1，2－二氢－3H－吲哚－3－酮类化合物的光化学合成

１，２－二氢－３Ｈ－吲哚－３－酮类化合物的光化学合成凌可庆（淮北煤炭师范学院化学系，淮北，２３５０００）关键词吲哚衍生物，单重态氧反应，１，２－二氢－３Ｈ－吲哚－３－酮衍生物，光合成１，２－二氢－３Ｈ－吲哚－３－酮是重要的有机合成中间体，广泛用于多种...     

6H－1，2－氧硫杂环己烷并［5，6－c］异苯并吡喃类衍生物的合成及其抗炎活性

６Ｈ－１，２－氧硫杂环己烷并［５，６－ｃ］异苯并吡喃类衍生物的合成及其抗炎活性王进军，崔昌亿，韩光范，魏永慧，姜贵吉（吉林化工学院精细化工系吉林１３２０２２）（吉林医学院检验系吉林）（延边大学化学系延吉）关键词异苯并二氢吡喃，杂环化合物，抗炎活性可用...     

1－羟基－2（1H）－吡啶硫酮及其甲基衍生物与Au（Ⅲ）配合物的合成和性质

合成了１－羟基－２－（１Ｈ）－吡啶硫酮（ＨＰＴ）及其甲基衍生物的［ＡｕＬ２］ＯＨ型配合物（Ｌ＝ＰＴ－，３－ＣＨ３－ＰＴ－和４－ＣＨ３－ＰＴ－）．用元素分析，紫外光谱，红外光谱，１ＨＮＭＲ谱，摩尔电导，ＴＧ－ＤＴＡ－ＤＴＧ进行了表征，用循环伏安法研究其氧化还原性质，含甲基的配合物有较强的抑菌活性。     

苯甲酸（1H－1，2，4－三唑－1－基）－3，3－二甲基－2－丁酮酯衍生物的合成

用冠醚作催化剂，通过苯甲酸盐同１－溴代－１－（１Ｈ－１，２，４－三唑－１－基）－３．３－二甲基丁酮－２－反应，合成了一系列苯甲酸（１Ｈ－１，２，４－三唑－１－基）－３，３－二甲基－２－丁酮酯类新化合物，并对合成方法进行了探讨。通过ＩＲ、￣１ＨＮＭＲ及元素分析，确定了化合物的结构。     

1－（1－H－苯并三唑－1－乙酰基）－4－（邻氯苯甲酰基）氨基硫脲（Ⅴ）及其噻二唑衍生物（Ⅵ）的合成

１－（１－Ｈ－苯并三唑－１－乙酰基）－４－（邻氯苯甲酰基）氨基硫脲（Ⅴ）及其噻二唑衍生物（Ⅵ）的合成魏太保，陈继畴，张有明，李清河，陈真吉（西北师范大学化学系，兰州７３００７０）三唑类化合物是一类新型的植物生长调节剂。这类化合物能够控制植物生长，增加...     

4－羟基－3－酰基（酯基）－2H－1，2－苯并噻嗪－1，1－二氧化物衍生物的合成及生物活性

利用４－羟基－３－酰基（酯基）－２Ｈ－１，２－苯并噻嗪－１，１－二氧化物分别与芳基异氰酸酯、苯肼、氯甲酸甲酯和乙二醇反应合成了２０种新衍生物，研究了其与异氰酸酯在不同摩尔比碱作用下的加成反应。生物活性测定结果表明，大部分化合物具有较好的除草活性和植物生长调节活性。     

2－烷基环戊－2－烯酮衍生物的合成及抗炎活性研究

２－烷基环戊－２－烯酮衍生物的合成及抗炎活性研究齐传民计志忠，李玉兰，王彪（北京农业大学应用化学系，北京，１０００９４）（沈阳药科大学）关键词环戊烯酮衍生物，β－氨基甲基酮，Ｍａｎｎｉｃｈ反应，缩合反应，抗炎活性目前，许会抗炎药物是芳香酸类比合物，它...     

螺［异苯并呋喃－1（3H），9＇－（9H）－2＇－N，N－二苄胺基－6＇－二乙胺基占吨］－酮－3的合成及晶体结构研究

合成了螺［异苯并呋喃－１（３Ｈ），９＇－（９Ｈ）－２＇－Ｎ，Ｎ－二苄胺基－６＇－二乙胺基占吨］－酮－３，Ｃ＿（３７）Ｈ＿（３４）Ｎ＿２Ｏ＿３，单斜晶系，空间群Ｃｃ，晶体学参数为ａ＝１６．８２６（４），ｂ＝１０．６４８（４），ｃ＝１７．６１８（７），β＝９２．２５（２）°，Ｖ＝３１５４（２），Ｚ＝４，Ｍ＿ｒ＝５６６．７，Ｄ＿ｘ＝１．１９ｇ／ｃｍ３，Ｆ（０００）＝１２００。结构由直接法解出，偏离因子Ｒ＝０．０８０。分子由占吨和异苯并呋喃两部分组成Ｙ形结构，占吨部分相连的苄基的两个苯环位于占吨部分的两侧。     

Ebselen氨基酸衍生物的合成及抗脂质过氧化作用

Ｅｂｓｅｌｅｎ氨基酸衍生物的合成及抗脂质过氧化作用肖颖歆，刘秀芳，徐汉生，孙士勇，徐波（武汉大学化学系，武汉，４３００７２）（北京医科大学天然药物及仿生药物国家重点实验室）关键词２－苯基－１，２－苯并异硒唑－３（２Ｈ）－酮，苯并异硒唑酮，氨基酸衍生物...     

