氢作用下Nd14Fe73Co6B7的相转变

利用X射线衍射、透射电子显微镜、扫描电镜及磁测量技术观察和分析了Nd_(14)Fe_(73)Co_6B_7合金于770℃吸氢后相结构组成与变化发现铸锭中的Nd_2Fe_(14)B基体吸氢后分解成约为0.1μm的NdH_2,α-Fe和Fe_2B三相混合物,脱氢后重新结合的Nd_2Fe_(14)B相尺寸约为0.3μm;铸锭中分布在基体相周围的富Nd边界相在吸氢时扩散入Nd_2Fe_(14)B基体,在脱氢过程中保留下来,均匀地分布在由若干Nd_2Fe_(14)B细小晶粒组成的晶粒团周围     

PHASE COMPONENT AND CURIE TEMPERATURE OF Nd_4(Fe_(1-x)Cr_x)_(77.5)B_(18.5)ALLOYS

1.IntroductionThenewhard-magneticNdFeBall0yswithlowNdc0ncentration(35at.%)havebeenobtainedbycrystallization0fam0rphous.ibbo.sI1-3].Theirmagneticpr0pertiesatr0omtemperatureareasfollows:coercivityHc=16O-24OkA/m,remanenceB,=1'2-1.25T,andmagneticenergy(BH).ax=64108kJ/m'.ThevaluesofB.and(BH).axaremuchhigherthanth0se0fthewidelyusedanis0tropic(Ba,Sr)Fe12Ol9ferritesandAlNiC0alloys.Inpreyi0uspapers['-'1,wehavereportedthestructuralandmagneticpr0perties.Recentlywestudiedtheinfluenceofthesubstit…     

Temperature Dependence of the Magnetocrystalline Anisotropy in Nd_2Co_(14)B Compound

Easy and hard magnetization curves of Nd_2Co_(14)B compound have been measured withextracting-sample-magnetometer(μ_0H_(max)=6T)at 10～300 K.Magnetic anisotropy constants K_1 and K_2have been determined by fitting the hard magnetization curves,in which only K_1 ,K_2 and misalignment anglehave been taken as fitting parameters.The values of K_1 and K_2 at 4.2 K were derived by extrapolation.Anisotropy coefficients,x_2~° and x_4~°were derived from the anisotropy constants.The anisotropy constant K_2increases rapidly with increasing temperature when TT_(sr).The temperature depen-dence of the magnetic anisotropy coefficient x_2~° was fitted with the formula.The anisotropy coefficients x_2~°can be well described by the tenth-power law from 4.2 K to T_(sr)and by the sixth-power law from T_(sr_ to 300 K.     

溅射Fe82Si6B12非晶合金膜的晶化动力学研究

用动态原位电镜观察方法了直流溅射Ｆｅ８２Ｓｉ６Ｂ１２非晶合金膜的晶化动力学过程，结果表明：溅射Ｆｅ８２ＳｉＢ１２非晶合金膜的晶化类型为初晶晶化。初晶产物为α（Ｆｅ，Ｓｉ），长大以枝晶方式进行，长大方向沿＜１１０＞晶向。α（Ｆｅ，Ｓｉ）初晶形核采取瞬态均匀形枝，晶核初始的形状为圆形的多角形。并很快发展成枝晶，α（Ｆｅ，Ｓｉ）枝晶的长大是由Ｂ原子在非晶合金中的长程扩散控制的。根据长大过程的动力学分析，     

THERMAL DEMAGNETIZATION AND RANDOMNESS OF DOMAIN NUCLEATION OF SINGLE PHASE Nd_2 Fe_(14) B

Based on the observation of temperature variation of both domain structure and magnetic con-trast.the thermal demagnetization and randomness of domain nucleation was discussed.     

超过冷条件下Fe_(83)B_(17)共晶合金的凝固行为及显微组织演化

采用深过冷技术研究了块体Fe_(83)B_(17)共晶合金在超过冷度条件下的凝固行为.该合金的组织演化规律为:当过冷度达到理论临界超过冷度(300K)时,组织为α-Fe相和Fe_2B相组成的共晶组织;当过冷度大于临界值达到386K时,组织粗化,为完全的非规则共晶,稳定相Fe_2B消失,亚稳相Fe_3B出现并且在室温下也不会分解;获得了460K的超过冷度以及亚稳相组织.并讨论了这些结果产生的原因.     

