Fe基非晶态合金的低温电阻研究

本文报道Fe_100-xB_x,Fe_87-xSi_xB₁₃,(Fe_1-xCo_x)₇₈Si_9.5B_12.5,(Fe_1-xM_x)_80-84B_16-20(M=Zr,V,Nb,Ta,Cr,Mo,W,Mn)非晶态合金的 关键词：     

非晶态合金Fe83B17和Ni64B36结构的研究

本文叙述了用偏振中子衍射方法对Fe₈₃B₁₇非晶合金和中子衍射方法对Ni₆₄B₃₆非晶合金的结构研究。由实验数据计算了每种合金的偏干涉函数(PSF)S_ij(Q),和偏简约径向分布函数G_ij(r)。并得到原子短程结构上的各项参数。在此基础上,讨论了这一类非晶态合金的结构模型,计算了其一种模型简单单元的中子衍射散射强度,并和实验所得的结果作了比较。 关键词：     

多晶硼和含硼金属玻璃的表面广延能量损失精细结构研究

本文用反射型芯能级电子能量损失谱的广延部分,即所谓广延能量损失精细结构,研究了硼原子在多晶硼、非晶Fe₈₀B₂₀和Fe_78.5Si₅B_16.5样品表面的行为和这些样品表面的微观结构。测得的谱显示的振荡结构在硼k壳层吸收边以上延续约300电子伏。利用我们实验室发展的计算程序,对所测得的广延能量损失精细结构(SEELFS)谱进行数据分析,得到了被测样品受激原子附近的径向分布函数(RDF);经相移修正后 关键词：     

中子辐照对Pd80Si20与Pd77.5Cu6Si16.5非晶态合金结构的影响

本工作用X射线衍射技术示差扫描量热法(DSC)和内耗测量等手段研究金属-类金属非晶态合金Pd₈₀Si₂₀和Pd_77.5Cu₆Si_16.5中子辐照前后的微观结构变化。结果表明,辐照在两种样品的对关联函数g(r)以及径向分布函数RDF(r)上都引起明显的变化;辐照后样品的晶化温度和晶化热有所提高,结构变得更加无序,Pd₈₀Si₂₀非晶态合金的内耗在T关键词：     

尺寸效应对非晶态TM100-xMx合金结构的影响

本文通过对非晶态合金结构的计算机模拟,研究非晶态TM_100-xM_x合金在成分基本相同条件下,M原子与TM原子尺寸比的变化对合金结构的影响。为此,分别模拟了Fe₈₀P₂₀,Co₈₁P₁₉和Fe₈₀B₂₀等非晶态合金的结构,并从径向分布函数、拓扑短程序、结构的稳定性和电子迁移引起的原子尺寸变化等方面讨论了原子尺寸的变化对非晶态合金结构的 关键词：     

用X射线异常色散效应测定二元非晶合金Fe82B18偏径向分布函数方法的简化

本文采用Mo,Cu,Co三种不同波长的X射线辐射,测定了Fe₈₂B₁₈二元非晶合金的径向分布函数。比较了不同波长辐射对测定径向分布函数的影响。应用X射线异常色散方法计算了Fe₈₂B₁₈二元非晶合金的偏径向分布函数。在计算时略去了B-B原子对对径向分布函数的贡献,因而简化了计算过程,并相对提高了计算精度。所得结果与国际上使用同类方法或其它方法的结果相近。 关键词：     

二元非晶态合金结构模型化的Rt判据

类金属原子的相对分布是过渡金属-类金属(TM-M)型非晶态合金结构中化学短程序的一个重要特征。本文根据这一思想定义了一个新的制作此类非晶态合金结构模型的判据,并使用此判据制作了几个组分和成分都各不相同的结构模型,分别模拟Ni₆₄B₃₆,Fe₈₀B₂₀,Ni₈₁B₁₉和Co₈₁P₁₉非晶态合金的结构。所得的各部分径向分布函数G_ij(r)都与实验相符。将这些结果与前人的工作作了比较,并进行了讨论。 关键词：     