6,7—取代—1H—苯并（de）异喹啉—1,3（2H）二酮的合成

从二氢苊出发合成了６－溴－７－氨基２－（２′，４′－二甲基）苯基－１Ｈ－苯并（ｄｅ）异喹啉－１，３（２Ｈ）－二酮，６－甲氧基－７－氨基－２－（２′，４′－二甲基）苯基－１Ｈ－苯并（ｄｅ）异喹啉－１，３（２Ｈ）－二酮和６，７－二氨基－２－（２′，４′－二甲基）苯基－１Ｈ－苯并（ｄｅ）异喹啉－１，３（２Ｈ）－二酮，测定了它们的荧光量子产率，讨论了分子内重原子溴和给电子基对化合物荧光性质的影响。     

The formation of highly excited H in the reaction H2+(v) + H2 → H + H

A quasiclassical trajectory surface hopping method has been used to study H(v) + H₂ → H + H for v = 0, 3, 7, 10, 13, and 17 with an emphasis on determining the H internal energy and angular momentum distributions for high v. For v = 13 and 17, significant cross sections are found for producing H at energies above its dissociation energy. An average metastable H lifetime of 11.5 ps for v = 13 and 4.7 ps for v = 17 is found, but there is also a much longer lived component to the lifetime distributions that is more important for v = 13 than for v = 17. Some of the longer lived metastables correspond to high angular momentum orbiting states of H, but other sources of metastability are also present.     

A pseudopotential study of the hydrogen bond in H2O·H2S,H2S·H2S and H2O·H2Se systems

Intermolecular potential energy curves for the hydrogen bonded systems H₂O·H₂S, H₂O·H₂Se and H₂S·H₂S were calculated with nonempirical pseudopotentials using optimized-in-molecules basis sets augmented by polarization functions. The H₂O·H₂O interaction energy curve has been also considered as a test case. The present results for H₂O·H₂S and H₂S·H₂S indicate much weaker intermolecular interactions than those found in previous ab initio calculations. The H₂O·H₂Se interaction was found to be quite similar to H₂O·H₂S.This work was partly supported by the Polish Academy of Sciences within the Project PAN-09, 7.1.1.1On leave from Quantum Chemistry Laboratory, Dept. of Chemistry, University of Warsaw, Pasteura 1, 02-093. Warsaw, Poland     

New calculations on the ion-molecule processes C2H2(+) + H2 --> C2H3(+) + H and C2H2(+) + H2 --> C2H4+

New high-level quantum chemical calculations have been undertaken to understand the rates and mechanisms of the reactive and associative channels for the reactants C2H2(+) + H2. The reactive channel, which produces C2H3(+) + H, has been shown to be slightly endothermic, confirming earlier calculations at a somewhat lower level and in agreement with some recent experimental work. The associative channel, leading to C2H4+, has been shown to proceed via a transition state with negative energy relative to the reactants, so that association is predicted to be efficient. This result is in conflict with an earlier theoretical study but in agreement with low-temperature experimental measurements.     

Deuterium exchange in the systems of H2O+/H2O and H3O+/H2O

The reactions of H₂O⁺, H₃O⁺, D₂O⁺, and D₃O⁺ with neutral H₂O and D₂O were studied by tandem mass spectrometry. The H₂O⁺ and D₂O⁺ ion reactions exhibited multiple channels, including charge transfer, proton transfer (or hydrogen atom abstraction), and isotopic exchange. The H₃O⁺ and D₃O⁺ ion reactions exhibited only isotope exchange. The variation in the abundances of all ions involved in the reactions was measured over a neutral pressure range from 0 to 2 × 10⁻⁵ Torr. A reaction scheme was chosen, which consisted of a sequence of charge transfer, proton transfer, and isotopic exchange reactions. Exact solutions to two groups of simultaneous differential equations were determined; one group started with the reaction of ionized water, and the other group started with the reactions of protonated water. A nonlinear least-squares regression technique was used to determine the rate coefficients of the individual reactions in the schemes from the ion abundance data. Branching ratios and relative rate coefficients were also determined in this manner.A delta chi-squared analysis of the results of the model fitted to the experimental data indicated that the kinetic information about the primary isotopic exchange processes is statistically the most significant. The errors in the derived values of the kinetic information of subsequent channels increased rapidly. Data from previously published selected ion flow tube (SIFT) study were analyzed in the same manner. Rigorous statistical analysis showed that the statistical isotope scrambling model was unable to explain either the SIFT or the tandem mass spectrometry data. This study shows that statistical analysis can be utilized to assess the validity of possible models in explaining experimentally observed kinetic behaviors.     

