Fe/RE多层膜磁性及其变化机制

研究了Ｆｅ／ＲＥ多层膜（Ｆｅ单层厚度〈２．０ｎｍ）沉积态退火过程中（温度≥４７３Ｋ）的结构与磁性，分析了磁性变化的原因。沉积态的Ｆｅ单层由分离的Ｆｅ岛组成，小尺寸的Ｆｅ岛呈超顺磁性导致了整个膜显示顺磁性，退火时Ｆｅ岛合并长大，膜由超顺磁转变为铁磁，同时磁化强度和妖顽力增加。     

Fe—RE磁性多层膜的结构稳定性研究

用真空双源蒸镀法在ＮａＣｌ和Ｓｉ单晶衬底上沉积了ＲＥ－Ｆｅ（ＲＥ：Ｄｙ、Ｙ）成分调制多层膜，借助透射电子显微镜（ＴＥＭ）热台及真空退火方式研究了多层膜受热过程中的结构变化规律。受热温度≤２００℃时，多层膜各单层的非晶结构不发生显著变化，且成分调制结构不被破坏，因此，可以认为非昌单支在多层膜在２００℃以下的结构是稳定的。     

ICP-AES 法测定 RZnAl5RE 合金中的镧、铈、铁、铝、铅、镉

采用ＩＣＰ－ＡＥＳ测定了ＲＺｎＡｌ５ＲＥ合金中的Ｌａ、Ｃｅ、Ｆ３、Ａｌ、Ｐｂ、ＣＤ元素含量。考察了基体及无机酸浓度对６种元素线强度的影响。选择了仪器工作条件,检出限在０．０３～１．００μｇ／Ｌ之间,加标回收率为９３％～１０８％,相对标准偏差小于１２．６８％（ｎ＝１０）。     

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。     

GdAlO_3∶Tb,RE中Tb,RE的能量传递研究

采用柠檬酸盐硝酸盐燃烧法制备了GdAlO3∶Tb,RE荧光粉体.在紫外激发下(254nm),GdAlO3∶Tb发射绿色荧光(5D4→7F5,544nm),Dy共掺杂对绿色发光有增强作用,Ce共掺杂对GdAlO3∶Tb绿色发光有降低作用.激发谱和能谱研究表明:Dy能级嵌入Tb主发射能级5D4(绿色发光能级)、5D3(蓝色发光能级)能级之间,Ce能级嵌入Tb主发射能级5D4、5D3能级上方.这种能级嵌入方式,使得稀土离子之间存在声子支持的共振能量传递,但Tb→Dy→Tb能量传递使Tb绿色发射(5D4→7FJ(J=3,4,5,6))增强,蓝色发射(5D3→7FJ(J=3,4,5,6))减弱;而Ce→Tb能量传递使Tb蓝色发射增强,绿色发射减弱.     

ChemInform Abstract: RE10TCd3 (RE: Y,Tb - Tm,Lu; T: Fe,Co, Ni,Ru, Rh,Pd) - Rare Earth-Rich Phases with Ordered anti-Co2Al5 Structure.

The title compounds are synthesized from the elements (flowing Ar, 1500 K for 2 min, 1300 K for 45 min, and 900 K for 2 h) and characterized by powder XRD.     

电感耦合等离子体原子发射光谱法测定稀土富集物中稀土元素

稀土富集物的测定,一般采用X荧光光谱法[1],这种方法对常量分析结果较好,但测定低含量元素时,分析下限较高.随着稀土工业的发展,对稀土产品要求愈来愈高,其中对镧铈镨钕富集物中界限元素的测定下限,用X荧光光谱法测定已不能满足要求.     

