LaNi4Co晶体及电子结构的理论分析

根据密度泛函理论,采用总体能量计算方法,以扩展平面波函数为基集,并结合超软赝势技术,对LaNi5的不同Ni位分别被Co取代后的晶体几何结构进行了优化,从理论上给出了其结构参数及性质。计算结果表明,该方法能较好地符合LaNi4Co晶体结构的实验值,为该类合金的结构预测提供了理论依据。计算了LaNi4Co的总体能量、电子态密度以及Mulliken布居电荷。根据计算结果,分析了LaNi4Co的电子结构,及Co取代前后合金中电子结构的变化,比较了Co分别位于Ni的2c和3g位时的稳定性。分别从晶体结构、能量和电子结构的角度分析了Co取代时影响合金稳定性的因素。给出了LaNi4Co的生成热的理论计算值。     

层状化合物La2Ni1-yCoyO4+δ的合成、结构与性能

采用氨基多羧酸配合物法合成La2Ni1-yCoyO4+δ(y=0~0.2)超细粉料, 研究陶瓷样品的结构和混合导电性能. 研究结果表明, La2Ni1-yCoyO4+δ具有正交结构(Fmmm空间群), Co离子取代增加了钙钛矿层中ab平面上Ni/Co—O键的键长、岩盐层中沿c 轴方向上La—O键的键长和非化学计量氧含量, 并有利于改善材料的烧结性能. 随着Co离子含量的增加, 总电导率的峰值温度向高温移动, 高温段总电导率随温度的变化趋于平缓, 但总电导率水平出现降低; 增加Co离子含量还有利于提高氧离子导电性能. Co离子取代对陶瓷样品混合导电性能的影响与晶体结构参数的变化紧密相关.     

储氢合金La0.7-xCexMg0.3Ni2.4Co0.6(x=0～0.4)电化学性能研究

研究了以Ce部分取代La对AB3型储氢合金La0.7-xCexMg0.3Ni2.4Co0.6(x=0~0.4)结构和电化学性能的影响.实验表明,该系列合金主要包含LaNi3相和LaNi5相.随着Ce含量的增加,合金电极的最大放电容量逐渐降低,但循环稳定性得到了明显改善.     

硼对La17Fe76B7型储氢合金结构和电化学性能的影响

采用中频感应熔炼-快淬方法制备了La17Fe3Mn5Al2Ni73-xBx(x=0,1,3,5)储氢合金。结构分析表明,不含B的合金为双相结构,主相为LaNi5相,第二相为La2Ni7相,含B合金均由LaNi5相、La2Ni7相和La3Ni13B2相组成,且随着B含量的增加,LaNi5相和La2Ni7相减少,La3Ni13B2相逐渐增加。电化学测试表明,随着B含量的增加,合金的活化性能、最大放电容量不同程度下降,而循环稳定性有所改善。合金电极的倍率放电能力(HRD)随着B含量的增加呈先增大后减小的趋势,表明适量的B有利于提高合金的高倍率放电性能。合金电极的交换电流密度(I0)随着B含量的增加先增大后减小,而氢在合金中的扩散系数(D)则逐渐增大,表明合金的高倍率放电性能主要取决于合金表面的电荷转移能力。     

M_2M_2′Te_4型层状异金属簇合物的SCC—DV—Xα研究(M=Co、Ni;M′=Ta、Nb)

标题簇合物的电子结构采用电荷自洽离散变分Xα方法(SCC—DV—Xα)计算得到。在前线区轨道密集,具有半导体的特征;层状结构内存在离域性d-p(π+α)键,这是该类簇合物导电的依据;Ni—Ni或Co—Co之间不存在成键。描述了它们的态密度图,并说明了与合金的DOS图相似点。     

La-Mg-Ni系A2B7型贮氢合金的结构与电化学性能

合金结构研究表明,La2-xMgxNi7(x=0.3～0.8)主要由Ce2Ni7,Gd2Co7,PuNi3型物相组成.合金中Mg含量对合金相结构有着重要影响,主相的晶胞参数随Mg含量(x)的增加呈线性减小,合金的吸放氢平台也随之升高.电化学测试表明,随合金中Mg含量的增加,合金电极的放电容量先增大后减小,合金电极的循环稳定性呈恶化趋势,La1.4Mg0.6Ni7合金电极具有最高的电化学放电容量(378 mAh·g-1),La1.6Mg0.4Ni7合金电极具有最佳的循环稳定性(S270=81%).合金电极的高倍率放电性能(HRD)随Mg含量的增加而增大.当合金中Mg含量较低时(x≤0.5),合金电极反应速度控制步骤为氢在合金体相中的扩散;当Mg含量较高时(x≥0.5),合金电极反应速度控制步骤转变为电极表面的电荷转移.     

