镧(Ⅲ)系锑硒化合物[Ln(en)_4]SbSe_4·0.5en(Ln=Dy,Ho)的溶剂热合成与晶体结构(英文)

本文研究了Ln2O3/Sb/Se/en溶剂热反应体系,合成了2个镧(Ⅲ)系锑硒化合物[Ln(en)4]SbSe4·0.5en[Ln=Dy(1),Ho(2)],用元素分析和红外光谱对化合物进行了表征,并用X-射线单晶衍射测定了化合物的单晶结构,两者都属于单斜晶系,P21/n空间群。结构对比研究发现,在en溶剂中,SbSe43-离子可以与半径较大的La3+和Nd3+离子配位,而不与半径较小的Dy3+和Ho3+离子配位,可见镧系收缩效应对SbSe43-离子与镧系金属离子Ln3+的配位有重要影响。     

UO22+·nH2O和PuO22+·nH2O(n=2,4,5,6)密度泛函理论研究

首先用密度泛函理论(DFT)方法研究了铀酰和钚酰离子的几何与电子结构,计算结果与实验基本符合,表明DFT方法也能用于含铀和钚重原子的化合物计算.然后对铀酰和钚酰水合离子的几何构型、Mulliken集居数分布以及铀酰(钚酰)与配体水分子的结合能进行计算,计算结果表明UO22+·5H2O和PuO22+·5H2O分别为铀酰和钚酰系列水合离子中最稳定的配合物.     

某些镧系化合物化学键特性的INDO研究

本文用INDO方法研究了不同价态镧系化合物的成键性质和4f轨道在成键中的作用,结果表明,镧系化合物的成键受许多因素,如价态、半径、配体、配位数、空间构型等影响。不同配体与镧系元素成键的强度差别较大;高价态的共价性大于低价态的;配位数低的大于配位数高的。某些特殊构型的镧系化合物除σ键外,还形成重叠较好的π配键,使Ln—L键共价性大大增强。4f轨道在成键中的作用比5d的少得多,三价(二价态)的4f轨道基本定域(<0.1％),四价态的4f轨道对成键的贡献明显增大,可接近1％。     

二(2-乙基己基)膦酸从盐酸介质中萃取钪(Ⅲ)、钇(Ⅲ)、镧系离子(Ⅲ)和铁(Ⅲ)

本文研究了二(2-乙基己基)膦酸(H[DEHP])的正辛烷溶液从盐酸介质中萃取钪(Ⅲ)、钇(Ⅲ)、镧系离子(Ⅲ)和铁(Ⅲ)的平衡规律。结果表明,H[DEHP]对上述离子的萃取次序是Sc³⁺>Fe³⁺>Lu³⁺>Yb³⁺>Er³⁺>Y³⁺>Ho³⁺。讨论了Sc(Ⅲ)与Fe(Ⅲ)、Y(Ⅲ)、Ln(Ⅲ)(镧系离子)以及Fe(Ⅲ)与重镧系离子(Ⅲ)分离的可能性,并与HEH[EHP]萃取上述离子的性能进行了比较。借助IR、NMR和斜率法,饱和法研究了低酸度下H[DEHP]萃取Sc(Ⅲ)、Y(Ⅲ)和Ln(Ⅲ)的平衡反应,计算了浓度平衡常数和萃取反应的热力学函数。     

镧系元素硝酸盐与1,8-萘啶氮单氧化物固态配合物的合成及性质研究

合成了组成为Ln(C8H6N2O)2(NO3)3.(Ln=La-Lu)的镧系硝酸盐化合物与1,8-二氮萘-N-单氧化物的固体络合物,用元素分析,UV,IR,摩尔电导,差热分析,热重分析及X光粉末衍射等测定了新化合物的组成及有关性质.     

钕(Ⅲ)和铒(Ⅲ)的氨基酸配合物

合成和鉴别了Nd~(3+)、Er~(3+)与谷氨酸(Glu)、天冬氨酸(Asp)形成的四个新的配合物,其组成为Ln_4Glu_(11)ClO_4·8H_2O、Ln_4Asp_(11)ClO_4·8H_2O(Ln=Nd、Er),其中配体通过羧基的氧原子与镧系离子配位。并通过配合物的水溶液的f-f光谱,计算了能级、成键和强度等参数。     