Cobalt Centered Trigonal RE6 Prisms and Mg4 Clusters as Basic Structural Units in RE4CoMg (RE = Y,La, Pr,Nd, Sm,Gd–Tm)

The new rare earth metal rich intermetallic compounds RE₄CoMg (RE = Y, La, Pr, Nd, Sm, Gd–Tm) were prepared via melting of the elements in sealed tantalum tubes in a water‐cooled sample chamber of a high‐frequency furnace. The compounds were investigated by X‐ray diffraction of powders and single crystals: Gd₄RhIn type, , a = 1428.38(9) pm, wR2 = 0.0638, 680 F² values, 20 variables for La₄CoMg, a = 1399.5(2) pm, wR2 = 0.0584, 589 F² values, 20 variables for Pr₄CoMg, a = 1390.2(3) pm, wR2 = 0.0513, 634 F² values, 20 variables for Nd_3.90CoMg_1.10, a = 1381.0(3) pm, wR2 = 0.0730, 618 F² values, 22 variables for Sm_3.92Co_0.93Mg_1.08, a = 1373.1(4) pm, wR2 = 0.0586, 611 F² values, 20 variables for Gd_3.92CoMg_1.08, a = 1362.1(3) pm, wR2 = 0.0576, 590 F² values, 20 variables for Tb_3.77CoMg_1.23, a = 1344.8(2) pm, wR2 = 0.0683, 511 F² values, 20 variables for Dy_3.27CoMg_1.73, and a = 1343.3(2) pm, wR2 = 0.0560, 542 F² values, 20 variables for Er_3.72CoMg_1.28. The cobalt atoms have trigonal prismatic rare earth coordination. Condensation of the CoRE₆ prisms leads to a three‐dimensional network which leaves larger voids that are filled by regular Mg₄ tetrahedra at a Mg–Mg distance of 316 pm in La₄CoMg. The magnesium atoms have twelve nearest neighbors (3 Mg + 9 RE) in icosahedral coordination. In the structures with Nd, Sm, Gd, Tb, Dy, and Er, the RE1 positions which are not involved in the trigonal prismatic network reveal some RE1/Mg mixing and the Sm_3.92Co_0.93Mg_1.08 structure shows small cobalt defects. Considering La₄CoMg as representative of all studied systems an analysis of the chemical bonding within density functional theory closely reproduces the crystal chemistry scheme and shows the role played by the valence states of the different constituents in the electronic band structure. Strong bonding interactions were observed between the lanthanum and cobalt atoms within the trigonal prismatic network.     

钇基重稀土合金变质团球γ+(Fe,Mn)3C共晶体增强奥氏体钢基自生复合材料

采用Y基重稀土合金变质处理钢液,通过影响钢液中C, Mn 等合金元素的偏析和相的生成,从而控制钢液凝固组织,在铸态下获得团球γ+(Fe, Mn)3C共晶体增强奥氏体钢基自生复合材料(AMGE). Y基重稀土合金增大C, Mn 元素的偏析,使凝固后期初生奥氏体枝晶间小熔池中的成分达到共晶反应区,在非平衡凝固条件下生成γ+(Fe, Mn)3C共晶体.干摩擦磨损试验表明,在中、低载工况下AMGE的磨损量比基体合金奥氏体中锰钢低1～3倍,并且AMGE发生严重磨损时的载荷高于基体合金.     

Thermal Decompositions of (RE)Ba2Cu3O6 (RE=Y,Nd, Er)

Thermogravimetric in situ measurements of oxygen loss from (RE)Ba₂Cu₃O₆ samples (RE=Y, Nd, Er) heated isothermally in a relatively high dynamic vacuum were made with a Cahn RG electrobalance. Single-phase orthorhombic samples of composition (RE)Ba₂Cu₃O_7-x (highest oxygen content) were synthesized from stoichiometric (1:2:3) mixtures of high-purity (RE)₂O₃, BaCO₃ and CuO. The original 1:2:3 mixture was prepared by the two-stage procedure described earlier. The crystal structure of the sample in the original orthorhombic phase was controlled by the X-ray powder method (CuKα radiation) using a Stadi P Stoe diffractometer with a position-sensitive detector. The decomposition curves are described by the sum of exponential terms corresponding to rapid and slow first-order processes in which differently sized grains of the powder samples are involved. The activation energies are estimated from appropriate Arrhenius plots. This revised version was published online in July 2006 with corrections to the Cover Date.     

