2,6-萘二甲酸二甲酯质子化机理的研究

本文通过对含有不同硫酸浓度的2,6-萘二甲酸二甲酯溶液的吸收光谱、室温和低温下的荧光光谱及荧光寿命的研究,观察到了2,6-萘二甲酸二甲酯与硫酸分子之间各种不同的相互作用:即基态下的电荷转移复合物吸收谱,激基复合物的发射谱,氢键作用吸收谱,质子转移后的吸收谱和发射谱以及质子化前后不同的荧光寿命。提出了2,6-萘二甲酸二甲酯与硫酸分子之间的相互作用是通过激基复合物过渡到氢键,然后由氢键过渡到质子转移的过程。     

碱(土)金属离子与2-(3′-羟基-2′-吡啶基)苯并噁唑阳离子-π复合物及其分子内质子转移过程的理论研究

采用密度泛函B3LYP方法,在6-311++G(d,p)基组水平上对碱(土)金属离子(Li+,Na+,K+,Be2+,Mg2+和Ca2+)与2-(3’-羟基-2’-吡啶基)苯并噁唑(HPyBO)的36种阳离子-π复合物的初始构型进行了几何全优化,并计算了其相互作用能.结果表明,碱(土)金属离子与HPyBO复合物有较强的阳离子-π相互作用,部分复合物甚至达到了化学键的强度.相对能量的变化表明碱(土)金属离子的作用能改变HPyBO分子内质子转移过程的能垒,甚至可以导致优势构型反转.当考虑水的溶剂效应后,各质子转移异构体的相对能量及质子转移的能垒均有一定程度的改变.另外,应用分子中的原子(AIM)方法对复合物分子内氢键的键临界点性质进行了分析.     

2-[(4-氯苯基亚氨基)甲基]-8-羟基喹啉质子转移的理论研究

研究了2-[(4-氯苯基亚氨基)甲基]-8-羟基喹啉的三种质子转移途径: 分子内质子转移、水分子辅助质子转移和甲醇分子辅助质子转移. 以该席夫碱化合物的晶体结构作为模型, 在B3LYP/6-31＋G(d)水平上, 优化得到稳定态和过渡态的几何构型. 对三类质子转移前后的结构、能量、红外光谱、化学位移进行研究, 结果表明水分子辅助质子转移和甲醇分子辅助质子转移中, 水和甲醇分子利用氢键作用参与质子转移过程, 形成七元环状过渡态, 大大降低了反应的能垒, 有利于质子的转移, 氢键在降低活化能方面起着重要作用.     

儿茶素-胞嘧啶分子间相互作用的密度泛函研究

采用密度泛函理论的B3LYP方法,在6-31+G*基组水平上研究了儿茶素-胞嘧啶分子间相互作用机制,得到稳定的儿茶素-胞嘧啶复合物11个.计算结果表明氢键对于复合物的稳定性起着重要的作用,并且当复合物形成2个或更多的氢键时,氢键的类型及强度共同决定着复合物的稳定性.我们还应用了分子中的原子(AIM)理论和自然键轨道(NBO)理论对这11种复合物中氢键的性质和特征进行了分析.通过研究发现,所有的氢键复合物进行基组重叠误差(BSSE)校正后的相互作用能为-17.35～-43.27kJ/mol,相互作用能主要由氢键所贡献.振动分析显示,氢键的形成使相对应键的对称伸缩振动频率减小,说明这些复合物中形成的氢键都是正常的红移型氢键,与实验结果相一致.     

B型DNA中鸟嘌呤-胞嘧啶碱基对内双质子转移反应

采用ONIOM(M06-2X/6-31G^*:PM3)方法研究了单个鸟嘌呤-胞嘧啶(GC)碱基对和含GC碱基对的四种排序的DNA三聚体(dATGCAT, dGCGCGC, dTAGCTA, dCGGCCG)的双质子转移反应. 通过分析其双质子转移方式、质子转移过程中各结构的能量和氢键变化, 总结出环境因素对GC碱基对双质子转移机理的影响. 气相中, dCGGCCG三聚体中发生分步双质子转移, 其它四种模型中均发生协同双质子转移. 分析发现质子转移方式受上下相邻碱基对的静电相互作用和质子接受位的质子亲和势影响, dATGCAT和dGCGCGC排序有助于质子H4a转移, 而dTAGCTA和dCGGCCG排序有助于质子H1转移, 胞嘧啶的N3位较高的质子亲和势有助于质子H1转移. 水溶剂中, 上下相邻碱基对的静电相互作用被减弱, 水溶剂稳定了分步转移过程中的单质子转移产物, 因此分步转移机理占据优势, 五种模型中均出现分步双质子转移, 在此过程中能量变化趋势相似. 溶剂效应有利于单质子转移, 却增加了双质子转移反应的反应能.     

