苯并噻二嗪吸电子基取代衍生物电子性质的理论研究

运用量子化学半经验方法对1，2，4-苯并噻二嗪-1，1二氧类化合物的8种取代衍生物进行了量子化学计算，从体系能量、几何构型、电子结构、前线分子轨道等几方面分析了吸电子基-CN，-NO2等取代后体系的电子性质变化规律．结果表明：随着取代基吸电子能力的增强，体系的活性增强，可为药物合成提供一定的理论指导．     

苯并噻二嗪衍生物电子结构和非线性光学性质的研究

运用量子化学PM3方法，对苯并噻二嗪几种衍生物的几何构型、电子结构和前线分子轨道成分进行了分析，研究了电荷分布规律。同时，基于体系中电子转移的特点，利用有限场FF方法探讨了其非线性光学性质的变化。结果表明，苯并噻二嗪分子具有较好的二阶非线性光学性质，并可能成为一类良好的光学材料。     

2H-1,2,4-苯并噻二嗪-1,1-二氧类化合物的简便合成

2H- 1 ,2 ,4 -苯并噻二嗪 - 1 ,1 -二氧类化合物在药物化学中有广泛的应用。常作为利尿剂 ,促进肾脏对尿的排泄 ,和其他药物混合使用还具有一定的降压作用 ,常作为高血压病的辅助治疗药物。本世纪五十年代发现的氯噻嗪 ( )和双氢氯噻嗪( ) ,利尿作用很强 ,成为利尿药和降压药的重大突破。此外这类化合物还具有抗菌、消炎、刺激毛发生长 [1] 等作用。在这类化合物的合成中 ,关环反应是关键步骤 ,文献报道过的主要方法为 :( 1 )用甲酸或原甲酸乙酯关环 [2 ] ;( 2 )用醛关环 [3 ] ;( 3)高温 (～ 2 0 0℃ )关环[4] 。当磺酰胺 (氮 )上的氢未…     

新型1,1-二氧代-4H-苯并[1,2,4]-噻二嗪类衍生物的合成及其抗肿瘤活性

以2-硝基苯磺酰氯为起始原料,经多步反应合成了12种新型1,1-二氧代-4H-苯并[1,2,4]-噻二嗪类衍生物,产物收率高,水溶性好,并经¹H NMR、¹³C NMR、MS-ESI和元素分析法确证结构。 用MTT法测试了这类衍生物对肝癌细胞HepG-2生长的抑制作用,结果显示目标化合物能不同程度地抑制肿瘤细胞生长,其中7-氨甲基-3-环丙基-1,1-二氧代-4H-苯并[1,2,4]-噻二嗪 (7c)对肝癌细胞HepG-2的抗性显著,最高抑制率达到79.3%。     

聚对苯撑乙烯齐聚物及其衍生物电子结构和发光机理的理论研究

运用量子化学从头算ab initio HF方法对聚对苯撑乙烯剂聚物及其衍生物的几何结构进行了优化,分析了前线分子轨道成分,确认了电子光谱的跃迁轨道。计算结果表明,聚苯撑乙烯剂聚物及衍生物的电子云分布与其结构密切相关,不同取代基修饰下的二聚苯撑乙烯的电子光谱发生红移,且随取代基推电子能力加强红移显。电子光谱跃迁主要是最高占据轨道向最低空轨道之间的π－π^*跃迁,计算结果和实验吻合得很好。     

[1,2,4]三唑并[3,4-b][1,3,4]噻二嗪类衍生物的合成及生物活性研究进展

[1,2,4]三唑并[3,4-b][1,3,4]噻二嗪作为极具前景的活性基团,在抗菌、抗肿瘤等方面具有多种药理活性,在药物和化学领域受到了广泛的关注。本文以含三唑并噻二嗪结构化合物的合成及其在抗肿瘤、抗菌等方面的生物活性为依据,对近几年国内外关于[1,2,4]三唑并[3,4-b][1,3,4]噻二嗪类化合物的研究进行分析总结,以期为后续该类新型抗肿瘤化合物的设计合成提供参考。     

微波法合成2，2＇-二苯-1，4-苯并噁嗪-3（4H）-酮及其结构表征

苯并噁嗪酮化合物广泛存在于禾本科植物中，这类化合物在前药合成和生物活性研究方面具有广泛的应用前景．目前已知的合成方法中，大多都是采用邻氨基酚与ClC（R1R2）COCl（氯酰氯）在碱性条件下长时间回流制得的，反应时间较长；除反应原料外，还需要加入其它碱性物质和溶剂．     

吡唑类化合物的研究（Ⅵ）：—吡唑[3,4—e]并—1，2，4—三嗪和吡唑[3,4—e]并—1，2，3，4—四嗪衍生物的合成

合成了14种1－苯基－3－氨基－5－氧代－4－取代腙吡唑及其关环产物吡唑[3,4-e]并－1，2，4－三嗪和吡唑[3,4-e]并－1，2，3，4－四嗪衍生物，经元素分析，IR^1H NMR和MS确定了其结构，并讨论了一些化合物的IR和1H NMR波谱性质。     

