LiAl的电子与几何结构

应用平面波展开和第一原理赝势法研究了锂铝单晶的电子和几何结构,给出LiAl各种可能结构的能量～体积关系图以及相关的能带结构,电子态密度和电荷密度分布等各种性质变化关系.讨论了B32结构与其他结构电子键合性质的不同,指出B32结构之所以成为LiAl最稳定的结构是由于Al＿Al原子形成了类似于Si＿Si的共价键合.计算得到的能量最低的稳定结构与实验以及其它的理论计算结果一致.     

难熔固体MX(M=Sc,Ti,V;X=C,N,O)电子结构和力学性质的密度泛函研究

采用密度泛函方法对MX(M=Sc,Ti,V;X=C,N,O)固体的体相电子结构和力学性质进行了系统研究.计算结果表明,对于金属原子相同的同一系列化合物,氮化物具有最大的体模量;进一步的研究可知,随着外界压力的增大,化合物由NaCl构型向CsCl构型转变由易到难的顺序依次是氧化物、氮化物和碳化物.本文还首次用密度泛函方法系统地计算了各化合物的能带结构和态密度,并对该类型化合物的导电性能进行了探讨.     

TiC固体的相稳定性和高压相变的密度泛函研究

采用基于第一性原理的密度泛函方法对TiC固体的NaCl,WC和CsCl三种相的电子结构进行了研究,结果表明,在零压力下相稳定次序为NaCl>WC>CsCl,该顺序可用费米能级附近电子态的大小加以解释,当增加外压力时,随着单胞体积的减小,CsCl相逐渐成为稳定相,在外压约为475.9GPa时,NaCl相将向CsCl相转变,而CsCl相转变为WC相要求的外压较高.此外,还进一步探讨了压力对三种相的能带结构、化学键以及电荷密度的影响.     

有机-无机杂化化合物[Cu（μ-cbdca）（H2O）]n的电子结构及铁磁性

利用基于密度泛函理论(DVF)的第一性原理的FP_LAPW方法,对以铜离子为磁性中心的化合物[Cu(μ-cbdca)(H2O)]n(cbdca=cyclobutanedicarboxylate)的电子结构及磁性质进行了计算.对该材料的铁磁性、反铁磁性和非磁性三种状态下的总能量进行了计算.计算结果表明,[Cu(μ-cbdca)(H2O)]n的铁磁态能量最低,该化合物为稳定的铁磁性物质,该结果与实验吻合较好.对原子磁矩的计算结果发现,铜原子对化合物磁性的贡献较大,双齿配体上的氧原子和碳原子的贡献相对较小.     

有机-无机杂化化合物[Cu(μ-cbdca)(H2O)]n的电子结构及铁磁性

利用基于密度泛函理论(DFT)的第一性原理的FP_LAPW方法, 对以铜离子为磁性中心的化合物[Cu(μ-cbdca)(H2O)]n(cbdca=cyclobutanedicarboxylate)的电子结构及磁性质进行了计算. 对该材料的铁磁性、反铁磁性和非磁性三种状态下的总能量进行了计算. 计算结果表明, [Cu(μ-cbdca)(H2O)]n的铁磁态能量最低, 该化合物为稳定的铁磁性物质, 该结果与实验吻合较好. 对原子磁矩的计算结果发现, 铜原子对化合物磁性的贡献较大, 双齿配体上的氧原子和碳原子的贡献相对较小.     

BaTiO3的电子结构和光学性质

采用第一性原理赝势平面波方法, 在局域密度近似(LDA)和广义梯度近似(GGA)下分别计算了BaTiO3立方相和四方相的电子结构, 并在局域密度近似下计算了BaTiO3立方相的光学性质. 结果表明, BaTiO3立方相和四方相都为间接带隙, 方向分别为Γ-M和Γ-X, 大小分别为2.02和2.20 eV. 对BaTiO3和PbTiO3铁电相短键上电子布居数的对比分析, 给出了它们铁电性大小的差别. 且在30 eV的能量范围内研究了BaTiO3 的介电函数、吸收系数、折射系数、湮灭系数、反射系数和能量损失系数等光学性质,并基于电子能带结构对光学性质进行了解释. 计算结果与实验数据相符合.     

