Nd(Fe_(1-x)Co_x)_(10)V_2的Mssbauer谱

通过X射线衍射、磁测量和M ssbauer谱等测试方法研究了Nd(Fe1-xCox) 10 V2 的结构和磁性。结果表明 :Nd(Fe1-xCox) 10 V2 (x =0 ,0 .0 5 ,0 .1,0 .15 ,0 .2 )化合物的晶体结构均为ThMn12 型结构 ;随着Co含量增大 ,晶格常数将单调减少 ,居里温度Tc 呈单调增大 ,饱和磁化强度Ms 逐渐增加。Co部分取代Nd(Fe1-xCox) 10 V2 中的Fe原子 ,将择优占据 8i铁晶位。     

Nd（Fe1—xCox）10V2的Moessbauer谱

通过X射线衍射，磁测量和Noessbauer谱等测试方法研究了Nd(Fe1-xCox)10V2的结构和磁性。结果表明：Nd(Fe1-xCox)10V2(x=0,0.05,0.1,0.15,0.2)化合物的晶体结构均为ThMn12型结构；随着Co 含量增大，晶格常数将单调减少，居里温度Tc呈单调增大，饱和磁化强度Ms逐渐增加。Co部分取代Nd(Fe1-xCox)10V2中的Fe原子，将择优占据8i铁晶位。     

金属间化物Nd(Fe_(1-x)Co_x)_(10)V_2的磁性能机制

通过X射线衍射.磁测量和M(?)ssbauer谱测定了Nd（Fe1-Cox）10V2的结构和磁性.结果表明,Nd（Fe1-xCox）10V2（x=0,0.05,0.10,0.15,0.20）化合物的晶体结构均为ThMn12型结构;随着 Co含量x的增大,晶格常数将单调减少.Co原子的替代将导致化合物各个Fe晶位上的磁超精细场值Bhf逐渐增加.Co部分取代Nd（Fe1-xCox）10V2中的Fe原子时.将择优占据8i铁晶位.取向样品NdFe10V2的热磁曲线和变温M(?)ssbauer谱研究结果表明.该化合物在T=120K条件下存在自旋重取向现象.     

金属间化物Nd(Fe1-xCox)10V2的磁性能机制

通过X射线衍射，磁测量和Moessbauer谱测定了Nd(Fe1-xCox)10V2的结构和磁性。结果表明：Nd(Fe1-xCox)10V2(x=0,0.05,0.10,0.15,0.20)化合物的晶体结构均为ThMn12型结构；随着Co含量x的增大，晶格常数将单调减少。Co原子的将导致化合物各个Fe晶位上的磁超精细场值Bhf逐渐增加。Co部分取代Nd(Fe1-xCox)10V2中的Fe原子时，将择优占扰8i铁晶位。取向样品NdFe10V2的热磁曲线和变温Moessbauer谱研究结果表明，该化合物在T＝120K条件下存在自旋重取向现象。     

ω相对Ti10V2Fe3Al合金性能的影响

采用透射电镜和金相显微镜等分析方法,研究Ti10V2Fe3Al合金ω相的形成规律和ω相对合金性能的影响.结果表明:当采用双重退火制度时,第一退火温度高于相变点或第二退火温度低于再结晶温度时,有大量ω相析出,此时合金的强度较高,但塑性非常差,无法满足使用要求;同时,在采用单重热处理制度的条件下,当处理温度高于相变点时,随着处理温度的升高,ω相析出迹象越明显,合金的塑性降低.     

（Sm_（1－x）Y_x）_2Fe_（17）N_y的Mossbauer谱研究

通过Ｍｏｓｓｂａｕｅｒ谱等研究（Ｓｍ１－ｘＹｘ）２Ｆｅ（１７）Ｎｙ的磁性。结果表明：Ｓｍ次格子的单轴各向异性较强，对总的各向异性贡献起主导机制；Ｙ原子的择优占位导致晶体结构的变化，而对各向异性的影响较小。     

非晶合金(Fe_(1-x)Co_x)_(86)Hf_7B_6Cu_1(x=0.4~0.6)磁性的EET理论研究

采用熔体单辊急冷法制备了非晶(Fe1-x Co x)86Hf7B6Cu1(x=0.4~0.6)合金,使用穆斯堡尔谱仪、透射电镜(TEM)和振动样品磁强计(VSM)对其进行了表征,穆斯堡尔谱和TEM结果表明所制样品均为非晶态。然后借助于固体与分子经验电子理论(EET理论),计算了非晶(Fe1-x Co x)86Hf7B6Cu1合金的价电子结构和磁矩,磁矩的理论计算值与实验测定值的误差小于10%,满足一级近似要求,实现了从价电子层次上计算非晶(Fe1-x Co x)86Hf7B6Cu1合金的磁矩,这对于优化非晶合金(Fe1-x Co x)86Hf7B6Cu1的软磁性能将具有理论指导意义。     

(Mn1-xFex)5Sn3合金晶体结构和居里温度

用粉末冶金法(磁场压制烧结)制备(Mn1-xFex)5Sn3(x=0.1～0.5)合金,对其晶体结构、居里温度进行研究。室温XRD分析表明,该系列合金均保持Mn5Sn3的InNi2型相结构,计算发现合金的晶格常数随着x量增大而减小。通过M-T曲线测量结果表明:居里温度TC在室温附近244～391K连续可调,且随着Fe含量的增加而提高,居里温度随成分近似呈线性变化;成分为(Mn0.70Fe0.30)5Sn3合金的居里温度为295K,在外加磁场为0～1.5T下,最大磁熵变约为0.87J·(kg·K)-1,是一种成本低廉的室温磁制冷候选材料。     

