n-C_3H_7I和i-C_3H_7I的激光裂解

Wilson等人曾研究过碘代烷在266nm的激光光解RI→R+I＊(~2P_(1/2))(1)RI→R+I(~2P_(3/2))(2)由于他们所用的光解产物谱仪不能改变产物的检测方向,因而对C_2H_5I,n-C_3H_7I和i-C_3H_7I的光解通道(1)和(2)在飞行时间(TOF)谱上的分离没有成功。我们用束源可转动的分子束激光裂解产物谱仪(飞行距离531mm)研究了CH_3I和C_2H_5I在248nm的激光裂解后,又分别对n-C_3H_7I和i-C_3H_7I进行研究,并实现了I＊(~2P_(1/2))和I(~2P_(3/2))光解通道在TOF谱上的分离,测得光解通道比见表1。     

F原子与i-C3H7I反应的动力学研究

本文利用交叉分子束技术和激光诱导萤光方法, 研究了F+i-C3H7I→IF+i-C3H7反应的动力学过程. 获得了产物IF相对初生振动分布和相对细致反应速率常数. 初生态布居接近于模型III下的统计理论斯待值, 这不仅表明反应经过长寿命“配合物", 而且也说明自由基i-C3H7的内态是激发的. 另外, 确定了反应的产物IF内部能量分配和总反应截面σ, σ=(3.6±0.5)×10^-^1^6cm^2.     

配合物3AgNO3·2[C3H7S(CH2)2SC3H7]的晶体结构

本文测定了配合物3AgNO3·2BPrTE的晶体结构, 该晶体属三斜晶系, 空间各为PI,晶胞参数: a=0.8945(1), b=1.2355(2), c=1.3572(5)nm; α=98.69(2)°, β=92.74(2)°, γ=90.45(1)°; V=1.480nm^3; Z=2, 分子中三个Ag原子的配位数均为5, 但它们的配位多面体各不相同, Ag(3)为四方锥体, Ag(2)为三角双锥, Ag(1)则介于两者之间, NO3^-以单齿、不等长双齿和等长双齿两种形式配位于Ag原子。配体BPrTE也具有两种构象, 反式构象具有C1对称性, 并以两种形式和Ag原子配位, 偏转式构象不具有C4对称性, 与Ag原子形成五元螯合环, 分子为三维无限长链结构。     

(C5H7S2)2[Cu3I5]的合成和晶体结构

我们曾经对二硫代乙酰丙酮和多种金属离子的配合反应进行了系统的研究.在成功合成(C_5H_7S_2)_2[CuBr_3]的基础上,最近我们试图用类似方法合成(C_5H_7S_2)[CuI_3].但对产物晶体的X 射线衍射分析结果却表明,所得到的化合物的分子式为(C_5H_7S_2)_2[Cu_3I_5].[Cu_3I_5]~(2-)是以[CuI_3]配位三角形和两个相邻[CuI_4]配位四面体连接的无限链状配合阴离子形式存在.     

