效应对氧化产物环己醇的产率有良好线性相关性. 亚碘酰苯的衍生物苯亚碘酸二醋酐与苯亚碘酸单对甲苯磺酸酐对环己烷的充氧化能力和邻、间、对亚碘酰苯甲酸与邻亚碘酰苯甲酸酯相似, 环己醇产率接近零. 从而提出亚碘酰苯甲酸及邻亚碘酰苯甲酸酯存在分子内或分子间I(oh)oco成键结构的论点.     

CF_3I在238 nm的光解碎片平动能谱研究:CF_3光解碎片的振动态分布和势能曲线交叉穿越几率

利用高分辨弱电场加速型光解碎片平动能谱仪,对CF3I在238 nm的光解动力学进行了研究.结果表明,来自3Q0平行跃迁的I*通道[CF3I(X)hν→‖CF3I(3Q0)→CF3(ν1,ν2)+I*],信号最强,并可以分辨出碎片CF3(ν1,ν2)的振动峰.通过对峰间距的分析,可以基本分辨出同时具有CF3碎片的振动波带CF3(ν1,ν2=0)与CF3(ν1,ν2=1).其中ν1=701 cm-1为对称伸缩振动,ν2=1086 cm-1为CF3伞形振动.测量了这些振动态的分布及振动波带分配比为∑P(ν1,1)/∑P(ν1,0)=0.48/0.52.还测得238 nm处4个光解通道的分支比:通道1(X→3Q0→I*)为0.664,通道2(X→3Q0→1Q1→I)为0.084,通道3(X→1Q1→I)为0.178,通道4(X→1Q1→3Q0→I*)为0.074.实验结果表明,3Q0→1Q1过程中的势能曲线交叉穿越几率P0→1=0.112,1Q1→3Q0过程中P1→0=0.294;I*通道的各向异性参数β(I*)=1.70,I通道β(I)=-0.04.     

μ-氧-双四苯基卟吩合铁(Ⅲ)在CH_2Cl_2-氧化剂体系中的转化反应研究

本文报道了以CH_2Cl_2为溶剂,μ-氧-双四苯基卟吩合铁(Ⅲ)[(TPPFe)_2O]分别在亚碘酰苯(PhIO),H_2O_2和空气氧存在下转化为氯合、四苯基卟吩合铁(Ⅲ)(TPPFeCl)的反应.动力学初步研究表明在H_2O_2或PhIO存在下对(TPPFe)_2O为一级反应,而在空气氧中则为零级反应.反应速率常数与反应温度的关系符合Arrhenius方程式.根据动力学数据提出了该反应的可能机理.     

聚乙烯吡咯烷酮存在时反相微乳液中水的状态

运用傅立叶变换红外光谱（FTIR）研究不同分子量的聚乙烯吡咯烷酮（PVP）存在时,十二烷基甜菜碱(C12BE)/正庚烷 /正戊醇 /水（Ⅰ）及二（2 乙基）己基磺化琥珀酸钠（AOT）/正庚烷 /水（Ⅱ） 反相微乳液中水的存在状态.采用计算机分峰技术将微乳液中水分子的O－H伸缩振动进行曲线拟合, （Ⅰ）得到三个子峰,分别位于(3560±20)cm－1,(3430±10)cm－1,(3280±10)cm－1附近; （Ⅱ）得到四个子峰,分别位于3618 cm－1, 3550 cm－1, 3446 cm－1和3292 cm－1处.尽管PVP均增溶于W/O型微乳液中表面活性剂分子的极性基团附近,却没有引起长链间自由水的变化.但由于两体系的差异,PVP的存在,导致微乳液（Ⅰ）的本体水减少,结合水增多,却使体系（Ⅱ）的结合水减少,本体水增多.由于W/O型微乳液中水与生物膜中水相似,这些研究有助于理解生物膜界面上的生物化学和生物物理现象.     