EFFECTS OF HDDR PROCESS ON STRUCTURE AND MAGNETIC PROPERTIES OF Nd(Fe,Ti)_(12)N_δ PREPARED BY MECHANICAL ALLOYING

1.IntroductionThec0mparableintrinsicmagneticpropertiesofNd(Fe,Ti)12N6withthose0fNd,Fe,'B[1]andthep0ssibility0fpreparingmagnetswithahighc0ercivitybyusingmechanicalall0y-ing(MA)inc0mparis0nwithtraditionalmeth0dsl2'3'4'5]havedrawnextensiveattentioninexploringnewcandidates0frareearthpermanentmagnets(REPM).Especially,thiskindofcompoundhasalowrareearthc0ntent(withoutscarceSm),whichisofbenefittoalow-costproductionofREPM.Ontheotherhand,itiswellknownthatHDDRpreparati0nofREPMcanpr0ducec0ercive…     

Structural and magnetic properties of (Sm_0.5Nd_0.5)_2(Fe_(1-x)Co_x)_(17)compounds

The structure, magnetization, and magnetocrystalline anisotropy were investigated using X-ray diffraction, vibrating sample magnetometer, and AC susceptibility-meter. It is found that the microstructure of (Sm0.5Nd0.5)2(Fe1-xCox)17 alloys is an (Sm,Nd)2(Fe,Co)17 phase with the rhombohedral Th2Zn17-type structure. The Curie temperature Tc increases with the Co concentration increasing, and the magnetization first increases as the Co content increases in (Sm0.5Nd0.5)2(Fe1-xCox)17 alloys and then decreases slowly. The easy magnetization direction (EMD) of (Sm0.5Nd0.5)2(Fe0.25Co0.75)17 is along the c-axis and a strong enhancement of the crystalline anisotropy energy constant K is produced by the addition of some Co atoms. The anisotropy energy constant reaches the maximum when x = 0.75 and then decreases slowly with the Co content further increasing. The (Sm0.5Nd0.5)2(Fe0.25Co0.75)17compound is an optical candidate for the new permanent magnet, which possesses a high magnetization, a high Curie temperature,     

(Fe_(1-x)Co_x)_(80)Zr_(10)B_(10)(x=0,0.1,0.2,0.3)合金的热性能、结构和磁性能研究

采用单辊快淬法制备(Fe1-x Cox)80Zr10B10(x=0,0.1,0.2,0.3)非晶合金,并对4种合金在不同温度下进行等温热处理。利用差热分析仪(DTA),X射线衍射仪(XRD),透射电镜(TEM)和振动样品磁强计(VSM)等测试手段对样品的热性能、微观结构及磁性能进行研究。结果表明,未添加Co元素的Fe80Zr10B10合金的热稳定性明显高于添加Co元素的合金,而(Fe1-x Cox)80Zr10B10(x=0.1,0.2,0.3)合金的热稳定性相差不大。Fe80Zr10B10和Fe72Co8Zr10B10合金的晶化过程相似;Fe64Co16Zr10B10和Fe56Co24Zr10B10合金的晶化过程相似。4种合金的矫顽力(Hc)呈现先上升后下降的趋势,在873 K达到最大值。     

Chemical bond properties and M(?)ssbauer spectroscopy in (La_(1-x)M_x)_2CuO_4(M=Ba,Sr)

By using the average band-gap model, the chemical bond properties of (La1-xMx)2CuO4(M=Ba, Sr) were calcu-lated . The calculated covalencies for Cu-O and La-O bond in the compounds are 0.3 and 0.03 respectively. Mossbauerisomer shifts of 57Fe doped in La2CuO4 and 119Sn doped in La2CuO4 were calculated by using the chemical surroundingfactor defined by covalency and electronic polarizability. Four valence state tin and three valence iron sites were identifiedin 57Fe and 119Sn doped La2CuO4.     

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.     

球磨制备的La(Fe1-xCox)11.2Si1.8化合物的相形成和磁热效应

将LaSi母合金和元素粉末混合,利用球磨工艺制备了La(Fe1-xCox)11.2Si1.8 (x = 0, 0.02, 0.04, 0.06)样品。在1423K的温度下烧结30分钟,然后放入水中快速冷却,就可以获得几乎为NaZn13型结构的单相化合物。磁性质的研究表明,样品的居里温度随着Co含量从x=0到x=0.06而提高,但是磁熵变减小。在0-1.5T的外加磁场下,LaFe11.2Si1.8合金在其居里温度附近的最大磁熵变达到的6.5 J/kg,而x=0.06的样品的最大磁熵变约为2.1 J/kg K。另外,球磨制备的样品还呈现了二级磁相变的特点,这对于磁热效应的应用非常有意义。     

纳米晶复合Nd10Fe80-xNbxB10(x=0~6)永磁合金的磁性能

采用熔体快淬法制备成分为Nd10Fe80-xNbxB10(x=0～6)的非晶条带,退火处理后得到纳米晶复合永磁合金。利用振动样品磁强计(VSM)分析该合金系的磁性能和软、硬磁性相间的交换耦合作用。结果表明,适量的Nb元素的添加可以使软、硬磁性相的晶粒细化,从而有效地增强合金中软、硬磁性相间的交换耦合作用,进而提高合金的综合磁性能。当Nb含量为4at%时,制得的合金条带具有最佳的综合磁性能:Hcj=936.02kA/m,Br=0.91T,(BH)max=125.86kJ/m3。