Ti掺杂Nd2Fe14B/α-Fe纳米双相复合永磁体晶化动力学

纳米双相复合稀土永磁材料,利用硬磁相高磁晶各向异性和软磁相高饱和磁化强度的优点,通过铁磁交换耦合作用获得优异的磁性能.但是如何解决软硬磁双相纳米微结构不匹配的问题,控制软硬磁相同时达到理想的纳米尺度复合是关键.本文研究了掺杂合金元素Ti对熔体快淬法制备的Nd₂Fe₁₄B/α-Fe快淬薄带晶化过程的影响.结果表明,掺杂合金元素Ti能影响Nd₂Fe₁₄B/α-Fe交换耦合磁体整个晶化动力学过程,使α-Fe相的晶化激活能升高,抑制其从非晶相中析出.同时,降低1∶7亚稳相的晶化激活能,起到稳定亚稳相的作用.而且随着晶化温度的进一步提高, α-Fe和Nd₂Fe₁₄B两相由1∶7亚稳相分解产生,从而有效避免了α-Fe相的优先析出.显微组织观察表明,掺杂Ti的样品晶粒细小、分布均匀,平均晶粒尺寸在20 nm左右,没有特别大的α-Fe粒子出现.当Ti的掺杂量原子百分数为1.0%时,获得了最佳磁性能(BH)_max=12 MG·Oe(1 G=10     

高压淬火直接形成Pd-Si块状纳米晶合金

介绍通过液态合金的高压淬火直接形成Pd-Si块状纳米晶合金的方法及其研究结果.X射线衍射及高分辨电子显微镜分析表明,Pd-(?)Si-(?)合金在低于5.0GPa的压力下以100K/s的冷却速率淬火时形成普通晶粒组织.而当在5.0至6.5GPa的压力下以同样的冷却速率淬火时,得到了晶垃尺寸为30—40nm的块状纳米晶合金.采用这种方法制备的Pd-Si块状纳米晶合金具有高密度、无微孔及晶界间无杂质的特点. 关键词：     

制备条件对纳米晶吸收剂的吸波性能影响的实验研究

采用柠檬酸盐溶胶凝胶法制备出不同Co掺杂的Ba纳米晶铁氧体吸收剂,分析了制备条件对其物性、吸波性能等的影响,确定了最佳制备工艺条件. 研究了粒径对纳米晶吸波性能的影响,同时还测试了纳米晶吸收剂的雷达波吸收性能. 结果表明,纳米晶吸收剂是一种性能优良的雷达波吸收材料. 关键词： 纳米晶吸收剂 烧结温度 溶胶凝胶法     

铝纳米晶的正电子湮没研究

采用自悬浮定向流-真空热压法,在不同压强下制得铝纳米晶材料,并利用X射线衍射(XRD)和正电子湮没寿命谱(PALS)分析手段对铝纳米晶的结构和微观缺陷进行表征.XRD分析表明:所制备的铝纳米晶的晶粒度为48 nm.PALS分析表明:铝纳米晶的微观缺陷主要为类空位以及空位团,而微孔洞很少;短寿命τ1,中间寿命τ2以及其对应的强度I1,I2随压强变化而呈现阶段性变化;压制压强(P)低于0.39 GPa时制得的纳米晶空位团随压强的增加而逐渐转变为类空位;0.39 GPa P 0.72 GPa时,各类缺陷发生消除;P 0.72 GPa时,各类缺陷进一步发生消除.随压强的提高,铝纳米晶的密度增加,其显微硬度也明显增高.     

Pr基大块纳米晶合金及其特性研究

研究了Pr₆₀Al₁₀Ni₁₀Cu₂₀ 大块金属玻璃 的结构和磁性随Fe含量 的变化关系，结果表明Pr基合金逐步从玻璃状态，转变为非晶与纳米晶的复合状态，最后成 为纳米晶合金，Pr基合金的磁性也相应地发生变化.提出了一种通过对大块稀土基金属玻璃 进行Fe掺杂，制备出微观结构和性能具有可调控性的大块纳米晶合金的方法, 并讨论了纳米 晶结构和性能的关系. 关键词： 金属玻璃 大块纳米晶 掺杂     