MAGNETIC PROPERTIES AND CRYSTALLIZATION OF RAPIDLY QUENCHED(Fe_(1-x)Ga_x)_(77.5)Nd_4B_(18.5) ALLOYS

The Curie temperature increases but crystallization temperature decreases with the in-crease of Ga content,x,of amorphous(Fe_(1-x)Ga_x)_(77.5)Nd_4B_(18.5) alloys.The averagemagnetic moment of Fe atoms is almost a constant.By X-ray diffraction and ther-momagnetic measurements,the crystalline phases of the alloys,an unknown phase andα-(Fe,Ga)besides Fe_3 B as major one,were identified.The relationship between roomtemperature coercive field and Ga.content was also studied.     

Nd_2(Fe_(0.9)Si_(0.1))_(14)B的中子衍射研究SCIEI

本文用中子衍射对Nd_2(Fe_(0.9)Si_(0.1))_(14)B在室温及77K进行了测量,用衍射峰的形状分析法进行了数据拟合。结果表明,在室温,Si择优占据4c,8j_1及16k_2晶位;Nd与Fe的磁矩平行于C轴排列。在77K,Si仍择优占据上述三个晶位。算得的Nd磁矩的方向偏离C轴37.8°。     

非晶态Fe_（80）B_（20）合金的表观晶化动力学研究

研究了非晶Ｆｅ（８０）Ｂ（２０）合金的表观晶化动力学过程，分析表明，非晶态的Ｆｅ－Ｂ共晶合金在晶化过程中，晶体的生长行为与传统观点所认为的完全由界面控制的机制不同，还同时存在扩散控制机制．     

Fe78B13Si9纳米晶合金的热性能研究

采用适当的热处理工艺将相同成分的Fe_(78)B_(13)Si_9非晶态合金条带晶化制备成纳米晶合金;测定并研究了纳米晶合金的微观结构(晶体结构及尺寸)和一些结构敏感性能(热膨胀、比热),同时,将其与同样成分的非晶态、大晶粒状态合金的性能进行比较分析,认为由于纳米晶合金特殊的微观结构(短程无序),使其在性能上表现出与通常材料有很大差异。     

等温退火过程中Co66Fe4Mo2Si16B12非晶合金磁性及结构的变化

将Co66Fe4Mo2Si16B12非品合金在460℃等温退火30～120min。合金在460℃等温退火过程中，相对起始磁导率μi随退火时间的延长先增大，在t≈45min时达到最大值，然后随着退火时间的延长快速下降。电子衍射花样的结果表明，合金此时仍保持非品态结构．同时发现，合金的饱和磁致伸缩系数λs随退火时间的延长由负值逐渐变为正值，当t＝45min时，λs≈0，由此可知，合金在等温退火过程中相对起始磁导率的峰值与零磁致伸缩系数相对应。     

DIFFUSIVITY OF Al IN AMORPHOUS ALLOY Fe_(78)Si_9B_(13)

Ion beam sputtering profiling in combination with SIMS technique was employed toinvestigate the Al diffusion in Fe_(78)Si_0B_(13)amorphous alloy.Between 320 and 380℃,thediffusion coefficients vary from 2.43×10~(-22) to 2.01×10~(-21)m~2s~(-1),and an Arrheniusrelationship was established as:D_0=2.02×10~_(12)exp(-1.17/kT)     

EFFECT OF PREPARATION CONDITION ON THERMAL EXPANSION ANISOTROPY FOR AMORPHOUS Fe_(78)B_(13)Si_9 ALLOY

The thermal expansion along the longitudinal and transverse directions for amorphousFe_(78)B_(13)Si_9 alloy prepared under various preparing conditions were investigated.The thermalexpansion anisotropy appears in all specimens.The expansion along the longitudinal directionis less than that along the transverse direction.The cooling rate,the melt temperature beforejet casting and the cycling temperature affect the thermal expansion coefficients andanisotropy.The amisotropy of thermal expansion originates from the orientation of atomicinteraction force,the atomic oscillatory frequency and short range order structure or thedirectional arrangement of defects in the alloy.     

制备条件对非晶态Fe78B13Si9合金的热膨胀各向异性的影响

本文研究了不同条件下形成的非易态Fe_(78)B_(13)Si_9合金在长轴和短轴方向上的热膨胀。结果表明,在所有条件下均存在热膨胀的各向异性。热膨胀系数随着冷却速度的增加而增加,但其各向异性减小;随着熔体喷铸温度的提高两者均减小。在热循环的作用下,短轴方向的热膨胀系数及其各向异性均减小;而在长轴方向的热膨胀系数却增大。我们认为热膨胀各向异性来源于原子交互作用力的方向性、原子振动频率和短程有序结构或缺陷的方向性。     