微波法合成2,2′-二苯-1,4-苯并噁嗪-3(4H)-酮及其结构表征

苯并噁嗪酮化合物广泛存在于禾本科植物中,这类化合物在前药合成和生物活性研究方面具有广泛的应用前景[1～4].目前已知的合成方法中,大多都是采用邻氨基酚与ClC(R1R2)COCl(氯酰氯)在碱性条件下长时间回流制得的,反应时间较长;除反应原料外,还需要加入其它碱性物质和溶剂[5～7]     

苯并咪唑苯并异喹啉酮及其衍生物的电子结构和光谱性质的理论研究

采用密度泛函、含时密度泛函和单激发组态相互作用(CIS)方法研究了苯并咪唑苯并异喹啉酮(1)及其衍生物的电子结构特性和光谱性质,并用极化连续模型考虑了溶剂的影响.结果表明,化合物1及其衍生物的吸收和荧光发射过程的电子垂直跃迁是由于分子内的电荷迁移.化合物1中取代基的位置及给吸电子能力影响其HOMO-LUMO能隙和电荷迁移量.在分子中引入吸电子和给电子取代基,均使最大吸收波长和最大荧光发射波长红移,计算的结果与实验结果吻合得较好.     

Theoretical study on the spectroscopic properties and electronic structures of heteroleptic phosphorescent Ir(III) complexes

The geometries, spectroscopic and electronic structures properties of a series of heteroleptic phosphorescent Ir(III) complexes including N981, N982, N983, N984 have been characterized by density functional theory calculations. The excited‐state properties of the Ir(III) complexes have been characterized by CIS method. The ground‐ and excited‐state geometries were optimized at the B3LYP/LANL2DZ and CIS/LANL2DZ levels, respectively. By using the time‐dependent density functional theory method, the absorption and phosphorescence spectra were calculated based on the optimized ground‐ and excited‐state geometries, respectively. The results show that the absorption and emission data agree well with the corresponding experimental results. The calculated results also revealed that the nature of the substituent at the 4‐position of the pyridyl moiety can influence the distributions of HOMO and LUMO and their energies. In addition, the charge transport quality has been estimated approximately by the calculated reorganization energy (λ). Our result also indicates that the positions of the substitute groups not only change the transition characters but also affect the charge transfer rate and balance, and complex N982 is a very good charge transfer material for green OLEDs. © 2008 Wiley Periodicals, Inc. Int J Quantum Chem, 2009     

RM1: a reparameterization of AM1 for H, C, N, O, P, S, F, Cl, Br, and I

Twenty years ago, the landmark AM1 was introduced, and has since had an increasingly wide following among chemists due to its consistently good results and time-tested reliability--being presently available in countless computational quantum chemistry programs. However, semiempirical molecular orbital models still are of limited accuracy and need to be improved if the full potential of new linear scaling techniques, such as MOZYME and LocalSCF, is to be realized. Accordingly, in this article we present RM1 (Recife Model 1): a reparameterization of AM1. As before, the properties used in the parameterization procedure were: heats of formation, dipole moments, ionization potentials and geometric variables (bond lengths and angles). Considering that the vast majority of molecules of importance to life can be assembled by using only six elements: C, H, N, O, P, and S, and that by adding the halogens we can now build most molecules of importance to pharmaceutical research, our training set consisted of 1736 molecules, representative of organic and biochemistry, containing C, H, N, O, P, S, F, Cl, Br, and I atoms. Unlike AM1, and similar to PM3, all RM1 parameters have been optimized. For enthalpies of formation, dipole moments, ionization potentials, and interatomic distances, the average errors in RM1, for the 1736 molecules, are less than those for AM1, PM3, and PM5. Indeed, the average errors in kcal x mol(-1) of the enthalpies of formation for AM1, PM3, and PM5 are 11.15, 7.98, and 6.03, whereas for RM1 this value is 5.77. The errors, in Debye, of the dipole moments for AM1, PM3, PM5, and RM1 are, respectively, 0.37, 0.38, 0.50, and 0.34. Likewise, the respective errors for the ionization potentials, in eV, are 0.60, 0.55, 0.48, and 0.45, and the respective errors, in angstroms, for the interatomic distances are 0.036, 0.029, 0.037, and 0.027. The RM1 average error in bond angles of 6.82 degrees is only slightly higher than the AM1 figure of 5.88 degrees, and both are much smaller than the PM3 and PM5 figures of 6.98 degrees and 9.83 degrees, respectively. Moreover, a known error in PM3 nitrogen charges is corrected in RM1. Therefore, RM1 represents an improvement over AM1 and its similar successor PM3, and is probably very competitive with PM5, which is a somewhat different model, and not fully disclosed. RM1 possesses the same analytical construct and the same number of parameters for each atom as AM1, and, therefore, can be easily implemented in any software that already has AM1, not requiring any change in any line of code, with the sole exception of the values of the parameters themselves.     