1,2,4-三氮杂苯-(H2O)n复合物氢键相互作用的密度泛函理论研究

用密度泛函理论方法在B3LYP／6—31 G**水平上对1，2，4-三氮杂苯-(H2O)n(n=1，2，3)氢键复合物的基态进行了结构优化和能量计算，结果表明复合物之间存在较强的氢键作用，所有稳定复合物结构中形成一个N…H--O氢键并终止于弱O…H—C氢键的氢键水链的构型最稳定．同时，用含时密度泛函理论方法(TD—DPT)在TD—B3LYP／6—31 G**水平上计算了1,2，4-三氮杂苯单体及其氢键复合物的单重态第-1(n，π*)垂直激发能．     

Alkali （Alkali Earth） Metal Ions with 2-（3＇-Hydroxy-2＇-pyridyl）benz- oxazole Cation-π Complexes and Its Intramolecular Proton Transfer Process： A Theoretical Investigation

采用密度泛函B3LYP方法,在6—311＋＋G（d,p）基组水平上对碱（土）金属离子（Li＋,Na＋,K＋,Be2＋,Mg2＋和Ca2＋）与2-（3’-羟基-2’-吡啶基）苯并噁唑（HPyBO）的36种阳离子-π复合物的初始构型进行了几何全优化,并计算了其相互作用能．结果表明,碱（土）金属离子与HPyBO复合物有较强的阳离子-π相互作用,部分复合物甚至达到了化学键的强度．相对能量的变化表明碱（土）金属离子的作用能改变HPyBO分子内质子转移过程的能垒,甚至可以导致优势构型反转．当考虑水的溶剂效应后,各质子转移异构体的相对能量及质子转移的能垒均有一定程度的改变．另外,应用分子中的原子（AIM）方法对复合物分子内氢键的键临界点性质进行了分析．     

4-(9-蒽基)-6-辛氧基-1,3,5-三嗪-2-胺的合成及其在酸性介质中的光谱行为研究

以2,4-二氯-6-辛氧基-1,3,5-三嗪为原料,经Kumada偶联及胺化两步反应合成了三嗪胺衍生物:4-(9-蒽基)-6-辛氧基-1,3,5-三嗪-2-胺(AOOTA),总产率为38%.通过紫外-可见吸收光谱及荧光光谱研究了氯仿溶液中AOOTA在乙酸(HOAc)及三氟乙酸(TFA)作用下的光谱行为.研究发现AOOTA与HOAc在基态及激发态下均不能发生双氢键作用,而AOOTA与TFA相互作用基态下形成双氢键复合物,激发态下由于分子中蒽基及辛氧基与三嗪环间的C-C单键以及C-O单键的自由旋转,从而使得AOOTA与TFA分子间不能形成有效的氢键相互作用.     

三氮杂苯-水氢键复合物的结构与性质

使用密度泛函理论B3LYP方法对三氮杂苯-水氢键复合物的基态结构与相互作用进行理论研究. 结果表明1,2,3-三氮杂苯-水, 1,2,4-三氮杂苯-水和1,3,5-三氮杂苯-水复合物基态分别具有Cs, Cs和C₁对称性和强的氢键相互作用, 经基组重叠误差和零点振动能校正后的相互作用能分别为–17.83, –17.38和–13.55 kJ/mol. 三氮杂苯-水复合物中, N∙∙∙H—O氢键的形成使水的H—O对称伸缩振动频率明显红移. 同时使用含时密度泛函理论研究了三氮杂苯单体及其与水形成的氢键复合物的第一¹(n, π^*)激发态的垂直激发能.     