Ti-Zr-Ni单相准晶合金的室温力学性能研究

以Ti40₄₀Zr40₄₀Ni20₂₀合金为研究对象，用铜 模吸铸法制备出直径为3mm的致密单相准晶棒，通过维氏显微硬度测定和单向压缩实验方 法研究了该合金的室温力学性能 .结果表明：Ti40₄₀Zr40₄₀Ni20₂₀准晶具有良好 的弹性变形能力，室温弹性应 变可达125%.同时，它具有相对高的室温硬度（约55GPa），是普通Ti合金的15倍.T i40_{40 关键词： 准晶 Ti-Zr-Ni合金 解理断裂}     

Co3O4纳米晶的制备和表征

发现了一种新制备Co3O4纳米晶的新方法。这种方法是先将高分子聚乙烯吡咯烷酮(PVP)和乙酸钴溶解到溶剂中缓慢蒸发溶剂,然后干燥形成的前驱体,最后在400℃温度下煅烧制备了Co3O4纳米晶。生成的产物用XRD,SEM,TEM等测试方法进行了表征。结果发现在不同的溶剂中形成前驱体所制备的Co3O4纳米晶具有不同的形貌特征,使用乙醇溶剂时生成了大量的由Co3O4纳米晶自组装形成的Co3O4微米球;而使用水溶剂时则生成的全都是Co3O4纳米晶。实验结果表明在不同溶剂中形成的前驱体对于最终制备的Co3O4纳米晶形态有着很大的影响。     

Fe73.5Cu1Nb3Si13.5B9非晶合金的激波纳米晶化速率和晶化度的对比研究

对Fe735Cu1Nb3Si135B9等非晶合金进行了退火和激波诱导两种方式的晶化实验以及XRD和DSC分析.着重对合金的晶化速率和晶化度等特性展开了研究和讨论.进一步证实了激波纳米晶化是一种包含着新机理的寓意丰富的晶化现象.也再次验证了作者曾经提出过的“激波流化相变”模型的合理性. 关键词： 非晶合金 激波 纳米晶化     

快速凝固Co-Cu包晶合金的电学性能

研究了Co-Cu包晶合金快速凝固过程中的相选择和组织形成特征, 探索了冷却速率、组织结构和晶体位向与合金电阻率之间的相关规律.实验发现, 快速凝固可使Co在(Cu)中的固溶度扩展至20%.Cu含量大于80%时, L+αCo→(Cu)包晶转变被抑制, (Cu)可从过冷熔体中直接形核析出.Cu含量在40%—70%范围时, Co-Cu合金的液相分离受到抑制, 凝固组织沿条带厚度方向分为两个晶区.细晶区中αCo和(Cu)相竞争形核并生长, αCo枝晶形态细密，细小的（Cu）等轴晶均匀分布于αCo的基体之中.粗晶区αCo相为领先相, 富Cu相分布于αCo枝晶的晶界处.随着冷速的增大, 合金组织显著细化, 晶界增多,对自由电子的散射作用增强, 合金电阻率显著增大.当晶界散射系数r＝0996—0999时, 可采用M-S模型综合分析快速凝固Co-Cu合金的电阻率. 关键词： 电阻率 快速凝固 相结构 晶体生长     

反钙钛矿结构GaCMn_3纳米晶的磁热效应和临界行为研究

我们通过高能球磨的方法,制备出平均晶粒尺寸为45纳米(nm)的GaCMn_3纳米晶样品,并研究了其磁热和铁磁-顺磁相变的临界行为.在磁场变化2T时,相比于块体GaCMn_3,虽然纳米晶GaCMn_3的磁熵变(-ΔSM)减小了,但是其相对磁制冷能力(RCP)却增强了.通过Kouvel-Fisher方法,我们确定了GaCMn_3纳米晶铁磁-顺磁相变的临界指数β=0.463和γ=1.161,根据Widom标度理论,得出第三个临界指数δ=3.51.这些临界指数和平均场模型的临界指数(β=0.5,γ=1.0,andδ=3.0)很接近,表明GaCMn_3纳米晶中的铁磁耦合是长程的.     

