合金元素对HDDR工艺Nd—Fe—B合金粉显微组织和磁各向异性的影响

研究了Ｃｏ和Ｚｒ对ＮｄＦｅＢ合金ＨＤＤＲ粉显微组织和磁各向异性的影响。磁测量结果表明，Ｎｄ１３Ｆｅ８０．４Ｚｒ０．１Ｂ６．５基本上是磁各向同性的，而Ｎｄ１５Ｆｅ６６．９Ｃｏ１１Ｚｒ０．１Ｂ７合金粉末则具有较强的磁各向异性，显微组织观察发现，退火后ＮｄＦｅＢ合金中存在一些富Ｚｒ的新相，并且这些新相在ＨＤＤＲ处理过程中并不发生变化，而Ｃｏ在一定程度上抑制了这些新相的出现，不仅减小了该相的体积份数而且降低了其中的Ｚｒ含量。分析表明，对ＮｄＦｅＢ合金化学成分进行优化以保证硬磁相内溶有一定量的合金元素（例如Ｚｒ）是获得各向异性ＨＤＤＲ粉的关键所在。     

不同时效状态的Sm（Co,Fe,Cu,Ti）7合金高分辨电子显微观察

采用高分辨电子显微术，从不同的晶体学方向观察了Ｓｍ（Ｃｏ，Ｆｅ，Ｃｕ，Ｔｉ）７合金的结构和缺陷，研究表明，它是由富Ｆｅ并含有Ｔｉ的Ｓｍ２（Ｃｏ，Ｆｅ，Ｃｕ，Ｔｉ）１７（简称２：１７）相和富Ｃｕ的Ｓｍ（Ｃｏ，Ｆｅ，Ｃｕ）５（简称１：５）相组成，在峰时效状态，２：１７相成胞状包的平均尺寸约为３３ｎｍ。１：５相分布在２：１７相胞的周围，像是它们的胞壁。２：１７相和１：５相之间存在［０００１］２：１７∥［     

Ce0.5Zr0.5O2固溶体的原位拉曼光谱

控制合成条件以湿化学法制备了Ｃｅ－Ｚｒ－Ｏ（Ｃｅ）／ｎ（Ｚｒ）＝１固溶体,ＸＲＤ结果证实催化剂前体经９２３Ｋ焙烧后可获得立方相Ｃｅ０．５Ｚｒ０．５Ｏ２固溶体,ＴＥ倒固溶体颗粒大小均一、分散、呈纤毛状、在氧化和还原气氛条件下分别对固溶体进行了原位拉曼光谱研究,结果表明,除４５０－４７０ｃｍ＾－１处出现而心立方晶格Ｆ２ｇ拉曼地应的强拉曼谱峰外,２９０－３２０ｃｍ＾－１,５７－６２０ｃｍ＾－１,７７０－     

Ce—Zr—固溶体的制备和表征

采用硝酸盐直接分解法、共沉淀法、苹果酸溶胶、凝胶 柠檬酸溶胶－凝胶法制备了Ｃｅ－Ｚｒ－Ｏ复合氧化物并进行了表征。溶胶－凝胶法制得的Ｃｅ－Ｚｒ－Ｏ为立方的Ｃｅ０．５Ｚｒ０．５Ｏ２复合氧化物（其中少量具有立方性质的ｔ＾〃相）,而直接分解和共沉淀法制得的是由立方Ｃｅ０．８Ｚｒ０．２Ｏ２和四方Ｃｅ０．２Ｚｒ０．８Ｏ２固溶体组成的复合氧化物。不同制备方法制得的样品由于物相组成不同,还原性能也有较大差别。差热     