密度泛函理论及光谱对CuCl2溶液中微团簇的研究

利用密度泛函理论和拉曼光谱对氯化铜溶液第一溶剂化层中的微团簇进行了研究。采用B3LYP方法对溶液中可能存在的团簇构型进行优化,从动力学和热力学方面分析得出溶液中团簇结构信息。理论拉曼光谱在100~500 cm~(-1)主要为Cu—O的伸缩振动峰,3400~4000 cm~(-1)范围内为O—H的对称和不对称伸缩振动。实验光谱在200~340 cm~(-1)出现明显新峰,位于2500~4000 cm-1的O—H伸缩振动峰随着溶液浓度的增加,峰的强度逐渐减小,峰形有明显变化。实验光谱和理论光谱验证和比对,表明溶液的实验光谱中产生的新峰为Cu—O振动,CuCl_2水溶液中产生短程离子相互作用及溶剂化现象,且随着溶液浓度的增加,溶剂化数目减小。     

磷脂酰胆碱与牛血清白蛋白相互作用的FT-IR研究

利用傅立叶变换红外(FT-IR)和拉曼(FT-Raman)光谱研究了高浓度磷脂酰胆碱(PC)与牛血清白蛋白(BSA)的相互作用,及Eu3＋对该作用的影响.FT-IR结果显示,PC/BSA混合体系中二者的相互作用主要发生在PC头部极性基团,且这一作用随BSA含量的增加而增强,作用后蛋白质二级结构中α螺旋的比例有所增加. FT-Raman光谱说明PC与BSA的相互作用影响磷脂CH链的排列有序程度. PC/BSA/Eu3＋体系的红外光谱显示, Eu3＋与PC的磷氧键发生了强相互作用,并使蛋白α螺旋的比例进一步增加.     

聚偏氟乙烯全反式分子链振动模式的研究

利用ab initio分子轨道计算,对β相聚偏氟乙烯(PVDF)的全反式分子链进行了结构优化,计算值和实验值基本符合,且发现C－C－C键角有两种不同的值,112.8°和113.3°.对该分子的频率进行了计算,得到了红外强度谱.在400～4 000 cm-1范围内,对30 μm厚的聚偏氟乙烯取向膜和取向极化膜进行了红外光谱的测量，红外吸收光谱和红外强度谱基本一致.把所有振动模式分成六个系列:系列Ⅰ（544～415 cm-1）,系列Ⅱ（913～792 cm-1）,系列Ⅲ（1 353～998 cm-1）,系列Ⅳ（1 458～1 361 cm-1）,系列Ⅴ和系列Ⅵ.其中只有系列Ⅲ能改变分子的电偶极矩,该系列振动模式和β相的PVDF的自发极化有着密切的关系.     

FT-Raman and infrared spectra and vibrational assignments for 3-chloro-4-methoxybenzaldehyde, as supported by ab initio, hybrid density functional theory and normal coordinate calculations

Fourier-transform laser Raman (3500-50 cm(-1)) and infrared (4000-400 cm(-1)) spectral measurements have been made for the solid 3-chloro-4-methoxybenzaldehyde. The electronic structure calculations -ab initio (RHF) and hybrid density functional methods (B3LYP and B3PW91) -- have been performed with 6-31G* and 6-311G* basis sets. Molecular electronic energies, equilibrium geometries, IR and Raman spectra have been computed. Potential energy distribution (PEDs) and normal mode analysis have also been performed. A complete assignment of the observed spectra has been proposed. Investigation of the relative orientation of the aldehydic oxygen and chlorine atom with respect to the methoxy group has shown that two forms, O-cis and O-trans exist, with O-trans form being more stable. The energy difference between O-cis and O-trans forms is 0.057 kcal/mol (21 cm(-1)) with B3LYP/6-31G*, which is less than the calculated torsional vibrational frequencies of the aldehyde and methoxy group. In the CH (O) aldehydic stretching region five observed bands are probably due to multiplet Fermi resonance. An infrared doublet near 1700 cm(-1) with nearly equal intensities has been ascribed to the Fermi resonance: the two bands at 1696 and 1679 cm(-1) arise due to the interaction between the CO stretching fundamental and a combination of O-CH(3) and CC stretching vibrations.     