Gas-phase solvation of Cl− with H2O,CH3OH,C2H5OH,i-C3H7OH,n-C3H7OH,and t-C4H9OH

The gas-phase clustering reactions Cl⁻ (ROH)n−1 + ROH ⇄ Cl⁻ (ROH)_n with n ⩽ 11 for ROH = H₂O, CH₃OH, C₂H₅OH, i-C₃H₇OH, n-C₃H₇OH, and t-C₄H₉OH were measured using a high-pressure mass spectrometer. It seems likely that for CH₃OH and C₂H₅OH, six ligands complete the shell structure and that ligands with n ⩾ 7 belong to the outer shell. The bond energies D(ROH---Cl⁻) increase in the order H₂O < CH₃OH < C₂H₅OH < i-C₃H₇OH < t-C₄H₉OH < n-C₃H₇OH. The observed strong bond of n-C₃H₇OH---Cl⁻ may be due to the fact that both the acidic hydrogen atoms in the −OH and terminal −CH₃ of n-C₃H₇OH interact with Cl⁻ with the most favorable configuration. For Cl⁻ switching reactions, Cl⁻ (H₂O)_n + (ROH)_n ⇄ Cl⁻ (ROH)_n + (H₂O)_n, the ΔG⁰_n values converge to the values of free energies of transfer of Cl⁻ from water to ROH solvent ( = ΔG⁰_n with n → ∞) with n ≈ 7. The observed convergence of ΔG⁰_n is due to compensation of changes in enthalpy and entropy, i.e. both ΔH⁰_n and TΔS⁰_n show increasing divergence from the values of enthalpies and entropies of transfer of Cl⁻ from water to ROH solvent, respectively, with n = 1 → 7. This is due to the stronger interactions of ROH with Cl⁻ than that of H₂O in the inner shell of Cl⁻ (ROH)_n at the expense of the less favorable entropy changes (less freedom of motion for ligands in the inner shell).     

Structure of (C3H5NH3)2H2P2O7·H2O

The bis(cyclopropylammonium)dihydrogenodiphosphate monohydrate is a new diphosphate associated with the organic molecule C₃H₅NH₂. We report the chemical preparation and the crystal structure of this organic cation diphosphate. (C₃H₅NH₃)₂H₂P₂O₇.H₂O is orthorhombic (S.G. : P2₁2₁2₁), with Z = 4 and the following unit-cell parameters : a = 4.828(1) Å, b = 11.011(1) Å, c = 25.645(2) Å. The P₂O₇ groups and H₂O water molecules form a succession of bidimensional layers perpendicular to the c axis. The organic cations ensure the three-dimensional cohesion by NH-O hydrogen bonds.     

Synthesis,crystal structure,and catalytic performance of two 3-D supramolecular compounds: (C7N2H7)3(C7N2H6) · PMo12O40 · 2H2O and (C7N2H7)3(C7N2H6)2 · AsMo12O40 · 3H2O

Two organic–inorganic compounds based on Keggin building blocks have been synthesized by hydrothermal methods, (C₇N₂H₇)₃(C₇N₂H₆)?·?PMo₁₂O_40?·?2H₂O (1) and (C₇N₂H₇)₃(C₇N₂H₆)_2?·?AsMo₁₂O_40?·?3H₂O (2) (C₇N₂H₆?=?benzimidazole). Single-crystal X-ray analysis revealed that 1 crystallized in the triclinic system, P-1 space group with a?=?9.8980(4)?Å, b?=?11.2893(4)?Å, c?=?25.8933(9)?Å, α?=?93.307(2)°, β?=?90.630(2)°, γ?=?108.330(2)°, V?=?2740.68(18)?ų, Z?=?2, R ₁(F)?=?0.0740, ωR ₂(F ²)?=?0.1511, and S?=?1.037; 2 crystallized in the triclinic system, P-1 space group with a?=?12.3353(4)?Å, b?=?13.2649(4)?Å, c?=?20.2878(6)?Å, α?=?95.6630(10)°, β?=?100.1720(10)°, γ?=?99.3940(10)°, V?=?3195.72(17)?ų, Z?=?2, R ₁(F)?= 0.0329, ωR₂ (F ²)?=?0.1236, and S?=?1.088. The two compounds show a layer framework constructed from Keggin-polyoxoanion clusters and benzimidazole via hydrogen bonds and π–π stacking interactions, resulting in a 3-D supramolecular network. Both have high catalytic activity for oxidation of methanol. When the initial concentration of the methanol is 5.37?g?m^?3 in air and the flow velocity is 4.51?mL?min^?1, methanol is completely eliminated at 150°C for 1 (160°C for 2).     