New layered germanide halides RE2GeX2 (RE = Y, Gd; X = Br, I)

The title compounds were synthesized from RE, REX3, and Ge under an Ar atmosphere at 1200-1370 K. Y2GeI2 and Gd2GeI2 crystallize in space group Rm with lattice constants a = 4.2135(3) and 4.2527(1) A and c = 31.480(2) and 31.657(1) A, respectively. Gd2GeBr2 crystallizes in two modifications, the 1T-type (space group Pm1; a = 4.1668(2) A, c = 9.8173(6) A) and the 3R-type (space group Rm; a = 4.1442(9) A, c = 29.487(7) A). The structural motifs of RE2GeX2 compounds are Ge-centered slightly distorted RE6 octahedra connected via their common edges and extending in the a and b directions. The resulting close-packed double layers are separated by halogen atoms. The electrical resistivity measurements revealed semiconductor behavior for Y2GeI2 and Gd2GeI2 and a metal-semiconductor transition for 1T-Gd2GeBr2. Magnetic susceptibility and heat capacity measurements show long-range magnetic ordering for Gd2GeI2 and 1T-Gd2GeBr2 at approximately 15 and approximately 13 K, respectively.     

CaBPO5∶RE(RE=Eu,Tb)的水热合成及其发光特性

利用水热法合成了CaBPO5∶RE(RE=Eu,Tb)荧光体并测试了其结构和光谱, 讨论了其发光性质, 并与高温固相法合成的产物作了对比. 结果表明, 由于电子转移, Eu3+, Tb3+和Eu2+共存于同一体系中, 而且Eu2+的发射位置从402 nm移至428 nm. 在双掺杂体系中引入Ce3+, Eu3+, Tb3+和Eu2+的发光强度均有所增强, 这可能是Ce3+与Eu3+之间的电子转移及各种稀土离子之间能量传递相互竞争的结果.     

Closely related rare-earth metal germanides RE2Li2Ge3 and RE3Li4Ge4 (RE = La-Nd, Sm): synthesis, crystal chemistry, and magnetic properties

Reported are the syntheses, crystal structures, and magnetic susceptibilities of two series of closely related rare-earth metal-lithium germanides RE(2)Li(2)Ge(3) and RE(3)Li(4)Ge(4) (RE = La-Nd, Sm). All title compounds have been synthesized by reactions of the corresponding elements at high temperatures, and their structures have been established by single-crystal X-ray diffraction. RE(2)Li(2)Ge(3) phases crystallize in the orthorhombic space group Cmcm (No. 63) with the Ce(2)Li(2)Ge(3) structure type, while the RE(3)Li(4)Ge(4) phases crystallize in the orthorhombic space group Immm (No. 71) with the Zr(3)Cu(4)Si(4) structure type, respectively. Both of their structures can be recognized as the intergrowths of MgAl(2)Cu- and AlB(2)-like slabs, and these traits of the crystal chemistry are discussed. Temperature-dependent direct-current magnetization measurements indicate Curie-Weiss paramagnetism in the high-temperature regime for RE(2)Li(2)Ge(3) and RE(3)Li(4)Ge(4) (RE = Ce, Pr, Nd), while Sm(2)Li(2)Ge(3) and Sm(3)Li(4)Ge(4) exhibit Van Vleck-type paramagnetism. The data are consistent with the local-moment magnetism expected for RE(3+) ground states. At temperatures below ca. 20 K, magnetic ordering transitions have been observed. The experimental results have been complemented by tight-binding linear muffin-tin orbital electronic-band-structure calculations.     

Polydentate-ligand-supported self-assembly of heterometallic T-shaped Co4RE (RE = Gd, Tb, Y) clusters: synthesis, structure and magnetism