纳米腔限制环境下2-(2-羟苯基)苯并噻唑的质子转移

采用稳态和瞬态荧光法对2-(2-羟苯基)苯并噻唑(HBT)与七元瓜环(CB7)的超分子作用及CB7分子纳米腔限制作用对HBT激发态质子转移(ESIPT)过程进行了研究,并采用Benesi-Hildebrand方程对荧光数据进行处理,以确定超分子复合物的组成比.结果表明,在N,N-二甲基甲酰胺(DMF)和二氯甲烷溶液中,CB7与HBT的作用均形成化学计量比为1∶1的主客体复合物,HBT的质子转移对溶剂很敏感,CB7的加入,使HBT的荧光寿命降低,量子产率增大.在DMF溶液中,CB7的加入促进了酚氧负离子的形成,而在二氯甲烷溶液中,CB7的加入限制了HBT的激发态质子转移.结构优化计算表明,CB7与HBT能形成化学计量比为1∶1的复合物.     

Structures and energetics of Be(n)Si(n) and Be(2n)Si(n) (n = 1-4) clusters

The structures and energies of Be(n)Si(n) and Be(2n)Si(n) (n = 1-4) clusters have been examined in ab initio theoretical electronic structure calculations. Cluster geometries have been established in B3LYP/6-31G(2df) calculations and accurate relative energies determined by the G3XMP2 method. The two atoms readily bond to each other and to other atoms of their own kind. The result is a great variety of low-energy clusters in a variety of structural types.     

Experimental and computational study of the Zn(n)S(n) and Zn(n)S(n)+ clusters

Zinc sulfide clusters produced by direct laser ablation and analyzed in a time-of-flight mass-spectrometer, showed evidence that clusters composed of 3, 6, and 13 monomer units were ultrastable. The geometry and energies of neutral and positively charged Zn(n)S(n) clusters, up to n = 16, were obtained computationally at the B3LYP/6-311+G level of theory with the assistance of an algorithm to generate all possible structures having predefined constraints. Small neutral and positive clusters were found to have planar geometries, neutral three-dimensional clusters have the geometry of closed-cage polyhedra, and cationic three-dimensional clusters have structures with a pair of two-coordinated atoms. Physical properties of the clusters as a function of size are reported. The relative stability of the positive stoichiometric clusters provides a thermodynamic rationale for the experimental results.     

Structure and vibrations of Ga(n)N(n) (n = 3-10) clusters

The structure and harmonic vibrations of Ga(n)N(n) (n = 3-10) clusters have been investigated using the B3LYP (Becke 3-parameter-Lee-Yang-Parr) density functional theory. All structures are found to be cumulenic D(nh) rings (equal bonds, alternating angles), with one intense out of plane mode and three infrared-active degenerate modes, of which the highest one is extremely intense and asymptotically increases to 1029 cm(-1) for n = 10. Comparisons with C2n, B(n)N(n), and Al(n)N(n) clusters, the structure and bonding type for the Ga(n)N(n) (n=3-10) clusters are consistent with those of the C2n (n = 3, 5, 7, ...) clusters, the B(n)N(n) (n = 3-10), and Al(n)N(n) (n = 3-9) clusters.     

The structure and energetics of (GaAs)n, (GaAs)n(-), and (GaAs)n+ (n=2-15)

Electronic and geometrical structures of neutral, negatively, and positively charged (GaAs)n clusters are computed using density functional theory with generalized gradient approximation. All-electron computations are performed on (GaAs)2-(GaAs)9 while effective core potentials (ECPs) are used for (GaAs)9-(GaAs)15. Calibration calculations on GaAs and (GaAs)9 species support the use of the ECP for the larger clusters. The ground-state geometries of (GaAs)n(-) and/or (GaAs)n+ are different from the corresponding neutral ground-state geometry, except for n=7, 9, 12, 14, and 15, where the neutral and ions have similar structures. Beginning with n=6, all atoms are three coordinate, except for (GaAs)10+ and (GaAs)13+. For the larger species, there is a competition between fullerenes built from hexagons and rhombi and geometrical configurations where Ga-Ga and As-As bonds are formed, which results in the formation of pentagons. As expected, the static polarizability varies in the order of anion>neutral>cation, but the values are rather similar for all three charge states. The thermodynamic stability for the loss of GaAs is reported.     

