K3Na(FeO4)2的电合成及其晶体结构

本文采用间接法电合成出较高纯度的复盐K₃Na(FeO₄)₂晶体，用粉末XRD结构分析法对其晶体结构作了详细研究。用EDX和AAS确认了其化学式。结构分析表明，K₃Na(FeO₄)₂晶体属三方晶系，具有六方晶胞，空间群为P3m1(No.164)，Z=1,晶胞中有6个O位于6(i)位，O,Fe和K各自有2个位于2(d)位，1个K和Na分别位于1(b)位和1(a)位，晶胞参数a=0.583 3(1) nm,c=0.755 9(1) nm，D=2.824 g·cm^-3。同时晶胞中各原子间化学键键长得到确定。     

大气中HSO-3异构体的“量子化学后”研究

在量子化学计算的基础上，用统计热力学方法，计算了亚硫酸氢根离子的两种异构体HOSO^-₂(C_S)和HSO^-₃(C₃V)的热力学性质及它们相互转化的平衡常数(相对稳定性随温度的变化)等。通过计算数据的回归分析，给出了摩尔熵、摩尔热容等随温度变化的表达式。     

两个手性氧钒配合物[VO(Naph-Leu)(OMe)(CH3OH)] 和[VO(Naph-Phe)(OMe)(CH3OH)] 的合成、晶体结构和光谱表征

合成了2个新的手性L-亮氨酸萘酚醛和L-苯丙氨酸萘酚醛希夫碱氧钒配合物, [VO(Naph-Leu)(OMe)(CH₃OH)] (1)和[VO(Naph-Phe)(OMe)(CH₃OH)] (2)。X-射线单晶衍射分析表明, 1晶体属于正交晶系, P2₁2₁2空间群, 晶胞参数为:a=0.946 80(8) nm, b=3.246 3(3) nm, c=0.662 37(5) nm, V=2.035 9(3) nm³, Z=4, F(000)=864, R₁=0.046 3, wR₂=0.112 7, S=1.076。2晶体属于单斜晶系, P2₁空间群, 晶胞参数为:a=1.113 41(11) nm, b=0.724 09(6) nm, c=1.342 99(12) nm, V=1.047 95(16) nm³, Z=2, F(000)=464, R₁=0.035 8, wR₂=0.088 8, S=1.024。测定了它们的红外光谱、紫外光谱和圆二色光谱, 讨论了紫外吸收光谱和圆二色光谱性质。     

原子簇FenB2(n=1～6)结构和性质的DFT研究

本文对上百个Fe_nB₂和Fe_n(n=1～6)原子簇模型进行密度泛函理论计算，用来模拟非晶态合金Fe-B体系的局域结构，并考察类金属元素硼的引入对体系性质的影响。将优化构型的键长和电荷分布与实验数值进行比较，发现本文所使用的原子簇模型在一定程度上可以真实、准确地反映非晶态合金Fe-B体系的局域结构。利用这些构型，我们对其键级、电子、催化以及磁学性质进行了讨论。结果表明：原子簇中均存在着强烈的Fe-B键作用，其中在高铁含量原子簇中Fe-Fe键的作用也较为明显；综合热力学、费米能级及态密度的研究结果，发现原子簇Fe₄B₂在合成氨和固氮过程中有可能表现出更为优越的催化活性。结合对原子簇Fe_n和Fe_nB₂(n=1～6)平均3d轨道布居数的分析，发现原子簇Fe_nB₂(n=1～6)的平均磁矩均小于相应原子簇Fe_n(n=1～6)的理论数值和纯金属铁的实验数值(5.7～6.0 BM)，也就是说原子簇Fe_nB₂(n=1～6)均表现出软磁性。     

