间隙原子氮对化合物RE2Fe17磁性的影响

用自旋极化的MS-Xα方法计算了稀土-过渡族化合物Nd2Fel7Nx(x=0,3)中含哑铃Fe原子对的Fe8及含Nd和N原子的NdFe6和NdFe6N3原子簇的电子结构和磁矩。计算结果显示，在化合物Nd2Fe17中，Fe(c)和Fe(f)晶位间的分子轨道中，有3个奇宇称轨道呈现负交换耦合。通过比较α-Fe的MX-Xα计算结果，能够很好地说明RE2Fel7化合物居里温度较低的原因。在化合物Nd2Fel7M中，Fe(c)-Fe(f)晶位间分子轨道只剩下一个奇宇称轨道呈现弱的负交换耦合，通过比较N2Fe17和Nd2Fe17N3化合物Fe8原子簇的计算结果，能够很好地说明间隙原子M对化合物RE2Fel7Mx(M表示N，H或C)的居里温度产生影响的物理机制。对RE2Fel7型化合物中影响Fe-Fe交换耦合的主要因素，本文也做了讨论。     

稀土硫代磷酸盐REPS4的磁性

在２－３００Ｋ温度范围内测定了ＲＥＰＳ４系列化合物的磁化率,进而研究了各个化合物的磁化率和倒易磁化率随温度的变化,最后用５０－３００Ｋ温度范围的磁化率数据拟合得到各个顺磁稀土离子ＲＥ＾３＋的居里－外斯常数和有效顺磁磁矩μｅｆｆ。     

混合稀土化合物Y_（1－x）Tb_xCo_（5＋0．1x）的磁性

研究了白旋一轨道作用、晶场作用、交换作用、自旋一自旋偶极作用和Ｚｅｅｍａｎ作用，对稀土化合物Ｙ＿（ｌ－ｘ）ＴｂｘＣｏ＿（５＋０．１ｘ）的磁性实验数据进行了理论分析，理论计算结果与实验符合得较好，并进一步讨论了各种作用对磁性的贡献．     

金属间化合物Ho2Co17-xSix的结构和磁性研究

研究了非磁性原子Si替代Co对Ho2Co17金属间化合物结构和磁性的影响.X射线衍射结果表明, 所有Ho2Co17-xSix(x=0.5,1.0,1.5,2.0,2.5,3.0)化合物都为Th2Ni17型六角结构;化合物的晶格常数和单胞体积都随Si含量的增加而呈线性下降.磁性测量结果表明, Ho2Co17-xSix化合物的饱和磁化强度随Si含量的增加而呈线性下降.从热磁曲线测量观察到, Ho2Co17-xSix化合物在x=0.5时可能呈面各向异性,当0.5≤x≤3.0时出现由易面到易轴的自旋重取向,自旋重取向温度Tsr随Si原子含量的增加先下降,而后又上升,在x=2.5处出现最低点.     

R2Fe17CNx的结构和磁性

采用适当的热处理,使碳原子和氮原子先后进入到R_2Fe(17)的结构中去。利用X射线折射和磁测量技术研究了R_2Fe_(17)CN_x的晶体结构和内禀磁性。碳、氮的加入使晶胞体和膨胀、居里温度升高、饱和磁矩增大,并加强了稀土晶位的轴各向异性。     

混合稀土化合物Y1—xTbxCo5＋0.1x的磁性

研究了自旋－轨道作用、晶场作用、交换作用、自旋－自旋偶极作用和Ｚｅｅｍａｎ作用，对稀土化合物Ｙｚ－ｘＴｂｘＣｏ５＋０．１ｘ的磁性实验数据进行了理论分析，理论计算结果与实验符合得较好，并进一步讨论了各种作用对磁性的贡献。     

