Structure and magnetic properties of mechanically alloyed Tb0.2Pr0.8（Fe0.4Co0.6）1.93 and magnetostriction of its epoxy composite

The C15 Laves phase with composition Tb_0.2Pr_0.8(Fe_0.4Co_0.6)_1.93 was synthesized by mechanical alloying (MA) and subsequent annealing process. The structure and magnetic properties of Tb_0.2Pr_0.8(Fe_0.4Co_0.6)_1.93 were investigated by means of X-ray diffraction (XRD), a vibrating sample magnetometer, and a standard strain technique. The effect of annealing on the structure and magnetic properties was studied. The analysis of XRD shows that the high Pr-content Tb_0.2Pr_0.8(Fe_0.4Co_0.6)_1.93 alloy with the single phase of MgCu₂-type structure can be successfully synthesized by MA method. The sample annealed at 450°C is found to have a coercivity of 196 kA/m at room temperature. An epoxy/Tb_0.2Pr_0.8(Fe_0.4Co_0.6)_1.93 composite was produced by a cold isostatic pressing technique. A large magnetostriction of 400 ppm, at an applied magnetic field of 800 kA/m, was found for the composite. The epoxy-bonded Tb_0.2Pr_0.8(Fe_0.4Co_0.6)_1.93 composite combines a high magnetostriction with a significant coercivity, which is a promising magnetostrictive material.     

Structure and magnetostriction of Tb0.4Nd0.6(Fe0.8Co0.2)1.90 alloy prepared by solid-state synthesis

Mechanical alloying (MA) and subsequent solid sintering process was used to prepare the Nd-containing magnetostrictive Tb0.4Nd0.6(Fe0.8Co0.2)1.90 alloy. The structure, thermal stability and phase transformation were investigated as functions of composition, milling process and annealing temperature. An amorphous phase was formed by high-energy ball milling for 5 h with the ball-to-powder weight ratio of 20:1, which crystallized into MgCu2-type and PuNi3-type crystalline structure with different annealing temperatures. The magnetoelastic properties were investigated by means of a standard strain technique. The high Nd-content (Tb,Nd)(Fe,Co)2 Laves phase for the composition Tb0.4Nd0.6(Fe0.8Co0.2)1.90 was synthesized by MA process plus annealing at 500 ℃ for 30 min.     

聚合-热解法制备Co0.2Zn0.2Mn0.6Fe2O4纳米颗粒及其表征

采用聚合-热解法制备了Co0．2Zn0．2Mn0．6Fe2O4磁性纳米颗粒,借助热重分析法（TG）、X射线衍射（XRD）、透射电镜（TEM）和振动样品磁强计（VSM）对产物进行了表征．结果表明,产物具有尖晶石结构,无杂相,粒径分布范围在8-15nm之间．常温下该材料的剩磁强度和矫顽力分别为0．516和2．388kA／m．     

Sr0.8Re0.2Fe11.8Co0.2O19(Re=La,Nd)的制备、表征及吸波性能

采用溶胶凝胶法,制备Sr0.8Re0.2Fe11.8Co0.2O19(Re=La,Nd)复合铁氧体。采用X射线衍射仪、扫描电子显微镜、振动样品磁强计和矢量网络分析仪表征粉体的结构及电磁性能。结果表明:得到的粉体为纯净的磁铅石型铁氧体,La3+掺杂样品的各项性能明显改善。在室温条件下,稀土离子掺杂后样品的Ms受到稀土离子掺杂的影响较小,Hc则明显提高;La^3+掺杂样品和Nd3+掺杂样品的Ms值接近,前者的Hc值则明显强于后者的,Sr0.8La0.2Fe11.8Co0.2O19的Ms和Hc分别为58.08A m^2/kg和362.0kA/m。稀土离子掺杂使铁氧体样品的复介电常数(ε′和ε″)增大,与Nd3+掺杂样品相比,La3+掺杂样品的介电损耗和磁损耗改善更为明显。利用传输线理论优化设计时发现,在1.2~2.4 mm之间,随着厚度的增加,Sr0.8La0.2Fe11.8Co0.2O19的反射率峰值先减少后增加,逐渐向低频移动;在厚度为2.0 mm时,其反射率峰值达到最小值为27.8 dB(11.8 GHz),小于10 dB的吸波带宽为5.2 GHz(9.5~14.7 GHz)。     