3d过渡金属碳化物相稳定性和化学键的第一性原理研究

采用第一性原理方法对具有NaCl相、CsCl相以及WC相结构的3d过渡金属碳化物MC(M=Sc～Ni)的电子结构进行了详细研究,研究结果表明,对于同一类型相结构的Mc化合物具有相似的能带结构,均可用刚性带模型来描述,并由此得到了三种相统一的态密度(1DOS)分布．基于该DOS分布,通过分析费米能级附近DOS的大小并结合体系的结合能,对三种相的稳定性进行了探讨．结果表明,CsCl相构型最不稳定;对于3d电子数较少的MC化合物(M=Sc～V),以NaCl相为稳定构型;对于M=Cr～Ni的MC化合物,则以WC相为稳定相．此外,通过采用双子晶格模型,进一步从化学键角度对影响三种相稳定性的内在原因进行了探讨．     

环己硅烷类液晶化合物的量子化学研究: 联苯基乙烷类系列

运用AM1和PM3两种SCF-MO方法, 通过能量梯度全优化计算, 给出了25种环己硅烷类液晶化合物的稳定几何构型、电子结构和生成热、偶极矩等基本性质。联系有机电子结构理论进行了讨论。     

CdO及CdxZn1-xO化合物的结构、能量和电子性能分析

采用基于密度泛函理论的第一性原理的平面波超软赝势计算方法, 研究了纤锌矿结构的CdxZn1-xO化合物以及CdO在纤锌矿结构、岩盐结构和闪锌矿结构的基态电子特性和体结构, 分析了CdO的稳定性. 通过对比纤锌矿结构、岩盐结构和闪锌矿结构CdO的内聚能, 发现岩盐结构和纤锌矿结构CdO的稳定性好, 闪锌矿结构相对较差; 通过对CdxZn1-xO化合物在不同Cd组分下的电子结构计算, 得到了较好的禁带宽度拟合结果, 能带弯曲参量B=1.02 eV; 通过形成能与组分关系的分析, 我们认为当Cd的组分x=0.4左右时, CdxZn1-xO化合物最不稳定, 容易出现相分离现象.     

CdO及CdxZn1-xO化合物的结构、能量和电子性能分析

采用基于密度泛函理论的第一性原理的平面波超软赝势计算方法,研究了纤锌矿结构的cdxZn1-xO化合物以及CdO在纤锌矿结构、岩盐结构和闪锌矿结构的基态电子特性和体结构,分析了CdO的稳定性.通过对比纤锌矿结构、岩盐结构和闪锌矿结构CdO的内聚能,发现岩盐结构和纤锌矿结构CdO的稳定性好,闪锌矿结构相对较差;通过对CdxZn1-xO化合物在不同Cd组分下的电子结构计算,得到了较好的禁带宽度拟合结果,能带弯曲参量B=1.02 eV;通过形成能与组分关系的分析,我们认为当Cd的组分x=0.4左右时,CdxZn1-xO化合物最不稳定,容易出现相分离现象.     

NiAs- versus zinc-blende-type intermetallic insertion electrodes for lithium batteries: lithium extraction from Li2CuSn

The extraction of lithium from Li₂CuSn with a lithiated zinc-blende-type structure has been investigated both chemically and electrochemically. The data show that the resulting Li_xCuSn (x≈0) product has a NiAs-related structure similar to that of Cu₆Sn₅ (CuSn_0.83). The Li₂CuSn structure is described in detail; this structure type has important implications for designing new intermetallic insertion electrodes with zinc-blende-type structures.     

Ab initio study on the electronic and mechanical properties of ReB and ReC

The structural, electronic, and mechanical properties of ReB and ReC have been studied by use of the density functional theory. For each compound, six structures are considered, i.e., hexagonal WC, NiAs, wurtzite, cubic NaCl, CsCl, and zinc-blende type structures. The results indicate that for ReB and ReC, WC type structure is energetically the most stable among the considered structures, followed by NiAs type structure. ReB-WC (i.e., ReB in WC type structure) and ReB-NiAs are both thermodynamically and mechanically stable. ReC-WC and ReC-NiAs are mechanically stable and becomes thermodynamically stable above 35 and 55 GPa, respectively. The estimated hardness from shear modulus is 34 GPa for ReB-WC, 28 GPa for ReB-NiAs, 35 GPa for ReC-WC and 37 GPa for ReC-NiAs, indicating that they are potential candidates to be ultra-incompressible and hard materials.     