新型稀土富铁永磁化合物NdFe10Mo2Cx的制备和磁性研究

用气－固反应将碳原子渗入到母体合金ＮｄＦｅ１０Ｍｏ２的晶格间隙位，形成稳定的化合物ＮｄＦｅ１０Ｍｏ２Ｃｘ，其晶体结构保持ＴｈＭｎ１２型方结构不变，但晶胞积增大３％左右，居里温度提高１１０Ｋ以上，且ＮｄＦ３１０Ｍｏ２Ｃｘ具有单轴各向异性，磁晶各向异性场ＨＡ达到９２３３．６ｋＡ／ｍ．结果表明，ＮｄＦｅ１０Ｍｏ２Ｃｘ具备了研制高矫顽力永磁体的内禀磁性，另外，穆堡尔谱实验表明，ＮｄＦｅ１０Ｍｏ２Ｃｘ中不同     

稀土化合物RE(HCO2)3(HNO2)的合成与表征

合成了系列新化合物ＲＥ（ＨＣＯ２）３（ＨＮＯ２）（Ｈ２ＣＯ２）（ＲＥ＝Ｙ,Ｔｂ,Ｄｙ,Ｈｏ,Ｅｒ,Ｙｂ,Ｔｍ）,用Ｘ射线方法表征了其结构。单晶结构分析表明此新类型的结构为正交晶系且具有非中心对称空间群（２０）Ｃ２２２１,晶体结构为三维网络结构,结构的...     

稀土金属化合物的结构和磁性

本文介绍了稀土金属间化合物的结构特点，通过晶体结构和稀土－３ｄ过滤金属化合物中的三种相互作用分析，解释了磁性特点，同时介绍了矫顽力的两种模型。     

CuO2链的磁性

(La, Sr)14Cu24O41的结构中包含一维的CuO2链和Cu2O3梯子, 在室温以下Cu2O3梯子对磁化率的贡献很小, 实验测量的磁化率反映了CuO2链的磁性, 是研究一维磁性的理想材料.研究了非磁性的Zn2+替代Cu2+和Sr2+替代La3+对La6Sr8Cu24O41中CuO2链磁性的影响.     

化合物Y1—xPrxCo5和Y1—xSmxCo5的磁性分析

用改进的哈密顿,通过参数拟合法对稀土化合物Y_(1-x)Pr_xCo_5和Y_(1-x)Sm_xCo_5的磁化曲线、自发磁化曲线及易磁化方向随温度的变化曲线进行了分析.计算结果与实验符合较好,并得到了较为合理的Y_(1-x)Pr_xCo_5二阶晶场参量数值.     

聚(2,4-噻唑)的合成及其稀土螯合物的磁性能研究

合成了一种新型的共轭高分子(PTz)．并制备了它与稀土离子Nd^3 的螯合物(PTz-Nd^3 ),利用红外、核磁、元素分析及X射线能谱仪对它们的结构进行了表征。PTz-Nd^3 的磁性研究表明,该高分子螯合物具有软铁磁性。     

Fe_(6-x)Al_x团簇的结构和磁性能

在密度泛函理论的BPW91水平上,对Fe6-xAlx团簇进行了结构优化,并将获得的最低能结构进行稳定性分析以及电子结构和磁性能的计算.计算结果表明,铁原子倾向团聚在一起并占据最高配位,Al原子则倾向分布在铁簇的周围尽最大可能地与Fe配位成键.Fe6-xAlx团簇的磁性随Al原子数目增加呈现下降趋势,自然轨道分析揭示Fe4s和Al3s与Fe3d之间的杂化是导致团簇磁矩下降的主要原因.     