Fe—15Cr—4Al—Y合金中的Y—Fe相及其作用

在含０．２％－１．４％Ｙ的Ｆｅ－１５Ｃｒ－４Ａｌ－Ｙ合金中，１－１０μｍ的Ｙ－Ｆｅ相质点弥散分布，其硬度高于ａ相的２倍，组成可用Ｙ２（Ｆｅ７６Ｃｒ１２Ａｌ１１Ｓｉ）１７表示。Ｙ－Ｆｅ相强烈俘获ａ相中的碳原子，使合金在固溶处理状态下的Ｓｎｏｅｋ内耗峰消失，在７００℃下析出碳化物。Ｙ－Ｆｅ相南点通过阻止闰长大而抑制合金的高温脆化，通过俘获碳原子而延缓４７５℃脆性发展。此外，它们还有提高热强性和抗氧化性     

柄型金属有机化合物（Ⅳ）：四甲基二硅桥连取代环戊二烯？…

四甲基二硅桥连取代环戊二烯基配体相继与丁基锂及ＭＣ１４。２ＴＨＦ作用,生成四甲基二硅桥连取代环戊二烯基钛和锆化合物（Ｍｅ２ＳｉＳｉＭｅ２）（Ｃ５Ｈ４Ｒ）（Ｃ５Ｈ４Ｒ１）ＭＣ１２「Ｒ＝Ｈ,Ｒ１＝ｔ－Ｂｕ,Ｍ＝Ｔｉ（１）,Ｚｒ（２）,Ｈｆ（３）;Ｒ＝Ｈ,Ｒ１＝Ｍｅ,Ｍ＝Ｔｉ（４）;Ｒ＝Ｒ１＝Ｍｅ,Ｍ＝Ｔｉ（５）,Ｚｒ（６）」。通过元素分析、ＭＳ和Ｈ１ＮＭＲ谱表征了化合物的分了结构,并通过Ｘ射线衍射分析     

柄型金属有机化合物（Ⅱ）：硅氧硅桥联二（1—茚基及四氢茚基…

１，３－二（１－茚基）四甲基二硅氧烷相继与丁基锂及ＺｒＣｌ４．２ＴＨＦ作用，生成硅氧桥联二（１－茚基）二氯化锆（Ｍｅ２ＳｉＯＳｉＭｅ２）（Ｉｎｄ）２ＺｒＣｌ２（１）。对其进行催化氢化得到相应的四氢茚基化合物（Ｍｅ２ＳｉＯＳｉＭｅ２）ＩｎｄＨ４）２ＺｒＣｌ２（２）．１和２均含有顺式和反式二种异构体（１和１以及２和２），通过重结晶得到纯的单一异构体，１，２和２，１和２的晶体结构经Ｘ射线衍射测定，二者均     

Fe_2O_3／ZrO_2催化剂上一氧化碳加氢反应制低碳烯烃 Ⅱ．预处理条件对催化剂结构及性能的影响

用ＴＰＲ，Ｍｏｓｓｂａｕｅｒ谱法，ＸＰＳ，ＸＲＤ及反应评价等手段研究了Ｆｅ２Ｏ３／ＺｒＯ２催化剂的还原行为、铁物种状态和ＣＯ加氢反应性能．结果表明，预处理条件明显影响Ｆｅ２Ｏ３／ＺｒＯ２催化剂表面铁原子的数量、铁锆间的相互作用、催化剂的物相变化以及ＣＯ加氢反应的催化性能．以Ｆｅ２Ｏ３／ＺｒＯ２经氢氟混合气程序升温至７５３Ｋ还原生成的Ｆｅ－Ｚｒ－Ｏ物种为前身，在合成气中进一步还原得到的铁锆催化剂，具有较好的Ｆ－Ｔ反应合成低碳烯烃的选择性．     