某些镧系化合物化学键特性的INDO研究

本文用INDO方法研究了不同价态镧系化合物的成键性质和4f轨道在成键中的作用,结果表明, 镧系化合物的成键受许多因素, 如价态、半径、配位数、空间构型等影响。不同配体与镧系元素成键的强度差别较大; 高价态的共价性大于低价态的; 配位数低的大于配位数高的。某些特殊构型的镧系化合物除σ键外, 还形成重叠较好的π配键,使Ln-L键共价性大大增强。4f轨道在成键中的作用比5d的少得多, 三价(二价态)的4f轨道基本定域(<0.1%), 四价态的4f轨道对成键的贡献明显增大, 可接近1%。     

镧系三氟化物的SCF-Xα-SW研究

对10个镧系元素(Ln)三氟化物进行了非相对论和相对论SCF-Xα-SW计算, 通过能级、轨道、结合能及布居数对比, 讨论化学键本质: 共价键中4f轨道的作用及相对论效应,结果表明, LnF3中Ln原子轨道参与成键的次序是: 轻稀土d>f>p>s, 而重稀土则有f>d>p>s。相对效应使Ln4f能级上移, 扩大了与F2p能级的距离, 减弱成键。原子序数增大, Ln4f能级下移, F2p能级距离缩小, 使重稀土氟化物中成键增强, 结合能计算值与实验值定性趋势一致, 重稀土氟化物电离能的计算表明, 相对论方案是获得定量符合所应该采用的。     

镧系金属高氯酸盐与1.8-萘啶氮氧化物配合物的合成、性质和结构

本文合成了镧系金属高氯酸盐与1,8-萘啶氮氧化物形成的Ln(C8H6N2O)4(ClO4)3(Ln=Sm-Lu)的固体配合物. 进行了元素分析、红外光谱、差热-热重分析和摩尔电导测定, 并作了Eu(ClO4)2与1,8-萘啶氮氧化物配合物的X射线单晶结构分析. 结果表明Eu^3^+离子与4个配体的氧原子和氮原子配位, 配位数为8.     

聚氧乙烯-镧系金属盐(Ln3+)的络合对聚氧乙烯形态结构的影响

采用偏光显微镜(POM)、差示扫描量热(DSC)和X 射线衍射,对聚氧乙烯(PEO)的形态结构和热物理行为随6种镧系盐对PEO的摩尔比变化的规律进行了系统的探讨.结果表明,随六合水氯化镧系盐摩尔比的增加,PEO球晶行为、熔点和熔融热均逐渐减弱,当盐对PEO的摩尔比达到一定值时(如YbCl3·6H2 O :PEO =2 0 ) ,则PEO完全不结晶.不同的镧系盐对PEO结晶的影响程度不同.X 射线衍射分析的结果也表明PEO晶面衍射峰随Ln3+ 盐摩尔比的增加而下降,与POM和DSC结果一致的.结果还表明较高的干燥温度(6 0℃)对PEO与Ln3+ 的相互作用有促进作用.对比二次降温的试样与原始试样的结晶行为,降温后结晶试样的特征表明络合在降温结晶后还存在.红外结果表明PEO与Ln3+ 的相互作用是络合作用.     

镧系元素4f轨道在成键中的作用的理论研究

用密度泛函方法在冻结或不冻结4f轨道的条件下计算一系列含镧系元素双原子 分子,对结果进行分析,得出以下结论：镧系元素4f轨道按传统的化学键理论观点 是不直接参与成键的,但对成键有一定作用：通过与匹配物的轨道混合使键长变短 ,键能增加,一般可达百分之几。随着镧系原子序数的增加4f轨道对成键的贡献减 少。电负性高或价态高的匹配物对4f轨道的作用较强,4f轨道对成键的影响比较大 。对于重镧系元素,匹配物不是F或O时,4f轨道对成键的贡献相当小,可以看成芯 轨道,但对于轻稀土,在比较精确的计算中则应作为价轨道处理。镧系元素与氟结 合时,只有对靠近Yb的重镧系元素才可以把4f当作芯轨道,而与氧结合时即使对于 YbO把Yb4f作为芯轨道仍会带来较大误差。     

Solvothermal syntheses of [Ln(en)3(H2O)x(mu(3-x)-SbS4)] (Ln = La, x = 0; Ln = Nd, x = 1) and [Ln(en)4]SbS4.0.5en (Ln = Eu, Dy, Yb): a systematic study on the formation and crystal structures of new lanthanide thioantimonates(V)