配合物Nd(C7H7N2O2)3(H2O)3的合成及其晶体结构

用水热法合成了3,5-二氨基苯甲酸与Nd(Ⅲ)的配合物Nd(C7H7N2O2)3(H2O)3(1),其结构经IR,元素分析和X-射线单晶衍射仪表征。1为单核结构,属六方晶系,R3空间群,晶胞参数:a=1.887 29(18)nm,b=1.887 29(18)nm,c=0.603 53(12)nm,β=90,°γ=120°,V=1.861 7(4)nm3,Z=3,μ=2.154 mm-1,Dc=1.744 g.cm-3,R1=0.014 3,wR2=0.033 2。1中Nd(Ⅲ)与来自3个3,5-二氨基苯甲酸的6个氧原子及3个配位水的氧原子进行配位,形成9配位化合物。     

分子导体θ-(ET)(C7H7SO3)·3H2O的合成、结构和导电性

用恒电流电化学结晶的方法合成了一种新的基于电子给体BEDT-TTF(双亚乙基二硫四硫富瓦烯) 的电荷转移盐θ-(ET)(C7H7SO3)·3H2O (ET为BEDT-TTF的简写,C7H7SO-3=对甲苯磺酸根).用四圆X衍射的方法测定了θ-(ET)(C7H7SO3)·3H2O的结构.晶体属于三斜晶系,P-1空间群;a=0.8682(1) nm, b= 1.2027(1) nm, c=2.5890(3) nm, α=87.025(6)°, β=89.117(8)°, γ=69.071(7)°, V=2.5216(5) nm3, R=0.0580.晶体中ET自由基沿a轴方向堆积成柱,相邻两个分子柱中的ET分子平面的夹角为49.30°.在b轴方向存在着分子柱侧向间的S…S近距作用.ET阳离子层与对甲苯磺酸根阴离子层沿c轴方向上交替排列.位于阳离子层与阴离子层之间的许多H2O形成了有利于晶体导电性的二维氢键网络.θ-(ET)(C7H7SO3)·3H2O在(001)晶面上某方向上的室温导电率为0.011 S·cm-1,所测变温电导曲线表明,该晶体在120～278 K温度区间内表现为半导体导电行为,导电激活能Ea=0.316 eV.从278～286 K表现为金属导电性.在276 K附近存在金属-半导体相变.     

碘乙烷激光裂解反应通道及产物的能量分布

用分子束和飞行时间技术测量了248 nm激光光解过程C_2H_5I→C_2H_5+I°(~2p_(1/2))和C_2H_5I→C_2H_5+I(~2p_(3/2))裂解碎片的平动能和内能分布。测得通道比I~*/I为2.37。根据实验结果, 对光解过程中电子激发态特性, 产生I(~2p_(3/2))通道的机理以及乙基自由基的振动激发作了讨论。     

单次碰撞条件下，反应Ba+C2H5Br、n-C3H7Br、1,2-C2H4Br2、1,3-C3H6Br2的动力学研究

Under single-collision beam-gas scattering conditions the reactions Ba+ C_2H, Br、n-C_3H_7Br、1, 2-C_2H_4Br_2、1,3-C_3H_6Br_2 have been studied using laser induced fluore-scence to detect the BaBr X~2∑~+ product. The vibrational distributions, the fractions of the available energy going into vibrational and rotational energy of the BaBr products have been calculated by means. of computer simulation. It has been found that the average vibrationel energies of the BaBr products can be described as a linear function of the mass factors for the reactions Ba+CH_3Br、C_2H_5Br、n-C_3H_7Br、1,3-C_3H_6Br, and that the potential energy surfaces for these reactions are similar. For the reactions Ba+CH_3Br、C_2H_5Br、n-C_3H_7Br, the vibrational increae, but for the reactions Ba+CH_2Br_2、1,2-C_2H_4Br_2、1,3-C_3H_6Br_2, the vibrational excitations of the BaBr products decrease greatly when the number of the carbons increase.     

CH3I分子束激光裂解产物的分布

The photofragmentation of CH_3I at 249 nm has been investigated by means of our crossed laser-molecular beam apparatus with rotatable supersonic beam source. The measured I~*/I yield ratio is about 4/1. The C—I bond dissociation energy obtained is 56±1 kcal mol~(-1). The vibrational energy distribution of CH_3 fragments has been roughly estimated.     

