镨叶绿素a分子结构的确定

通过合成镨叶绿素a(Pr-Chla)研究了稀土在叶绿素中的结合方式.Pr-Chla的紫外可见光谱(UV-Vis)、红外光谱(FTIR)证实镨离子已配位到叶绿素a的卟啉环上.其磁圆二色谱(MCD)在Soret带具有双层夹心卟啉的特征结构;通过扩展X射线吸收精细结构谱(EXAFS),采用双层夹心结构模型拟合,确定了Pr周围的近邻结构.表明合成镨叶绿素a具有双层夹心结构.Pr(Ⅲ)夹于两个卟啉环之间,与上下卟啉环上共8个N原子配位,Pr-N键平均键长0.242nm.     

咪唑钴啉酯的合成及钴—氮键稳定性的研究

合成了维生素B_(12)(VB_(12))模型分子—单腈N-甲基3-咪唑基钴啉酯高氯酸盐8。通过8在不同pH缓冲溶液中的UV-Vis谱,计算了Co—N键的平衡常数,独立配位体N-甲基咪唑与咕啉环中心钴原子配位键的键强与自身键连配位体的配位键强要弱。     

叶绿素稀土配位结构的EXAFS研究: 镧叶绿素a双层夹心分子 结构的确认

通过合成镧叶绿素a(La-Chla),研究稀土在叶绿素中的赋存状态。La-Chla的紫外可见光谱(UV-vis)、红外光谱(FT-IR)证实,镧离子已配位到叶绿素a的卟啉环上。其磁圆二色谱(MCD)在Soret带具有双层夹心卟啉结构的特征结构。通过扩展X射线吸收精细结构谱(EXAFS),采用双层夹心结构模型拟合,确定La周围的近邻结构,取得满意结果。表明合成镧叶绿素a具有双层夹心结构。La夹于两个卟啉环之间,与上下卟啉环上共八个N原子配位,La-N平均键长0.261nm。     

时间域方法分析镍卟啉的共振拉曼强度与S2激发态结构

研究了入射光波长与S0→S2跃迁共振的情形下,卟啉镍配合物（NiP）的振动拉曼光谱。用时间域方法计算了NiP的共振拉曼强度和吸收光谱。结果表明,相对于基态,S2态NiP的分子构型沿着ν8和ν2简正坐标有较大的位移。这些简正坐标主要涉及卟啉环的CαCm键和CβCβ键伸缩运动,以及CαCmCα变角运动。与基态相比, S2态的CβCβ、 CαCm和CαN键分别增大0.27、 0.14、 0.07 pm,而CαCβ键则减小0.20 pm,与前人的赝势分子轨道计算（SPMO）结果相近。还从RR强度角度讨论了S2态的Jahn-Teller畸变。     

非水介质中金属卟啉电化学

本文概述在非水介质中合成金属卟啉络合物的电化学。总结反应机理与金属卟啉的氧化和还原的关系,阐明半波电位及电子转移途径与一些因数的关系,如取代基效应,与氮基的轴向配位体配位,与卤素阴离子的轴向配位体配位,与二原子分子的轴向配位体配位,卟啉环体系的特性结构(即立栅式卟啉等),卟啉环的碱度,与溶剂的氢离子键合等。     

X-H (X = C, N, O, Si, P, S) 键离解能计算的密度泛函方法研究

使用了不同密度泛函方法计算X-H (X = C, N, O, Si, P, S) 键离解能，并分析不同密度泛函方法的计算精度。研究发现大多数密度泛函方法包括B3LYP, B3P86, B3PW91, G96LYP, PBE1PBE，和BH&HLYP都明显低估键离解能13-25 kJ/mol。该现象与是否使用无限基组无关，因为即使使用无限基组键离解能仍然被低估。因此密度泛函方法不适合用于键离解能的估算。其中B3P86方法的偏差最小。进一步分析表明，使用限制性开壳层计算并无任何优势，在大多数情况下非限制性开壳层计算实际上比限制性开壳层计算要好。最后，我们发现了密度泛函方法对键离解能的低估是系统的，因此建议利用校准后的UDFT/6-311++G(d, p)方法计算化学键离解能。     

