氯代甲苯异构体双电荷离子电子捕获诱导解离谱研究

研究了４种Ｃ７Ｈ７Ｃｌ异构体在７０ｅＶ电子轰击下产生的［Ｃ７Ｈ７Ｃｌ］＾２＋、［Ｃ７Ｈ６Ｃｌ］＾２＋．和［Ｃ７Ｈ５Ｃｌ］＾２＋ ３种双电荷离子的电子捕获诱导解离（ＥＣＩＤ）反应。分子离子的ＥＣＩＤ反应明显的邻位效应，表明其结构仍保持中性分子的结构特征；而由各异构体产生的［Ｃ７Ｈ６Ｃｌ］＾２＋．和［Ｃ７Ｈ５Ｃｌ］＾２＋离子异构化成同一结构。３种双电荷离子ＥＣＩＤ反应的产物与离子所带电子的奇偶性有关，     

C60[RuHCl（CO）（PPh3）]3配合物的合成和表征

富勒烯配合物的制备及其性质的研究是目前富勒烯化学最为活跃的研究领域之一［１］,人们正致力于探索富勒烯各类衍生物的结构与性质之间的依赖关系,以期合成出具有特殊性能的富勒烯配合物,为富勒烯的实际开发应用奠定基础。本文首次合成Ｃ６０［ＲｕＨＣｌ（ＣＯ）（ＰＰｈ３）］３配合物,采用元素分析、红外光谱、电子光谱进行鉴定和表征,并推测了其结构。１　实验部分１．１　Ｃ６０［ＲｕＨＣｌ（ＣＯ）（ＰＰｈ３）］３的合成合成按下列反应进行：ＲｕＣｌ３＋３ＰＰｈ３＋ＨＣＨＯ→ＲｕＨＣｌ（ＣＯ）（ＰＰｈ３）３ＲｕＨＣｌ（…     

（C_5H_7S_2）_3〔Bi_2Cl_9〕的合成和晶体结构

标题化合物由ＢｉＣｌ３和乙酰丙酮在ＨＣＩ（气）／Ｃ２Ｈ５ＯＨ溶剂中通入Ｈ２Ｓ气体反应而得。晶体属四方晶系，Ｍｒ＝１１３０．７６，空间群Ｐ４１２１２。晶胞参数ａ＝ｂ＝８．８６７（２），ｃ＝４１．５１１（４）Ａ；Ｖ＝３２６４（１）Ａ３，Ｚ＝４，Ｄｃ＝２．３０ｇｃｍ（－３），μ（ＭｏＫα）＝１１８．６０７ｃｍ（－１），Ｆ（０００）＝２１０４．晶体结构由重原子法求得。最终偏离因子Ｒ＝０．０７２。晶体由分立的（Ｃ５Ｈ７Ｓ２）＋阳离子和［Ｂｉ２Ｃｌ９］３－阴离子组成。每个Ｂｉ原子和６个Ｃｌ原子形成畸变的八面体配位。２个［ＢｉＣｌ６］八面体共面构成具有２次轴对称的［Ｂｉ２Ｃｌ９］（３－）配阴离子。还讨论了阳离子种类对Ｂｉ配阴离子结构类型的影响。     

金属离子与卟啉的嵌入反应动力学研究──Ⅶ．一元酸根催化Cu(Ⅱ)与溴化间－四(N－乙酸甲酯基－3－吡啶基)卟啉的配位反应

研究了在３５±０．１℃、离子强度０．５ｍｏｌ／Ｌ（ＫＣｌ）条件下，甲酸根、乙酸根、丙酸根和丁酸根分别催化Ｃｕ（Ⅱ）离子与四溴化间－四（Ｎ－乙酸甲酯基－３－吡啶基）卟啉（Ｈ２Ｔβ－Ｎ－ＡＣＭｓｐｙＰＢｒ４）的反应动力学及其机理，该类反应对卟啉和Ｃｕ（Ⅱ）离子均为一级反应，反应动力学方程为：ｄ［ＣｕＰ＾４＋］／ｄｔ＝ｋ｛１．０＋ｂ［Ａ＾－］）／（１．０＋Ｋ３，４．［Ｈ＾＋］＾２｝［Ｃｕ＾２＋］［Ｐ］Ｔ     