含锡AB_5型非化学计量贮氢合金Ⅰ.合金的结构

采用X射线衍射法研究了LaNi5 .1 5 ,La(NiSn) 5 .1 4 ,La(NiSnCo) 5 .1 2 ,La(NiSnMn) 5 .1 2 ,La(NiSnCoMnAl) 5 .1 0 5种AB5 型非化学计量贮氢合金的结构。发现主物相中并未产生第二物相 ,AB5 型贮氢合金中B原子数发生正偏移时 ,晶胞体积减小 ,当B侧含有取代元素时 ,这种变化更加明显。对于非化学计量贮氢合金而言 ,少量Sn取代Ni后 ,晶胞体积大大提高。Mn ,Co和Al的加入也会影响晶胞常数。Sn ,Co ,Mn ,Al均会降低贮氢合金放氢平台压力。     

镁含量对RE-Mg-Ni系A2B7型储氢合金结构与性能的影响

采用感应熔炼方法制备了La0.8-xGd0.2MgxNi3.1Co0.3Al0.1(x=0, 0.1, 0.15, 0.2, 0.25, 0.3, 0.4)储氢合金, 并在氩气气氛和1173 K下进行退火处理. 合金相结构分析结果表明, 镁含量(x)较低时合金以Ce2Ni7型为主相结构, A2B7型相丰度(Ce2Ni7+Gd2Co7)达到98.8%; 镁含量较高时合金相由A2B7型、 CaCu5型和PuNi3型物相构成, 随着镁含量的增加, PuNi3型和CaCu5型相组成逐渐增多, 其晶胞参数随Mg含量的增加而减小, 同时合金的吸氢平台也随之升高. 电化学测试结果表明, 随着合金中Mg含量增加, 合金电极的最大放电容量和循环稳定性均呈先增大后减小的规律, 其中x=0.15时合金电极具有最高的电化学放电容量(393 mA·h/g)和最佳的循环寿命(S100=92.82%). 合金电极的高倍率放电性能(HRD)随Mg含量的增加先减小再增大然后又减小, 适量的Mg元素改善了合金电极的动力学性能.     

Mg_2Ni_(1-x)Co_x合金相的固溶烧结法制备及结构和储氢性能

采用固溶烧结法制备了Mg_2Ni_(1-x)Co_x(x=0.10,0.15,0.20)合金,利用X射线衍射仪和压力-组成-温度测试仪等研究了Co含量对合金相结构和储氢性能的影响.结果表明,合金由Mg_2Ni型Mg_2(Ni,Co)主相及少量Mg和Mg Ni3Co新相组成.Mg2(Ni,Co)具有良好的可逆储氢性能,吸氢形成Mg_2Ni_(0.9)Co_(0.1)H_4型四元氢化物,其具有与父系氢化物HT-Mg_2NiH_4相近的放氢焓变(ΔHd=63.9 k J/mol H2).Mg_2Ni_(1-x)Co_x(x=0.10,0.15,0.20)合金具有良好的放氢动力学性能,二维相界面迁移为放氢过程的控制步骤.随着Co含量的增加,合金的放氢活化能(Ea)降低,其中,Mg_2Ni_(0.8)Co_(0.2)的Ea降低到54.0 k J/mol.     

镍系复合氧化物Li_aNi_(0.78)Co_(0.2)Cd_(0.02)O_2的合成及电化学性能

以LiOH·H2O,含镉球状Ni(OH)2和Co2O3为原料,采用改进固相反应法合成镍系复合氧化物LiaNi0.78Co0.2Cd0.02O2锂离子电池正极材料,并通过ICP＿AES,XRD,SEM,TEM及电化学性能测试对该材料进行表征.实验表明,由Co和Cd部分取代Ni元素的复合正极材料LiaNi0.78Co0.2Cd0.02O2仍具有较完好的层状结构,表面分布均匀,颗粒粒径分布窄,且电化学性能稳定.常温下具有较高的可逆容量和优异的循环稳定性,其可逆容量最高达157.8mAh/g,循环50次后容量仍保持138.3mAh/g左右.     

