非晶Tb/Fe/Dy和Fe/Tb/Fe/Dy纳米多层膜磁性能及超磁致伸缩性能(英文)

研究非晶Tb/Fe/Dy(样品A)和Fe/Tb/Fe/Dy(样品B)纳米多层膜超磁致伸缩性能和磁性能.磁滞回线表明样品A的垂直磁各向异性而样品B有面向磁各向异性,样品B比样品A更好的磁性能.样品B有很好的低场超磁致伸缩性能,在外磁场为0.12T情况下样品B的超磁致伸缩性能是样品A的五倍,即从16ppm变为82ppm.     

稀土超磁致伸缩材料的磁场热处理研究

超磁致伸缩材料是一种先进的能量转换材料,在高新技术和国防军工领域具有重要的应用价值。在概述TbDyFe超磁致伸缩材料的特点及发展现状基础上,重点介绍了<110>取向材料的磁场热处理研究。在实验方面,采用区熔定向凝固技术制备了<110>取向TbDyFe多晶材料,在略高于居里点温度退火时施加磁场,不改变晶体学择优取向和凝固组织,但能调控初始磁畴分布状态,改变服役时的磁矩运动过程,从而改善材料磁致伸缩和力学性能。在模拟研究方面,建立了基于能量最低原理的磁畴旋转模型,模拟了磁热感生各向异性诱导的初始磁矩再取向过程,得到了形成单轴各向异性的临界值;模拟了感生各向异性强弱对磁致伸缩"Jump"效应的影响规律,探讨了磁场热处理对<110>取向晶体磁致伸缩的作用机理。     

应力对非晶超磁致伸缩薄膜形变影响的理论计算

分析材料磁化过程中引起磁致伸缩的机理,考虑应力对磁化过程的影响,通过将应力作用等效为磁场,并假设非晶超磁致伸缩薄膜的低场磁化为可逆过程,根据能量最低原理,建立了磁致伸缩薄膜形变与应力之间的关系,给出了表达式.     

超负磁致伸缩晶体Sm—Fe,Sm—Dy—Fe和Sm—Dy—Fe—Al的研究

本文研究了轻稀土负磁致伸缩ＳｍＦｅｘ（１．４０≤ｘ≤１．９４），ＳｍｘＤｙ１－ｘＦｅｙ（０．８４≤ｘ≤０．９２，１．８０≤ｙ≤１．９０），Ｓｍ０．９０Ｄｙ０．１０（Ｆｅ０．９５Ａｌ０．０５）１．８０晶体的制备，热处理及磁学性能，发现ＳｍＦｅｘ合金的λ－ｘ曲线存在两个峰值，峰值的ｘ点热处理发生的变化有一定的规律性，还比较了热处理前后，Ｓｍ－Ｆｅ、Ｓｍ－Ｄｙ－Ｆｅ和Ｓｍ－Ｄｙ－Ｆｅ－Ａｌ的相组成对性能     

Dy0.6Tb0.3Pr0.1(Fe0.95Mn0.05)x取向晶体的结构与磁致伸缩

采用Ｃｚｏｃｈｒａｌｓｋｉ方法生长了Ｄｙ０．６Ｔｂ０．３Ｐｒ０．１（Ｆｅ０．９５Ｍｎ０．０５）ｘ（１．８５≤ｘ≤１．９５）取向合金。所有合金主相为立方Ｌａｖｅｓ相结构,择优取向不完整择优取向的方向与Ｘ的大小有关。研究了沿着这些样品的生长方向的磁致伸缩性能以及磁致伸缩性能与压力之间的关系。     

Pr0.15Tb0.30Dy0.55Fe1.85-xNix合金的磁性和磁致伸缩研究

用电弧炉熔炼得到Pr0.15Tb0.30 Dy0.55Fe1.85-xNix系列合金.通过X射线对合金进行结构分析,并拟合衍射峰得到晶格常数;样品的居里温度采用交流磁化率测量系统得到;磁化强度、磁致伸缩分别由振动样品磁强计和标准应变测试系统在室温下测量得到.实验表明所有的样品均呈现MgCu2型Laves相结构;随着Ni替代量的增加,样品晶格常数、居里温度和磁化强度呈现下降趋势;磁致伸缩系数亦表现为下降趋势,但在x=0.2、0.3处有所反弹,且x=0.3时样品在低场下的磁致伸缩值略高于无Ni替代的样品.     

