Al86-xFe14+x准晶相合金的M?ssbauer谱

本文研究了Al_86-xFe_14+x(x=0,2,4,6,8.5)准晶相合金的M?ssbauer谱,结果表明对x=0的Al₈₆Fe₁₄合金中以decagonal准晶相为主,谱拟合结果为两套面积积分比为1.69,近于黄金分割的亚谱组成,支持了准晶相为两种“Penrose”多面体组成的观点。当x增加时,出现的晶态含量增加;x=8.5时,几乎全部为晶态Al₃Fe相。 关键词：     

穆斯保尔(Mssbauer)效应

(一) 穆斯保尔效应是近年来核物理实驗工作中一項异軍突起似的发現。这一效应已被应用到物理学各部門的基本研究,成为一种重要的新的測試方法,同时在时間标准或頻率标准的技术上如能利用这一效应也将发展到空前未有的水平。这类工作无需直接使用加速器或反应堆等巨型装置,在获得供应适当的放射性同位素的条件下,完全可能在小型实驗室中进行。本文将对这一效应的实貭及其应用作一簡单的介     

非晶Nd_3Fe_(81)B_(16)合金的晶化及其对磁性和Mssbauer谱的影响

本文报道利用单辊方法制备的非晶Nd_3Fe_(81)B_(16)合金的晶化及其对磁性和Mossbauer谱的影响。发现在非晶Fe_(81)B_(19)合金中用3at％Nd取代B,使非晶Fe_(81)B_(19)合金的晶化温度提高88℃。在适当的退火条件下晶化后样品在室温下的磁性是:σ_2=189emu/g,σ_r/σ_5=0.7,_iH_c=2.15kOe,B_r≈12kG,_bH_c=2kOe,(BH)_(max)≈8MGOe。与目前广泛使用的六角铁氧体相比,_bH_c相近,但B_r和(BH)_(max)远比六角铁氧体高。这种材料仅含有少量的Nd,因此可能开发为一种新的廉价永磁材料。本文对少量Nd的添加对非晶FeB合金的晶化温度,磁性和Mossbauer谱的影响进行了讨论。初步探讨了高矫顽力的来源,认为它的磁化和反磁化过程可以用畴壁钉扎理论解释。     

Mssbauer studies on the shape effect of Fe_(84.94)Si_(9.68)Al_(5.38) particles on their microwave permeability

Ball milling for long time (such as 10, 20, and 30 h) can transform Fe 84.94 Si 9.68 Al 5.38 alloy powders with irregular shapes into flakes. X-ray diffraction (XRD) and Mssbauer measurements have proven that the unmilled particles and the flakes obtained by milling for 10 h have the same D0 3 -type superlattice structure. The flakes obtained by milling for 20 h and 30 h have the same disorder α-Fe(Si, Al) structure. There are more than 6 absorption peaks in the transmission Mssbauer spectra (TMSs) for the particles with D0 3 -type superlattice structure, which can be fitted with 5 sextets representing 5 different Fe-site environments. However, only 6 TMS absorption peaks have been found for particles with a disorder α-Fe(Si, Al) structure, which can be fitted with the distributions of Mssbauer parameters (Bhf, isomer shift). The TMS results show that the flaky particles have a stronger tendency to possess the planar magnetic anisotropy. As the result, the flakes have larger microwave permeability values than particles with irregular shapes. The conversion electron Mssbauer spectra (CEMSs) also show the significantly different Fe-sites environments between the alloy surface and the inside.     

Mssbauer谱线的热致宽

本文研究了晶体点阵热运动涨落对于Mssbauer谱线宽度的影响——加宽谱线(称热致宽)。定量地讨论了完整晶体和杂质原子Mssbauer谱线的这种致宽,并以各向同性三维谐振子为例,对退化情形作了特别讨论。最后还讨论了一个具体例子——单原子立方晶体结点上杂质原子Mssbauer谱线的热致宽。     

机械合金化Fe-B合金的Mssbauer谱研究

用Mossbauer谱分析方法研究了配料原子比为Fe_(70)B_(30),Fe_(55)B_(45)和Fe_(30)B_(70)各样品经机械合金化所形成的合金相的结构特点及其非晶相在退火过程中的转变。揭示出此类非晶相与相应的Fe-B化合物之间存在一定程度的联系。     

La_(2/3)Ca_(1/3)Mn_(1-x)Fe_xO_3化合物铁掺杂效应的Mssbauer谱研究

利用固相反应方法制备了名义成分为La2 / 3Ca1 / 3Mn1 -xFexO3(0 .0 1≤x≤ 0 .2 0 )的一系列样品 .在整个掺杂范围内晶体结构没有明显变化 .在室温下测量了各样品的M ssbauer谱 ,拟合结果表明 +3价高自旋态的铁离子占据锰的八面体晶位 ,随Fe掺杂量的增加 ,铁离子的 3d电子出现局域化趋势 ,并伴随Fe O配位体畸变程度的增强 .本文对此进行了讨论 .     