Long range H,H coupling constants in cycloheptatrienes

The ¹H NMR spectra of 1,6-dicarbomethoxycyclohepta-1,3,5-triene ( 2 ) and 3,4-benzocyclohepta-1,3,5-triene ( 3 ) have been analysed in terms of chemical shifts and coupling constants. A method for the assignment of δ(AA′) and δ(BB′) in AA′BB′ systems, based on the observation of ¹³C satellites in the ¹H NMR spectrum, is described. For J(1,5) in 3 , a negative sign was established. Spin tickling experiments were used to determine the positive sign for J(2,5) in 2 and the negative sign for J(2,7) in 3. The conformation of 3 is discussed.     

Coherent excitation of H(n=2) in H+, H - He collisions

The coherent excitation of H(n=2) in H⁺, H - He collisions was investigated at incident energies of 5–25 keV. From a polarization analysis of the emitted Lyman-α radiation as a function of an external electric field, the partial cross sections for excitation to the H(2s) and the H(2p _m) magnetic substates and the real part of thes ?p ₀-coherence were extracted. For H⁺-He collisions, the measured partial cross sections are in fair agreement with previous two-electron calculations by Kimura and Lin; the agreement with one-electron calculations of Jain et al. is, particularly at the lower incident energies, less satisfactory. For both collision systems, an energy-dependent forward-backward asymmetry corresponding to a shift of the center-of-charge relative to the center-of-mass (dipole moment) was observed. In H⁺ - He collisions, the measured dipole moment was positive; it thus corresponds to an electron trailing behind the proton. The same analysis applied to the H - He system showed the electron riding in front of the proton.     

Syntheses of 1,3,6,8,10,11,14-heptaazapentaphene-2,4,7,9(14H,3H,8H, -11H)-tetrones (angular mixed flavins), 1,3,5,6,8,10,11,14-octaazapentaphene-2,4,7,9(14H,3H,8H,11H)-tetrones (angular doubled flavins), and their related compounds

Cyclization of N, N′-dialkyl-N-(3-methyluracil-6-yl)-N′-(5-nitro-3-methyluracil-6-yl)- p-phenylenediamines with the Vilsmeier reagent gives the corresponding 1,3,6,8,10,11,14-heptaazapentaphene-2,4,7,9-(14H,3H,8H,-11H) -tetrones (angular mixed flavins) 2. Cyclization of N, N′-di(5-nitro-3-methyluracil-6-yl)-p-phenylenedi-amines with the Vilsmeier reagent gives the corresponding 1,3,5,6,8,10,11,14-octaazapentaphene-2,4,7,9-(14H,3H,8H,11H)-tetrones (angular doubled flavins) 11 along with the angular mixed flavins 2.     

H atom yields from the reactions of CN radicals with C2H2, C2H4, C3H6, trans-2-C4H8, and iso-C4H8

The kinetics and H atom channel yield at both 298 and 195 K have been determined for reactions of CN radicals with C2H2 (1.00+/-0.21, 0.97+/-0.20), C2H4 (0.96+/-0.032, 1.04+/-0.042), C3H6 (pressure dependent), iso-C4H8 (pressure dependent), and trans-2-C4H8 (0.039+/-0.019, 0.029+/-0.047) where the first figure in each bracket is the H atom yield at 298 K and the second is that at 195 K. The kinetics of all reactions were studied by monitoring both CN decay and H atom growth by laser-induced fluorescence at 357.7 and 121.6 nm, respectively. The results are in good agreement with previous studies where available. The rate coefficients for the reaction of CN with trans-2-butene and iso-butene have been measured at 298 and 195 K for the first time, and the rate coefficients are as follows: k298K=(2.93+/-0.23)x10(-10) cm3 molecule(-1) s(-1), k195K=(3.58+/-0.43)x10(-10) cm3 molecule(-1) s(-1) and k298K=(3.17+/-0.10)x10(-10) cm3 molecule(-1) s(-1), k195K=(4.32+/-0.35)x10(-10) cm3 molecule(-1) s(-1), respectively, where the errors represent a combination of statistical uncertainty (2sigma) and an estimate of possible systematic errors. A potential energy surface for the CN+C3H6 reaction has been constructed using G3X//UB3LYP electronic structure calculations identifying a number of reaction channels leading to either H, CH3, or HCN elimination following the formation of initial addition complexes. Results from the potential energy surface calculations have been used to run master equation calculations with the ratio of primary:secondary addition, the average amount of downward energy transferred in a collision DeltaEd, and the difference in barrier heights between H atom elimination and an H atom 1, 2 migration as variable parameters. Excellent agreement is obtained with the experimental 298 K H atom yields with the following parameter values: secondary addition complex formation equal to 80%, DeltaEd=145 cm(-1), and the barrier height for H atom elimination set 5 kJ mol(-1) lower than the barrier for migration. Finally, very low temperature master equation simulations using the best fit parameters have been carried out in an increased precision environment utilizing quad-double and double-double arithmetic to predict H and CH3 yields for the CN+C3H6 reaction at temperatures and pressures relevant to Titan. The H and CH3 yields predicted by the master equation have been parametrized in a simple equation for use in modeling.