Fe及Fe83Ga17和Fe83Ga17Pr0.3合金的微结构与磁致伸缩性能

本研究对比研究了Fe、Fe_(83)Ga_(17)及Fe_(83)Ga_(17)Pr_(0.3)磁致伸缩材料的微结构与磁致伸缩性能。采用真空非自耗电弧炉在氩气保护下熔炼制备了合金样品。采用X射线衍射仪(XRD)和光学显微镜(OM)分析观察了合金样品的晶体结构和显微组织。采用扫描电镜配合能谱仪(SEM/EDS)测定了稀土Pr元素在Fe_(83)Ga_(17)Pr_(0.3)合金中的分布。通过电阻应变法测量了合金的磁致伸缩性能。结果表明:Fe和Fe_(83)Ga_(17)合金均由单一的bcc结构A2相组成,而Fe_(83)Ga_(17)Pr_(0.3)合金由A2主相和少量的富稀土Pr相组成。稀土Pr掺杂使合金中的A2相沿〈100〉晶向择优取向。Fe及Fe_(83)Ga_(17)和Fe_(83)Ga_(17)Pr_(0.3)合金的微观组织分别呈现细长的条状晶、晶粒粗大的等轴晶和晶粒细小的柱状晶。Fe的磁致伸缩系数为负值,而Fe_(83)Ga_(17)和Fe_(83)Ga_(17)Pr_(0.3)合金的磁致伸缩系数均为正值,三种材料的磁致伸缩系数绝对值的排序为FeFe_(83)Ga_(17)Fe_(83)Ga_(17)Pr_(0.3)。     

超磁致伸缩作动器用于振动主动控制中的仿真研究

目前对于太阳和地球引力变化引起的微振动，采用先进的主动控制能达到高精度的隔振要求。主要是推导并建立了超磁致伸缩作动器（GMA：Giant Magnetostriction Actuator）的动力学方程和数学模型，并将其运用到振动主动控制中，采用PID（Proportional-Integral-Differential）反馈控制方法，对双层隔振下层受到激扰的系统进行仿真计算，仿真结果表明它能对微幅低频振动衰减20-50dB，能起到明显的减振效果。     

热处理温度对TbFe2/Fe交换耦合磁致伸缩多层膜的影响

采用直流磁控溅射在20mm×5mm×240μm抛光单晶硅片上制备了TbFe2/Fe磁致伸缩多层膜,主要研究了热处理温度对TbFe2/Fe磁致伸缩多层膜磁致伸缩系数的影响.采用量热分析法(DSC)、XPS以及光杠杆测试法对TbFe2/Fe磁致伸缩多层膜的晶化曲线、成分随深度的变化以及磁致伸缩系数进行了分析与测试.结果表明TbFe2薄膜的起始晶化温度为327℃,晶化温度为372℃;TbFe2/Fe磁致伸缩多层膜的最佳热处理温度为327℃,在此热处理温度下热处理60min,外加磁场1.6×104A/m时,TbFe2/Fe磁致伸缩多层膜磁致伸缩系数可达1.56×10-4.采用XPS分析了一个周期的TbFe2/Fe成分随薄膜深度的变化,未经热处理的薄膜Fe层和TbFe2层之间界面清晰,两层之间有少量的扩散.经327℃热处理60min的薄膜Fe层和TbFe2层界面发生了互扩散,原子数之比也发生了改变.     