La_xBa_(1-x)Fe_(12-x)Zn_xO_(19)铁氧体磁性与穆斯堡尔谱的研究

采用草酸盐共沉淀工艺制备了La_xBa_(1-x)Fe_(12-x)Zn_xO_(19)六角铁氧体,当x<0.8时生成磁铅石型六角铁氧体,随x值增大,比磁化强度σ值增加,居里温度下降,磁晶各向导性降低,由穆斯堡尔谱分析推断锌离子从尤过于4f_2晶位。     

急冷Al_(80)Mn_(20)合金准晶T相的晶化动力学

本文研究了急冷Al_(80)Mn_(20)合金准晶T相的晶化过程。DSC实验证实在晶化过程中激活能保持不变,从而得到了晶化转变机理实验曲线,并确定了晶化激活能和频率因子的数值,它们分别为224kJ/mol和1.2×10~(12)s~(-1)。分析结果表明准晶T相的晶化是由长程扩散所控制的,并在晶化过程中没有显著的新核形成。     

Y_2(Fe_(1-x)Si_x)_(14)B的中子衍射研究

Nd_2Fe_(14)B是一种磁能积很高的优良的永磁材料,但在实用上稍嫌它的居里温度低了一点。为了提高它的居里温度,人们曾用某些元素替代其中的一些铁作了尝试。文献[9]及我们最近的实验表明:用硅代替部分铁之后,材料的居里点都获得了提高。本文用中子衍射法研究了Si在Y_2Fe_(14)B中的占位情况,以了解Si对磁性能产生的影响。中子衍射的结果表明:Si择优地占据c,j_1及k_2晶位。最后,用磁交换作用对结果进行了讨论。     

Mössbauer study of intergranular phase in Nd 8 Fe86 − x Nb x B6(x = 0, 1, 2, 3) nanocomposite magnet

Nd₈Fe_86???x Nb _x B₆ (x = 0, 1, 2, 3) nanocomposite magnet has been studied by Mössbauer spectroscopy and nanostructure observation. It was found that intergranular phase formed between α-Fe and Nd₂Fe₁₄B phase in NdFeNbB alloys plays a significant role on the magnetic properties. By the addition of Nb into Nd₈Fe₈₆B₆ composition, coercivity was found to increase by 25% due to the grain refinement of both the soft and hard magnetic phases which was decreased from 50 nm of virgin Nd₈Fe₈₆B₆ to 25 nm in Nd₈Fe₈₅Nb₁B₆ alloys. The role of Nb addition was confirmed to stabilize the Nd₂Fe₁₄B lattice preventing from thermal vibration of the corresponding sites at where Fe atoms are substituted by Nb in the Nd₂Fe₁₄B lattice. The enhanced coercivity was originated from the exchange hardening of soft and amorphous phases surrounding the hard magnetic Nd₂Fe₁₄B crystal.     

非晶态Fe_(90-x)B_xZr_(10)合金的磁性、电性和晶化

本文研究了部分B元素替代Fe对非晶态FeZr基合金磁性、电性和晶化的影响,并与非晶态FeB合金作了比较。解释了样品中每个FeZr原子的平均磁矩μ_(FeZr)和居里温度T_C随B含量x的增加而增加的原因,讨论了在不同的温区样品中可能存在的散射机制对电阻率的贡献以及影响晶化温度的因素。     

A structural, magnetostrictive and Mssbauer study of Tb_(0.3)Dy_(0.7)(Fe_(0.9)T_(0.1))_(1.95) alloys

The pseudobinary rare-earth iron alloys Tb0.3Dy0.7Fe2 (commercially known as Ter- fenol-D) is an excellent magnetostrictive material and has relatively low magnetocrys- talline anisotropy[1], which can be used as ultrasonic transducers and micro-actuators. However, its application is limited because of its low tolerance to tensile and shear forces, low electrical resistivity, and higher saturation field. At present considerable re- search works have been done on substituting Fe with other el…     

A study of magnetostriction,spin reorientation,and Mssbauer spectra of Tb_(0.3)Dy_(0.6)Pr_(0.1)(Fe_(1-x)Al_x)1.95 alloys with substitution of Fe by Al