几种金属玻璃结构的X射线研究

本工作用X射线散射技术研究了金属一类金属玻璃合金Pd₇₇Si_16.5Ag_6.59,Co_42.9Ni_27.3Fe_7.8Si₈B₁₄和Co_50.7Ni_19.5Fe_7.8Si₆B₁₆的结构。求出了它们的干涉函数I(s)和原子径向分布函数RDF(r),并由此获得了有关结构信息的原子平均距离、最近邻配位数和短程有序畴半径。此外,对这些合金的RDF(r)第一峰作了高斯分布拟合,求得了比较好的拟合方程,并用近似方法估算了其中金属-金属原子间的配位数。 关键词：     

局部塑性变形下铁基金属玻璃的致密化和非均匀性增强

本文研究了经局部塑性变形后, Fe₇₈Si₉B₁₃金属玻璃在原子尺度上的结构演变及其对合金显微硬度的影响.借助砂纸作为传力的媒介,充分放大了作用于带材表面上的等效压力,发生塑性变形后合金表面产生了大量的剪切带.基于倒空间和实空间的同步辐射X射线衍射分析,在塑性变形后,合金结构的致密度增大,过剩自由体积被排出,并由此揭示了Fe₇₈Si₉B₁₃金属玻璃在短程及中程尺度上原子协同重排行为.结合高分辨透射电子显微镜观察的结果, Fe₇₈Si₉B₁₃金属玻璃在发生塑性变形后,结构不均匀的程度将会加剧.此外,不同于单轴加载下金属玻璃的加工软化, Fe₇₈Si₉B₁₃金属玻璃在发生局部塑性变形后,维氏硬度增大,表现出局部的加工硬化行为.从自由体积的角度看,合金表面的大量剪切带可能是由于剪切带影响区域的重叠和交叉发生相互作用,并加速原子迁移,...     

铁基非晶合金磁致伸缩的温度效应

本文研究了Fe_80-xCu_xSi₅B₁₅,(Fe_1-xCo_x)₈₂Cu_0.4Si_4.4B_13.2两系列非晶合金的磁致伸缩系数λ₄随温度T的变化关系,温度范围分别为室温至非晶态居里点和室温至晶在居里点。分析了Fe基非晶合金随温度变化所产生的结构变化,并讨论了其磁致伸缩的单离子微观机制。 关键词：     

Study of local environment of Cu atoms in Fe73.5Cu1Nb3Si13.5B9 alloy with different annealing temperature

The local environment of Cu atoms in Fe73.5Cu1Nb3Si13.5B9 alloy was investigated by extended X-ray absorption fine structure(EXAFS).Cu clusters began to order when the annealing temperature was around 733 K from the results of the Fourier transform curves.The fitting results showed that the first shell of the near fcc(face-centered cubic)Cu clusters only contained Cu atoms.The coordination number increased with the annealing temperature.Subsequently,the occupancy rate increased from 33.3%(annealed at 733 K)to 100% (annealed at 853 K).This local structural change of Cu atoms could probably affect the distribution of the bcc(body-centered cubic)α-Fe in Fe73.5Cu1Nb3Si13.5B9 alloy.     

EXAFS measurements on FeB metallic glasses: Asymmetry of the radial distribution function

The EXAFS structure measured above the K-edge of Fe in the disordered Fe₈₀B₂₀ alloy is reported. Complete agreement is obtained with X-ray diffraction results in the position of the first neighbours coordination shell when the asymmetry of the Radial Distribution Function (R.D.F.) into the EXAFS formula is included. A Finney-like R.D.F. is used to describe the pair distribution of these metallic glasses. The weak temperature dependence of the spectra is discussed in terms of the structural properties of these amorphous alloys.     