磁致伸缩液位变送器在焦油氨水界面检测中的应用

分析原回收工序焦油氨水分离槽界面检测存在的问题,提出用AT100高精度磁致伸缩液位变送器解决现场问题,并介绍其工作原理、性能特点、安装使用以及应用效果。     

Synthesis and characterization of a new organic dihydrogen phosphate-arsenate: [H2(C4H10N2)][H2(As, P)O4]2

Chemical preparation, crystal structure, calorimetric and spectroscopic investigations (IR and RMN) are given for a new non-centrosymmetric organic-cation dihydrogen phosphate-arsenate [H₂(C₄H₁₀N₂)][H₂(As, P)O₄]₂. This compound is triclinic P1 with the following unit-cell parameters: a = 7.082(2) Å, b = 7.796(1) Å, c = 12.05(3) Å, α = 95.37(2)°, β = 98.38(3)°, γ = 62.98(1)°, Z = 2, V = 586.2(1) Å³ and D_x = 1.836 g cm⁻³. The crystal structure has been solved and refined to R = 0.03 using 2328 independent reflections. The structure can be described as infinite (H₂XO)_n chains spreading parallel to the b direction. These chains are themselves interconnected by a set of NH?O hydrogen bonds generated by the organic entities, alternating with the chains. Solid-state ¹³C, ¹⁵N and ³¹P MAS NMR spectroscopies are in agreement with the X-ray structure.     

Syntheses and structures of Ta2(WO2)0.87H0.26(PO4)4 and Ta2(MoO2)(PO4)4

Tantalum hydrogen phosphate, β-TaH(PO₄)₂, has a three-dimensional structure that is stable to remarkably high temperature (∼600 °C) presumably due to the presence of strong hydrogen bonds. Impedance measurements indicate a low conductivity, 2.0 × 10⁻⁶ S/cm at 200 °C in 5% H₂. In further studies aimed at enhancing the conductivity by aliovalent doping, we have investigated systematically the synthesis of compounds in the TaH(PO₄)₂-W₂P₂O₁₁ system at 380 °C. As a result, a new phase, Ta₂(WO₂)_0.87H_0.26(PO₄)₄, was identified and subsequently the molybdenum analog Ta₂(MoO₂)(PO₄)₄ was also prepared. The structures were determined by single crystal X-ray diffraction techniques. The structures of Ta₂(WO₂)_0.87H_0.26(PO₄)₄ and Ta₂(MoO₂)(PO₄)₄ can be formally derived from the structure of β-TaH(PO₄)₂ by the replacement of two P-OH protons with an MO₂²⁺ (M = Mo and W) group together with a change in the orientation of some phosphate tetrahedra.     

Crystal structures of CdTi2O4(OH)2 and LaTiSbO6

The crystal structures of two PbSb₂O₆-type compounds containing titanium, CdTi₂O₄(OH)₂ and LaTiSbO₆ were refined by X-ray powder diffraction data. For both compounds structure refinements with the space group were successful and the R-factors were R_WP = 6.46% and R_P = 4.90% for CdTi₂O₄(OH)₂ and R_WP = 9.55% and R_P = 7.17% for LaTiSbO₆. These crystal structures were the same as that of the typical PbSb₂O₆-type compound in spite of the existence of protons in the interlayer or two different metal ions in the layer.     

Synthesis, crystal structure and infrared study of LiEr(PO3)4

A single-crystal X-ray diffraction analysis has been performed on LiEr(PO₃)₄ prepared by the flux method. The compound crystallizes in the monoclinic system with space group C2/c and cell parameters: a = 16.262(2), b = 7.032(1), c = 9.549(2) Å and β = 125.95(1)°. The crystal structure was refined based on 1272 independent reflections with I > 2σ(I). Final values of the reliability factors were improven considerably: R(F²) = 0.0180 and wR(F²) = 0.0490. The LiEr(PO₃)₄ structure is characterized by infinite chains (PO₃)_n, extending parallel to the b direction. The ErO₈ dodecahedra and LiO₄ tetrahedra alternate on two-fold axes in the middle of four (PO₃)_n chains. The vibrational study by infrared absorption spectroscopy is reported.     