稀土硝酸盐二甲亚砜络合物的振动光谱研究

合成了十四个稀土硝酸盐二甲亚砜络合物, 并对其振动光谱进行了系统的研究。对络合物的谱带进行了归属和讨论。对重镧系络合物中S=O伸展振动和Ln—O伸展振动的分裂归因于相同基团间的共振偶合。在络合物中, NO_3基组频1775 cm~(-1)因所属群发生变化而产生了分裂, 并可以此来确定NO_3基在络合物中的配位方式。指认了络合物中Ln—O键伸展振动频率, 其随稀土角动量的变化呈现“斜W”效应。     

Using MD snapshots in ab initio and DFT calculations: OH vibrations in the first hydration shell around Li+(aq)

The average OH stretching vibrational frequency for the water molecules in the first hydration shell around a Li(+) ion in a dilute aqueous solution was calculated by a hybrid molecular dynamics + quantum-mechanical ("MD + QM") approach. Using geometry configurations from a series of snapshots from an MD simulation, the anharmonic, uncoupled OH stretching frequencies were calculated for 100 first-shell OH oscillators at the B3LYP and HF/6-31G(d,p) levels of theory, explicitly including the first shell and the relevant second shell water molecules into charge-embedded supermolecular QM calculations. Infrared intensity-weighting of the density-of-states (DOS) distributions by means of the squared dipole moment derivatives (which vary by a factor of 20 over the OH stretching frequency band at the B3LYP level), changes the downshift from approximately -205 to -275 cm(-1) at the B3LYP level. Explicit inclusion of relevant third-shell water molecules in the supermolecular cluster leads to a further downshift by approximately -30 cm(-1). Our final estimated average downshift is approximately -305 cm(-1). The experimental value lies somewhere in the range between -290 and -420 cm(-1). Also, the absolute nu(OH) frequency is well reproduced in our calculations. "In-liquid" instantaneous correlation curves between nu(OH) and various typical H-bond strength parameters such as R(O...O), R(H...O), the intramolecular OH bond length, and the IR intensity are presented. Some of these correlations are robust and persist also for the rather distorted instantaneous geometries in the liquid; others are less so.     

The search for bishomoaromatic semibullvalenes and barbaralanes: computational evidence of their identification by UV/Vis and IR spectroscopy and prediction of the existence of a blue bishomoaromatic semibullvalene

Time-dependent B3LYP/6-31G calculations have been performed at the optimized C(2) or C(2v) geometries of several substituted semibullvalenes (1(deloc)) and barbaralanes (2(deloc)), to compare the computed vertical electronic excitation energies with the temperature-dependent, long-wavelength absorptions that have been observed in the UV/vis spectra of some of these compounds by Quast and co-workers. The excellent agreement between the calculated vertical excitation energies and the observed values of lambda(max) provides strong support for the identification of the bishomoaromatic species 1(deloc) and 2(deloc) as the source of these absorptions. Furthermore, the CN stretching frequencies, computed for the C(2) geometry of 1,5-dimethyl-2,6-dicyano-4,8-diphenylsemibullvalene (1f(deloc)), fit the low-frequency absorptions seen in the IR spectrum of 1f, thus furnishing independent evidence that bishomoaromatic geometries of semibullvalenes have, in fact, been observed spectroscopically. B3LYP/6-31G calculations predict that 2,6-dicyano-4,8-diphenylsemibullvalene 1c has a C(2) equilibrium geometry (1c(deloc)) and that the long-wavelength UV/vis absorption (lambda(max) = 585 nm) and CN stretching frequencies (2192 and 2194 cm(-1)) computed for 1c(deloc) should serve to identify this bishomoaromatic semibullvalene when it is synthesized.     

Catalytic sulfoxidation and epoxidation with a Mn(III) triazacorrole: evidence for a "third oxidant" in high-valent porphyrinoid oxidations

The reaction between (TBP)8(Cz)Mn(III) (1) and the oxygen atom donors iodosylbenzene (PhIO) or p-cyanodimethylaniline-N-oxide (CDMANO) leads to the manganese(V)-oxo complex (TBP)8(Cz)Mn(V)O (2), which has been isolated and characterized previously. Under catalytic conditions with 1 as added catalyst and PhIO as oxidant, both sulfoxidation of PhSMe and epoxidation of cis-stilbene is observed, whereas with CDMANO no sulfoxidation takes place, suggesting that 2 is not the active oxidant. Examination of the independent reactivity of isolated 2 toward PhSMe and cis-stilbene supports this conclusion. A mechanism which relies on a novel type of oxidant involving Lewis acid activation of PhIO by the Mn(V)-oxo complex 2 accounts for these observations and is confirmed by 18O-labeling experiments.     