取代氯苯化合物的电子结构和键离解能的理论研究

利用密度泛函（DFT）三种交换／相关函数（B3LYP,B3PW91,B3P86）结合6—31G^＊＊和 6-311G^＊＊基组,计算了13个取代氯苯化合物的键离解能．结果表明B3PS6／6—311G^＊＊方法是计算取代氯苯化合物键离解能的可信方法,研究发现C—Cl键的键离解能与所使用的基组和计算方法密切相关,取代基对C—Cl键的键离解能的影响不明显．研究了目标化合物的前线轨道能级差,并对取代氯苯化合物的热稳定性做了评估．     

氮磷配位的钛酸酯络合物的X射线光电子能谱研究

制备了单烷基羧酸型和磺酸型钛酸酯氮配位与磷配位的配合物.用XPS法证明有N→Ti或P→Ti配位键生成,并从化学位移量推测了键的强度,磺酸型较羧酸型易配位,羟基取代胺的氮配体配位较容易发生;磷配位由于存在Ti→P的反馈作用,使化学位移不如氮配位明显.此外,异丙基钛酸酯与乙醇胺的反应物,证明分子内有N→Ti配位键生成.     

界面缩聚法合成聚卟啉金属配合物及其表征

利用对苯二甲酰氯交联meso-5,10,15,20一四（对羟基苯基）卟啉单体制备了聚卟啉配体及其Co（Ⅱ）、Mn（II）和Zn（Ⅱ）金属配合物,并对聚卟啉配体和金属配合物进行了红外光谱、扫描电镜和X射线光电子能谱分析。结果表明,卟啉单体是典型的晶体结构,而发生界面聚合过程中以平面二维方式进行,形成膜状聚合物;当金属离子与卟啉形成配合物后,其中一对N—H键中质子被配位金属取代,N1s轨道的电子结合能变化小于0．2eV,环中另外两个N原子与配位金属形成σ配位键,导致配位金属M2p3／2的电子结合能变化大于0．5eV,引起了卟啉环内层电子密度的变化。     

咪唑钴啉酯的合成及钴-氮键稳定性的研究

合成了维生素B~1~2(VB~1~2)模型分子-单腈N-甲基3-咪唑基钴啉酯高氯酸盐8。通过8在不同pH缓冲溶液中的UV-Vis谱,计算了Co-N键的平衡常数,独立配位体N-甲基咪唑与咕啉环中心钴原子配位键的键强与自身键连配位体的配位键强要弱。     

Highlevel ab initio and hybrid density functional theory study of the energy profile for the CO+CO reaction

Two complete basis set and three hybrid density functional computational studies were applied in the exploration of the ¹CO+²CO⁺ reaction potential energy surface. One molecular carbon monoxide–carbon monoxide cation molecular associate was elucidated as the structure with the lowest energy on the potential energy surface. Ionization energies, bond dissociation energies, and enthalpies of formation for every di and tri-atomic molecule on the potential energy surface were estimated with the two complete basis sets and the three hybrid density functional theory methods. Six different endothermic channels for the ¹CO+²CO⁺ reaction were evaluated with ab initio and DFT methods. The computed energies and structural parameters are compared with experimental values where available. Some new energies for this reaction system were suggested.     

B2F2分子异构体结构的量子化学计算研究

采用abinitio方法对B₂F₂分子异构体的结构进行了计算研究,并与Al₂F₂分子进行了比较.结果表明,B₂F₂具有D_∞h对称性,³Σ_g电子态的直线型结构FBBF是B₂F₂分子的最稳定异构体,对文献的结果进行了修正.在UCCSD(T,full)/6－311+G(2df)水平下,F-B和B-B键长分别为0.12942和0.14820nm,振动频率出现在1860.00和1320.62cm^-1处.在UQCISD(T,full)/6－311+G(2df)//UMP2(full)/6－311+G(d)+ZPVE水平下,³Σ_g态的线性FBBF分子的垂直电离势为848.58kJ/mol,而由³Σ_g电子态的BF二聚为³Σ_g态的线性FBBF分子的焓变为59.86kJ/mol,此二聚化反应是放热反应,说明二聚化过程在能量上是有利的.     