Theoretical study on the influence of ancillary ligand on the spectroscopic properties and electronic structures of phosphorescent Pt(II) complexes

The geometries, energies, and electronic properties of a series of phosphorescent Pt(II) complexes including FPt, CFPt, COFPt, and NFPt have been characterized within density functional theory DFT calculations which can reproduce and rationalize experimental results. The properties of excited‐states of the Pt(II) complexes were characterized by configuration interaction with singles (CIS) method. The ground‐ and excited‐state geometries were optimized at the B3LYP/LANL2DZ and CIS/LANL2DZ levels, respectively. In addition, we also have performed a triplet UB3LYP optimization for complex FPt and compared it with CIS method in the emission properties. The datum (562.52 nm) of emission wavelength for complex FPt, which were computed based on the triplet UB3LYP optimization excited‐state geometry, is not agreement with the experiment value (500 nm). The absorption and phosphorescence wavelengths were computed based on the optimized ground‐ and excited‐state geometries, respectively, by the time‐dependent density functional theory (TD‐DFT) methods. The results revealed that the nature of the substituent at the phenylpyridine ligand can influence the distributions of HOMO and LUMO and their energies. Moreover, the auxiliary ligand pyridyltetrazole can make the molecular structure present a solid geometry. In addition, the charge transport quality has been estimated approximately by the predicted reorganization energy (λ). Our result also indicates that the substitute groups and different auxiliary ligand not only change the nature of transition but also affect the rate and balance of charge transfer. By summarizing the results, we can conclude that the NFPt is good OLED materials with a solid geometry and a balanced charge transfer rate. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2010     

Application of the FAKE molecular-orbital method to diatomic molecules XY (X,Y = H,F, Cl,Br, I)

Theoretical Chemistry Accounts - The FAKE (fast, accurate kinetic energy) method of semiempirical molecular orbital calculation is applied to diatomic molecules XY (X, Y= H, F, Cl, Br, I). The...     

钴卟啉催化剂的前线轨道能级与其催化活性的相关性研究

设计并合成了12种钴卟啉催化剂,在温和反应条件(55℃, 2.0 MPa氧压)下考察其催化氧气液相氧化对硝基甲苯制取对硝基苯甲酸的催化活性,发现其对上述反应均有显著的催化活性.采用PM3半经验分子轨道法对所设计的钴卟啉化合物模型体系进行了计算,将计算结果与实验结果相结合,探讨了钴卟啉分子前线轨道能级与其催化活性之间的关系.经研究发现,四配位或五配位钴卟啉催化剂的催化活性与E_HOMO和ΔE_L-H均有一定的相关性,且ΔE_L-H对催化活性的影响大于E_HOMO对催化活性的影响;EHOMO值越低、ΔE_L-H越小,其催化活性越高.     

HCCO自由基与LiX(X=F,Cl,Br)锂键复合物的从头算研究

在MP2/6-311++G**水平上优化乙烯酮自由基与LiX(X=F,Cl,Br)形成锂键复合物.当卤素的电负性很强(如F元素),使得Li原子处于缺电子状态,此时,电子给体会把电子偏移向锂,形成共价性较强的锂键.而当卤素的电负性减弱时,锂键中主要成分逐渐变为离子键,并且此时锂键性质还要受电子给体影响.另外,由于HCCO为缺电子结构,电负性较弱且体积较大的卤素中的孤对电子会与HCCO之间通过静电相互作用,使得HCCO…Li—X键夹角变小,接近120°.锂键性质对HCCO…LiX(X=F,Cl,Br)复合物中Li—X的伸缩振动频率有直接影响.当锂键表现为共价性时,该频率红移,而当锂键表现为离子性时,该频率蓝移.但是,由于Cl的电负性与O的接近,C的电负性与Br接近所以,在O…Li…Cl和C…Li…Br中容易形成共振结构,导致远大于在其他复合物中的红移.     

三聚氰胺结构和热力学性质的密度泛函理论研究

采用Materials Studio 软件中的DMol~3模块对三聚氰胺的结构和性质进行了理论研究.得到了分子的几何构型、振动频率、各原子上的电荷分布、热力学、以及Fukui指数和前线分子轨道.计算结果表明:三聚氰胺分子中的C原子易得电子,是亲核试剂进攻点,而胺基上的N原子因含孤对电子是亲电反应中心.     

Theoretical study on tetranuclear boron clusters: B4X4 (X = H, F, Cl, Br, I)

The molecular orbitals for B4H4, B4F4, B4Cl4, B4Br4 and B4I4 have been calculated by using all-electron or effective core potential ab initio method at the self-consistent field level using basis sets with diffuse and polarization functions. The boron-boron and boron-halide (-hydrogen) distances of these cage compounds are optimized with three kinds of basis sets constrained to a tetrahedral symmetry. According to the localization scheme of Boys, four three-centered two-electron (3c2e) B-B-B bonds localized on each of the faces of the B4 tetrahedron are derived for B4X4 clusters. The HOMO-LUMO energy gaps, atomization energies and Mulliken overlap populations of these compounds indicate that the stabilities of the clusters decrease in the sequence of B4F4 > B4Cl4, B4H4 > B4Br4 > B4I4.