2-(三甲氧基苯基)色胺盐酸盐的合成

2,3,4-及3,4,5-三甲氧基苯乙酮苯腙在多聚磷酸存在下进行Fischer反应,可生成相应的吲哚(1_a,1_b),但2,4,6-三甲氧基苯乙酮苯腙必须用无水氯化锌催化环化才能得到相应的吲哚(1_c)。1_a、1_b、1_c经Vilsmier反应生成相应的吲哚-3-醛(2_a,2_b,2_c);经与硝基甲烷缩合得到相应的2-(三甲氧基苯基)-3-(2-硝基乙烯基)吲哚(3_a,3_b,3_c);3_a及3_b用LiAlH₄还原即可制备成相应的色胺盐酸盐(4_a和4_b),3_b还被制成苦味酸盐(4_b)。     

第五、六族元素的有机化合物在合成中应用的研究Ⅳ.全氟炔-[2]-酸酯的合成与反应

本文报导通过分子内Wittig反应顺利地合成了三氟丁炔-[2]-酸甲酯(Ⅱ_a)和七氟己炔-[2]-酸甲酯(Ⅱ_b).将这些产品在水溶液中用氢氧化钠皂化,分别得到3-甲氧基-4,4,4-三氟丁烯-[2]-酸(Ⅲ_a)和3-甲氧基-4,4,5,5,6,6,6-七氟己烯-[2]-酸(Ⅲ_b).其结构经元素分析、红外吸收光谱与核磁共振谱证明.其成因推测可能是由于Ⅱ经分子内重排的反应的结果.Ⅲ.经稀酸水解,转变为三氟丙酮.     

乙炔基自由基C2H与氧气反应的密度泛函理论研究

应用量子化学从头算和密度泛函理论(DFT)对C₂H自由基和O₂的反应进行了研究.在B3LYP/6-311G^**水平上优化了反应通道上各驻点(反应物、中间体、过渡态和产物)的几何构型,并计算出它们的振动频率和零点振动能(ZPVE).各物种的总能量由CCSD(T)/6-311G^**//B3LYP/6-311G^**给出,并对能量进行了零点能校正.计算结果表明,反应物中自由基C₂H中的边端C进攻O₂形成了中间体1 (HCCOO),中间体1是一个加合产物.由中间体1经过不同的反应通道可以生成不同的产物P₁ (HCO+CO), P₂ (HCCO+O), P₃(CO₂+CH), P₄ (C₂O+OH)和P₅ (2CO+H).反应通道之间存在着竞争机制.其中P₁, P₂是主要产物,其次还有一定比例的P5生成,而产物P₃, P₄的生成几率较低.各条反应通道化学反应热的计算与实验吻合较好.     

腈氧化物的研究(Ⅱ)——合成新诺明(SMZ)的新路线

利用腈氧化物的1,3-偶极加成反应,合成新诺明(SMZ),以1,2,3-三氯代丁醛肟(Ⅰ_a),经转化为α,β-二氯代丁腈氧化物(Ⅱ_a)后,与对乙酰氨基苯磺酰胺加成,继而就地进行环合、消除反应,浮5-甲基-3-(对乙酰氨基苯磺酰氨基)异噁唑(Ⅲ_a),(Ⅲ_a)水解即得SMZ(Ⅳ_a)。同时依法制得5-苯基-3-(对氨基苯磺酰氨基)异噁唑(Ⅳ_b)。     

具有植物激素活性的Schiff碱化合物的研究(Ⅱ)——三氮唑类Schiff碱的合成及其生物活性

合成了11个新的含三氮唑环的Schif碱类化合物,UV、IR、¹HNMR谱和元素分析确定了它们的结构.生物活性测试表明,一些化合物具有明显的植物生长调节活性,其中化合物Ⅱ_e、Ⅰ_b、Ⅰ_c和Ⅰ_e具有良好的细胞分裂素活性,化合物Ⅱ_a、Ⅰ_a、Ⅰ_e、Ⅰ_i和Ⅰ_j具有优异的生根性能.     