双(三有机锡)2，3-吡啶二甲酸酯的合成、表征和体外抗癌活性

合成了2个新的双(三有机锡)2，3-吡啶二甲酸酯2，3-C₅H₃N(CO₂SnR₃)₂ (R=c-C₆H₁₁，1；C₆H₅C(CH₃)₂CH₂，2)，利用元素分析、IR和¹H NMR表征了其结构。通过X-射线单晶衍射测定了配合物2的晶体结构。该化合物晶体属单斜晶系，空间群P2₁/n，a=0.955 3(1)，b=1.811 8(2)，c=3.533 9(4) nm，β=94.914(2)°，Z=4，V=6.094 1(13) nm³，R=0.038 4，wR=0.096 6，S=1.015。2，3-吡啶二甲酸的2个羧基键连2个三有机锡，2个锡原子均为畸变的四面体配位构型。生物活性测试结果表明，化合物1和2对3种人癌细胞HeLa、CoLo205和MCF-7具有好的体外抗癌活性。     

La（Ⅲ）、Nd（Ⅲ）与甜菜碱类衍生物形成的包含（H2O）6分子簇的配合物的晶体结构

利用配体1,5-二（3-羧基吡啶基）-N-甲基二乙胺（L）合成2种稀土金属配合物{[La₂L₄（H₂O）₂]（ClO₄）₆·6H₂O}_n（1）和[Nd₂L₄（DMF）₆（H₂O）₂]₂（ClO₄）₆·4H₂O（2）。用红外光谱和X-射线单晶衍射表征配合物的晶体结构。结构分析表明：配合物1属于三斜晶系,P1空间群,其晶胞参数为a=1.4966（3）nm,b=1.5597（4）nm,c=1.9568（4）nm,α=86.776（6）°,β=77.723（7）°,γ=87.168（7）°,Z=2。在配合物1中,一对La（Ⅲ）原子被2个羧基桥联,形成双核结构;双核结构进一步被羧基连接,从而形成平行于c轴的一维链。值得注意的是配合物1的晶体结构中包含着由氢键连接的6个H₂O分子组成的水分子簇。配合物2属于三斜晶系,P1空间群,晶胞参数为a=1.0408（4）nm,b=1.3541（5）nm,c=2.975（1）nm,α=94.390（8）°,β=91.720（7）°,γ=95.230（4）°,Z=2。配合物2中4个羧基连接一对Nd（Ⅲ）原子,形成四轮状结构,其中2个羧基采取syn-syn双原子桥联模式,而其余2个羧基则采取单原子桥联模式。     

S2N2环桥连配合物的MO研究

本文根据MAD-SCC-EHMO法的计算结果，对典型硫氮环S₂N₂与过渡金属单啮和双啮桥连的配合物的电子结构和成键情况做了研究。用衡量相对稳定性的三个指标：稳定性能，HOMO-LUMO能隙和重迭布居比较了1∶2，1∶1和2∶1型配合物的稳定性，并用碎片分子轨道法分析了S₂N₂环的分子轨道与过渡金属d轨道间的相互作用。     

一维双核锌配合物[Zn2(SHSH)2(2-Me-py)2]的合成、晶体结构及理论研究

The crystal of one-dimensional binuclear zinc complex [Zn₂(SHSH)₂(2-Me-py)₂] was obtained in DMF and 2-methylpyridine, where SHSH is salicylaldehyde salicylhydrazone. It has been characterized by IR, UV, element analysis and X-ray diffraction analysis. The crystallographic data were as follows: monoclinic system, space group P2₁/c, a=1.144 49 nm, b=1.206 69 nm, c=1.379 39 nm, β=97.039°, Z=2, V=1.890 6 nm³, M_r=825.47, D_c=1.450 g·cm^-3, μ=1.324 mm-1, F(000)=848 and the final R=0.033 6 and wR=0.094 7 for 3 752 observed reflections with I≥2σ(I). The theoretical investigation of title complex as a structure unit was carried out at B3LYP/6-31G and HF/6-31G levels with Guassian 03W program, and the atomic charges, natural bond orbital analysis and bond energies were also discussed. CCDC: 260920.     