二正丙基胂酸合六聚钼酸四胍盐(CN3H6)4[(n-C3H7As)2Mo6O24]的晶体和分子结构

一种新型有机胂合聚钼酸盐(CN_3H_6)_4[(n-C_3H_7As)_2Mo_6O_(24)]的晶体属于正交晶系, 空间群为Cmca, 晶胞参数为: a=1.3938(1), b=1.6350(2), c=1.6173(2) nm直接法得出所有钼、砷原子的位置, 再由差值Fourier合成得到全部其他非氢原子位置。采用全矩阵最小二乘法精修, 最后的R因子为0.047。在该结构中, 阴离子呈笼状结构并具有较高的C_(2h)的对称性。键长数值在正常的范围内, 配位氧与钼原子的键角呈有规律的变化。氢键联结阴、阳离子并纵横于整个空间的各个方向, 形成网状分布, 对晶体的稳定起着重要的作用。     

Photoionization of hot radicals: C2H5, n-C3H7, and i-C3H7

The combination of ion-imaging and vacuum-ultraviolet (vuv) single-photon ionization is used to study the internal energy dependence of the relative photoionization yields of the C(2)H(5),n-C(3)H(7), and i-C(3)H(7) radicals following the 266 nm photodissociation of the corresponding alkyl iodides. The comparison of the ion images obtained by vuv photoionization of the radical with those obtained by two-photon-resonant, three-photon ionization of the complementary I (2)P(32) and I*(2)P(12) atoms allows the extraction of the internal energy dependence of the cross sections. Factors influencing the appearance of the ion images in the different detection channels are discussed, including the secondary fragmentation of the neutral radicals, Franck-Condon factors for the photoionization process, and the unimolecular fragmentation of the parent photoions.     

Two- and three-body photodissociation of gas phase I(3) (-)

The photodissociation dynamics of I3- from 390 to 290 nm (3.18 to 4.28 eV) have been investigated using fast beam photofragment translational spectroscopy in which the products are detected and analyzed with coincidence imaging. At photon energies < or = 3.87 eV, two-body dissociation that generates I- + I2(A 3Pi1) and vibrationally excited I2- (X 2Sigmau+) + I(2P(3/2)) is observed, while at energies > or = 3.87 eV, I*(2P(1/2)) + I2- (X 2Sigmau+) is the primary two-body dissociation channel. In addition, three-body dissociation yielding I- +2I(2P(3/2)) photofragments is seen throughout the energy range probed; this is the dominant channel at all but the lowest photon energy. Analysis of the three-body dissociation events indicates that this channel results primarily from a synchronous concerted decay mechanism.     

Photofragment translational spectroscopy of n-C3H7I and i-C3H7I near 280 and 304 nm

The photodissociation dynamics of propyl iodides n-C3H7I and i-C3H7I near 280 and 304 nm has been investigated with our mini-TOF photofragment translational spectrometer. When a single laser is applied for both the photodissociation of parent molecules and the REMPI of I atom photofragments, the TOF spectra of photofragments I*(2P1/2) and I (2P3/2) are obtained at four different wavelengths for these two iodides. For n-C3H7I, some small vibrational peaks are partially resolved (with separation of approximately 522 cm-1, corresponding to the RCH2 deformation frequency of the fragment n-C3H7) at 281.73, 279.71, and 304.67 nm. These results show that the RCH2 deformation is mostly excited. For i-C3H7I, we obtain some partially resolved vibrational peaks (with separation of approximately 352 cm-1, corresponding to the HC(CH3)2 out-of-plane bending frequency of the fragment i-C3H7) at 281.73 nm only. For n-C3H7I, the partitioning values of the available energy Eint/Eavl are 0.48 at 281.73 nm and 0.49 at 304.02 nm for the I* channel, and 0.52 at both 279.71 and 304.67 nm for the I channel. These energy partitioning values are comparable with the previous results at different wavelengths in the literature. For i-C3H7I, the Eint/Eavl values are 0.61 at 281.73 nm, 0.65 at 304.02 nm for the I* channel, and 0.62 at 279.71 nm, 0.49 at 304.67 nm for the I channel. The potential-energy-surface crossing and the beta values have also been discussed.     