C2H与HO2双自由基反应的密度泛函理论研究

应用量子化学从头算和密度泛函理论(DFT)对C₂H与HO₂双自由基的单重态反应进行了研究.在UB3LYP/6-311G水平上优化了反应通道上各驻点(反应物、中间体、过渡态和产物)的几何构型.在CCSD(T)/6-311G^{**水平上计算了各物种的单点能,并对总能量进行了零点能校正.研究结果表明,反应物中自由基C₂H的边端C进攻自由基HO₂的边端O是主要的进攻方式.首先形成了中间体1(HCCOOH),由此经过不同的反应通道可以得到主要产物P1,次要产物P2,P3和P5.生成P1的反应热为-814.40kJ/mol.自由基C₂H的中间C进攻自由基HO₂的边端O是次要的进攻方式,可以得到产物P4和P6.根据势能面分析,所有反应均是放热反应.}     

联苯负离子自由基与萘分子间长程电子转移的从头算研究

分离处理π σ π体系中的给体 ,受体和σ桥体 ,在HF/4 31G和HF/DZP水平上优化了联苯 ,联苯负离子自由基 ,萘和萘负离子自由基的几何构型 ,计算了分子间电子转移的内重组能 .取线性反应坐标R =0 .5 ,在STO 3G水平上用变分原理和分子轨道跃迁能方法 ,计算了π σ π体系自交换反应的电子转移矩阵元 .对交叉反应体系 ,沿线性反应坐标搜寻最小轨道能级分裂Δmin,确定了电子转移矩阵元和过渡态构型 .用Marcus双球模型计算液相电子转移的溶剂重组能 ,结合半经典模型计算了几种以联苯负离子自由基为给体 ,联苯和萘为受体的π σ π体系分子内电子转移速率常数 .     

肿瘤的化学治疗——ⅩⅫ.DL-N-二氯乙酰基-7-硝基色氨酸及其有关化合物的合成

1.本文叙述以7-硝基吲哚(ⅩⅣ)为原料,合成DL-N-二氯乙酰基-7-硝基色氨酸(Ⅷ)及其乙酯(Ⅺ);从DL-色氨酸(Ⅰ_a)制备DL-N-二氯乙酰基色氨酸(Ⅶ).2.从7-硝基克胺(ⅩⅤ)合成7-硝基吲哚乙酸(Ⅹ)及其甲酯(ⅩⅢ_a)和乙酯(ⅩⅢ_b).3.化合物Ⅷ和Ⅺ对HeLa细胞有明显的抑制作用.     

异质富勒烯C58BN的结构与光谱研究

用AM1、MNDO和INDO半经验方法研究了异质富勒烯C₅₈BN各异构体的结构、稳定性和电子光谱.所有这些半经验方法给出了相似的稳定性顺序.结果表明,在6-6位置取代的异构体是最稳定的,异构体的稳定性随杂原子间距离的增加而降低;与C₆₀相比,硼氮杂富勒烯C₅₈BN具有较低的前线轨道能级差、较小的电离势和较低的稳定化能.C₅₈BN很可能具有与C₆₀分子相似的反应活性,易发生亲核反应,但比C₆₀更易失去电子形成正离子.以AM₁优化构型为基础,利用INDO/CIS方法计算了各异构体的电子光谱.     

鸟嘌呤受羟基自由基损伤反应机理的量子化学研究

用密度泛函理论(DFT)研究羟基自由基与鸟嘌呤分子加成反应的过渡态, 并进行内禀反应坐标(IRC)反应路径解析, 结果表明, 羟基自由基加成到鸟嘌呤碳碳双键上. 利用B3LYP/6-31++G**对反应物、反应物络合物、过渡态以及产物络合物等反应通道上各个能量驻点的能量进行了计算, 得到反应活化能E_a=28.0867 kJ/mol. AIM计算结果显示, 过渡态结构中鸟嘌呤分子碳碳双键结构被削弱, 羟基自由基氧原子与鸟嘌呤分子碳碳双键中的C4原子具有较强的相互作用, 双键中剩余的π电子离域到了环体系中.     

原子簇Ni2Fe2P结构稳定性的密度泛函理论研究

利用DFT(密度泛函理论)方法在B3LYP/Lan12dz水平下对原子簇模型Ni₂Fe₂P的二十余种可能构型分别在二、四重态下进行优化计算,分析比较了优化结果的能量、结合能、吉布斯自由能变化和过渡态.结果表明:原子簇Ni₂Fe₂P十种异构体没有虚频,有可能稳定存在于非晶态合金中;其中以具有二重态的构型1的能量最低,结合能、吉布斯自由能变化及过渡态能垒最大,最为稳定;四重态中异构体1',2',3'和4'共存的可能性比较大.     

HSCCS自由基势能面的理论研究

在CCSD(T)/6-311G(d,f)//MP2/6-311G(d,f) ZPE水平下,计算得到含有8个异构体和11个过渡态的HSCCS自由基体系势能面,讨论了异构体的结构与稳定性及异构体之间的异构化过程.结果表明异构体m1的能量最低,除m1以外,异构体m2和m3的能量也比较低,在MP2水平上,过渡态TS1的能量比异构体m2仅高3.9kJ/mol,而在CCSD(T)水平上,TS1的能量比m2低14.6 kJ/mol,这说明异构体m2可以迅速转化为能量更低的m1.异构体m3的能量比异构体m1高49.99 kJ/mol,可以推断,在合适的实验条件下可以观测到异构体m1.     