First principles investigation on the ultra‐incompressible and hard TaN

The structural, electronic, and mechanical properties of TaN were investigated by use of the density functional theory (DFT). Eight structures were considered, i.e., hexagonal WC, TaN, NiAs, wurtzite, and CoSn structures, cubic NaCl, zinc‐blende and CsCl structures. The results indicate that TaN in TaN‐type structure is the most stable at ambient conditions among the considered structures. Above 5 GPa, TaN in WC‐type structure becomes energetically the most stable phase. They are also stable both thermodynamically and mechanically. TaN in WC‐type has the largest shear modulus 243 GPa and large bulk modulus 337 GPa among the considered structures. The volume compressibility is slightly larger than diamond, but smaller than c‐BN at pressures from 0 to 100 GPa. The compressibility along the c axis is smaller than the linear compressibility of both diamond and c‐BN. The estimated hardness is 34 GPa. Thus, TaN in WC‐type structure is a potential candidate to be ultra‐incompressible and hard. The unique mechanical properties of TaN in WC‐type structure would make it suitable for applications under extreme conditions. © 2009 Wiley Periodicals, Inc. J Comput Chem, 2009     

Electronic and mechanical properties of 5d transition metal mononitrides via first principles

The electronic and mechanical properties of 5d transition metal mononitrides from LaN to AuN are systematically investigated by use of the density-functional theory. For each nitride, six structures are considered, i.e., rocksalt, zinc blende, CsCl, wurtzite, NiAs and WC structures. Among the considered structures, rocksalt structure is the most stable for LaN, HfN and AuN, WC structure for TaN, NiAs structure for WN, wurtzite structure for ReN, OsN, IrN and PtN. The most stable structure for each nitride is mechanically stable. The formation enthalpy increases from LaN to AuN. For LaN, HfN and TaN, the formation enthalpy is negative for all the considered structures, while from WN to AuN, except wurtzite structure in ReN, the formation enthalpy is positive. The calculated density of states shows that they are all metallic. ReN in NiAs structure has the largest bulk modulus, 418 GPa. The largest shear modulus 261 GPa is from TaN in WC structure. Trends are discussed.     

Electronic structures of M21S8 (M = Nb, Zr) and (M,M')21S8 (M, M' = Hf, Ti; Nb, Ta) phases and reasons for variations in the metal site occupations

The electronic structures of binary M21S8 (M = Nb, Zr) and isostructural ternary (M,M')21S8 (M, M' = Hf, Ti; Nb, Ta) phases have been studied by means of extended Hückel tight-binding band structure calculations. For the valence electron concentration in the binary group 5 metal phase Nb21S8, metal-metal bonding is optimized whereas, in the isostructural group 4 metal phase Zr21S8, metal-metal bonding levels exist above the Fermi level. However, the electronic structure analysis suggests a stable structure for M21S8 phases with group 4 metals and that (M,M')21S8 phases with mixed group 4 and group 5 metals, even if not yet reported, could well exist. In the ternary phase Nb6.9Ta14.1S8, a linear relationship exists between the magnitude of the metal-metal bonding capacity (as expressed by the total metal-metal Mulliken overlap population) of each crystallographically independent metal site and the occupation of the site with the heavier metal (i.e., the element with the greater bonding capability). The situation is quite more complex in Hf7.5Ti13.5S8, where the metal-metal bonding capacity of each site, differences in electronegativity between Ti and Hf, and site volume arguments must be taken into account to understand the metal site occupation.     

First Principles Investigation of Electronic Property and High Pressure Phase Stability of SmN

An investigation of electronic property and high pressure phase stability of SmN has been conducted using first principles calculations based on density functional theory. The electronic properties of SmN show a striking feature of a half metal, the majority-spin electrons are metallic and the minority-spin electrons are semiconducting. It was found that SmN undergoes a pressure-induced phase transition from NaCl-type (B1) to CsCl-type structure (B2) at 117 GPa. The elastic constants of SmN satisfy Born conditions at ambient pressure, indicating that B1 phase of SmN is mechanically stable at 0 GPa. The result of phonon spectra shows that B1 structure is dynamically stable at ambient pressure, which agrees with the conclusion derived from the elastic constants.     