HEAT CAPACITIES OF Fe_（40）Ni_（40）B_（20） GLASSY ALLOY MEASURED BY ENTHALPY METHOD

ＨＥＡＴＣＡＰＡＣＩＴＩＥＳＯＦＦｅ_（４０）Ｎｉ_（４０）Ｂ_（２０）ＧＬＡＳＳＹＡＬＬＯＹＭＥＡＳＵＲＥＤＢＹＥＮＴＨＡＬＰＹＭＥＴＨＯＤ￥ＪＩＡＮＧＱｉｎｇ;ＺＨＡＯＭｉｎｇ;ＬＩＪｉａｎｃｈｅｎ（ＪｉｌｉｎＵｎｉｖｅｒｓｉｔｙｏｆＴｅｃｈｎｏｌ?..     

Co66Fe4Mo2Si16非晶合金的磁性与晶化

Ｃｏ６６Ｆｅ４Ｍｏ２Ｓｉ１６非晶合金在等温退火和等时退火过程中起始磁导率μｉ随退火时间的延长而增大，在ｔ＝４５ｍｉｎ时达到最大值。然后随着退火时间的延长μｉ快速下降，电子衍射图表明合金此时仍保持非晶结构；合金的饱和磁致伸缩系λｓ随退火时间的延长由负值逐渐变为正值，当ｔ＝４５ｍｉｎ时，λｓ≈０，合金在等温退火过程中起台磁导率的峰值主要来源于零磁致伸缩系数。     

THERMAL PROPERTIES OF NANOCRYSTALLINE Fe_78B_13Si_9 ALLOY

A new method was developed for preparing nanocrystalline alloy made of the identi-cal compositional Fe_(78)B_(13)Si_9 amorphous ribbon by suitable isothermal annealing.Itsmicrostructure and some structure-sensitive properties.including thermal expansion,spe-cific heat,etc.,have been studied and measured.Comparative analysis of properties wasalso carried out with amorphous and coarse-grained crystalline alloys of same composi-tion,thus.it is believed that so novel differences in properties from usual materials wouldbe made by the particular microstructure of short range disorder of the nanocrystallinealloy.     

退火变脆Fe75Si10B15金属玻璃的脆韧性转变

研究了机械研磨对退火变脆Fe_(75)Si_(10)B_(15)金属玻璃的弛豫过程,晶化行为及脆韧性转变的影响。发现退火变脆的Fe_(75)Si_(10)B_(15)金属玻璃,经不同时间机械研磨,Curie温度T_C逐渐回落,总的弛像焓ΔH_?逐渐回升。在DSC曲线上观察到明显的玻璃转变温度T_(g_1)和一个附加的宽放热峰T_(x_1),随着研磨时间的增加,T_(x_1),T_(x_1),T_C同步降低,与T_(x_1)对应的放热面积ΔH_(x_1)逐渐增大,并在片状粒子表面形成切变带以及与其对应的剪切带,玻璃在退火过程中失掉的韧性逐渐得到恢复。     

BRITTLE-DUCTILE TRANSITION OF ANNEALEMBRITTLED Fe_(75)Si_(10)B_(15)METALLIC GLASS

Studies were made of the effect of mechanical pulverization on relaxation,crystallizationand brittle-ductile transition of the anneal-embrittled Fe_(75)Si_(10)B_(15) metallic glass rib-bon.Results show that the Curie temperature,T_C,decreases and the total enthalpy ofrelaxation increases gradually with variation of pulverized time.DSC traces reveal anextra exothermic peak,T_X_1,and a distinct glass transition endothermic peak,T_g_1,withincreasing pulverized time,T_C,T_X_1,and T_g_1 decrease simultaneously,and the exother-mic peak area corresponding to T_X_1 increases gradually.The surface slip-steps of flakyparticles and their corresponding shear are produced by pulverizing the pre-embrittledamorphous glass.The lost ductility of the glass may restore during annealing.     

活化非晶Fe80Zr12B8合金的表面状态与催化活性

采用Auger电子能谱(AES),X射线光电子能谱(XPS)及扫描Auger探针(SAM)等分析手段,并结合氩离子轰击剥层对非晶Fe_(80)Zr_(12)B_8合金条带的表层成分分布、元素化学状态及表面形貌进行了研究。实验结果表明:原始条带的贴辊侧和自由侧表面均为一层铁的氧化物覆盖。经活化后,条带两侧表面均发生了组元B的显著富集和氧化,出现了α-Fe微细晶粒,近表层发生了B和Zr的选择氧化,形成了多孔的表面结构,比表面积从原始条带的0.11m~2/g增加到了2.68m~2/g。对原位活化的主要机制进行了分析