Simplified models for anharmonic numbers and densities of vibrational states. I. Application to NO2 and H3

Numbers and densities of vibrational states of non-rotating polyatomic molecules are calculated by a simplified model which accounts for Morse anharmonicities of stretching and for generalized empirical stretch-bend couplings of bending modes. At energies above the dissociation limit, adiabatic channel maxima restrict the molecular phase space. The model is applied to the NO₂( 2A₁), NO₂(Ã ²B₂), and H₃⁺ systems for which satisfactory agreement with the available experimental or calculational results is obtained.     

Theoretical determination of the ionization potentials of the 1σ and 2σ electrons of CO(Σ)

Large-basis-set calculations of near Hartree-Fock accuracy were performed on CO⁺(1σ-hole ²Σ⁺) and CO⁺)2σ-hole, ²Σ⁺); correlation energies for these systems and for CO were calculated using an atoms-in-molecule approach, relativistic energies and vibrational structure corrections were also considered. The results are: IP(CO, 1σ) = 542.4 (542.57) eV, IP(CO,2σ) = 297.0 (296.24) cV, D_c(CO, ¹Σ⁺) = 10.8 (11.1) Ev, D₃(CO⁺, 1σ, ²Σ⁺) = 11.9 eV, D_e(CO⁺, 2σ, ²Σ⁺) = 9.1 eV, where IP and D_e stand respectively for ionization potential and dissociation energy, and where the numbers in parentheses refer to the most recent experimental values. The electron transfers resulting from the ionization of inner-shell electrons are discussed. Finally a quantitative correlation is developed correlating absolute chemical shifts to charge densities. Agreement between the calculated values and those derived from the correlation is quite satisfactory.     

次氟酸分子的势能函数及其振动光谱的同位素效应的理论研究

用三原子振动激发态的变分计算程序(TRIATOM)精确计算次氟酸分子H¹⁶OF的振动激发态的能级以及次氯酸分子中的H和O分别被D和¹⁸O取代后的H¹⁸OF,D¹⁶)OF和D¹⁸OF的同位素效应,理论计算值与已有的实验结果吻合较好。预测了一些尚未观测到的谱线频率及同位素效应,并确立了一个同位素位移的加和规则。     

外电场作用下离子液体振动光谱变化的分子动力学模拟研究

Vibrational spectroscopy is a powerful tool for studying the microstructure of liquids, and anatomizing the nature of the vibrational spectrum (VS) is promising for investigating changes in the properties of liquid structures under external conditions. In this study, molecular dynamics (MD) simulations have been performed to explore changes in the VS of 1-ethyl-3-methylimidazolium hexafluorophosphate ([Emim][PF₆]) ionic liquid (IL) under an external electric field (EEF) ranging from 0 to 10 V·nm^-1 at 350 K. First, the vibrational spectra for [Emim][PF₆] IL as well as its cation and anion are separately obtained, and the peaks are strictly assigned. The results demonstrate that the VS calculated by MD simulation can well reproduce the main characteristic peaks in the experimentally measured spectrum. Then, the vibrational spectra of the IL under various EEFs from 0 to 10 V·nm^-1 are investigated, and the intrinsic origin of the changes in the vibrational bands (VBs) at 50, 183, 3196, and 3396 cm^-1 is analyzed. Our simulation results indicate that the intensities of the VBs at 50 and 183 cm^-1 are enhanced. In addition, the VB at 50 cm^-1 is redshifted by about 16 cm^-1 as the EEF is varied from 0 to 2 V·nm^-1, and the redshift wavenumber increases to 33 cm^-1 as the EEF is increased to 3 V·nm^-1 and beyond. However, the intensities of the VBs at 3196 and 3396 cm^-1 show an obvious decrease. Meanwhile, the VB at 3396 cm^-1 is redshifted by about 16 cm^-1 when the EEF increases to 3 V·nm^-1, and the redshift increases to 33 cm^-1 with an increase in the EEF beyond 4 V·nm^-1. The intensity of the VB at 50 cm^-1 increases because of the increase in the total dipole moment of each anion and cation (from 4.34 to 5.46 D), and the redshift is attributed to the decrease in the average interaction energy per ion pair (from -378.7 to -298.0 kJ·mol^-1) with increasing EEF. The intensity of the VB at 183 cm^-1 increases on account of the more consistent orientations for cations in the system with increasing EEF. The VB at 3196 cm^-1 weakens visibly because a greater number of hydrogen atoms appear around the carbon atoms on the methyl/ethyl side chains and the vibrations of the corresponding carbon-hydrogen bonds are suppressed under the action of the EEF. Furthermore, the intensity of the VB at 3396 cm^-1 decreases due to the decrease in the intermolecular ⁺C-H···F^- hydrogen bonds (HBs), while the relaxation effect that is beneficial for the formation of HBs simultaneously exists in the system under the varying EEF, thus causing a redshift of the VB at 3396 cm^-1.     