非活化苯环的缩合反应

让过氧化来甲酰和五氯化钼与氯苯反应，生成一个新的双核钼配合物［（Ｃ＿６Ｈ＿４Ｃｌ）＿２Ｃ（ｐｈ）］＿２［Ｍｏ＿２（μ－Ｃｌ）＿３Ｃｌ＿４Ｏ＿２］［Ｍｏ＿２（μ－Ｃｌ）＿２Ｃｌ＿４Ｏ＿２（μ－ＯＣＯＰｈ）］。用Ｘ－射线单晶衍射的方法测定了它的晶体结构。同时还研究了该化合物的谱学性质，并用ＡＳＥ—ＭＯ方法计算了它的电子结构。     

三（8－羟基喹啉）镍（Ⅱ）合高氨酸钠Na［NiQ_2（HQ）］（ClO_4）的制备和晶体结构

在使用８－羟基喹啉为配体试图制备钆和镍的异双核配合物时，分离出Ｎａ［ＮｉＱ２（ＨＱ）］（ＣｌＯ４）单晶，首次测定了它的晶体结构．Ｒａｎｅ等曾从ＮｉＱ２·２Ｈ２Ｏ的晶胞参数推测出ＮｉＱ２·２Ｈ２Ｏ的键参数［１］．最近我们将高氯酸钇、醋酸镍和８－羟基喹啉在丙酮中反应，制备了［ＹＱ（ＨＱ）２］［ＮｉＱ３（ＣｌＯ４），并测定了它的晶体结构［２］     

铱(I)苯乙胺Schiff碱络合物催化苯乙酮的不对称氢转移反应

以光学活性的苯乙胺和吡啶－２－甲醛缩合而得到的Ｓｃｈｉｆ碱（ＰＰＥＩ）（ＰＰＥＩ＝２－［［Ｎ－（１－ｐｈｅｎｙｌｅｔｈｙｌ）ｉｍｉｎｏ］ｍｅｔｈｙｌ］ｐｙｒｉｄｉｎｅ或２－［［Ｎ－（１－苯乙基）亚胺］甲基］吡啶）为配体，进而与［Ｉｒ（ＣＯＤ）Ｃｌ］２（ＣＯＤ＝１，５－环辛二烯）反应，合成了８个光学活性铱络合物，考察了它们在异丙醇存在下催化苯乙酮不对称氢转移反应的光学活性，发现［Ｉｒ（ＣＯＤ）（ＰＰＥＩ）Ｉ］具有较好的立体选择性．其光学产率最高可达３５．７％ｅ．ｅ．．     

Rh—V／SiO2上H2的化学吸附方式

ＣＯ加氢反应机理是许多研究者感兴趣的课题．负载的Ｒｈ是ＣＯ加氢反应的优良催化剂．ＣＯ在Ｒｈ上吸附态的研究已有许多报道［１～７］,而对Ｈ２有关的吸附态的研究却少见报道．Ｗｏｒｌｅｙ等［８］利用高压超纯Ｈ２在２．２％Ｒｈ／Ａｌ２Ｏ３膜上首次观测到Ｒｈ—Ｈ...     

Nd（OPr~i）_2Cl－AlEt_3均相二元催化剂异戊二烯聚合动力学Ⅰ．一般动力学研究

用膨胀计研究了Ｎｄ（ＯＰｒｉ）２Ｃｌ－ＡｌＥｔ３均相稀土催化剂异戊二烯聚合动力学．在实验条件下，本体系显示稳态聚合特征；聚合速度对单体浓度和催化剂浓度均为一级关系，即聚合速度方程为Ｒｐ＝Ｋｐ［Ｎｄ］［Ｍ］；本体系总的活化能Ｅａ为５７．４ｋＪ／ｍｏｌ．     

［Fe（Phen）_3］（ClO_4）_3与Na_2SO_3在室温下的固相氧化还原反应

本文研究室温下［Ｆｅ（Ｐｈｅｎ）３］（ＣｌＯ４）３·Ｈ２Ｏ与Ｎａ２ＳＯ３发生的固－团相氧化还原反应．用Ｍｏｓｓｂａｕｅｒ谱、ＸＲＤ、ＩＲ、元素分析和磁化率测定等手段表征了反应２４ｈ后的团相产物．实验表明，室温下该反应速度快，反应进行完全．     