Effect of Doping of Ti and C on Crystallization and Magnetic Properties of NdPrFeB Thick Melt-Spun Ribbons

系统研究了添加Ti和C对NdPrFeB合金厚带晶化过程及磁性能的影响。结果表明,Ti的添加可以抑制合金中(Nd,Pr)2Fe23B3亚稳相的生成并细化晶粒从而极大地提高矫顽力;而同时添加Ti和C,随着C含量的增加,矫顽力逐渐降低而剩磁升高。最佳热处理后(Nd0.4Pr0.6)9Fe72Ti4B11C4合金的磁性能达到Jr为0.88T,Hcj为618kA/m,(BH)max为109.8kJ/m3。     

热处理对<110>取向Tb0.36Dy0.64(Fe0.85Co0.15)2合金磁致伸缩的影响

采用区熔定向凝固方法,制备<110>取向Tb0.36Dy0.64(Fe0.85Co0.15)2合金棒.用管式炉,在1000℃进行4h的均匀化处理;沿垂直合金棒轴向,在240kA]m中进行磁场退火处理.研究了热处理方式对合金取向、显微组织和磁致伸缩的影响.结果表明,均匀化处理和磁场退火处理均不改变合金轴向择优取向;均匀化处理后,网状富稀土相球状聚集,有效地提高了合金的磁致伸缩,"跳跃"效应增强;磁场退火处理后,合金在无预压力下的磁致伸缩显著提高,而"跳跃"效应减弱.     

Effect of Pr on the Structure and Magnetic Properties of CoPt Alloys

对PrxCo50-xPt50(x=0,0.2,0.4,0.6,0.8,1.0)合金的显微结构和磁性能进行了研究。X射线衍射结果表明:经1000℃均匀化后合金为单一的面心立方相(fcc),而经675~750℃退火后合金由硬磁相(面心四方结构,fct)和软磁相组成。随着Pr含量增加,fct的(111)衍射峰向高角度偏移,并且c/a增大导致有序度S减小。合金Pr0.4Co49.6Pt50经675°C退火60min后,矫顽力和剩磁比达到最大值。PrxCo50-xPt50(x=0,0.2,0.4,0.6,0.8,1.0)经675°C退火60min的样品,矫顽力随着Pr含量的增加而单调减小,但剩磁比先增大后减小。     

Fe44Co20Nd7Nb4B25大块非晶合金磁性及热稳定性研究

采用铜模吸铸法制备了Fe44Co20Nd7Nb4B25大块非晶合金,利用差示扫描量热仪(DSC)、X射线衍射仪(XRD)、高分辨透射电镜(HRTEM)和振动样品磁强计(VSM)研究了该合金的结构、非晶形成能力、热稳定性及磁性能.结果表明:该合金为完全非晶结构,在室温下表现为良好的软磁性,并具有较好的非晶形成能力和热稳定性,晶化激活能Ep为642 kJ/mol.退火后该合金表现为硬磁性,退火温度为1003 K时,内禀矫顽力iHc达到最大值,为l164kA/m;退火温度为963 K时,剩余磁感应强度研和最大磁能积(BH)max的值最大,分别为0.27 T和15.79 kJ/m3.     