Soft Magnetic Materials in a Bulk Form Prepared by Powder Compaction

The amorphous, nanocrystalline and polycrystalline ferromagnetic alloys are known as materials with excellent soft magnetic properties. These attractive magnetic properties are challenge for researchers to extend investigation of these materials with the aim to broaden their technical exploitation. The shape in which amorphous, nanocrystalline and polycrystalline materials are usually prepared, is in many cases not suitable shape for application, therefore it is logical to attempt to prepare such material in a more “bulk” form, for example in the form of a cylinder or a ring, that would be more convenient for industrial applications. One of the ways to prepare material in bulk form is to compact the powder. There is rational assumption that the non-magnetostrictive alloys (amorphous Co-Fe-Si-B, nanocrystalline Fe-Nb-Cu-Si-B, and polycrystalline Ni-Fe) may be suitable for the preparation of bulk samples by high-pressure compression, because mechanical stress does not induce magnetic anisotropy in ferromagnetic material during preparation process.We observed that milling of ribbons prepared by rapid quenching method leads to the increase of coercivity, which is caused by the increase of the fraction of magnetization vector rotation in the magnetization processes (the fraction of domain wall motion decreases). After long milling the powder particles become single-domain and can be magnetized by the magnetization vector rotation only, exhibiting maximum value of coercivity.Consolidation of powder with high value of coercivity leads to the “magnetic contact” between powder particles resulting in the decrease of coercivity to the value comparable with that for as-spun ribbons.     

Stability,electronic structures,and mechanical properties of Fe–Mn–Al system from first-principles calculations

The stability, electronic structures, and mechanical properties of the Fe–Mn–Al system were determined by firstprinciples calculations. The formation enthalpy and cohesive energy of these Fe–Mn–Al alloys are negative and show that the alloys are thermodynamically stable. Fe_3Al, with the lowest formation enthalpy, is the most stable compound in the Fe–Mn–Al system. The partial density of states, total density of states, and electron density distribution maps of the Fe–Mn–Al alloys were analyzed. The bonding characteristics of these Fe–Mn–Al alloys are mainly combinations of covalent bonding and metallic bonds. The stress-strain method and Voigt–Reuss–Hill approximation were used to calculate the elastic constants and moduli, respectively. Fe_(2.5)Mn_(0.5)Al has the highest bulk modulus, 234.5 GPa. Fe_(1.5)Mn_(1.5)Al has the highest shear modulus and Young's modulus, with values of 98.8 GPa and 259.2 GPa, respectively. These Fe–Mn–Al alloys display disparate anisotropies due to the calculated different shape of the three-dimensional curved surface of the Young's modulus and anisotropic index. Moreover, the anisotropic sound velocities and Debye temperatures of these Fe–Mn–Al alloys were explored.     

Annealing dependence of magnetic properties in nanostructured Sm0.5Y0.5Co5

Nanocrystalline Sm_0.5Y_0.5Co₅ powders with high coercivity H_C and enhanced remanence M_r were prepared by mechanical milling and subsequent annealing. Annealing temperatures T ranging from 973 to 1173 K, and times t ranging from 1 to 5 min were used. X-ray diffraction (XRD) and DC-magnetization measurements were carried out to study the microstructure and magnetic properties of these samples. XRD patterns demonstrate that the average grain size D of the nanocrystalline powders depends on the annealing temperature T and time t: D ranges from 11 nm (for T=973 K and t=1 min) to 93 nm (for T=1173 K and t=5 min). Magnetic measurements performed at room temperature indicate high coercivity values (H_C>955 kA/m), and enhanced remanence (M_r/M_max>0.5) for all samples. A strong annealing-induced grain size dependence of these magnetic properties was found.     