具有强绿色荧光发射效应的2，2′-二硝基4，4′-联苯酸铀(Ⅵ)配聚物

A very complex 3D Uranium(Ⅵ) metal-organic framework was obtained by the hydrothermal treatment of UO₂(NO₃)₂·6H₂O with (R，S)-2，2′-dinitro-biphenyl- 4，4′-dicarboxylic acid (BTNCA) (L) in water at 180 ℃ in Pyrex tubes. The crystal belongs to monoclinic system with space group P2₁/c， and a=0.545 90(3) nm， b=3.676 01(18) nm， c=2.659 81(13) nm， β=91.4060(10)°， V=5.335 9(5) nm³， Z=4. CCDC: 659615.     

过渡金属配合物为模板合成两个新的硫代锡酸盐(英)

利用溶剂热方法在温和的条件下合成了二个新的硫代锡酸盐[Mn(en)₃]₂Sn₂S₆·2H₂O(en=H₂NC₂H₄NH₂) (1)和[Mn(dien)₂]₂Sn₂S₆ (dien=H₂NC₂H₄NHC₂H₄NH₂) (2)，通过X-射线衍射分析表征其晶体结构。化合物1的晶体学参数：C₁₂H₄₈Mn₂N₁₂S₆Sn₂·2H₂O，M_r=936.28，单斜晶系，P2₁/c，a=1.012 9(3)，b=1.574 6(4)，c=1.152 4(3) nm，β=102.36(1)°，V=1.795 5(8) nm³，Z=2，D_c=1.732 g·cm^-3，μ(MoKα)=2.442 mm^-1，F(000)=940，R=0.063 3，wR=0.081 4；化合物2的晶体学参数：C₁₆H₅₂Mn₂N₁₂S₆Sn₂，M_r=952.32，单斜晶系，P2₁/c，a=1.248 12(3)，b=0.937 60(4), c=1.776 17 (7) nm，β=121.752(2)°，V=1.767 5(1) nm³，Z=2，D_c=1.789 g·cm^-3，μ(MoKα)=2.479 mm^-1，F(000)=956，R=0.057 9，wR=0.137 4。在两个化合物中存在的[Sn₂S₆]^4-阴离子均由共边的两个SnS₄四面体构成。在1中，锰离子螯合3个乙二胺做为阳离子模板，而在2中锰离子螯合2个二乙烯三胺做为阳离子模板。金属配合物作为模板对阴离子[Sn₂S₆]^4-在晶体结构中的排列产生重要的影响。     

Raman and structural characterization of LuAlO3

The structural and vibrational properties of lutetium orthoaluminate perovskite (LuAlO₃) were investigated by means of Raman spectroscopy and EXAFS measurements.The analysis of Raman spectra taken in four different polarized configurations along the principal axes at 20 K and room temperature conditions permits to assign the principal vibrational modes in LuAP single crystals and to confirm the belonging to the D_2h¹⁶ space group.EXAFS measurements were performed at room temperature in order to obtain local structural informations on the first and next nearest neighbors around lutetium absorptions sites. Unit cell parameters and bond lengths were determined by the analysis of the EXAFS spectroscopy at the L₃ absorption edge of lutetium.The informations thus gathered on this compound can offer a useful addition in the framework of a full structural characterization of LuAlO₃.     

Polarised IR and Raman spectra of non-centrosymmetric Na3Li(SeO4)2.6H2O crystal--a new Raman laser material

Polarised IR and Raman spectra of Na₃Li(SeO₄)₂·6H₂O single crystal have been recorded. Discussion of the results has been based on the factor group approach for the trigonal R3c (C_3v⁶) space group with Z = 2. The obtained results for the spontaneous Raman scattering have been used in the discussion of the stimulated Raman spectra of the material studied—a new Raman laser crystal.     

Raman Spectroscopy of Oxides of GaAs Formed in Solution

Electrochemical treatment of crystalline GaAs in 1 M HCl results in the formationof porous GaAs. As a by-product of the electrochemical dissolution process,small transparent crystals may grow on the porous GaAs skeleton under certainchemical conditions. These surface crystalline deposits have been investigatedby Raman scattering spectroscopy. From surface chemical analysis and byreference to the Raman spectra of appropriate chemical compounds, it was determinedthat the crystallites comprise As₂O₃ and Ga₂O₃.Their Raman spectra and that of As₂O₅ · xH₂Oare presented here for the first time in detail.     