Density Functional Studies of the C?F Bond Activation of CF3 Radical by Bare Co+

The C? F bond activation mechanism of CF₃ radical by bare Co⁺ has been studied by density functional theory. Three local minima and two first‐order saddle points were located for the potential energy surface (PES) of [Co, C, F₃]⁺. The activation barrier involving C? F bond activation was calculated to be only 14.73 kJ/mol, while the largest barrier of 149.29 kJ/mol on the FES involves Co? C bond rupture. The bonding mechanism between Co⁺, C and F atoms were discussed based on Mulliken population. The relevant bond dissociation energy and thermochemistry data were calculated with the limited experimental values, and the results are in good agreement with the experimental findings.     

Composition-structure relationships in polar intermetallics: experimental and theoretical studies of LaNi(1 + x)Al(6 - x) (x = 0.44)

A new ternary aluminide, LaNi(1 + x)Al(6 - x ) (x = 0.44), has been synthesized from La, Ni, and Al in sealed silica tubes. Its structure, determined by single-crystal X-ray diffraction, is tetragonal P4/mmm (No. 123) with Z = 1 and has the lattice parameters a = 4.200(8) and c = 8.080(8) angstroms. Refinement based on Fo2 yielded R1 = 0.0197 and wR2 = 0.020 [I > 2sigmaI]. The compound adopts a structure type previously observed in SrAu2Ga5 and EuAu2Ga5. The atomic arrangement is closely related to the one in BaAl4 as well as in other rare-earth gallide compounds such as LaNi0.6Ga6, HoCoGa5, Ce4Ni2Ga20, Ce4Ni2Ga17, Ce4NiGa18, and Ce3Ni2Ga15. This structure exhibits a large open cavity which may be filled by a guest atom. Band structure calculations using density functional theory have been carried out to understand the stability of this new compound.     

2-(N，N-二羧甲基氨甲基)氢醌金属配合物(钴、镍、锌)的合成、晶体结构及电化学性质研究

合成了3个新的氢醌金属配合物:[Co(H2cah)(H2O)2].H2O(1),Ni(H2cah)(H2O)2].H2O(2),[Zn(H2cah)(CH3OH)(H2O)].H2O(3)(H4cah=2-(N,N-二羧甲酸氨甲基)氢醌),通过X-射线单晶衍射,红外光谱,元素分析对它们进行了表征。这些配合物均为单核结构,并且通过分子间的氢键形成了无限的超分子网状结构。电化学研究显示配合物1中的Co2+/Co+对和配合物2中的Ni2+/Ni+对的氧化还原是一个不可逆的过程,但是氢醌到半醌之间的转换是一个准可逆的过程。     

A DFT study on the interaction of Co with an anatase TiO2 (001)-(1×4) surface

The substitution/adsorption structures of Co on an anatase TiO2 (001)-(1×4) surface are investigated using the DFT/local density approximation (LDA) method.Theoretical calculation shows that the Co ion prefers to be adsorbed on the surface of anatase TiO2.The density of states (DOS) analysis finds that the Co 3d is located mainly in the energy gap region.The Co 3d partial density of states (PDOS) indicates that there is a substantial degree of hybridization between O 2s and Co 3d in valence band (VB) regions in the substitution models.The conclusion is that the mode of substitution is more active when the catalyst is a higher-energy surface.     

First Principle Calculation of the Geometrical and Electronic Structure of Impurity-Doped β-FeSi2 Semiconductors

The geometrical and electronic structures of impurity (Cr, Mn, Co, Ni)-doped β-FeSi₂ were investigated using first principles pseudopotential calculations based on generalized gradient approximation (GGA) density function theory. The calculated structural parameters depend strongly on the kinds of dopants and sites. The total energy calculations for substitution of dopants at the Fe_I and the Fe_II sites revealed that Mn prefers the Fe_I site, whereas Cr, Co, and Ni prefer the Fe_II site. The electronic structure is analyzed and discussed in terms of the atomic charges, bond overlap population, and total and partial densities of states (DOS).     