（四甲基二硅撑）二（3－三甲硅基环戊二烯基）四羰基二铁及其相关化合物的合成及结构

１，２－二（三甲硅基环戊二烯基）四甲基二硅烷与Ｆｅ（ＣＯ）_５在二甲苯中于１０５～１１０℃反应除分离到少量标题化合物（Ｍｅ_２ＳｉＳｉＭｅ_２）［η－（３－Ｍｅ_３ＳｉＣ_５Ｈ_３Ｆｅ（ＣＯ）］_２（μ－ＣＯ）_２（５）外，主要是生成了脱Ｍｅ_３Ｓｉ基的产物（Ｍｅ_２ＳｉＳｉＭｅ_２）［η－Ｃ_５Ｈ_４Ｆｅ（ＣＯ）］_２（μ－ＣＯ）_２（１）及１的热重排异构体［Ｍｅ_２ＳｉＣ５Ｈ４－Ｆｅ（ＣＯ）_２］_２（２）．将５的二甲苯溶液加热回流１８ｈ，则转化为其异构体［Ｍｅ_２Ｓｉ（Ｍｅ_３ＳｉＣ_５Ｈ_３）Ｆｅ（ＣＯ）_２］_２（６）．脱硅基发生在由相应反应物制备５的过程中。且脱硅基是与反应物中（Ｍｅ_２ＳｉＳｉＭｅ_２）桥的存在有关．５的晶体结构经Ｘ射线衍射测定属单斜晶系，Ｐ２_１／ｍ空间群，晶体学数据：ａ＝０．６７８０（１）ｎｍ，ｂ＝２．２３０３（９）ｎｍ，ｃ＝０．９９８８（１）ｎｎ，；β＝９８．９６（１）°，Ｖ＝１．４９６０ｎｍ~３．Ｚ＝２，Ｄ_ｃ＝１．３６ｇ／ｃｍ~３．     

环状配合物Me_2Si［η~5－C_5H_4Fe（CO）_2］_2SnR_2的合

通过ＳｎＣｌ_２对化合物Ｍｅ_２Ｓｉ［η~５－Ｃ_５Ｈ_４Ｆｅ（ＣＯ）］_２（μ－ＣＯ）_２（Ⅰ）中Ｆｅ－Ｆｅ键的插入反应以及Ⅰ被Ｎａ－Ｈｇ齐还原所生成的相应双铁负离子｛Ｍｅ_２Ｓｉ［η~５－Ｃ_５Ｈ_４Ｆｅ（ＣＯ）_２］_２｝~（２－）与ＳｎＲ_２Ｃｌ_２（Ｒ＝Ｍｅ，Ｐｈ）的亲核反应，合成了环状化合物Ｍｅ_２Ｓｉ［η~５－Ｃ_５Ｈ_４Ｆｅ（ＣＯ）_２］_２ＳｎＲ_２［Ｒ＝Ｃｌ（１），Ｍｅ（２），Ｐｈ（３）］。以元素分析、ＩＲ和~１ＨＮＭＲ谱表征了它们的结构，并用Ｘ射线衍射测定了配合物３的晶体结构。３为单斜晶系，空间群Ｐ２_１／ｎ，ａ＝１．０３８４（３）ｎｍ，ｂ＝１．６３８４（１）ｎｍ，ｃ＝１．５７６２（５）ｎｍ，β＝９７．９３（２）°，Ｖ＝２．６５６（２）ｎｍ~３，Ｚ＝４，Ｄｘ＝１．７１ｇ／ｍＬ。     

V2.1TiNi0.4Zr0.06Cu0.03M0.10 (M=Cr,Co, Fe,Nb, Ta)储氢合金的微结构及电化学性能

采用磁悬浮感应熔炼方法制备了V2.1TiNi0.4Zr0.06Cu0.03M0.10(M=Cr, Co, Fe, Nb, Ta)储氢电极合金, 通过X射线衍射(XRD)、扫描电子显微镜(SEM)、电子衍射能谱(EDS)分析和电化学测试等手段系统研究了添加元素M对合金微结构与电化学性能的影响. 结果表明, 所有合金均由BCC结构的V基固溶体主相和C14型Laves第二相组成, 且第二相沿主相晶界形成三维网状分布; Cr、Nb 和Ta元素主要分布在合金主相中, 而Co和Fe元素主要分布在第二相中. 电化学性能测试表明, 在V2.1TiNi0.4Zr0.06Cu0.03合金中掺加Cr、Co、Fe、Nb或Ta元素后, 虽然会降低最大放电容量, 但能有效抑制合金中V和Ti的腐蚀溶出, 提高电极充放电循环稳定性; 同时还能明显改善合金的高倍率放电性能. 相比之下, V2.1TiNi0.4Zr0.06Cu0.03Cr0.10合金具有最佳的综合电化学性能.     