Proton migration and tautomerism in protonated triglycine.

Proton migration in protonated glycylglycylglycine (GGG) has been investigated by using density functional theory at the B3LYP/6-31++G(d,p) level of theory. On the protonated GGG energy hypersurface 19 critical points have been characterized, 11 as minima and 8 as first-order saddle points. Transition state structures for interconversion between eight of these minima are reported, starting from a structure in which there is protonation at the amino nitrogen of the N-terminal glycyl residue following the migration of the proton until there is fragmentation into protonated 2-aminomethyl-5-oxazolone (the b(2) ion) and glycine. Individual free energy barriers are small, ranging from 4.3 to 18.1 kcal mol(-)(1). The most favorable site of protonation on GGG is the carbonyl oxygen of the N-terminal residue. This isomer is stabilized by a hydrogen bond of the type O-H.N with the N-terminal nitrogen atom, resulting in a compact five-membered ring. Another oxygen-protonated isomer with hydrogen bonding of the type O-H.O, resulting in a seven-membered ring, is only 0.1 kcal mol(-)(1) higher in free energy. Protonation on the N-terminal nitrogen atom produces an isomer that is about 1 kcal mol(-)(1) higher in free energy than isomers resulting from protonation on the carbonyl oxygen of the N-terminal residue. The calculated energy barrier to generate the b(2) ion from protonated GGG is 32.5 kcal mol(-)(1) via TS(6-->7). The calculated basicity and proton affinity of GGG from our results are 216.3 and 223.8 kcal mol(-)(1), respectively. These values are 3-4 kcal mol(-)(1) lower than those from previous calculations and are in excellent agreement with recently revised experimental values.     

Structures, stabilities, and electronic and optical properties of C62 fullerene isomers

The 2385 classical isomers and four nonclassical isomers of fullerene C62 have been studied by PM3, HCTH/3-21G//SVWN/STO-3G, B3LYP/6-31G(d)//HCTH/3-21G, and B3LYP/6-31G(d)//B3LYP/6-31G(d). The Cs:7mbr isomer, with a chain of four adjacent pentagons surrounding a heptagon, is predicted to be the most stable isomer, followed by C2v:4mbr which is 3.15 kcal/mol higher in energy. C2:0032 with three pairs of adjacent pentagons is the most stable isomer in the classical framework. To clarify the relative stabilities of C62 isomers at high temperatures, the entropy contributions are taken into account on the basis of the Gibbs energy at the B3LYP/6-31G(d) level. Analyses reveal that Cs:7mbr prevails in a wide temperature range. The vibrational frequencies of the five most stable C62 fullerene isomers are also predicted at the B3LYP/6-31G(d) level, and the simulated IR spectra show important differences in positions and intensities of the vibrational modes for different isomers. The nucleus-independent chemical shift and the density of states of the three most stable isomers show that the square in C2v:4mbr and the adjacent pentagons in Cs:7mbr and C2:0032 possess high chemical reactivity. In addition, the electronic spectra and second-order hyperpolarizabilities are determined by means of ZINDO and the sum-over-states mode. The intensity-dependent refractive index gamma(-omega; omega, omega, -omega) at omega = 2.3305 eV of Cs:7mbr is very large because of resonance with the external field. The second-order hyperpolarizabilities of the five most stable isomers of C62 are predicted to be larger than those of C60.     

原子簇Ni2Fe2P结构稳定性的理论研究

利用DFT(密度泛函理论)方法在B3LYP/Lan12dz水平下对原子簇模型Ni2Fe2P的二十余种可能构型分别在二、四重态下进行优化计算,分析比较了优化结果的能量、结合能、吉布斯自由能变化和过渡态.结果表明原子簇Ni2Fe2P十种异构体没有虚频,有可能稳定存在于非晶态合金中;其中以具有二重态的构型1的能量最低,结合能、吉布斯自由能变化及过渡态能垒最大,最为稳定;四重态中异构体1',2',3'和4'共存的可能性比较大.     