Global optimization of ionic Mg(n)F(2n) (n=1-30) clusters

The global optimization basin-hopping (BH) method has been used to locate the global minima (GM) of Mg(n)F(2n) (n=1-30) clusters using a Born-Mayer-type potential. Some of the GM were particularly difficult to find, requiring more than 1.5 x 10(4) BH steps. We have found that both the binding energy per MgF2 unit and the effective volume of the GM isomers increase almost linearly with n, and that cluster symmetry decreases with cluster size. The data derived from the BH runs reveal a growing density of local minima just above the GM as n increases. Despite this, the attraction basin around each GM is relatively large, since after all their atomic coordinates are randomly displaced by values as high as 2.0 bohrs, the perturbed structures, upon reoptimization, relax back to the GM in more than 50% of the cases (except for n=10 and 11). The relative stabilities derived from energy second differences suggest that n=8,10,13,15, and 20 are probably the magic numbers for these systems. Mass spectrum experiments would be very useful to clarify this issue.     

Theoretical study of Al(n) and Al(n)O (n = 2-10) clusters

The stable structures, energies, and electronic properties of neutral, cationic, and anionic clusters of Al(n) (n = 2-10) are studied systematically at the B3LYP/6-311G(2d) level. We find that our optimized structures of Al5(+), Al9(+), Al9(-), Al10, Al10(+), and Al10(-) clusters are more stable than the corresponding ones proposed in previous literature reports. For the studied neutral aluminum clusters, our results show that the stability has an odd/even alternation phenomenon. We also find that the Al3, Al7, Al7(+), and Al7(-) structures are more stable than their neighbors according to their binding energies. For Al7(+) with a special stability, the nucleus-independent chemical shifts and resonance energies are calculated to evaluate its aromaticity. In addition, we present results on hardness, ionization potential, and electron detachment energy. On the basis of the stable structures of the neutral Al(n) (n = 2-10) clusters, the Al(n)O (n = 2-10) clusters are further investigated at the B3LYP/6-311G(2d), and the lowest-energy structures are searched. The structures show that oxygen tends to either be absorbed at the surface of the aluminum clusters or be inserted between Al atoms to form an Al(n-1)OAl motif, of which the Al(n-1) part retains the stable structure of pure aluminum clusters.     

Activation cross-sections for some (n, 2n), (n,p) and (n, γ)-reactions

The average fission neutron cross-sections of the reactions²³³U(n, 2n)²³²U,⁶⁰Ni(n, p)⁶⁰Co and²⁷Al(n, p)²⁷Mg and the resonance integrals of the (n, γ)-reactions of the nuclides¹⁸¹Ta,¹⁷⁶Lu,¹⁷⁵Lu,⁶⁴Ni,⁵⁹Co and²⁶Mg have been determined by the activation method following the well-known conventions. The results verify some of the existing values and present data for hitherto unknown or poorly known reactions.     

Zur Darstellung der Schichtverbindungen (SiH) n und (SiF) n

Zusammenfassung Aus schichtförmig gebauten (SiCl) _n bzw. (SiBr) _n läßt sich durch vorsichtige Fluorierung mit SbF₃ das entsprechende (SiF) _n herstellen. Durch Hydrierung von (SiBr) _n mit LiAlH₄ entsteht (SiH) _n . Die Eigenschaften der beiden neuen Verbindungen werden beschrieben.

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Preparation of layered (SiH) _n and (SiF) _n resp

Careful fluorination of (SiCl) _n -or (SiBr) _n -layers with SbF₃ yields (SiF) _n . LiAlH₄ reacts with (SiBr) _n to (SiH) _n . The properties of these two new compounds are described.

     

Synthesis and X-Ray Crystal Structures of Fe2Ru(CO)12−n (CNBu t ) n and FeRu2(CO)12−n (CNBu t ) n (n=1, 2)

The clusters Fe₂Ru(CO)_12–n (CNBu ^t ) _n (3, n=1; 4, n=2), FeRu₂(CO)_12–n (CNBu ^t ) _n (5, n=1, 6, n=2) and FeRu₂(CO)₁₁(CNCy) (5a) have been prepared by direct substitution from the parent carbonyl precursors Fe₂Ru(CO)₁₂ (1) and FeRu₂(CO)₁₂ (2). All compounds have been characterized spectroscopically and clusters 3, 4, 5, and 6 by single crystal X-ray determinations. In all cases, the isonitrile ligands adopt axial or pseudo-axial positions on a ruthenium atom. The structures of 3–5 are very similar to their parent clusters, but the extent of metal framework disorder is significantly less. Cluster 6 adopts the same C _2v Fe₃(CO)₁₂ type structure as 4, and thus differs markedly from the parent compound 2, which has a D ₃ structure .