PDMS改性环氧树脂/Sm2O3复合涂层的近红外光谱及疏水性研究

以聚二甲基硅氧烷（PDMS）改性环氧树脂（HYSZ）为粘合剂,Sm₂O₃为功能颜料,纳米SiO₂为微纳结构改性剂,制备得到了一种同时具有良好疏水性能和附着力的近红外吸收涂层。系统分析了PDMS和HYSZ质量比、邻苯二甲酸二辛酯(DOP)添加量、总填料添加量、Sm₂O₃和纳米SiO₂质量比对涂层性能的影响。结果表明：PDMS改性可明显降低涂层的表面能,从而使涂层的疏水性得到明显增强。利用DOP强化涂层韧性和微观搭桥作用可增强涂层整体性,从而可明显提高涂层的附着力和近红外吸收性能。涂层的表面粗糙度可随总填料添加量的增加而明显升高,进而可使涂层表现出更优的疏水性能。当涂层中PDMS和HYSZ质量比、DOP添加量、总填料添加量、Sm₂O₃和纳米SiO₂质量比分别为1∶9,20%,50%和5.5∶4.5时,涂层同时具有良好的近红外低反射率（59.1%）、疏水性能（水接触角为137°）及附着力（2级）。     

Effects of alloying element on stabilities,electronic structures,and mechanical properties of Pd-based superalloys

The thermodynamic stabilities, electronic structures, and mechanical properties of the Pd-based superalloys are studied by first principles calculations. In this work, we discuss the effect of Pd-based superalloys made from Al, Si, Sc, Ti,V, Cr, Mn, Fe, Cu, Zn, Y, Zr, Nb, Mo, Tc, Hf, Ta, W, Re, Os, Ir and Pt, and we also calculate a face centered cubic(fcc)structure 2 × 2 × 2 superalloy including 31 Pd atoms and one alloying element T M(Pd_(31)TM). The mixing energies of these Pd-Based superalloys are negative, indicating that all Pd-based superalloys are thermodynamically stable. The Pd_(31)Mn has the lowest mixing energy with a value of-0.97 eV/atom. The electronic structures of the Pd-based superalloys are also studied, the densities of states, elastic constants and moduli of the mechanical properties of the Pd-based superalloys are determined by the stress-strain method and Voigt–Reuss–Hill approximation. It is found that Pd_(31)TM is mechanically stable, and Pd_(31)Tc has the largest C_(11), with a value 279.7 GPa. The Pd_(31)Cr has the highest bulk modulus with a value of299.8 GPa. The Pd_(31)Fe has the largest shear modulus and Young's modulus with the values of 73.8 GPa and 195.2 GPa,respectively. By using the anisotropic index, the anisotropic mechanical properties of the Pd_(31)T M are discussed, and threedimensional(3 D) surface contours and the planar projections on(001) and(110) planes are also investigated by the Young modulus.     

质子辐照对永磁合金微观结构演化的研究

钐钴和钕铁硼稀土永磁合金已经广泛应用于粒子加速器的波荡器和其他器件中,作为加速器的重要组成部分,永磁合金在辐照环境中长期服役会出现磁性能损失的现象,这会影响束流的品质.为了探讨产生这个现象的微观机理,采用透射电镜对质子辐照前后的钐钴和钕铁硼稀土永磁合金进行了微观结构演化的表征和分析,统计了由辐照析出的纳米晶体积密度和粒径分布,并讨论了微观结构演化对宏观磁性能损失的影响.结果表明,随着质子辐照损伤程度的增加,永磁合金的微观结构从单晶结构转变为纳米晶多晶结构,且纳米晶和基体的晶体结构相同.钕铁硼的纳米晶体积密度先增大后减小,粒径分布先增大后不变;钐钴的纳米晶体积密度逐渐减小,粒径逐渐增大.在2 dpa的质子辐照损伤程度下,钕铁硼稀土永磁合金比钐钴永磁合金的非晶化趋势更明显.     

Ti-Al金属间化合物结构与性质的第一性原理模拟

采用软件CASTEP模拟Ti-Al金属间化合物的晶体结构、力学性质和电子性质.分析在0 K、0 GPa时,Ti-Al存在的四种热力学稳定结构：TiAl₃、TiAl₂、TiAl、Ti₃Al,发现TiAl₃、TiAl₂、TiAl可以看作由Al的面心立方结构衍化而来,而Ti₃Al的结构与Ti相似,为密排六方结构.随着Ti摩尔分数的增加,TiAl₃、TiAl₂、TiAl、Ti₃Al的体模量相当,剪切模量和Vickers硬度逐渐减小;Pugh比k值也逐渐减小,表示韧性逐渐变好.最后对态密度、Mulliken布居分析等进行模拟,发现这四种结构Ti-Al键都具有金属性、共价性及弱的离子性.     