Stereodynamics of chlorine atom reactions with organic molecules

A series of recent experimental and computational studies has explored how the dynamics of hydrogen abstraction from organic molecules are affected by the presence of functional groups in the molecule and by basic structural motifs such as strained ring systems. Comparisons drawn between reactions of Cl atoms with alkanes such as ethane, Cl + CH3CH3--> HCl + CH3CH2, which serve as benchmark systems, and with functionalized molecules such as alcohols, amines, and alkyl halides, Cl + CH3X --> HCl + CH2X (X = OH, NH2, halogen, etc.) expose a wealth of mechanistic detail. Although the scattering dynamics, as revealed from measured angular distributions of the velocities of the HCl with quantum-state resolution, show many similarities, much-enhanced rotational excitation of the HCl products is observed from reactions of the functionalized molecules. The degree of rotational excitation of the HCl correlates with the dipole moment of the CH2X radical and is thus attributed, at least in part, to post-transition-state dipole-dipole interactions between the separating, polar reaction products. This interpretation is supported by direct dynamics trajectories computed on-the-fly, and the HCl rotation is thus argued to serve as an in situ probe of the angular anisotropy of the reaction potential energy surface in the post-transition-state region. Comparisons between the dynamics of reactions of dimethyl ether and the three- and four-membered-ring compounds oxirane (c-C2H4O) and oxetane (c-C3H6O) raise questions about the role of reorientation of the reaction products on a time scale commensurate with their separation. The shapes and structures of polyatomic molecules are thus demonstrated to have important consequences for the stereodynamics of these direct abstraction reactions.     

Bond and mode selectivity in the reaction of atomic chlorine with vibrationally excited CH2D2

The title reaction is investigated by co-expanding a mixture of Cl2 and CH2D2 into a vacuum chamber and initiating the reaction by photolyzing Cl2 with linearly polarized 355 nm light. Excitation of the first C-H overtone of CH2D2 leads to a preference for hydrogen abstraction over deuterium abstraction by at least a factor of 20, whereas excitation of the first C-D overtone of CH2D2 reverses this preference by at least a factor of 10. Reactions with CH2D2 prepared in a local mode containing two quanta in one C-H oscillator /2000>- or in a local mode containing one quantum each in two C-H oscillators /1100> lead to products with significantly different rotational, vibrational, and angular distributions, although the vibrational energy for each mode is nearly identical. The Cl+CH2D2/2000>- reaction yields methyl radical products primarily in their ground state, whereas the Cl+CH2D2/1100> reaction yields methyl radical products that are C-H stretch excited. The HCl(v=1) rotational distribution from the Cl+CH2D2/2000>- reaction is significantly hotter than the HCl(v=1) rotational distribution from the Cl+CH2D2/1100> reaction, and the HCl(v=1) differential cross-section (DCS) of the Cl+CH2D2/2000>- reaction is more broadly side scattered than the HCl(v=1) DCS of the Cl+CH2D2/1100> reaction. The results can be explained by a simple spectator model and by noting that the /2000>- mode leads to a wider cone of acceptance for the reaction than the /1100> mode. These measurements represent the first example of mode selectivity observed in a differential cross section, and they demonstrate that vibrational excitation can be used to direct the reaction pathway of the Cl+CH2D2 reaction.     

