金属间化合物RMn_2Ge_2(R=La,Pr,Nd,Sm,Gd,Tb和Y)中的自发磁相变及相变时的磁弹性异常

在 10— 80 0K的温度范围内用X射线衍射方法测量了RMn2 Ge2 (R =La ,Pr,Nd ,Sm ,Gd ,Tb和Y)的晶格常数与温度的变化关系 .在各种类型的自发磁相变观察到晶格常数的磁弹性异常现象 .实验得出 ,自发磁相变时的磁弹性异常主要由Mn次晶格引起 ,并且Mn Mn交换相互作用能不仅与晶格常数a有关 ,而且与晶格常数c有关 .用Kittle的交换反转模型讨论了低温时的铁磁—反铁磁一阶相变 .     

Synthesis and properties of homoleptic 2,2′-bipyridyl complexes of rare-earth elements. Crystal and molecular structures of the complexes Ln(N2C10H8)4 (Ln=Sm, Eu, Yb, or Lu) and the ionic complex [Lu(N2C10H8)4][Li(THF)4]

Homoleptic 2,2′-bipyridyl complexes of lanthanides (Ln), Ln(bpy)₄, were prepared by the reactions of iodides LnI₂(THF)₂ (Ln=Sm, Eu, Tm, or Yb), LnI₃(THF)₃ (Ln=La, Ce, Pr, Nd, Gd, or Tb), or bis(trimethylsilyl)amides Ln[N(SiMe₃)₂]₃ (Ln=Dy, Ho, Er, or Lu) with bipyridyllithium in tetrahydrofuran (THF) or 1,2-dimethoxyethane in the presence of free 2,2′-bipyridine. The IR and ESR spectral data, the magnetic susceptibilities, and the results of X-ray diffraction analysis indicate that the complexes of all elements of the lanthanide series, except for the europium complex, contain Ln⁺³ cations and anionic bpy ligands. According to the X-ray diffraction data, the coordination polyhedra about the Sm and Eu atoms are cubes, whereas the environment about the Yb atom is a distorted dodecahedron. In the ionic complex [Lu(bpy)₄][Li(THF)₄], the geometry of the [Lu(bpy)₄]⁻ anion is similar to that of the Lu(bpy)₄ complex. The possible modes of charge distributions over the ligands,viz., Ln(bpy²⁻)(bpy^.−)(bpy⁰)₂ and Ln(bpy^.−)₃(bpy⁰), are discussed. Published inIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 11, pp. 1897–1904, November, 2000.     

K2NiF4型Co系稀土复合氧化物合成及氧化性能

K2NiF4型Co系稀土复合氧化物合成及氧化性能;氧化反应     

糠醛甘氨酸Schiff碱及其稀土La(Ⅲ)配合物的合成与表征

糠醛甘氨酸Schiff碱稀土配合物具有生理活性。本文采用分步法制得Schill碱配合物：     

电感耦合等离子体原子发射光谱(ICP-OES)法测定铝合金中微量的钆、镧、钕、镨、钐

研究了电感耦合等离子体发射光谱(ICP-OES)法测定6系铝合金中微量的钆、镧、钕、镨、钐的方法,优化了ICP-OES工作条件,用标准加入法和标准曲线法做了比较,测定微量含量时,标准加入法比标准曲线法准确,在定量限和检出限之间约5倍空白标准偏差(5σ)含量时,标准加入法的加标回收率在80%~112%,检测结果具有参考价值.     

Separation of Rare-Earth Elements from Nitrate Solutions by Solvent Extraction Using Mixtures of Methyltri-n-octylammonium Nitrate and Tri-n-butyl Phosphate

The article presents data on the solvent extraction separation of rare-earth elements (REEs), such as La(III), Ce(III), Pr(III), and Nd(III), using synergic mixtures of methyltrioctylammonium nitrate (TOMANO₃) with tri-n-butyl phosphate (TBP) from weakly acidic nitrate solutions. Specifically, experimental results on separation of REEs, for the pair Ce(III)/Pr(III) for quaternary mixtures of REEs (La(III), Ce(III), Pr(III), Nd(III)) and for the pair La(III)/Pr(III) for solutions containing La(III), Pr(III), and Nd(III), are presented. It was shown that effective separation for the pair Ce(III)/Pr(III) from a solution containing 219 g Ce(III)/L, 106 g La(III)/L, 20 g Pr(III)/L, 55 g Nd(III)/L, and 0.1 mol/L HNO₃, was achieved using 56 steps of a multistage, counter-current solvent extraction cascade with scrubbing, at an organic-to-aqueous phase volume ratio (O/A) equal to 2/1 on the extraction section and O/A equal to 4/1 on the scrubbing section, using 3.3 mol/L solutions of the mixture TOMANO₃-TBP with molar ratio 0.15:0.85 in dodecane. Separation for the pair La(III)/Pr(III) could be achieved using a solvent extraction cascade with scrubbing in 32 steps at O/A equal to 2/1 on the extraction section and O/A equal to 2.8/1 on the scrubbing section of the solvent extraction cascade from a solution containing 258 g La(III)/L, 58 g Pr(III)/L, 141 g Nd(III)/L, and 0.1 mol/L HNO₃ with 3.0 mol/L solution of the mixture TOMANO₃-TBP with molar ratio 0.2:0.8 in dodecane.     