Ternary Rare Earth (RE) Gold Compounds REAuCd and RE2Au2Cd

New intermetallic rare earth compounds REAuCd (RE = Y, La–Nd, Sm–Yb) and RE₂Au₂Cd (RE = La, Pr, Nd, Sm) were prepared by reaction of the elements in sealed tantalum tubes in a high‐frequency furnace. The compounds were investigated by X‐ray diffraction both on powders and single crystals. The equiatomic REAuCd compounds with RE = Y, La–Nd, Sm, and Gd–Tm adopt the ZrNiAl type structure with space group P62m. Single crystal X‐ray data yielded a = 786.2(2), c = 415.9(1) pm, wR2 = 0.0337, 402 F² values for LaAuCd and a = 782.91(9), c = 410.01(5) pm, wR2 = 0.0653, 395 F² values for CeAuCd with 14 parameters for each refinement. Geometrical motifs in CeAuCd are two types of gold centered tricapped trigonal prisms: [Au1Cd₃Ce₆] and [Au2Cd₆Ce₃]. The gold and cadmium atoms form a three‐dimensional [AuCd] polyanion in which the cerium atoms fill distorted hexagonal channels. EuAuCd and YbAuCd crystallize with a TiNiSi type structure, space group Pnma: a = 755.2(1), b = 450.59(5), c = 878.6(1) pm, wR2 = 0.0904, 500 F² values for EuAuCd, and a = 731.64(3), b = 432.94(2), c = 875.80(4) pm, wR2 = 0.1192, 457 F² values for YbAuCd with 20 parameters for each refinement. In these structures the europium(ytterbium) and cadmium atoms form zig‐zag chains of egde‐ and face‐sharing trigonal prisms which are centered by the gold atoms. Also in EuAuCd and YbAuCd a three‐dimensional [AuCd] polyanion occurs in which the europium(ytterbium) atoms are embedded. Europium and ytterbium are divalent in EuAuCd and YbAuCd. Susceptibility measurements show Pauli paramagnetism for YbAuCd and Curie‐Weiss behavior above 100 K for EuAuCd with an experimental magnetic moment of 7.86(6) μ_B/Eu. Ferromagnetic ordering is detected at 28 K. The saturation magnetic moment is 7.1(1) μ_B/Eu at 1.9 K. ¹⁵¹Eu Mössbauer spectra show an isomer shift of –9.2(2) mm/s and full magnetic hyperfine field splitting at 4.2 K with an internal hyperfine field of 19.5(4) T at the europium nuclei. The RE₂Au₂Cd compounds crystallize with the Mo₂FeB₂ structure, a ternary ordered version of the U₃Si₂ type. These structures may be considered as an intergrowth of distorted CsCl and AlB₂ related slabs of compositions RECd and REAu₂. Chemical bonding in REAuCd and RE₂Au₂Cd is briefly discussed.     

Novel Copper(I)‐Thioantimonates(III): Solvothermal Synthesis,Crystal Structures,Thermal Stability and Magnetic Properties of (C2N2H10)0.5Cu2SbS3, (C3N2H12)0.5Cu2SbS3, and (C4N2H14)0.5Cu2SbS3

The novel copper(I)‐thioantimonates(III) (enH₂²⁺)_0.5Cu₂SbS₃ ( I ) (en = ethylendiamine), (1, 3‐DAPH₂²⁺)_0.5Cu₂SbS₃ ( II ) (1, 3‐DAP = 1, 3 diaminopropane) and (1, 4‐DABH₂²⁺)_0.5Cu₂SbS₃ ( III ) (1, 4‐DAB = 1, 4‐diaminobutane) were synthesized under solvothermal conditions reacting Sb₂S₃, CuCl₂·2H₂O, S with the amines. The compounds crystallize in the monoclinic space group P2₁/n. The primary building units are a SbS₃ trigonal pyramid and two distorted CuS₃ units. In the structures the SbS₃ pyramid is connected to six CuS₃ moieties and every S atom has bonds to one Sb atom and to two Cu atoms. Further interconnection leads to the formation of ten‐membered (10 MR) Cu₃Sb₂S₅ and six‐membered (6 MR) Cu₂SbS₃ rings. Every 10 MR is condensed to four 10 MR and four 6 MR to form a single layer within the (010) plane. Two such single layers are connected to a double layer thus forming the final [Cu₂SbS₃]^— layered anion. The [CuSbS₃]^— protonated amines are located between the layers and the interlayer spacing depends on the size and orientation of these amines. Between the Sb atom and one Cu atom a remarkable short distance of about 2.7Å is observed. At elevated temperatures the compounds decompose into CuSbS₂ and Cu₃SbS₄ suggesting a complex redox reaction. Diamagnetic susceptibilities indicate the copper(I) in the metal sulfide frameworks. All three compounds are semiconductors with intermediate band gaps of about 2 eV.     