有机钛化学 Ⅲ.1,5-环辛二烯的钛催化均相氢化

本文研究了一系列有机钛化合物(R-C_5H_4)_2TiCl_2(R=H,CH_3,C_2H_5,n-C_3H_7,CH_2-CHCH_2,CH_3CH-CHCH_2,CH_3OCH_2CH_2,C_2H_5OCH_2CH_2,cyclo-C_6H_(11)等)和还原剂((i-Bu)_3Al,LiAlH_4,i-C_3H_7MgBr)组成的低价钛催化体系对1,5-环辛二烯的均相催化氢化反应。结果表明,低价钛催化体系在温和条件下具有较好的催化活性,氢化时还同时发生异构化反应。并讨论茂环上取代基对反应的影响及催化机理。     

4[CuCl(C5H5N)4]·[W10O32]·2(C5H5N)·3H2O的合成及晶体结构

标题化合物是通过(NH_4)_2WS_4, CuCl_2·2H_2O在吡咤溶液中反应制得。晶体呈蓝色, 属三斜晶系, 空间群P1, 晶胞参数为:a=1.3555(7), b=1.3666(5), c=1.7860(13) nm, α=69.08(4)°, β=87.39(5)°, γ=70.72(4)。V=2.907(3) nm, Z=1, D_m=2.56 g cm~(-3)。结构由Patterson法和Fourier法测出。对5692个收集到的独立衍射数据进行计算, 最后R=0.046。结构测定表明, 晶体由W_(10)O_(32)~(4-), [CuCl(C_5H_5N)_4]~+, C_5H_5N和H_2O所组成。W_(10)O_(32)~(4-)的结构见图1, W原子处在O原子的八面体配位中, 彼此共边和共顶点相连。[CuCl(C_5H_5N)_4]~+的结构见图2, Cu原子由1个Cl和4个N原子配位, 呈略有变形的四方锥形, 这种离子是首次报导。C_5H_5N和H_2O填入正负离子堆积的空隙中。     

State-to-state correlated study of CD3I photodissociation at 266 and 304 nm

High-resolution photofragment translational spectroscopy is used in this work to measure the translational and internal energy distributions in the CD3 and iodine fragments produced from the photodissociation of CD3I at 266 and 304 nm. Channel selected detection, via resonantly enhanced multiphoton ionization, combined with one-dimensional core sampling provides detailed information about vibrational state distributions of the CD3 fragments. The vibrational state distributions of CD3 fragments in the I*(2P12) channel have a propensity of nu2 ' umbrella bending mode with a maximum at nu2 ' = 1 for 266 nm photodissociation. For I*(2P12) channel at 304 nm photodissociation, vibrational state distributions of CD3 fragment have a maximum in the vibrational ground state. For the I(2P32) channel (1Q1 <-- 3Q(0+)), nu2 ' umbrella bending vibrational distribution is measured as the predominant vibrational mode but has a much broader distribution when compared to that of the I* channel. The vibrational state distributions of the CD3 fragment produced from the perpendicular transition, i.e., 3Q1, which was determined at 304 nm photodissociation, has a maximum at nu2 ' = 1. The curve crossing possibility between the 1Q1 and 3Q(0+) adiabatic potentials is determined as 0.19 for 266 and 0.85 for 304 nm. The trend in reaction dynamics in 266 and 304 nm photodissociation of CD3I is compared with theoretical calculations. A bond dissociation energy D0(C-I) = 56.60+/-0.5 kcal/mol was derived by applying laws of energy conservation.