Effect of bending and torsional mode excitation on the reaction Cl+CH4-->HCl+CH3

A beam containing CH(4), Cl(2), and He is expanded into a vacuum chamber where CH(4) is prepared via infrared excitation in a combination band consisting of one quantum of excitation each in the bending and torsional modes (nu(2)+nu(4)). The reaction is initiated by fast Cl atoms generated by photolysis of Cl(2) at 355 nm, and the resulting CH(3) and HCl products are detected in a state-specific manner using resonance-enhanced multiphoton ionization (REMPI). By comparing the relative amplitudes of the action spectra of Cl+CH(4)(nu(2)+nu(4)) and Cl+CH(4)(nu(3)) reactions, we determine that the nu(2)+nu(4) mode-driven reaction is at least 15% as reactive as the nu(3) (antisymmetric stretch) mode-driven reaction. The REMPI spectrum of the CH(3) products shows no propensity toward the formation of umbrella bend mode excited methyl radical, CH(3)(nu(2)=1), which is in sharp distinction to the theoretical expectation based on adiabatic correlations between CH(4) and CH(3). The rotational distribution of HCl(v=1) products from the Cl+CH(4)(nu(2)+nu(4)) reaction is hotter than the corresponding distribution from the Cl+CH(4)(nu(3)) reaction, even though the total energies of the two reactions are the same within 4%. An explanation for this enhanced rotational excitation of the HCl product from the Cl+CH(4)(nu(2)+nu(4)) reaction is offered in terms of the projection of the bending motion of the CH(4) reagent onto the rotational motion of the HCl product. The angular distributions of the HCl(nu=0) products from the Cl+CH(4)(nu(2)+nu(4)) reaction are backward scattered, which is in qualitative agreement with theoretical calculation. Overall, nonadiabatic product vibrational correlation and mode specificity of the reaction indicate that either the bending mode or the torsional mode or both modes are strongly coupled to the reaction coordinate.     

光引发BrC2F4Br+C2F4调聚反应的光强影响

实验发现，在光引发BrC2F4Br＋C2F4调聚反应中，光强（或光功率密度）能影响产品分布。提出了反应机理：此反应由加成反应与复合反应组成，而链转移反应可忽略．由此进行了动力学计算，为与实验结果吻合，拟合得的加成反应BrC2F4＋C2F4的速率常数为（2±1）×107cm3•mol-1•s-1，Br（C2F4）n≧2＋C2F4的速率常数为（1．2±0．4）×107Cm3•mol-1•s-1     

A crossed molecular beam study of the O(1D) + C(3)H(8) reaction: multiple reaction pathways.

The O((1)D) + C(3)H(8) reaction has been reinvestigated using the universal crossed molecular beam method. Three reaction channels, CH(3) + C(2)H(4)OH, C(2)H(5) + CH(2)OH, and OH + C(3)H(7), have been observed. All three channels are significant in the title reaction with the C(2)H(5) formation process to be the most important, while the CH(3) formation and the OH formation channels are about equal. Product kinetic energy distributions and angular distributions have been determined for the three reaction channels observed. The oxygen-containing radicals in the CH(3) and C(2)H(5) formation pathways show forward-backward symmetric angular distribution relative to the O atom beam, while the OH product shows a clearly forward angular distribution. These results indicate that the OH formation channel seems to exhibit different dynamics from the CH(3) and C(2)H(5) channels.     

State-to-state reaction dynamics: a selective review

A selective review of state-to-state reaction dynamics experiments is presented. The review focuses on three classes of reactions that exemplify the rich history and illustrate the current state of the art in such work. These three reactions are (1) the hydrogen exchange reaction, H+H2-->H2+H and its isotopomers; (2) the H+RH-->H2+R reactions, where RH is an alkane, beginning with H+CH4-->H2+CH3 and extending to much larger alkanes; and (3) the Cl+RH-->HCl+R reactions, principally Cl+CH4-->HCl+CH3. We describe the experiments, discuss their results, present comparisons with theory, and introduce heuristic models.     

Rotationally correlated reactivity in the CH (v = 0, J, F(i)) + O2 → OH (A) + CO reaction