Sm2Fe17N3晶体的价电子结构分析和结合能、最强键能计算

由EET理论直接建立了Sm2Fe17N3晶体的价电子结构,同时计算并筛选了晶体的结合能和最强键能,分别为EC^0=14716.8±13.7kJ·mol^-1和Eα=110.1311 kJ·mol^-1。分析计算结果表明:Sm2Fe17N3晶体内共价电子数主要分布在12对由Fe(c1),Fe(c2)和Fe(c3)参与形成的最强键能的键上,由这3种Fe晶位原子形成的共价键键距普遍小于0.3 nm,共价键较强对晶体结合能作主要贡献;并且其结合能相比Sm2Fe17晶体的小得多,解释了Sm2Fe17合金在低温和非真空状态条件下易氧化而经过渗氮后得到的Sm2Fe17N3则表现出常温下结构稳定、化学性能好的特性;计算出N原子参与形成的成键原子对的理论键能值普遍在1 kJ·mol^-1左右,反映出Sm2Fe17N3化合物内在渗氮特性,分析了制备钐铁氮永磁材料过程中Sm2Fe17合金较低温渗氮难、渗氮不稳定和渗氮不均匀的缺陷。     

铜、钛复合添加对结NdFeB磁体显微组织和磁性能的影响

研究了烧结NdFeB磁体晶间合添加Cu和Ti 对磁体显微组织和磁性能的影响，当钛含量小于1.2%时，Cu和Ti晶间复合添加可大幅度提高烧结NdFeB磁体的矫顽力，磁变化不大，矫顽力的提高归因于Cu和Ti在主相晶粒表面富集，细化晶粒，阻断主相晶粒之间的磁交换作用，阻碍反磁化畴的传播，当钛含量大于1.2%时，矫顽力略有下降，乘磁急剧下降，乘磁下降的原因在于出现了大量的条状纯钛相。与晶间单独合金化相比，晶间复合合金化可更有效改善NdFeB磁体显微组织与性能。     

CRYSTALLOGRAPHIC STRUCTURE AND MAGNETIC PROPERTIES OF R_(2)Fe_(17)N_(2.4)

By a proper thermal treatment, the nitrogen atoms can enter the R2Fe17 structure. The crystallographic and intrinsic magnetic properties as well as their relationship have been studied by magnetic measurements, X-ray and neutron diffraction techniques. The neutron data indicate that the nitrogen atoms occupy the interstitial sites in the Th2Zn17-type rhom-bohedral structure. The inserting nitrogen atoms are found to dilate the cell volume, increase the Curie temperature and enhance the saturation moment by raising the difference in the electron number between the spin-up and spin-down 3d subbands of the Fe atoms. Furthermore, the nitrogen atoms have an important effect on the magnetocrystallic anisotropy, which results in an easy axis with Sm2Fe17N2.4. All these make Sm2Fe17N2.4 favorable for permanent magnet applications.     

Low-temperature diffusion of oxygen through ordered carbon vacancies in Zr2C(x): the formation of ordered Zr2C(x)O(y)

Investigations are performed on low-temperature oxygen diffusion in the carbon vacancy ordered ZrC(0.6)and thus induced formation of the oxygen atom ordered ZrC(0.6)O(0.4). Theoretically, a superstructure of Zr(2)CO can be constructed via the complete substitution of carbon vacancies with O atoms in the Zr(2)C model. In the ordered ZrC(0.6), the consecutive arrangement of vacancies forms the vacancy channels along some zone axes in the C sublattice. Through these vacancy channels, the thermally activated oxygen diffusion is significantly facilitated. The oxygen atoms diffuse directly into and occupy the vacancies, producing the ordered ZrC(0.6)O(0.4). Relative to the ordered ZrC(0.6), the Zr positions are finely tuned in the ordered ZrC(0.6)O(0.4) because of the ionic Zr-O bonds. Because of this fine adjustment of Zr positions and the presence of oxygen atoms, the superstructural reflections are always observable in a selected area electron diffraction (SAED) pattern, despite the invisibility of superstructural reflections in ZrC(0.6) along some special zone axes. Similar to the vacancies in ordered ZrC(0.6), the ordering arrangement of O atoms in the ordered ZrC(0.6)O(0.4) is in nanoscale length, thus forming the nano superstructural domains with irregular shapes.     