A series of mixed-valent heterometallic pentanuclear Co(III)(3)Co(II)RE(III) (RE = Gd (1), Tb (2), Y (3)) clusters have been rationally assembled by taking advantage of a bifunctional ligand with o-vanillin and tripodal tris(hydroxymethyl)aminomethane units. Structural determinations reveal that all compounds are isomorphous and possess a T-shaped Co(4)RE core, which comprises two nearly linear Co(2)RE subunits sharing a common RE ion. Their magnetic properties were thoroughly studied. The static magnetic susceptibility studies of 1 demonstrate the presence of weak ferromagnetic interactions between the magnetic centres and magnetic anisotropy reflected by the single ion zero-field splitting (ZFS) D term. Both 1 and 2 behave magnetically as heterodinuclear metal systems, while the magnetic behaviour of 3 is identical to an isolated Co(II) ion. Moreover, alternating-current susceptibility measurements did not exhibit any out-of-phase signal, suggesting that slow magnetic relaxation is absent above 2 K within them. These isomorphous Co(4)RE clusters offer an opportunity to systematically probe the contribution of different metal ions to the overall magnetic behaviour in Co(II)-RE(III) systems.     

The carbides RE2MnC4 (RE = Y,Er, Tm) with Er2FeC4-type structure

The title compounds were prepared from coldpressed pellets of the elemental components by arcmelting. They crystallize with the orthorhombic Er₂FeC₄-type structure, which was refined from X-ray data of an Er₂MnC₄ single crystal: Ibam, a = 760.4(1)pm, b = 937.1(1)pm, c = 504.0(1)pm, R = 0.021 for 524 structure factors and 17 variable parameters. Y₂MnC₄ does not become superconducting down to 1.7 K. Chemical bonding in these compounds is briefly discussed.     

Large-scale synthesis of single-crystalline RE2O3 (RE=Y, Dy, Ho, Er) nanobelts by a solid-liquid-phase chemical route

Yttrium-group heavy rare-earth sesquioxide (RE(2)O(3), RE=Y, Dy, Ho, Er) nanobelts were successfully fabricated by thermolysis of solid RE(NO(3))(3)x H(2)O in a dodecylamine/1-octadecene mixed solvent system. The synthetic principle is based on separating the nucleation and growth processes by utilizing the poor solubility of RE(NO(3))(3)chi H(2)O in the solvent mixture and the heat-transportation difference between the liquid and solid. By using dodecylamine, RE(2)O(3) nanobelts can be readily obtained. X-ray diffraction (XRD) analysis shows that the synthesized RE(2)O(3) nanobelts are body-centered cubic and crystalline. Field-emission scanning electron microscopy (FE-SEM), transmission electron microscopy (TEM), selective-area electron diffraction (SAED), and high-resolution transmission electron microscopy (HR-TEM) demonstrate that the synthesized RE(2)O(3) compounds possess regular geometric structure (beltlike) with perfect crystallinity. Preliminary experimental results prove that the dodecylamine plays a key role in the formation of RE(2)O(3) nanobelts and cannot be replaced by other surfactants. Furthermore, this method can be extended to the synthesis of RE(2)O(3) nanobelt/metal nanocrystal nanocomposites and ABO(3) (A=Y, Dy, Ho, Er; B=Al) and A(3)B(5)O(12) (A=Y, Dy, Ho, Er; B=Al)-type ternary oxide nanobelts, using mixed-metal nitrate salts in the correct stoichiometry instead of single rare-earth nitrates.     

稀土－铌(钽)复合溴氧化物的结构与光谱特性

用高温固相法合成了系列化合物RE_0.06La_0.94M₂O₆Br(M=Nb,Ta;RE=Eu,Tb,Pr,Sm),并测定了其激发和发射光谱,室温下Eu³⁺、Tb³⁺、Pr³⁺、Sm³⁺在稀土-铌(钽)复合溴氧化物中呈现特征激发谱线,但Nb和Ta的光谱特性稍有不同。     

同位素示踪法测定稀土在土壤中的吸附,解吸和扩散

对９种不同性质土壤测定结果表明，ＲＥ的吸附或解吸均与Ｌａｎｇｍｕｉｒ方程有极好的拟合性。土壤ＲＥ吸附容量在１．５－１５ｍｇ／ｇ之间，它与土壤中伊利石的相对含量呈明显正相关土壤ＲＥ解吸量与吸附量之间呈显著指数曲线关系，曲线转折点的ＲＥ吸附量称为土壤特征吸附量，以它表征ＲＥ在土壤中运移难易，比土壤吸附容量表征更有意义。