超高分子量聚乙烯的红外光谱的特性研究

研究了超高分子量聚乙烯(M_w>1×10⁵)的红外光谱-温度特性.3条非晶谱带(1368、1352和1304cm^-1)的吸收强度均随温度升高而增大,但都比普通分子量聚乙烯增加的小,尤以高于140℃更甚.分子链中次甲基的近程构象序列分布随温度的变化不受分子量的影响,但旁式构象序列分布则随温度升高而增大.升温和降温过程的红外光谱均表明1352和1304cm^-1两谱带随结晶状态的变化比1368cm^-1更敏感.     

Determination of picogram amounts of 99tc by neutron activation analysis

A post-irradiation procedure for the determination of picogram amounts of ⁹⁹Tc in triply distilled water is described. The ⁹⁹Tc is irradiated in a thermal neutron flux of about 5.10¹³ n cm^-2 sec^-l to produce 16-sec ¹⁰⁰Tc. The chemical purification of the ¹⁰⁰Tc from other radionuclides requires 40–45 sec and the technetium yield is about 53%. The purified ¹⁰⁰Tc is counted in a low-background β-counter.     

Ordering effects of cholesterol on sphingomyelin monolayers investigated by high-resolution broadband sum-frequency generation vibrational spectroscopy

After adding cholesterol, the sphingosine backbones (red) of the three nature SMs become more ordered, and the N-linked acyl chain (blue) remains unaltered.     

An ab initio close-coupling calculation of the lower vibrational energies of the HCl dimer

We have previously determined an analytical ab initio six-dimensional potential energy surface for the HCl dimer, and in the present paper we use this potential, with the HCl bond lengths held fixed, in a full (four-dimensional) close-coupling calculation to determine the energies of the lowest 24 vibrational states. These vibrational states involve the intermolecular stretch ν₄, the trans-bend tunneling vibration ν₅, and the torsion ν₆. The highest of the 24 levels is the (ν₄ν₅ν₆)=(111) state, for which we calculate an energy of 200 cm⁻¹ above the (000) state. As well as determining tunneling energies up to 5ν₅=183 cm⁻¹, we determine ν₄=49 cm⁻¹, 2ν₄=93 cm⁻¹, 3ν₄=134 cm⁻¹, 4ν₄=172 cm⁻¹, ν₆=137 cm⁻¹ and ν₄+ν₆=178 cm⁻¹, together with tunneling energies in all these states. Making allowance for the HCl stretching zero-point energy we determine the dissociation energy D₀ as 390 cm⁻¹ on this analytical surface. We determine that below 300 cm⁻¹ there are 72 vibrational (J=K=0) states, and below dissociation there are 162 vibrational (J=K=0) states, for this potential surface.