Pr0.3TbxDy0.7-xFe1.9Ti0.1合金结构和磁致伸缩

采用电弧熔炼方法制备了Pr0.3TbxDy0.7-xFe1.9Ti0.1(x=0.18～0.21)合金,对样品进行不同条件退火处理,并测量了其磁性能。结果表明:退火前样品都有杂相,并且第二相很大程度上影响样品磁致伸缩;700℃,6d退火处理没有有效消除杂相,样品磁致伸缩没有明显得到改善;而900℃,3d退火处理有效地消除了样品的杂相,尤其是x=0.21的样品,几乎呈现完美的单一的MgCu2型Laves相,磁化强度和磁致伸缩系数均有所增加,当磁场为900kA/m时该样品磁致伸缩系数达到了1.12×10-3。     

Fe83Ga17R0.6(R=Ce,Tb和Dy)合金的微结构与磁致伸缩性能

为改善多晶Fe-Ga合金的磁致伸缩性能,在Fe-Ga合金中掺杂稀土Ce、Tb和Dy元素。 研究了Fe83Ga17和Fe83Ga17R0.6 (R=Ce、Tb和Dy)合金的结构和磁致伸缩性能。结果表明,Fe83Ga17合金由单一bcc结构Fe(Ga)固溶体相组成,而掺杂稀土后的Fe83Ga17R0.6合金中除保持bcc结构的Fe(Ga)固溶体相外,还出现了R2Fe17第二相。掺杂稀土后的Fe83Ga17R0.6合金磁致伸缩系数明显大于Fe83Ga17合金。掺杂不同种类的稀土元素对Fe-Ga合金磁致伸缩性能改善的程度不同。在外磁场为557 kA/m时,Fe83Ga17Ce0.6合金的磁致伸缩系数(206×10-6)明显大于Fe83Ga17Tb0.6 (165×10-6)和Fe83Ga17Dy0.6 (161×10-6)合金的磁致伸缩系数。     

AB3.8型La-Mg-Ni系储氢合金相结构和电化学性能研究

系统研究了La0.8-xPrxMg0.2Ni3.8和La0.8-xPrxMg0.2Ni3.2Al0.2Co0.4(x=0, 0.15, 0.3, 0.4)两组储氢合金的相结构与电化学性能。相结构分析表明,合金主要由Pr5Co19、Ce5Co19、CaCu5型物相组成。随着x的增加,合金中A5B19(Pr5Co19+Ce5Co19)型物相逐渐增多,同时各物相的晶胞参数(a, c)和晶胞体积(v)均减小。Al元素的加入有利于CaCu5型物相的形成。电化学测试表明, A5B19型相合金具有较好的电化学循环稳定性,Al、Co元素的加入有利于A5B19型相合金电极的电化学循环稳定性     

Structural,magnetic and magnetoelastic properties of Laves-phase Tb0.3Dy0.6Nd0.1(Fe1-xCox)1.93 compounds (0 ≤ x ≤ 0.40)

Structure, magnetization and magnetostriction of Tb_0.3Dy_0.6Nd_0.1(Fe_1-xCo_x)_1.93 (0 ≤ x ≤ 0.40) compounds have been investigated. X-ray diffraction (XRD) analysis shows the presence of single Laves phase with a cubic MgCu₂-type structure. The easy magnetization direction (EMD) is observed to be <111> direction when x ≤ 0.10, and deviates away with further increasing Co contents. The Co contributes an opposite role in the resultant magnetocrystalline-anisotropy compared to Tb. A small amount of Co substitution for Fe can enhance the Curie temperature for x ≤ 0.25. The magnetocrystalline-anisotropy compensation can be achieved in this system. A minimum in anisotropy is obtained for the Tb_0.3Dy_0.6Nd_0.1(Fe_0.8Co_0.2)_1.93 compound, which has good magneto-elastic properties, e.g., the large saturation magnetostriction λ_S (∼930 ppm) and the high low-field magnetostriction λ_a (∼670 ppm/3 kOe), and may make it technological interest in the field of magnetostrictive materials.     