供电子基团修饰对NNI-R系列分子光物理性质的影响

设计了一系列具有不同供电子基团的N-苯基-1,8-萘二甲酰亚胺衍生物(NNI-R), 对它们在二氯甲烷和气相中的几何结构、 电子结构以及室温磷光性能进行了研究. 在二氯甲烷极性溶剂中, NNI-R系列分子的最低单重激发态(S₁)有2个异构体, 分别表现为局域激发(LE)和电荷转移激发(CT). 具有弱给电子体(R=OMe, OH)时的NNI-R分子, 其S₁态为LE结构, 给体和受体间二面角垂直, 其总能量远低于CT结构, 会抑制系间窜越(ISC)的发生, 不会发生磷光现象. 在气相下, NNI-R系列分子的S₁态只有一种稳定的CT结构, 该特征能显著抑制荧光发射, 并有效促进系间窜越, 使NNI-R系列分子的室温磷光发射成为一种可能.     

从头算分子动力学模拟Pd团簇负载UiO-66材料结构及稳定性

采用从头算分子动力学模拟与密度泛函理论相结合的方法,计算模拟了不同尺寸的Pdn(n=1~32)金属团簇在UiO-66孔道中的稳定构型,并对金属团簇与材料骨架之间的作用方式、结合能及骨架形变能等进行了讨论.采用Bader电荷分析方法对该体系的电荷转移情况进行了计算分析.结果表明,Pdn团簇稳定负载于UiO-66材料的四面体笼中,且均呈堆积型构型.当Pd原子个数为28时体系的热力学稳定性最好,这与金属团簇和有机配体的成键方式相关,是金属团簇内部结合能和骨架形变能综合作用的结果.     

Polymorphic phases of sp3-hybridized carbon under cold compression

It is well established that graphite can be transformed into superhard carbons under cold compression (Mao et al. Science 2003, 302, 425). However, structure of the superhard carbon is yet to be determined experimentally. We have performed an extensive structural search for the high-pressure crystalline phases of carbon using the evolutionary algorithm. Nine low-energy polymorphic structures of sp(3)-hybridized carbon result from the unbiased search. These new polymorphic carbon structures together with previously reported low-energy sp(3)-hybridized carbon structures (e.g., M-carbon, W-carbon, and Cco-C(8) or Z-carbon) can be classified into three groups on the basis of different ways of stacking two (or more) out of five (A-E) types of buckled graphene layers. Such a classification scheme points out a simple way to construct a variety of sp(3)-hybridized carbon allotropes via stacking buckled graphene layers in different combinations of the A-E types by design. Density-functional theory calculations indicate that, among the nine low-energy crystalline structures, seven are energetically more favorable than the previously reported most stable crystalline structure (i.e., Cco-C(8) or Z-carbon) in the pressure range 0-25 GPa. Moreover, several newly predicted polymorphic sp(3)-hybridized carbon structures possess elastic moduli and hardness close to those of the cubic diamond. In particular, Z-carbon-4 possesses the highest hardness (93.4) among all the low-energy sp(3)-hybridized carbon structures predicted today. The calculated electronic structures suggest that most polymorphic carbon structures are optically transparent. The simulated X-ray diffraction (XRD) spectra of a few polymorphic structures are in good agreement with the experimental spectrum, suggesting that samples from the cold-compressed graphite experiments may consist of multiple polymorphic phases of sp(3)-hybridized carbon.     

Self-assembly and supramolecular transition of poly(amidoamine) dendrons focally modified with aromatic chromophores

Three novel series of amphiphiles based on poly(amidoamine) dendrons (from G1 to G3) and having different aromatic chromophores (Cz I, Cz II, and Py) at the focal point were synthesized and studied for their self-assembly behavior in aqueous solution by using electronic microscopies (i.e., SEM and TEM), UV-vis, fluorescence, IR, and (1)H NMR spectroscopy. It was found that the generation of dendrons affected significantly the self-assembly of these amphiphiles in aqueous solution and the morphological structures of the resulting assemblies depended greatly on the architecture of the focal chromophores. As a result, the first generation of dendrons assembled readily into vesicles at low concentrations. These vesicular structures subsequently fused to form a stable tubular structure. Similar tubular structures could also be directly obtained through self-assembly of these amphiphilic dendrons at high concentrations. X-ray investigations showed that the resulting tubules possessed a lamellar structure. A head-to-head packing model of amphiphilic dendrons in the assemblies was proposed.