红外光谱法研究重质油分子的轻度热转化

为了从分子水平快速经济地分析重质油在热转化过程中的变化规律，利用四种模型化合物萘、四氢萘、十氢萘和正庚烷组成的混合体系来模拟重质油及其热转化缩合产物分子的基本组成，研究其红外吸收特性与平均分子参数（亚甲基和甲基的数目之比 N CH2/NCH3、芳氢率faH、芳香环系氢碳原子比NHar/NCar等）的关系。将重质油焦化重蜡油馏分进行轻度热转化，利用不同强度的系列溶剂将热转化产物的重质馏分顺序分离成系列溶剂族组分，将这些族组分进行红外分析。结果表明，混合物系列模拟体系的〖ＷＴＢＸ〗f〖ＷＴＢ１〗aH同其红外吸收在2750cm－1～3100cm－1的3000cm－1～3100cm－1强度分率（S3000~3100/S2750~3100）之间存在良好的线性关系，同时NCH2/NCH3 同2920cm－1和2960cm－1处的吸光度比值A2920/A2960之间也存在良好的线性关系。依据这些关系式可以合理解释重质油分子在热转化过程中分子结构的变化规律。随着重质油热转化的进行，NCH2/NCH3 饱和烃分子先增大后减小，芳香性族组分分子则持续降低；faH或NHar/NCar芳香性族组分分子呈现升高的趋势。     

Raman spectroscopic study of the tellurite minerals: rajite and denningite

Tellurites may be subdivided according to formula and structure. There are five groups based upon the formulae (a) A(XO3), (b) A(XO3).xH2O, (c) A2(XO3)3.xH2O, (d) A2(X2O5) and (e) A(X3O8). Raman spectroscopy has been used to study rajite and denningite, examples of group (d). Minerals of the tellurite group are porous zeolite-like materials. Raman bands for rajite observed at 740, and 676 and 667 cm(-1) are attributed to the nu1 (Te2O5)(2-) symmetric stretching mode and the nu3 (TeO3)(2-) antisymmetric stretching modes, respectively. A second rajite mineral sample provided a more complex Raman spectrum with Raman bands at 754 and 731 cm(-1) assigned to the nu1 (Te2O5)(2-) symmetric stretching modes and two bands at 652 and 603 cm(-1) are accounted for by the nu3 (Te2O5)(2-) antisymmetric stretching mode. The Raman spectrum of dennigite displays an intense band at 734 cm(-1) attributed to the nu1 (Te2O5)(2-) symmetric stretching mode with a second Raman band at 674 cm(-1) assigned to the nu3 (Te2O5)(2-) antisymmetric stretching mode. Raman bands for rajite, observed at (346, 370) and 438 cm(-1) are assigned to the (Te2O5)(2-)nu2 (A1) bending mode and nu4 (E) bending modes.     

Theoretical modeling of the O-H stretching IR bands of hydrogen-bonded dimers of benzoic acid in S(0) and S(1) electronic states

Theoretical model for vibrational interactions in the hydrogen-bonded dimer of benzoic acid is presented. The model takes into account anharmonic-type couplings between the high-frequency O-H and the low-frequency O[cdots, three dots, centered]O stretching vibrations in two hydrogen bonds, resonance interactions (Davydov coupling) between two hydrogen bonds in the dimer, and Fermi resonance between the O-H stretching fundamental and the first overtone of the O-H in-plane bending vibrations. The vibrational Hamiltonians and selection rules for the C(2h) geometry in the S(0) state and for the C(s) in-plane bent geometry in the S(1) state of the dimer are derived. The model is used for theoretical simulation of the O-H stretching IR absorption bands of benzoic acid dimers in the gas phase in the electronic ground and first excited singlet states. Ab initio CIS and CIS(D)6-311++G(d,p) calculations have been performed to determine geometry, frequencies, and excited state energies of benzoic acid dimer in the S(1) state.