Combination of Resonance and Non-Resonance Chiral Raman Scattering in a Cobalt(III) Complex

Resonance Raman optical activity (RROA) spectra with high sensitivity reveal details on molecular structure, chirality, and excited electronic properties. Despite the difficulty of the measurements, the recorded data for the Co(III) complex with S,S-N,N-ethylenediaminedisuccinic acid are of exceptional quality and, coupled with the theory, spectacularly document the molecular behavior in resonance. This includes a huge enhancement of the chiral scattering, contribution of the antisymmetric polarizabilities to the signal, and the Herzberg-Teller effect significantly shaping the spectra. The chiral component is by about one order of magnitude bigger than for an analogous aluminum complex. The band assignment and intensity profile were confirmed by simulations based on density functional and vibronic theories. The resonance was attributed to the S₀→S₃ transition, with the strongest signal enhancement of Raman and ROA spectral bands below about 800 cm⁻¹. For higher wavenumbers, other excited electronic states contribute to the scattering in a less resonant way. RROA spectroscopy thus appears as a unique tool to study the structure and electronic states of absorbing molecules in analytical chemistry, biology, and material science.     

Structural and low temperature Raman scattering studies in SrTi<Subscript>1−<Emphasis Type="Italic">x</Emphasis></Subscript>Co<Subscript><Emphasis Type="Italic">x</Emphasis></Subscript>O<Subscript>3</Subscript> nanoparticles synthesized by sol–gel method

We investigate effects of Co dopant concentration on the structure and low temperature Raman scattering properties in SrTi_1−x Co _x O₃ (x = 0.00, 0.10, 0.20, 0.30) nanoparticles prepared by sol–gel method. The dopant induced changes are studied by XRD, and Raman scattering measurements. The results show an average particle size of about 20 nm depending on the Co content and the lattice parameters decrease as increasing the Co content. In the Raman spectra, a broad structure in the region 100–500 cm⁻¹ is almost absent and the peaks in the region 600–800 cm⁻¹ show different weights with respect to SrTiO₃, relating to structural changes. The anomalous change in the area ratio of Raman peaks as function of temperature suggests a phase transition in our samples in the range of 110–130 K. These results indicate that the Co ion has replaced the site of Ti in unit cell. This novel route also demonstrates the advantage of synthesizing the compound with low annealing temperature.     

Insights into photoluminescence property and photocatalytic activity of cubic and rhombohedral ZnIn2S4

Cubic and rhombohedral ZnIn₂S₄ were synthesized by thermal sulfidation of Zn-In mixed oxide precursor in H₂S atmosphere at different temperatures. Cubic ZnIn₂S₄ was obtained when Zn-In mixed oxide precursor was sulfurized at 400 °C. With sulfidation temperature increasing from 400 to 800 °C, the crystal phase of ZnIn₂S₄ gradually turned from cubic to rhombohedral, which was demonstrated by different analysis techniques such as XRD, Raman, SEM, etc. UV-vis absorption spectra indicated that cubic ZnIn₂S₄ displayed better light absorption property than rhombohedral ZnIn₂S₄, with band gaps calculated to be 2.0 and 2.5 eV, respectively. However, under visible light irradiation, rhombohedral ZnIn₂S₄ photocatalyzed H₂ evolution from aqueous sodium sulfite/sulfide solution efficiently, whereas cubic ZnIn₂S₄ was not active for this reaction. The photoluminescence property revealed the different dynamics of photogenerated carriers, which made a predominant contribution to the increasing photocatalytic performances of ZnIn₂S₄ with crystal phase turning from cubic to rhombohedral.     

