Co66Fe4Mo2Si16B12非晶合金的晶化及磁性的研究

本文研究了Ｃｏ６５Ｆｅ４Ｍｏ２Ｓｉ１６Ｂ１２非晶合金在６５３Ｋ￣８１３Ｋ之间的不同温度退火后的晶化及磁性的变化。实验结果表明，随着退火温度升高，试样的初始磁导率明显上升，当Ｔａ＝７５３Ｋ时，合金开始晶化，分析出Ｃｏ２Ｓｉ、Ｃｏ２Ｂ、其磁导率明显降低，但仍具有较高的磁感应强度；当退火温度继续提高，合金中析出的Ｃｏ２Ｓｉ、Ｃｏ２Ｂ、ＣＯ８Ｂ的量增多，同时析出Ｆｃｃ Ｃｏ相，合金的软磁性能变得很差。     

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。     

激波诱导非晶合金Fe78B13Si9的晶化

用ＸＲＤ和ＤＴＡ研究了波对Ｆｅ７８Ｂ１３Ｓｉ９非晶合金的影响。结果表明，一定强度的激波能使非晶态转变为晶态，且其晶粒尺寸在纳米范围内。     

非晶Nd6Fe81B13合金的晶化和磁性

本文研究了非晶Nd_6Fe_(81)B_(13)合金的磁性和晶化及其对样品结构和磁性的影响。讨论了非晶样品的低温磁性和Nd对昌化温度和Curie温度的影响。在873K退火的样品中得到一个新相。     

高密度脉冲电流对Fe—Si—B非晶合金晶化过程的影响

对非晶Ｆｅ７８Ｓｉ９Ｂ１３合金进行了连续高密度超短脉冲电流处理和对应的等温退火处理，用Ｍｏｓｓｂａｕｅｒ谱学技术研究处理后非晶试样的微观结构变化与晶化行为。实验结果表明，脉冲电流处理明显促进非晶合金的晶化，电脉冲对晶化的影响取决于脉冲电流对非晶中原子扩散的激励作用。     

Co72.5Fe1.5Mn4Si5B17非晶合金晶化行为的研究

利用差热分析仪和X射线衍射仪研究了非晶合金Co72．5Fe1．5Mn4Si5B17的晶化行为。结果表明，该非晶合金有两个晶化阶段，第一阶段的起始晶化温度为419．0℃，峰值温度为431．4℃，第二阶段的峰值温度为583．6℃。在430-490℃间退火30min后，析出Co的立方相；在550～600℃之间退火30min，晶化相为Co的立方相、Co3B、Co2B、FeSi2和Mn3CO7。     

非晶态Co90—xCrxZr10合金的磁性和晶化

本文研究了非晶态Co_(90-x)Cr_xZr_(10)(0≤x≤25)合金的磁性,得到样品的Curie温度T_C和每个磁性原子的有效磁矩μ均随Cr含量x的增加近似线性下降,计算出每个Co和Cr原子的平均磁矩分别为μ_(Co)=1.51μ_B和μ_(Cr)=-3.62μ_B低温下的磁化强度与温度的关系符合Bloch的T~(3/2)定律,由此算出的自旋波劲度系数D从x=4时的D=2.788meVnm~2下降到x=20时的D=0.727meVnm~2,相互作用范围从x=4时的2—3个原子减小到x=20时的最近邻原子之间,样品的晶化温度随Cr含量x的增加单调上升,认为与合金的平均外层电子浓度有关,用X射线衍射和热磁测量分析了热处理样品的结晶相。     

弯曲应变下Co66Fe4Cr2Si12B16非晶态合金带应力阻抗效应

对具有负磁致伸缩系数的Co66Fe4Cr2Si12B16非晶合金带在制备态下及经脉冲电流退火下的应力阻抗效应进行了研究.结果表明:长为50 mm的非晶带,在仅5 mm挠度的弯曲应变作用下材料可显示显著的应力阻抗效应,输出电压幅值变化率大于40%.非晶材料经电流密度为35 A/mm2,频率为2 Hz,持续时间为30 s的脉冲电流退火处理后,可改善应力阻抗效应灵敏度.该非晶材料受张应力作用时阻抗减小,受压应力作用时阻抗增大,弯曲应变下的应力阻抗效应可用于制作具有高应变因子的力传感器及新型智能材料.     