原子团Fe4B的电子结构

利用多重散射X_α自洽场法,对取为四面体的原子团Fe₄B的电子结构进行计算,分析、对比原子团Fe₄与Fe₄B的能级分布、轨道等高线图和态密度的分布,讨论B原子加入对原子团Fe₄B的电子结构的影响,并结合讨论了非晶态Fe₈₀B₂₀等合金的一些性质。 关键词：     

Predicting macroscopic thermal expansion of metastable liquid metals with only one thousand atoms

Results of thermal expansion prediction from atomic scale for metastable liquid metals are reported herein. Three pure liquid metals Ni, Fe, and Cu together with ternary Ni₆₀Fe₂₀Cu₂₀ alloy are used as models. The pair distribution functions were employed to monitor the atomic structure. This indicates that the simulated systems are ordered in atomic short range and disordered in long range. The thermal expansion coefficient was computed as functions of temperature and atom cutoff radius, which tends to maintain a constant when the cutoff radius increases to approximately 15 Å. In such a case, slightly more than 1000 atoms are required for liquid Ni, Cu, Fe and Ni₆₀Fe₂₀Cu₂₀ alloy, that is, the macroscopic thermal expansion can be predicted from the volume change of such a tiny cell. Furthermore, the expansion behaviors of the three types of atoms in liquid Ni₆₀Fe₂₀Cu₂₀ alloy are revealed by the calculated partial expansion coefficient. This provides a fundamental method to predict the macroscopic thermal expansion from the atomic scale for liquid alloys, especially in the undercooled regime.     

57Fe Mössbauer study of amorphous Fe81B13.5Si3.5C2

The amorphous ferromagnet Fe₈₁B_13.5Si_3.5C₂ (Metglas^® 2605SC) has been investigated with Mössbauer spectroscopy. The hyperfine interaction parameters are studied between 80 and 300 K from which some characteristic properties are deduced. The behaviour of the amorphous alloy at higher temperatures has been studied by the room temperature spectra of annealed samples. After a structural relaxation process, a two step crystallization transformation is observed leading to Fe-Si alloy and Fe₂(B, C). X-ray diffraction of samples annealed at higher temperatures reveals the presence of an orthorhombic Fe-B-Si phase of which the structure changes slightly with annealing temperature.     

Kinetics of the apparent isothermal and non-isothermal crystallization of the α-Fe phase within the amorphous Fe81B13Si4C2 alloy

Kinetics of the apparent isothermal and the non-isothermal crystallization of α-Fe phase within the amorphous Fe₈₁B₁₃Si₄C₂ alloy were investigated by an X-ray diffraction (XRD) and by a differential scanning calorimetry (DSC). It was established that the apparent isothermal crystallization of α-Fe phase within amorphous Fe₈₁B₁₃Si₄C₂ alloy could be described by the Johnson-Mehl-Avrami (JMA) kinetic model (with parameter n_iso=4.0). The apparent isothermal crystallization process includes a constant rate of nucleation and three-dimensional growth of nuclei. The results of X-ray diffraction (XRD) data of the isothermally crystallized samples confirmed the above established kinetic model. From the kinetic analysis of the non-isothermal crystallization of the α-Fe phase within this amorphous alloy, it was concluded that the autocatalytic two-parameter Šesták-Berggren (SB) reaction model (with kinetic exponents M=0.72 and N=1.02) describes well the studied process under the given conditions. The non-isothermal crystallization process involves the constant nucleation rate of stable nuclei with additional secondary two-dimensional (surface) nucleation and overlapping of the growing nuclei on account of the non-isothermal activation.     

Fe80B20,Fe80Si6B14金属玻璃中近邻原子间的相互作用

用转靶X射线源及弯晶EXAFS谱仪测定了Fe₈₀B₂₀及Fe₈₀Si₆B₁₄金属玻璃中铁的X射线K吸收谱。由EXAFS谱确定了两种金属玻璃的近邻结构参量。此外,通过测定XANES谱并与纯铁及其有关的化合物Fe₂B,FeB中铁的XANES比较发现:吸收边能量、“白线”结构等均出现一些变化,表明两种金属玻璃的近邻原子Fe-B,Fe-Si以及Fe-Fe之间的相互作用比铁与硼所形成的稳定化合物中要强,这对于决定金属玻璃的短程序结构具有重要的作用。 关键词：