New lanthanide thioantimonate(V) compounds, [Ln(en)3(H2O)x(mu(3-x)-SbS4)] (en = ethylenediamine, Ln = La, x = 0, Ia; Ln = Nd, x = 1, Ib) and [Ln(en)4]SbS4.0.5en (Ln = Eu, IIa; Dy, IIb; Yb, IIc), were synthesized under mild solvothermal conditions by reacting Ln2O3, Sb, and S in en at 140 degrees C. These compounds were classified as two types according to the molecular structures. The crystal structure of type I (Ia and Ib) consists of one-dimensional neutral [Ln(en)3(H2O)x(mu(3-x)-SbS(4))]infinity (x = 0 or 1) chains, in which SbS4(3-) anions act as tridentate or bidentate bridging ligands to interlink [Ln(en)3]3+ ions, while the crystal structure of type II (IIa, IIb, and IIc) contains isolated [Ln(en)4]3+ cations, tetrahedral SbS4(3-) anions, and free en molecules. A systematic investigation of the crystal structures of the five lanthanide compounds, as well as two reported compounds, clarifies the relationship between the molecular structure and the entity of the lanthanide(III) series, such as the stability of the lanthanide(III)-en complexes, the coordination number, and the ionic radii of the metals.     

Theoretical study of metal-ligand interaction in Sm(III), Eu(III), and Tb(III) complexes of coumarin-3-carboxylic acid in the gas phase and solution

The interaction of lanthanide(III) cations (Ln(III) = Sm(III), Eu(III), and Tb(III)) with the deprotonated form of the coumarin-3-carboxylic acid (cca-) has been investigated by density functional theory (DFT/B3LYP) and confirmed by reference MP2 and CCSD(T) computations. Solvent effects on the geometries and stabilities of the Ln(III) complexes were computed using a combination of water clusters and a continuum solvation model. The following two series of systems were considered: (i) Ln(cca)2+, Ln(cca)2+, Ln(cca)3 and (ii) Ln(cca)(H2O)2Cl2, Ln(cca)2(H2O)2Cl, Ln(cca)3. The strength and character of the Ln(III)-cca- bidentate bonding were characterized by calculated Ln-O bond lengths, binding energies, ligand deformation energies, energy partitioning analysis, sigma-donation contributions, and natural population analyses. The energy decomposition calculations predicted predominant electrostatic interaction terms to the Ln-cca bonding (ionic character) and showed variations of the orbital interaction term (covalent contributions) for the Ln-cca complexes studied. Electron distribution analysis suggested that the covalent contribution comes mainly from the interaction with the carboxylate moiety of cca-.     

4f fine‐structure levels as the dominant error in the electronic structures of binary lanthanide oxides

The ground‐state 4f fine‐structure levels in the intrinsic optical transition gaps between the 2p and 5d orbitals of lanthanide sesquioxides (Ln₂O₃, Ln = La…Lu) were calculated by a two‐way crossover search for the U parameters for DFT + U calculations. The original 4f‐shell potential perturbation in the linear response method were reformulated within the constraint volume of the given solids. The band structures were also calculated. This method yields nearly constant optical transition gaps between Ln‐5d and O‐2p orbitals, with magnitudes of 5.3 to 5.5 eV. This result verifies that the error in the band structure calculations for Ln₂O₃ is dominated by the inaccuracies in the predicted 4f levels in the 2p‐5d transition gaps, which strongly and non‐linearly depend on the on‐site Hubbard U. The relationship between the 4f occupancies and Hubbard U is non‐monotonic and is entirely different from that for materials with 3d or 4d orbitals, such as transition metal oxides. This new linear response DFT + U method can provide a simpler understanding of the electronic structure of Ln₂O₃ and enables a quick examination of the electronic structures of lanthanide solids before hybrid functional or GW calculations. © 2015 Wiley Periodicals, Inc.     

稀土冠醚配合物的XPS研究

近几年来,XPS已应用于研究稀土元素及其配合物的内层电子结合能,伴峰现象以及镧系化合物性质变化规律。我们合成了1,2-环己基-12-冠-4(C_(12)H_(22)O_4)与稀土离子(RE=La—Er,Y)的二元配合物,苯并-15-冠-5(B-15-C-5)、联吡啶与稀土离子(RE=La—Eu)的混合配体配合物。本文报导用XPS研究上述两类配合物的中心金属离子的3d_(5/2)的结合能变化规律以及伴峰现象;研究配合物以及配位体的N_(1S)和O_(1S)结合能,并通过比较结合能的变化规律,讨论了配位键的性质。     

Luminescent Eu(III) and Gd(III) trisbipyridine cryptates: experimental and theoretical study of the substituent effects.