Effect of isothermal treatments on the magnetic behavior of nanocrystalline Cu–Ni–Fe alloy prepared by mechanical alloying

The present study concerns magnetic behavior of nanocrystalline Cu–Ni, Cu–Fe and Cu–Ni–Fe alloys prepared by mechanical alloying. It has been found that the magnetic properties e.g. H_c, M_r and M_s of the nanocrystalline alloys were significantly influenced by the changes in microstructural constituents, grain size and evolution of phases. Microstructural changes in the alloys have been effected by carrying out isothermal treatments on the mechanically alloyed products in the temperature range of 450–650 °C. Phase evolution in the samples after the isothermal treatments were identified and characterized by X-ray diffraction (XRD) and differential scanning calorimetric (DSC) techniques and the results were correlated with the magnetic properties of the alloys.     

Ca~(2+)掺杂对SmFeO_3的介电、铁磁特性及磁相变温度的影响

采用固相反应法制备Sm_(1-x)Ca_xFeO_3(x=0,0.1,0.2,0.3)样品,研究Ca~(2+)掺杂对SmFeO_3介电性能、铁磁性及磁相变温度的影响.X射线衍射图谱分析表明:所有样品的主衍射峰与SmFe03相符合且具有良好的晶体结构.随着x的增加,SmFeO_3样品的晶粒尺寸由原来的0.5μm逐渐增大到2μm.当f=1 kHz时,Sm_(1-x)Ca_xFeO_3(x=0.1,0.2,0.3)样品的ε_r分别是SmFe03的5倍、3倍和2.6倍,而tgσ增大一个数量级.在3T磁场作用下,SmFe03样品的M-H呈线性,随着x的增加,M-H逐渐趋向饱和,Sm_(1-x)Ca_xFeO_3(x=0.1,0.2,0.3)样品的M_r分别是SmFeO_3的20倍、31倍和68倍.X射线光电子能谱分析表明:Fe~(2+)和Fe3+共存于Sm_(1-x)Ca_xFeO_3样品中,Fe~(2+)/Fe~(3+)比例随着x的增加而增大,证明Ca~(2+)掺杂增加了Fe~(2+)的含量,形成Fe~(2+)—O~(2-)—Fe~(3+)超交换作用,增强SmFe03的铁磁特性.测量了Sm_(1-x)Ca_xFeO_3样品在外加磁场为1000 Oe(1 Oe=79.5775 A/m)的M-T变化关系,观测到其自旋重组温度(T_(SR))和尼尔温度(T_N)分别为438 K和687 K,发现SmFe03样品的T_(SR)和T_N均随着x的增加向低温方向移动,当x=0.3时,自旋重组现象消失.这主要是SmFeO_3样品磁结构的稳定性和Fe~(3+)—O~(2-)—Fe~(3+)及Sm~(3+)—O~(2-)—Fe~(3+)超交换三者共同作用的结果.     

NANOSTRUCTURED Zr-BASED ALLOYS-PHASE FORMATION AND MECHANICAL PROPERTIES

Newly developed nanostructured Zr/Ti-Al-TM multiphase alloys can provide a large bandwidth of interesting properties, such as mechanical properties. Bulk materials with nanocrystalline/ amorphous and (nano)quasicrystalline/ amorphous microstructure with different volume fractions of nanophases and with different grain sizes can be obtained by slowly cooling the melt as well as by solid state reactions. Multiphase structures are realized either by partial de-vitrification of bulk glass-forming alloys or by defined addition of inert compounds upon alloying. Special preparation techniques e.g. copper mould casting and subsequent controlled annealing and mechanical alloying combined with hot consolidation of powders are described. The phase formation and transformation processes and the thermal stability of such materials in dependence on alloy composition and processing parameters are discussed in detail. Currently, the exploration of properties with respect to potential applications of these nanostructured alloys is still at the beginning. First investigations on the contributions of different phases/ volume fractions to the overall mechanical behaviour will be shown. At room temperature, the deformation behaviour of amorphous/crystalline bulk samples is governed by contributions of all existing phases yielding a high strength of the material.