化学镀Fe—Mo—W—B非晶态合金的晶化

利用化学镀获得非晶态Ｆｅ－Ｍｏ－Ｗ－Ｂ四元合金镀层。用Ｘ射线衍射方法研究了镀层的结构和晶化过程。结果表明;Ｂ含量在９．８ａｔ％－２７．３ａｔ％范围内镀层为非晶态结构,该区域大于Ｆｅ－Ｂ二元合金镀层,但不如Ｆｅ－Ｍｏ－Ｂ三元合金镀层。观察到两步晶化过程：首先析出的晶化相为α－Ｆｅ,Ｆｅ３Ｂ和（Ｍｏ,Ｗ）２Ｂ;然后在较高温度出现Ｆｅ２Ｂ,（Ｍｏ,Ｗ）Ｂ和Ｆｅ（Ｍｏ,Ｗ）的衍射峰。     

高密度脉冲电流对Fe－Si－B非晶合金晶化过程的影响

对非晶Ｆｅ（７８）Ｓｉ９Ｂ（１３）合金进行了连续高密度超短脉冲电流处理和对应的等温退火处理，用Ｍｏｓｓｂａｕｅｒ谱学技术研究处理后非晶试样的微观结构变化与晶化行为．实验结果表明，脉冲电流处理明显促进非晶合金的晶化，电脉冲对晶化的影响取决于脉冲电流对非晶中原子扩散的激励作用．     

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，     

PREPARATION OF AMORPHOUS Mo_5Si_3 BY MECHANICAL ALLOYING AND THE CRYSTALLIZATION

ＰＲＥＰＡＲＡＴＩＯＮＯＦＡＭＯＲＰＨＯＵＳＭｏ_５Ｓｉ_３ＢＹＭＥＣＨＡＮＩＣＡＬＡＬＬＯＹＩＮＧＡＮＤＴＨＥＣＲＹＳＴＡＬＬＩＺＡＴＩＯＮＬｉＭｉｎｇｗｅｉ；ＴａｎｇＲｅｎｚｈｅｎｇ；ＬｉＷｅｎｘｉａｎ（ＤｅｐａｒｔｍｅｎｔｏｆＭａｔｅｒｉａｌｓＳ...     

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。     

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.     

MAGNETIC PROPERTIES AND CRYSTALLIZATION OF AMORPHOUS ALLOYS Co_(90-x)Cr_xZr_(10)

Curie temperature of amorphous alloys Co_(90-x)Cr_x Zr_(10) decreases linearly with increas-ing x.Average magnetic moment per magnetic atom Co or Cr is 1.51 μB or -3.62 μBrespectively.The temperature dependence of spontaneous magnetization at low temper-atures is in agreement with Bloch's T~(3/2) law.The spin wave stiffness constant decreaseswith increasing x from 4 to 20.The range of interaction is 2—3 atoms for x=4 andnearest neighbour atom for x=20.The crystallization temperature increases mono-tonically with increasing x.It may relate to the average number of outer electrons peratom.The crystalline phase components of heat-treated alloys were analyzed by X-raydiffration and thermomagnetic measurement.     

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)     

CRYSTALLIZATION AND MAGNETIC PROPERTIES OF AMORPHOUS Nd_6Fe_(81)B_(13)ALLOY

The magnetic properties and the crystallization and its influence on the magnetic and struc-tural properties for rapidly quenched amorphous Nd_6Fe_(81)B-(13) alloy have been studied.The lowtemperature magnetic properties,the Curie temperature and the crystallization behavior arediscussed.A small addition(6at.-%)of Nd in amorphous Fe-B alloys increases largely thecrystallization temperature T_x but causes a decrease of the Curie temperature Tc·A newphase was observed in the sample annealed at 873 K.     

Fe_(70)Cr_(18)Mo_2Si_1B_9单辊激冷带中的特殊结晶现象

本文研究了真空下不同转速的Fe_(70)Cr_(18)Mo_2Si_1B_9单辊激冷带的显微组织,并与大气带作了比较。除了常见的均质形核与非均质形核的结晶过程之外,还出现具有强择优取向的自由面表层α-Fe柱状晶以及尺寸达μm级的α-Fe球状晶。可用动量传递模式的单辊带形成理论解释这些现象。早期过冷液态中的预存核是该材料能否形成非晶的控制因素。     

UNUSUAL SOLIDIFICATION MICROSTRUCTURE OF Fe_(70)Cr_(18)Mo_2Si_1B_9 SINGLE-ROLL QUENCHED RIBBON

The solidification microstructure of Fe_(70)Cr_(18)Mo_2Si_1B_9 single-roll quenched ribbons with dif-ferent rotating speed of roller and under different atmosphere conditions was investigated.Apart from usual crystallization by homogeneous and heterogeneous nucleation,it was foundthat α-iron cohnnnar grains with strong preferred orientation formed beneath free surface andthat spheres of α-iron single coastal with a size of several μm up to 20μm,which have rarelybeen reported,appeared inside the ribbons.There was experirnental evidence suggesting thatclusters of metal atoms formed from fluctuation in early undercooled liquid might play a roleas pre-existed nuclei and,in fact,control the formation of amorphous for this alloy.