乙烷在Ni(111)表面的吸附和分解

研究了乙烷在Ni(111)表面解离的可能反应机理, 使用完全线性同步和二次同步变换(complete LST/QST)方法确定解离反应的过渡态. 采用基于第一性原理的密度泛函理论与周期平板模型相结合的方法, 优化了C2H6裂解反应过程中各物种在Ni(111)表面的top, fcc, hcp和bridge位的吸附模型, 计算了能量, 并对布居电荷进行分析, 得到了各物种的有利吸附位. 结果表明, 乙烷在Ni(111)表面C—C解离的速控步骤活化能为257.9 kJ·mol-1, 而C—H解离速控步骤活化能为159.8 kJ·mol-1, 故C—H键解离过程占优势, 主要产物是C2H4和H2.     

Synthesis, structure and DFT study of dinuclear iron, cobalt and nickel complexes with cyclopentadienyl-metal moieties

Reactions of 1,1'-bis(dipheny1phosphino)cobaltocene with Co(PMe(3))(4), Ni(PMe(3))(4), Fe(PMe(3))(4), Ni(COD)(2), FeMe(2)(PMe(3))(4) or NiMe(2)(PMe(3))(3) afford a series of novel dinuclear complexes [((Me(3)P)[lower bond 1 start]Co(η(5)-C(5)H(4)[upper bond 1 start]PPh(2)))((Me(3)P)M[upper bond 1 end](η(5)-C(5)H(4)P[lower bond 1 end]Ph(2)))] (M = Co(1), Ni(2) and Fe(3)) [Co(η(5)-C(5)H(4)[upper bond 1 start]PPh(2))(2)Ni[upper bond 1 end](COD)](4), [Co(η(5)-C(5)H(4)[upper bond 1 start]PPh(2))(2)Ni[upper bond 1 end](PMe(3))(2)] (5) and [((Me(3)P)[lower bond 1 start]Co(Me)(η(5)-C(5)H(4)[upper bond 1 start]PPh(2)))((Me(3)P)Fe[upper bond 1 end](Me)(η(5)-C(5)H(4)P[lower bond 1 end]Ph(2)))] (6). Reactions of 1,1'-bis(dipheny1phosphino)ferrocene with Ni(PMe(3))(4), NiMe(2)(PMe(3))(3), or Co(PMe(3))(4) gives rise to complexes [Fe(η(5)-C(5)H(4)[upper bond 1 start]PPh(2))(2)M[upper bond 1 end](PMe(3))(2)] (M = Ni (7), Co (8)). The complexes 1-8 were spectroscopically investigated and studied by X-ray single crystal diffraction. The possible reaction mechanisms and structural characteristics are discussed. Density functional theory (DFT) calculations strongly support the deductions.     

Adsorption of Co2B2 and Ni2B2 Clusters on the TiO2 (110) Surface: a Density Functional Study

Based on density functional theory and generalized gradient approximation calculations, the adsorption of Co2B2 and Ni2B2 clusters on the rutile TiO2 (110) surface has been investigated utilizing periodic supercell models. Unambiguously, the results demonstrate that the hollow site turns out to be preferable for Co2B2 cluster while Ti2 site is for Ni2B2 cluster to adsorb. Orbital population analysis indicates a strong interaction between Co2B2 and O atom of TiO2 surface, which can be attributed to the overlap of Co 3d and surface O 2p orbital. Similarly, for Ni2B2 , the bonding interaction occurs mostly through the interaction of Ni 3d/4s and O 2p orbitals. Note that, there is also an interaction within the Co2B2 clusters (Ni2B2) through B 2s/2p and Co 3d orbitals (Ni 3d/4s). Moreover, orbital analysis results shows that the strong bonding between Ni2B2 and Ti2 site is due to the overlap of HOMO of Ni2B2 and d-orbital of five-coordinated titanium atoms.     

纳米晶Ni-Mo-Co合金镀层的结构与析氢行为

电沉积;结构;纳米晶Ni-Mo-Co合金镀层的结构与析氢行为