Density functional theory investigation of novel Eu(III) complexes with asymmetric bis(phosphine) oxides

Recently, we have developed novel Eu(III) complexes with three beta-diketonates and one asymmetric bis(phosphine) oxide whose light emission intensity is drastically increased. In this paper, one of these complexes is investigated by the density functional theory calculation. Sixteen isomers of this complex have been considered. The ratio of the existence for the most stable isomer (B1_1a) is found to be about 51%, and the sum of the ratio of the existence for the six most stable isomers (B1_1a, B1_3a, B1_8a, B1_2a, B1_1b, and B1_5a) is about 100%, assuming the Boltzmann distribution (T = 300 K). The coordination structures of the six most stable isomers in the ground states are similar, and we can expect asymmetric ligand fields for them, favorable for the efficient light emission. Vertical excitation energies and oscillator strengths for each isomer have been obtained by the time-dependent density functional theory. With the red-shift of the wavelength and the interpolation by Gaussian convolution, both the calculated absorption spectra for the most stable isomer B1_1a and the calculated absorption spectra for the ensemble average of the isomers are found to be similar to the experimental fluorescence excitation spectra. The efficiency of energy transfer from the triplet excited state to the Eu(III) ion is considered by calculating DeltaEET (difference between the adiabatic excitation energy of the complex for the lowest triplet state and the emission energy of the Eu(III) ion for 5D0 to 7F2). The characters for the lowest triplet states for the isomers are investigated by the spin density distributions of the triplet states.     

C60哌嗪加成物的结构及光谱研究

用ＩＮＤＯ系列方法研究了Ｃ６０的哌嗪衍生物Ｃ６０Ｎ２（Ｃ２Ｈ４）２的结构。结果表明［６，６］，异构体具有Ｃ２ｖ对称性［６，５］，异构体具有Ｃｓ对称性，前者能量较低。以优化构型为基础，计算两种加成产物的ＵＶ谱，结果表明，［６，６］异构体的特征吸收与实验值相符，同时对［６，５］异构体的ＵＶ谱进行理论预测，对电子跃迁进行了理论指认，并分析了光谱红移的原因。     

Energetics and bonding in beryllium metallized carbon clusters

Small carbon clusters C, C₂ and C₃ metallized with beryllium were studied by first principles within the hybrid density functional approach with generalized gradient correction. Cluster isomer structures for the ground state and several excited states where systematically calculated for C_xBe_y with x = 1–3 and y = 1–4 including the vibrational analysis of all states. Ionization potentials and electron affinities are calculated for the ground state cluster isomers. The thermal stability of the ground state isomers was verified within the harmonic approximation of the Helmholtz free energy up to temperatures of about 1000 K. Within the family of clusters studied, C₂Be₃ undergoes a solid-like structural transition at about 260 K changing from a planar structure at low temperatures to a linear isomer at high temperatures.     

New nonsymmetric P(OH)3 species. Comparison with the C3 isomer and themochemistry at the DFT, MP2, and CCSD(T) levels of theory

Two new less-symmetric P(OH)3 isomers that are more stable than the C3 structure are found at the density functional theory (B3PW91, B3LYP), MP2, and CCSD(T) levels with the large aug-cc-pvdz/pvtz basis sets. The C1 and C3 structures are qualitatively different from those found for the As(OH)3 molecule. An additional lower lying P(OH)3 structure with Cs symmetry has been obtained. With the largest basis set the Cs isomer is predicted to be the most stable. However, the inclusion of zero-point-energy corrections induces an inversion between the Cs and C1 isomers, with the latter becoming the lowest energy structure at the highest correlated level. Increasing inclusion of electronic correlation effects reduces the energy difference between the C1 and Cs structures while the C1-C3 energy difference and C1-Cs interconversion barrier become larger. In all cases, energy differences and barrier heights are around 1 kcal/mol.     

Conformational and NBO analysis on cis and trans isomers of methyl-1-(4-hydroxy-3-methoxyphenyl)-1,2,3,4-tetrahydro-9H-β-carboline-3-carboxylate

The cis and trans-methyl-1-(4-hydroxy-3-methoxyphenyl)-1,2,3,4-tetrahydro-9H-β-carboline-3-carboxylates were prepared and ¹H and ¹³C NMR spectra were recorded for both isomers. Conformational and NBO analysis were carried out for the cis and trans isomers. Conformer structures were pre-optimized using the hybrid method B3LYP along with the 6-311+G(d) basis set. Frequency calculations were employed to confirm the structures as minimum points. Potential energy surfaces (PES) were built at the same level of theory. Geometries obtained from DFT calculations were used to perform NBO analysis by the NBO 3.1 module in GAUSSIAN 03. The results obtained through theoretical calculations revealed that the shielding observed at C1 for the trans isomer can be attributed to carbomethoxy γ-effect, together with the hyperconjugative effect, while only hyperconjugative effects were found to explain the shielding of C3. The higher chemical shift value of C3 of the cis isomer was attributed to the carbonyl substituent, which plays an important role by capturing part of the electronic density in C3.