The rotational-state-selected CH (v = 0, J, F(i)) beam has been prepared by using an electric hexapole and applied to the crossed beam reaction of CH (v = 0, J, F(i)) + O(2) → OH (A) + CO at different O(2) beam conditions. The rotational state selected reactive cross sections of CH (RSSRCS-CH) turn out to depend remarkably on the rotational state distribution of O(2) molecules at a collision energy of ～?0.19 eV. The reactivity of CH molecules in the N = 1 rotational states (namely ∣J = 1∕2, F(2)> and ∣J = 3∕2, F(1)> states, N designates the angular momentum excluding spin) becomes strongly enhanced upon a lowering of the rotational temperature of the O(2) beam. The RSSRCS-CH in these two rotational states correlate linearly with the population of O(2) molecule in the specific K(O(2)) frame rotation number states: CH(|J = 1/2,F(2)>) with O(2)(|K(O(2)) = 1>);CH(|J = 3/2,F(1)>) with O(2)(|K(O(2)) = 3>). These linear correlations mean that the rotational-state-selected CH molecules are selectively reactive upon the incoming O(2) molecules in a specific rotational state; here, we use the term "rotationally correlated reactivity" to such specific reactivity depending on the combination of the rotational states between two molecular reactants. In addition, the steric asymmetry in the oriented CH (∣J = 1∕2,?F(2),?M = 1∕2>) + O(2) (|K(O(2)) = 1>) reaction turns out to be negligible (< ±1%). This observation supports the reaction mechanism as theoretically predicted by Huang et al. [J. Phys. Chem. A 106, 5490 (2002)] that the first step is an intermediate formation with no energy barrier in which C-atom of CH molecule attacks on one O-atom of O(2) molecule at a sideways configuration.     

Stereodynamics of the Ca + HCl → CaCl + H molecular reaction imposed by the rotational-excited states of HCl

The effects of the initial rotational-excited states of the HCl molecule on the stereodynamics properties of the Ca + HCl molecular reaction are investigated using the quasiclassical trajectory theory and the analytical potential energy surface. The orientation and alignment behaviors for the rotational angular momentum of the product, along with the generalized differential cross section (PDDCS)-dependent polarization, are calculated to explore the stereodynamics properties. The initial rotational-excited states of the HCl molecule impose a remarkable effect on the vector correlation distributions, regardless of the orientation, alignment, or PDDCS. The forward, backward, and weak sideway scatterings are found in the Ca + HCl → CaCl + H molecular reaction. The results demonstrate that the initial rotational-excited state of j = 3 results in more obvious stereodynamics effects.     

Imaging the dynamics of reactions between Cl atoms and the cyclic ethers oxirane and oxetane

Direct current slice velocity map ion images of the HCl(nu' = 0, J') products from the photoinitiated reactions of ground state Cl atoms with ethane, oxirane (c-C2H4O), and oxetane (c-C3H6O), at respective mean collision energies of 5.5, 6.5, and 7.3 kcal mol-1(-1), were analyzed using a Legendre moment fitting procedure. The experimental method and the fitting technique were tested by comparing the derived center-of-mass (CM) frame angular scattering distribution for the HCl(v' = 0, J' = 1) products from the reaction of Cl + C2H6 with those determined by Suits and co-workers from a crossed molecular beam experiment. For the Cl + c-C2H4O reaction, a broad, forward, and backward peaking CM frame angular distribution of HCl(nu' = 0, J' = 2) products was determined, with an average fraction of the available energy released as product translational energy of f t, equal to 0.52 +/- 0.18. The HCl consumes only 1% of the available energy, and conservation arguments dictate that the radical coproduct is significantly internally excited, corresponding to an average fraction of the available energy of f int(c-C2H3O), equal to 0.47 +/- 0.18. For the reaction of oxetane with Cl atoms, abstraction of H atoms is possible from carbon atoms from positions either alpha or beta to the O atom. The contributions to the reaction from these two H-atom abstraction channels were estimated to be 63 and 37%, consistent with an unbiased propensity for removal of alpha- and beta-H atoms that are present in 2:1 abundance. The angular scatter of products in the CM frame is also broad and forward-backward peaking and is reminiscent of the products of the Cl + CH3OH and CH3OCH3 reactions. The derived mean fraction of the available energy channelled into product translation is f t = 0.54 +/- 0.12 for each of the two abstraction pathways. With only a small amount of energy in the rotation of the HCl(nu' = 0), the remainder is accounted for by excitation of the radical coproduct internal modes, with f int(c-C3H5O) = 0.42 +/- 0.12 for both alpha- and beta-H abstraction. The broad product scattering in the CM frame observed for both reactions of Cl atoms with the cyclic ethers is consistent with reactive collisions over a wide range of impact parameters, as might be expected for barrierless reactions with loose transition states.