衬底温度对Fe3N薄膜生长和磁性的影响

采用直流磁控溅射方法, 以Si(100) 单晶片为衬底, 在衬底温度为150～450 ℃的范围内得到了ε-Fe3N薄膜样品. 利用 XRD, SEM和VSM等表征手段, 研究了衬底温度对ε-Fe3N薄膜的生长和磁性的影响. 实验结果表明, 随着衬底温度的升高, 薄膜的生长速率、晶粒尺寸和单位质量磁化强度均增大, 而矫顽力呈现先增加后减小的变化趋势, 当衬底温度为350 ℃时, 矫顽力达到最大值18.72 kA/m, 可以认为此时薄膜样品的晶粒尺寸接近于交换作用长度.     

Structure and Magnetic Investigation of a Series of Rare Earth Heterospin Monometallic Compounds of Nitronyl Nitroxide Radical

Five rare earth heterospin complexes [Ln(hfac)₃(NITptBuPh)₂], [Ln^III = Eu ( 1 ), Tb ( 2 ), Dy ( 3 ), Ho ( 4 ), Er ( 5 )] (hfac = hexafluoroacetylacetonate), were synthesized with the radical ligand NITptBuPh [2‐(4′‐tert‐butylphenyl)‐4, 4,5, 5‐tetramethylimidazoline‐1‐oxyl‐3‐oxide]. These complexes exhibit similar structures. All of them crystallize in the monoclinic space group P2₁/c, and consist of discrete mononuclear molecules. The central Ln^III ion is eight‐coordinate with a distorted dodecahedral environment. The NITptBuPh radical acts as monodentate ligand towards Ln^III ion through the NO group. The magnetic studies suggested weak antiferromagnetic interactions between Ln^III ion and radicals in 1 , 3 , 4 , and 5 , but weak ferromagnetic interaction in 2 .     

Preparation,Crystal Structure,and Magnetic Properties of Rare Earth Ruthenium and Osmium Carbides with La3.67FeC6 Type Structure

The new carbides Gd_3.67RuC₆ and Ln_3.67OsC₆ (Ln = La–Nd, Sm) were prepared by arc‐melting of cold‐pressed pellets of the elemental components. Their hexagonal (P6₃/m) La_3.67FeC₆ type crystal structure was refined from X‐ray powder diffraction data of La_3.67OsC₆ (a = 889.1(1) pm, c = 535.1(1) pm) and Pr_3.67OsC₆ (a = 874.9(2) pm, c = 523.7(1) pm). The occupancy parameters of one La and one Pr site were refined to 0.35(5) and 0.34(5), respectively, in agreement with the highest possible occupancy for steric reasons of 1/3. The C–C distances in the C₂ pairs are 139(6) pm and 137(3) pm, respectively, indicating double bonds. The environment of the osmium atoms is compatible with the 18‐electron rule. The magnetic properties of several carbides were determind with a SQUID magnetometer. The lanthanum compounds La_3.67RuC₆ and La_3.67OsC₆ are Pauli paramagnetic. The magnetic properties of the other compounds are dominated by the magnetic moments of the rare earth atoms. Most order ferrimagnetically with Curie temperatures varying between 5(± 3) and 32(± 6) K for Ce_3.67OsC₆ and Pr_3.67RuC₆, respectively. The cerium atoms in Ce_3.67RuC₆ and Ce_3.67OsC₆ are essentially trivalent, and the samarium compounds show Van Vleck behavior.