The effects of Al substitution for Fe on the structure, magnetics, magnetostriction, anisotropy and spin reorientation of a series of Tb0.3Dy0.6Pr0.1(Fe1-xAlx)1.95 alloys (x=0.05, 0.1, 0.15, 0.2, 0.25, 0.3) at room temperature have been investigated. The alloys of Tb0.3Dy0.6Pr0.1(Fe1-xAlx)1.95 substantially retain MgCu2-type C-15 cubic Laves phase structure when x0.2. The mixed phases appear with x = 0.2, and cubic Laves phase decreases with increasing x. The magnetostriction of the Tb0.3Dy0.6Pr0.1(Fe1-xAlx)1.95 alloys decreases drastically with increasing x and the giant magnetostrictive effect disappears for x 0.15. Fortunately, a small amount of Al substitution is beneficial to a decrease in the magnetocrystalline anisotropy. The spin reorientation temperature decreases with increasing x. The analysis of the Mssbauer spectra indicates that the easy magnetization direction in the {110} plane deviates slightly from the main axis of symmetry with the increase of Al concentration x, namely, spin reorientation, resulting in the change of macroscopical magnetic properties and magnetostriction. The hyperfine field decreases, but the isomer shifts increases with Al concentration increasing and the quadruple splitting QS shows a weak concentration dependence.     

Structural,M?ssbauer spectroscopy,magnetic properties,and thermal measurements of Y(3-x)Dy_x Fe_5O_(12)

Yttrium iron garnet powder samples((3-x)Dy_x Fe_5O_(12)), where part of yttrium ions are substituted by dysprosium ions with different concentrations are prepared by the solid state reaction method. The properties of the prepared samples are examined by different methods such as x-ray diffraction(XRD), Mssbauer spectroscopy, macroscopic magnetization measurements, and thermal measurements. The XRD measurements show that all the samples reveal the presence of a single garnet phase with a BCC structure. Room temperature Mssbauer spectra indicate that iron ions occupy three magnetic sites, i.e., two octahedral sites and one tetrahedral site. The saturation magnetization and the initial magnetic susceptibility decrease with the increase of Dy~(3+) substitution. The Curie temperature obtained from the thermal measurements seems to be independent of Dy~(3+) substitution.     

Fe/Pd金属超晶格的磁性和内转换电Mssbauer谱研究

利用真空双源蒸镀法成功地制备了Fe/Pd金属超晶格,并对其结构和磁性进行研究。发现其比饱和磁化强度在固定Pd层30不变时,随Fe层厚度减小而单调上升,这是界面处Fe对Pd的极化效应造成的,且得出0K下极化效应的等效Fe层厚度约为10;低温下σ-T关系满足Bloch的T~(3/2)定律,自旋波劲度系数随Fe层厚度减小而单调增大;居里温度则单调下降。~57Fe内转换电子Mssbauer谱(CEMS)的测量进一步证实极化效应的存在,而界面处Fe原子不存在磁性增强,也不存在“死层”效应。     

Tellurium-125 Mössbauer spectroscopy study of molybdenum metal tellurides of composition Mo6−x M x Te8 (M=Ru,Rh)

Tellurium-125 Mössbauer spectra have been recorded from some recently reported superconducting compounds Mo_6?x Ru _x Te₈ (x=0, 0.5, 1.0, 1.5) and Mo_5.5Rh_0.5Te₈. The spectra are characterised by single lines which probably contain contributions from the crystallographically dissimilar tellurium sites in these compounds. The trends in the linewidth and chemical isomer shift data are consistent with the enhanced polarisation of tellurium 5p electrons with increasing ruthenium content in the compounds. The results can be related to the nature of chemical bonding in the cluster of metal atoms.     

Mössbauer study of amorphous (Fe1−x Ga x )84B16

Using the⁵⁷Fe Mössbauer effect the influence of the Ga content in amorphous (Fe_1?x Ga _x )₈₄B₁₆ on the average hyperfine fields \(\bar H\) and isomer shift has been studied. For the sample (Fe_0.98Ga_0.02)₈₄B₁₆ the \(\bar H\) , as well as the recoilless fraction,f _a were measured as functions of temperature ranging from 12 K to 300 K. The experimental results show a linear correlation between Inf _a and δ, and well as between δ andx. In the temperature range \(\bar H(T)\) can be described by the Brillouin function and the second-order Doppler shift is appreciable. The characteristic temperature for such an amorphous alloy is 372 K. the effective vibrating massM _eff=79 a.u.     

高压下非晶Fe_(82)Si_4B_(14)合金的晶化

研究高压对非晶Fe_(82)Si_4B_(14)合金晶化过程的影响,给出常压下与77kbar下的时间-温度-变态图(即T-T-T图)。结果表明:合金晶化温度的压力梯度值随晶化进行的时间长短而改变。常压下晶化时,bcc-Fe(Si)固溶体相先形成;77kbar下晶化时,DOe型Fe_3B与bcc-Fe(Si)固溶体相同时出现。     

Fe_(20)Al_(80)非晶态粉末的晶化特征和穆斯堡尔效应

Fe_(20)Al_(80)非晶态粉末是通过180球磨而制备的。X射线衍射和透射电子显微镜实验不但证实它的非晶性,而且给出它的平均颗粒度大小和晶化产物。穆斯堡尔谱测量确定了该非晶态粉末的顺磁性和晶化度。