Actinide(lanthanide)-noble metal alloy phases,preparation and properties

Actinide (AThCm)-noble metal phases with platinum, palladium, rhodium, and iridium (B)- and lanthanide-noble metal phases with platinum and palladium have been prepared by reduction of corresponding oxides or fluorides in the presence of noble metals by extremely purified hydrogen. Alloy phases of composition AB₂, AB₃, and/or AB₅ have been identified, most of which crystallize in the Cu₂Mg, Cu₃Au, Ni₃Ti, Cd₃Mg, Ni₅U, and Pt₅Sm types of structure. The lattice constants of isostructural series show a trend which also is known for the radii of the actinide elements. Analytical data, self-irradiation effects, magnetic data, nuclear γ resonance spectra, and thermal behaviour of selected alloy phases as well as the preparation of alloy phases of some other transition and main group elements, e.g., Zr, Hf, Nb, Ta, MgBa, are reported.     

不同的烧结工艺对Sm-Co2:17型高温磁体性能的影响

采用中频感应熔炼法制备了Sm(Co0.79Fe0.09Cu0.085Zr0.032)7.95合金,采用传统烧结工艺,在1200～1240℃烧结1 h,1165～1190℃固溶处理3 h,快速风冷淬火后在840℃保温12 h,以0.4℃.min-1的冷速冷却至420℃,保温10 h,最后随炉冷却。磁体经过加工后,采用不同的磁性测试手段对磁体进行测试。结果表明,磁体的剩磁随烧结温度的升高而增大,矫顽力最好的工艺为1230℃烧结1 h,然后在1180℃固溶3 h。将此工艺制备的磁体采用中国计量科学院NIM-500C超高温永磁测量仪测试,磁体在773 K时的最大磁能积为10.94 MGOe,高于已经报道的同Z值的2∶17型永磁体。磁体的磁滞回线通过振动样品磁强计(VSM)测得,室温下Br=10.5 kGs,Hcj=30.21 kOe,(BH)max=25.60MGOe;773 K时磁体Br=7.45 kGs,Hcj=6.02 kOe,(BH)max=9.85 MGOe。剩磁温度系数α=-0.0624%.℃-1,矫顽力温度系数β=-0.169%.℃-1。     

Synthesis of L10 Fe–Pd films by electrodeposition and thermal annealing

Fe–Pd alloy films have been prepared by electrochemical deposition from an alkaline electrolyte containing Fe sulfate, Pd chloride and 5-sulfosalicylic acid onto polycrystalline titanium substrates. The as-deposited films were nanocrystalline and magnetically soft (coercivity ∼ 25 Oe). L1₀ Fe–Pd films with a (1 1 1) preferred orientation were obtained by post-deposition thermal annealing of films with composition about 37 at% Fe in an (Ar + 5% H₂) gas flow at 500 °C. Such films exhibit hard magnetic properties, with a coercivity up to 1880 Oe, and a slightly anisotropic magnetic response, with a larger in-plane remanence. Preliminary magnetic investigations support magnetization switching through pinning of domain walls.     