A complex of buckminsterfullerene with sulfur,C60·2S8: synthesis and crystal structure

The C₆₀·2S₈ complex was prepared by reaction of buckminsterfullerene C₆₀ with sulfur in trichloroethylene and its single-crystal X-ray structure was studied at room temperature. Crystals of this compound are monoclinic, space groupC 2/c, a=20.90(1),b=21.10(1),c=10.537(9) Å, =111.29(7)°,Z=4,d _calc=1.89 g·cm^–3. The crystal structure of the C₆₀·2S₈ complex consists of packed fullerene molecules that form hexagonal channels along thec axis with eight-membered crown-shaped S₈ cyclic molecules inside the channels. The distances between the centers of neighboring fullerene molecules are 10.036(7), 10.636(7), and 10.537(9) Å. Each C₆₀ molecule is linked to eight S₈ molecules with ten shortened intermolecular contacts C...S 3.41(1)–3.52(2) Å. The average values of the C=C and C-C bond lengths are 1.32(3) and 1.47(3) Å, which attest to a significant degree of localization of electron density in the c₆₀ molecule.Translated from Izvestiya Akademii Nauk. Seriya Khimicheskaya, No. 2, pp. 262–266, February, 1994.     

Theoretical study on contribution of charge transfer effect to surface-enhanced Raman scattering spectra of pyridine adsorbed on Ag(n) (n = 2-8) clusters

We investigate surface-enhanced Raman scattering (SERS) spectra of pyridine–Ag_n (n = 2–8) complexes by density functional theory (DFT) and time-dependent DFT (TDDFT) methods. In simulated normal Raman scattering (NRS) spectra, profiles of pyridine–Ag_n (n = 2–8) complexes are analogical with that of isolated pyridine. Nevertheless, calculated pre-SERS spectra are strongly dependent on electronic transition states of new complexes. Wavelengths at 335 nm, 394.8 nm, 316.9 nm and 342.6 nm, which are nearly resonant with pure charge transfer excitation states, are adopted as incident light when simulating pre-SERS spectra for pyridine–Ag_n (n = 2–8) complexes, respectively. We obtain enhancement factors from 10³ to 10⁵ in pre-SERS spectra compared with corresponding NRS spectra. The obvious increase in Raman intensities mainly result from charge transfer resonance Raman enhancement. A charge difference densities (CDDs) methodology is adopted in describing chemical enhancement mechanism. This methodology aims at visualizing charge transfer from Ag_n (n = 2–8) clusters to pyridine on resonant electronic transition, which is one of the most direct evidences for chemical enhancement mechanism.     

Interpretation of resonance cars and shpolskii spectra with calculated molecular geometries,vibrational frequencies and relative intensities: Chrysene in it's lowest excited singlet and triplet state

Coherent anti-Stokes Raman scattering (CARS) spectra of excited molecules as well as Shpolskii spectra provide information about geometry changes between ground and excited states. Vibrational frequencies and relative intensities from recently obtained CARS spectra of the chrysene S₁ and T₁ state and earlier observed Shpolskii spectra are interpreted in terms of molecular geometry and force-field changes by means of quantum-chemical consistent force field (QCFF) and Franck-Condon factor calculations. The comparison of observed and calculated relative intensities indicates a coupling between the S₁ and S₂ state enhancing some of the vibrational radiative singlet transitions both in absorption and fluorescence spectra whereas within the phosphorescence spectra proportionality to calculated Franck-Condon factors is obeyed. The T₁ state is the more loosely bound state and its geometry change is different from that of the S₁ state. The resonance CARS transitions in the S₁ state are assigned to totally symmetric vibrations getting their intensity by a coupling scheme analogous to the A term of the resonance Raman effect: the relative intensity of a transition is shown to be proportional to the Franck-Condon factor to the higher excited state and to the squared vibrational frequency. Using this relation this state can be identified by means of its finger-print-like intensity pattern.     

Observation of transient resonance raman spectra of the S1 state of trans-stilbene

Transient resonance Raman spectra of trans-stilbene in n-hexane have been obtained using two pulsed lasers at 266 and 585 nm. The former was used to pump the molecule to the first excited singlet state (S₁) and the latter to proble spontaneous Raman scattering in resonance with the S_n ← S₁ electronic transition. The dependence of the pump and probe laser power, the temporal behavior, and the excitation profile of the spectra clearly indicate that they are due to the S₁ state of trans-stilbene.