Synthesis, absorption spectra and luminescebce properties of a series of lanthanide trisbipyridine cryptates Ln within R-Bpy x R-Bpy x R-Bpy, where Ln = Eu, Gd and R = H, COOH, COOCH3, CONH(CH2)2NH2 are described. Comparison of the unsubstituted parent compound with the substituted compounds shows that bipyridine substitution doesn't alter significantly the photophysical properties of the lanthanide cryptate. The absorption maximum is slightly red-shifted when three bipyridines are substituted, whereas substituting one bipyridines has a negligible effect on the absorption spectra. The experimental triplet state energy is between 21600 and 22 100 cm(-1) for the series of compounds and the luminescence lifetimes at 77 K are between 0.5 and 0.8 ms in HO2 and equal to 1.7 ms in D2O. The experimental characterizations are completed by DFT and TD-DFT calculations to assess the ability of these approaches to predict absorption maxima, triplet state energies and structural parameters of lanthanide cryptates and to characterize the electronic structure of the excited states. The calculations on the unsubstituted parent and substituted compounds show that absorption maxima and lowest 3pipi* triplet state energies can be accurately determined from density functional theory (DFT) and time-dependent (TD) DFT calculations.     

Sensitized emission from lanthanide-doped nanoparticles embedded in a semiconductor sol-gel thin film.

In(2)O(3) sol-gel thin films made with LaF(3):Ln(3+) (Ln=Er, Nd, and Eu) nanoparticles were prepared and showed sensitized emission of the lanthanide ions after In(2)O(3) matrix excitation. The excitation spectra showed an In(2)O(3) absorption band in addition to the excitation peaks of the lanthanide ions, clearly demonstrating that there is energy transfer from the In(2)O(3) matrix to Ln(3+) (Er(3+), Nd(3+), and Eu(3+)). Similarly, HfO(2) and ZrO(2) sol-gel thin films made with LaF(3):Ln(3+) nanoparticles also showed energy transfer from the semiconductor matrix to the lanthanide ions.     

A Density Functional Theory Study of the Hydrates of 2NH_3:H_2SO_4 and Its Implications for the Formation of Atmosphere Particles

Density functional theory was used at the B3LYP/6-311++G(d,p) level of theory to study the hydrates of 2NH3:H2SO4:nH2O for n = 0～4. Neutrals of the most stable clusters, when n = 0 and 1, spontaneously formed and were determined to be hydrogen-bonded molecular complexes of monomeric species. Double ions (clusters containing a NH4+ cation and a HSO4- anion) or even ternary ions (clusters with two NH4+ cations and one SO42- anion) spontaneously formed in the most stable clusters of 2NH3:H2SO4:nH2O (n = 2, 3, 4). The energetics of binding and incremental association was also calculated. Double ions are not energetically favorable until 2NH3:H2SO4:2H2O because of the about equal free energies for forming the neutral (the most stable) and double ion (the second stable) isomers. The free energy of incremental association from free H2O and 2NH3:H2SO4:nH2O has a maximum at n = 2 at room temperature with ΔG ≈ -2 kcal/mol. The comparison of incremental association energies between 2NH3:H2SO4:nH2O, NH3:H2SO4:nH2O and H2SO4:nH2O clusters revealed that NH3 plays an important role in the atmospheric particle nucleation.     

Periodic trends in lanthanide and actinide phosphonates: discontinuity between plutonium and americium

The hydrothermal reactions of trivalent lanthanide and actinide chlorides with 1,2-methylenediphosphonic acid (C1P2) in the presence of NaOH or NaNO(3) result in the crystallization of three structure types: RE[CH(2)(PO(3)H(0.5))(2)] (RE = La, Ce, Pr, Nd, Sm; Pu) (A type), NaRE(H(2)O)[CH(2)(PO(3))(2)] (RE = La, Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy; Am) (B type), or NaLn[CH(2)(PO(3)H(0.5))(2)]·(H(2)O) (Ln = Yb and Lu) (C type). These crystals were analyzed using single crystal X-ray diffraction, and the structures were used directly for detailed bonding calculations. These phases form three-dimensional frameworks. In both A and B, the metal centers are found in REO(8) polyhedra as parts of edge-sharing chains or edge-sharing dimers, respectively. Polyhedron shape calculations reveal that A favors a D(2d) dodecahedron while B adopts a C(2v) geometry. In C, Yb and Lu only form isolated MO(6) octahedra. Such differences in terms of structure topology and coordination geometry are discussed in detail to reveal periodic deviations between the lanthanide and actinide series. Absorption spectra for the Pu(III) and Am(III) compounds are also reported. Electronic structure calculations with multireference methods, CASSCF, and density functional theory, DFT, reveal localization of the An 5f orbitals, but natural bond orbital and natural population analyses at the DFT level illustrate unique occupancy of the An 6d orbitals, as well as larger occupancy of the Pu 5f orbitals compared to the Am 5f orbitals.