Lanthanide-3d cyanometalate chains Ln(III)-M(III) (Ln=Pr, Nd, Sm, Eu, Gd, Tb; M=Fe) with the tridentate ligand 2,4,6-tri(2-pyridyl)-1,3,5-triazine (tptz): evidence of ferromagnetic interactions for the Sm(III)-M(III) compounds (M=Fe, Cr)

A series of cyanide-bridged chain mixed Fe(III)/Ln(III) (Ln=Pr, Nd, Sm, Eu, Gd, Tb) complexes with the tridentate ligand 2,4,6-tri(2-pyridyl)-1,3,5-triazine (tptz) used as a capping group has been prepared. Reactions of tptz and LnCl3 with K3Fe(CN)6 yield a family of air-stable 1-D compounds {[Pr(tptz)(H2O)4Fe(CN)6].8H2O}infinity, {[Nd(tptz)(H2O)4Fe(CN)6].8H2O}infinity, {[Sm(tptz)(H2O)4Fe(CN)6].8H2O}, {[Eu(tptz)(H2O)4Fe(CN)6].6H2O}infinity, {[Gd(tptz)(H2O)4Fe(CN)6].6H2O}infinity, and {[Tb(tptz)(H2O)4Fe(CN)6].8H2O}infinity. Temperature dependent magnetic susceptibility studies of reveal that in , the Sm(III) and Fe(III) ions are ferromagnetically coupled with 3-D ordering occurring below 3.5 K. The appearance of the frequency dependent out-of-phase signal is explained in terms of an ordering with a spin glass-like behavior. To compare the magnetic behavior of with related compounds, {[Sm(tptz)(H2O)4Co(CN)6].8H2O}infinity and {[La(tptz)(DMF)(H2O)3Fe(CN)6].5H2O}infinity, {[Sm(tmphen)(DMF)3(H2O)Fe(CN)6].2H2O}infinity, {[Sm(tmphen)2(H2O)2Fe(CN)6].MeOH.13H2O}infinity and {[Sm(tmphen)2(H2O)2Cr(CN)6].MeOH.9H2O}infinity with 3,4,7,8-tetramethyl-1,10-phenanthroline (tmphen) were also prepared.     

The First Mixed-Halide Zirconium Cluster Compounds: Zr(6)Cl(1.6)I(10.4)Be, Zr(6)Cl(1.3)I(10.7)B, and Zr(6)Cl(11.5)I(1.5)B. Matrix Effects and Halogen Substitution in Compact Network Structures

Investigations of the effect of halogen size on structure stability have been conducted in well-reduced and heavily interbridged zirconium chloride-iodide cluster systems. The title compounds are obtained in good yields from reactions of Zr, ZrCl(4), ZrI(4), and B or Be in sealed Ta tubes for approximately 4 weeks at 850 degrees C. Single-crystal diffraction at room temperature established these as Zr(6)Cl(1.65(4))I(10.35(4))Be and Zr(6)Cl(1.27(3))I(10.73(3))B [R&thremacr;, Z = 3, a = 14.3508(8), 14.389(1) ?, c = 9.8777(9), 9.915(2) ?, respectively] and Zr(6)Cl(11.47(2))I(1.53(2))B [P4(2)/mnm, Z = 2, a = 12.030(1) ?, c = 7.4991(8) ?]. These are derivatives of the Zr(6)I(12)C and orthorhombic Zr(6)Cl(13)B structures, respectively, the latter containing unusual linear chains of clusters interbridged by Cl(i-i) that are in turn interconnected by three-bonded Cl(a-a-a) atoms. The random substitution of fractional Cl at specific I sites in the first two, and I for certain Cl in the third, was positionally resolved in all cases. The replacement always occurs at two-bonded X(i), so that single types of halogen are left in sites that interconnect clusters and generate the three-dimensional array. Structural changes seen in both structures are specifically related to relief of X.X crowding in the parent structure (matrix effects). Substitution of Cl for I(i) in the Zr(6)I(12)C type greatly reduces intercluster I.I repulsions and allows, among other things, a 0.20 ? (5.8%) reduction in Zr-I(a-i) intercluster bond lengths. Increased Cl.I repulsions caused by I substitution in orthorhombic Zr(6)Cl(13)B (Pnnm) convert the twisted chains and angular Cl(a-a-a) interchain bridges to planarity in tetragonal Zr(6)Cl(11.5)I(1.5)B. Phase widths found are 0 相似文献