纳米ZnO-TiO2复合半导体的La3+改性及其光催化活性

采用溶胶-凝胶法对纳米ZnO-TiO2复合半导体进行了La3 改性,用热重-差示扫描量热、扫描电镜、X射线衍射和拉曼光谱分析了La3 /ZnO-TiO2的晶化温度和微晶结构,并以活性艳红K-2BP为模型降解物,在固定催化剂投加量和通气量条件下考察了La3 掺杂量和煅烧温度对La3 /ZnO-TiO2光催化活性的影响.结果表明,La3 掺杂使ZnO-TiO2晶型转变温度提高,衍射峰蓝移且峰强度减弱,晶粒进一步减小.La3 掺杂量为0.5%,煅烧温度为500℃,40min时对活性艳红K-2BP的降解率为100%,表观反应速率常数k值达到了0.182min-1,为不掺La3 的ZnO-TiO2复合半导体的1.4倍.     

Magnetic domain structures of 1:12 type nitrides NdFe10.5Mo1.5N x

The magnetic domain structures of the 1:12 type alloy NdFe_10.5Mo_1.5 and its nitride were firstly investigated by using magnetic force microscope (MFM). A complicated corrugation and spike magnetic domain structure was observed in NdFe_10.5Mo_1.5alloy. Upon nitrogenation, a stripe domain structure occurs due to the dramatic increase of the uniaxial magneto-crystalline anisotropy K₁ induced by nitrogenation. Based on the basic domain theories, the origin of these domain patterns was analyzed and the reason of domain structure transition is explained quantitatively. The domain wall energy γ, exchange constant A and single-domain particle size D_c of NdFe_10.5 Mo_1.5 and NdFe_10.5-Mo_1.5N _x were calculated in combination with the measured domain width ω and magnetic parameters. A comparison of magnetic parameters with those of SmCo₅ and Nd₂Fe₁₄B permanent materials was also made.     

Covalent bonding and J–J mixing effects on the EPR parameters of Er~(3+) ions in GaN crystal

The EPR parameters of trivalent Er~(3+) ions doped in hexagonal Ga N crystal have been studied by diagonalizing the 364×364 complete energy matrices. The results indicate that the resonance ground states may be derived from the Kramers doublet Γ_6. The EPR g-factors may be ascribed to the stronger covalent bonding and nephelauxetic effects compared with other rare-earth doped complexes, as a result of the mismatch of ionic radii of the impurity Er~(3+)ion and the replaced Ga~(3+) ion apart from the intrinsic covalency of host Ga N. Furthermore, the J–J mixing effects on the EPR parameters from the high-lying manifolds have been evaluated. It is found that the dominant J–J mixing contribution is from the manifold ~2K_(15/2), which accounts for about 2.5%. The next important J–J contribution arises from the crystal–field mixture between the ground state ~4I_(15/2) and the first excited state~4I_(13/2), and is usually less than 0.2%. The contributions from the rest states may be ignored.     

Large reversible magnetocaloric effect induced by metamagnetic transition in antiferromagnetic HoNiGa compound

The magnetic properties and magnetocaloric effects(MCE) of Ho Ni Ga compound are investigated systematically.The Ho Ni Ga exhibits a weak antiferromagnetic(AFM) ground state below the Neel temperature TNof 10 K, and the AFM ordering could be converted into ferromagnetic(FM) ordering by external magnetic field. Moreover, the field-induced FM phase exhibits a high saturation magnetic moment and a large change of magnetization around the transition temperature,which then result in a large MCE. A large-?S_M of 22.0 J/kg K and a high RC value of 279 J/kg without magnetic hysteresis are obtained for a magnetic field change of 5 T, which are comparable to or even larger than those of some other magnetic refrigerant materials in the same temperature range. Besides, the μ_0H~(2/3)dependence of |?S_M~(pk)| well follows the linear fitting according to the mean-field approximation, suggesting the nature of second-order FM–PM magnetic transition under high magnetic fields. The large reversible MCE induced by metamagnetic transition suggests that Ho Ni Ga compound could be a promising material for magnetic refrigeration in low temperature range.