稀土对La0.6R0.2Mg0.2（NiCoAlMn）3.3储氢合金相结构和电化学性能的影响

以La0.6R0.2Mg0.2Ni2.8Co0.2Al0.2Mn0.1(R=La、Ce、Pr、Nd、Y)合金为研究对象,研究稀土元素R部分替代La后对合金相结构和相组成及电化学性能的影响。X射线衍射(XRD)和显微电子探针(EPMA)方法分析结果表明,合金La0.8Mg0.2Ni2.8Co0.2Al0.2Mn0.1退火组织主要由Ce2Ni7型相(或Gd2Co7型)、PuNi3型相和CaCu5型相组成;Pr、Ce、Nd元素的替代对合金的相组成没有明显影响,而Y元素替代使合金中CaCu5型相明显减少,Ce2Ni7型(或Gd2Co7型)相显著增加,其相丰度达到79.03%。Y元素替代时合金中Gd2Co7型相基本消失。电化学测试和分析表明,稀土元素R替代La后对合金电极活化性能影响不大,其中Pr、Nd、Y部分替代La在一定程度上提高了合金的最大放电容量,而元素Y替代时合金电极容量最高达到392.6mAh/g;Y元素部分替代La使合金电极的循环稳定性得到明显提高,S100达到90.3%。     

MAGNETOSTRICTIVE BEHAVIOUR OF R（Fe_（1－x）Al_x）_y ALLOYS（R＝Dy_（0．65）Tb_（0．25）Pr_（0．1））

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A new candidate as the cathode material for intermediate and low temperature SOFCs

In order to develop the new cathode materials suitable for intermediate and low temperature solid oxide fuel cells (IT/LTSOFCs), LaNi1-xFexO3(x=0.4-0.8) (LNF) materials were synthesized using coprecipitation method. Their structures and morphologies were investigated by XRD and SEM, and their electronic conductivities at different temperatures were measured by dc four terminal method. Fuel cells were fabricated to evaluate the electrochemical properties of the LNF materials as cathodes at different temperatures. The performance of 450-497 mW·cm-2 was obtained in the temperature region of 580-650 ℃ for the LaNi0.2Fe0.8O3 cathode, and of 209-227 mW·cm-2 at 400-500 ℃ for the LaNi0.4Fe0.6O3. The excellent fuel cell performances indicate that the LNF materials are good cathodes for IT/LTSOFCs.     

Crystallization kinetics and magnetization behavior of RE_(3.5)Fe_(66.5)Co_(10)B_(20)(RE=Pr,Nd) nanocomposite ribbons

The influence of hard magnetic phase on the crystallization kinetics and magnetization behavior in nanocomposite RE3.5Fe66.5Co10B20(RE = Pr, Nd) ribbons prepared by melt-spinning was studied. Differential scanning calorimeter(DSC) measurement of the as-cast meltspun amorphous ribbons during the crystallization process shows that precipitation energy of Pr2Fe14 B phase is higher than that for Nd2Fe14 B phase, confirmed by X-ray diffraction(XRD) patterns. It can be explained by the different radii of Pr and Nd atoms. Scanning electron microscopy(SEM)images indicate that the average grain size in Pr3.5Fe66.5Co10B20 ribbon is smaller than that in Nd3.5Fe66.5Co10B20,resulting in an enhancement of exchange coupling between hard and soft phases. It is responsible for the better hard magnetic properties in Pr3.5Fe66.5Co10B20. In addition, the process of magnetization reversal of nanocomposite RE3.5Fe66.5Co10B20(RE = Pr, Nd) ribbons was discussed in detail by the recoil loops.     