Synthesis and characterization of a new organic dihydrogenomonophosphate [3,5-(CH3O)2C6H3NH3]2(H2PO4)2

Chemical preparation, crystal structure, calorimetric studies and spectroscopic investigation are given for a new organic cation dihydrogenomonophosphate [3,5-(CH₃O)₂C₆H₃NH₃]₂(H₂PO₄)₂. This compound is triclinic with the following unit cell parameters: a=9.030(6) Å, b=16.124(5) Å, c=8.868(3) Å, α=75.04(3)°, β=110.71(4)°, γ=104.61(1)°, Z=4, V=1148.0(1) Å³, Z=2 and ρ_cal.=1.454 g cm⁻³. Crystal structure was solved and refined to R=0.04, 2752 independent reflections. The atomic arrangement can be described as inorganic layers of H₂PO₄⁻ anions parallel to planes, between which are located the organic groups. Solid-state and MAS-NMR spectroscopies are in agreement with the X-ray structure. Ab initio calculations allow the attribution of the phosphorous and carbon signals to the independent crystallographic sites and to the various atoms of the organic groups.     

Negative thermal expansion in Th2O(PO4)2

High temperature X ray diffraction performed on recently discovered orthorhombic Th₂O(PO₄)₂ shows a continuous linear thermal contraction (−1.6 × 10⁻⁶ °C⁻¹) in 20–600 °C range and a near-zero expansion at higher temperatures resulting from a dual structural deformation involving oxygen oscillations and inter-cations repulsions. Although similar mechanisms were observed in isotypic Zr₂O(PO₄)₂ (+1.5 × 10⁻⁶ °C⁻¹) and U₂O(PO₄)₂ (−1.4 × 10⁻⁶ °C⁻¹), those observed in Th₂O(PO₄)₂ are particularly intense because of the high ionic radius of tetravalent thorium.     

One-dimensional lone electron pair micelles in the crystal structure of Pb5(SiO4)(VO4)2

The structure of Pb₅(SiO₄)(VO₄)₂ (hexagonal, P6₃/m, a = 9.9865(11), c = 7.3599(12) Å, V = 635.67(14) Å³, Z = 2) has been solved by direct methods and refined to R₁ = 0.051 on the basis of 440 unique observed reflections with |F_o|≥4σ_F. The compound belongs to the apatite structure type. The Pb coordination polyhedra are distorted due to the presence of stereoactive lone electron pairs Ψ. The structure contains channels running along the c axis and centered at (00z). The channels are most probably occupied by the lone electron pairs of the Pb²⁺ cations and thus represent lone electron pair micelles. The existence of such micelles in the structure may well be the reason for the electrogyratory effect and protonic conductivity observed in crystals of the title compound.     

Structural characterization of mixed conducting perovskites La(Ga,M)O3−δ (M=Mn, Fe, Co, Ni)

Comparative analysis of the structure refinement results of perovskite-like LaGa_0.5M_0.5O_3−δ (M=Mn, Fe, Co, Ni) and data on other LaGaO₃-based phases, heavily doped with transition metal cations, shows that on doping the structural changes in these oxides follow common trends for the perovskite-type systems. The maximum ionic conductivity, observed in various perovskites when the tolerance factor values are approximately 0.96-0.97, was found to correlate with the transition from orthorhombic to rhombohedral structure and maximum lattice distortion. The perovskite unit cell distortion near the orthorhombic-rhombohedral phase boundary may hence play a positive role in the ionic transport processes.     

Stress-induced anisotropy in LPE grown Ni(Fe,Al)2O4 films

Preliminary results are reported about the growth of single crystal Ni(Fe,Al)₂O₄ films, grown by means of liquid phase epitaxy on (111)MgO and on (111)ZnGa₂O₄ substrates using a PbO-B₂O₃-Fe₂O₃ solvent. While films grown upon MgO show stress relief at the growth temperature, films grown upon ZnGa₂O₄ possess a tensile strain due to elastic deformation. Since λ₁₁₁ for NiFe₂O₄ is strongly negative a stress-induced uniaxial anisotropy is present in the films. Stripe domains can be observed with the Bitter technique and when a magnetic field is applied perpendicular to the plane of the film, magnetic bubbles with a diameter of ～2 μm appear. A bubble stability factor q exceeding unity is obtained. For the first time magnetic bubbles are found in LPE grown spinel ferrites.