Structural,Dielectric, and Magnetic Properties of Ba-Doped Multiferroic Bismuth Ferrite

The main focus of the research was to correlate the microstructure with dielectric and magnetic properties of Bi1-xBaxFeO3 samples. Bi1-xBaxFeO3 samples(x = 0.1, 0.2 and 0.3) were synthesized by the conventional solid-state reaction method using nano-powders of Bi2O3, Fe2O3, and BaCO3. Thereafter, field emission scanning electron microscope and X-ray diffraction(XRD) techniques were used to examine the structure and phase of the samples. Phase analysis by XRD indicated that the single-phase perovskite structure was formed with possible increment in lattice parameter with increasing Ba doping. Complex permeability(u'iand u'i) measured using impedance analyzer confirmed the increase in magnetic property with increasing Ba doping. Finally, dielectric constant(k) was analyzed as a function of temperature at different frequencies. Dielectric constant as high as 2900 was attained in this research for Bi0.8Ba0.2FeO3 sample due to reduction in leakage current at this composition.     

Tm元素对SmCo_5晶体结构与磁性能的影响（英文）EI北大核心CSCD

采用X射线衍射分析(XRD)和磁性能测试等方法,分析了Tm元素掺杂对Sm Co5晶体结构和内禀磁性能的影响。XRD测试结果表明:Sm Co5和Sm0.8Tm0.2Co5.2均为Ca Cu5结构,掺杂Tm元素后,晶格常数c值增大,而a,b与晶胞体积减小;M-T曲线测试结果表明:Sm Co5和Sm0.8Tm0.2Co5.2的居里温度分别为957和965 K;在测试外加场为7 T的条件下,300 K时Sm Co5的各向异性场HA和饱和磁化强度M7T均高于Sm0.8Tm0.2Co5.2;当温度升高至473 K,Sm Co5的HA和M7T要低于Sm0.8Tm0.2Co5.2,说明Sm Co5中进行Tm元素掺杂可以有效的改善其在高温条件下的磁性能。     

Dy对Pr2Fe17合金微波吸收特性的影响

采用电弧熔炼及高能球磨工艺制备出 DyxPr2-xFe17 (x =0.0, 0.1, 0.2, 0.3, 0.4) 合金微粉,借助XRD、SEM、振动样品磁强计和网络矢量分析仪等仪器分别对合金微粉的结构、形貌、磁性能及其微波吸收性能进行了研究。研究发现, 随着Dy含量的增加,DyxPr2-xFe17微粉的饱和磁化强度降低。DyxPr2-xFe17合金的最小反射峰频率随Dy含量的增加往高频方向移动,最小反射损耗呈先增大后减小的变化趋势;其中Dy0.3Pr1.7Fe17合金具有最好的吸波效果,在最佳匹配厚度2.5 mm下,Dy0.3Pr1.7Fe17合金的最小反射损耗在5.04 GHz处达到-42.38 dB左右,反射损耗小于-10 dB的频带宽度达到了1.20 GHz。     

Dy元素对纳米复合(Nd,Pr)_(10.5-x)Dy_xFe_(83.5)B_6合金磁性能与显微结构的影响（英文）EI北大核心CSCD

采用快淬法制备了镨基(Nd,Pr)10.5-x Dyx Fe83.5B6(x=0.0,0.5,1.0,1.5,2.0,2.5)系列粘结磁体,研究了Dy元素添加对快淬合金显微组织结构、磁性能及快淬薄带热稳定性的影响。与Nd2Fe14B相比,硬磁相Dy2Fe14B具有较高的磁晶各向异性场HA和较低的饱和磁极化强度Js,因此,Dy元素添加能显著提高合金的内禀矫顽力Hcj,但会降低合金的剩磁Br。Dy元素替代Nd/Pr元素,增强了快淬薄带的热稳定性,提高了晶化退火温度。较高的晶化退火温度,使快淬薄带中已经形成的微晶更容易长大,形成一些粗大晶粒,降低了粘结磁体的磁性能。1.0%是较佳的Dy元素添加量,(Nd,Pr)9.5Dy1Fe83.5B6合金快淬粘结磁体的最大磁能积(BH)max为71.6 k J/m3,剩磁Br为0.638 T,内禀矫顽力Hcj为611 k A/m。