共查询到18条相似文献,搜索用时 62 毫秒
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通过在Co_(82)Zr_(18)合金中添加过渡族元素Cr的方法,利用快淬工艺,制备出了Co_(82-x)Zr_(18)Cr_x(x=0,2,3,4)快淬合金薄带,利用磁性测量、X光衍射、热磁分析、扫描电子显微镜,对其磁性能、相组成、微结构进行了研究,实验结果表明,在Co_(82)Zr_(18)合金中添加少量的Cr可以使其矫顽力(iHc)显著提高,其中,Co_(79)Zr_(18)Cr_3快淬薄带经600℃退火处理后iHc=6.5 kOe.相分析发现,600℃退火后的Co_(79)Zr_(18)Cr_3快淬薄带由单一Co_(11)Zr_2相组成,Cr原子进入到了Co_(11)Zr_2相的晶格之中替换了原子半径相对较小的Co原子,这导致了Co_(11)Zr_2居里温度(T_C)的降低却使其磁晶各向异性场(Ha)显著提高;另一方面,通过微结构研究发现,未退火的Co_(79)Zr_(18)Cr_3快淬薄带由50—80 nm的等轴晶粒组成,经600℃退火后,其晶粒形态并未发生改变然而晶粒尺寸却增长到400—500nm。 相似文献
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研究了PrxFe82-x-yTiyCo10B4C4 (x=9—10.5;y=0, 2)纳米晶薄带的结构与磁性. 结果表明,所有薄带皆主要由2∶14∶1, 2∶17和α-(Fe, Co)三相组成. 对于y=0的合金,其内禀矫顽力随Pr含量x的增加而增加,剩磁随Pr含量x的增加而减小. 以Ti置换部分Fe (y=2),合金的磁性能得到显著提高,表现为:添加Ti后,合金的剩磁Br基本不降低,x=10.5时合金的Br值甚至有较明显的提高;同时添加Ti后,合金的内禀矫顽力及退磁曲线的方形度都明显改善. 当x=10.5,y=2时,合金薄带的磁性能达到最佳值为: Br=9.6 kGs(1 Gs=10-4 T),iHc =10.2 kOe(1 Oe=79.5775 A/m)和(BH)max=17.4 MGOe. 随着Pr含量的提高,合金中的硬磁相2 ∶14 ∶1的含量相对增加,内禀矫顽力提高;而Ti置换Fe抑制了软磁相α-(Fe, Co)在快淬和热处理过程中的优先长大,使合金中软磁相和硬磁相的晶粒尺寸及比例趋向最佳组合,交换耦合作用明显增强.
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纳米晶永磁材料
2Fe14(C')" href="#">Pr2Fe14(C
B)
Ti添加
交换耦合 相似文献
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本文研究非晶态Co70Cr20Zr10合金在居里温度附近的磁性,样品的磁特性符合二级相变规律。得到临界指数β=0.45±0.02,γ=1.9±0.1,δ=5.13±0.05。Co70Cr20Zr10合金的居里温度为Tc=(186.7±0.2)K。临界指数β,γ,δ满足γ=β(δ-1)关系,但临界指数值都偏离三维Heisenberg模型的理论值,这种行为可能起源于非晶态合金磁的不均匀性。讨论了Kouvel-Fisher(K-F)参数γ(T)对温度T的依赖关系。
关键词: 相似文献
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基于金属熔体结构的遗传性, 激光熔池的快速熔凝导致粉末的晶化状态可能会对最终成形件的晶化产生重要影响, 理清其影响规律对于制备大块非晶合金具有重要意义. 本文选取等离子旋转电极法所制粉末和1000 K退火态粉末为沉积材料, 采用激光立体成形技术沉积Zr55Cu30Al10Ni5块体非晶合金, 考察了粉末中已有晶化相对熔池及热影响区晶化行为的影响. 结果发现, 原始粉末组织由非晶相及粗大的Al5Ni3Zr2相组成; 当激光线能量较低时, 相应熔覆层的熔池和热影响区皆含有Al5Ni3Zr2相; 随着线能量的提高, 熔池中Al5Ni3Zr2相消失, 保持了非晶态, 但热影响区晶化加重, 并有大量Al5Ni3Zr2相析出; 当采用退火态粉末时, 即使线能量较小, 相应熔覆层仍主要由非晶构成, 几乎无Al5Ni3Zr2相析出. 这是由于原始粉末在退火时其微观结构发生重排, 与Al5Ni3Zr2相关的原子短程/中程有序结构减少, 导致已沉积层非晶区的热稳定性提高, 不利于Al5Ni3Zr2相析出. 可见, 提高线能量将会加剧非晶沉积体的晶化, 而粉末中的Al5Ni3Zr2团簇相状态对Zr55Cu30Al10Ni5合金沉积层的晶化有重要影响. 相似文献
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利用透射电子显微镜对Ni67Zr33非晶合金晶化的研究发现了两个新的亚稳相T0与T10。其中T1相为体心正交(准四方〕晶体,点阵常数a≌b=0.89nm,c=3.14nm,空间群为Iba2或Ibam。温度升高,T1相转变为含有大量错排的A心正交Ni10Zr2相,用1/2(a+b)位移错排模型可以圆满地解释其电子衍射图中仅h+k为奇数的衍射斑沿c*方向拉长的现象,晶化稳定相为Ni10Zr,与Ni21Zr8(Ni5Zr2)相。
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基于平面波赝势密度泛函理论(DFT)和广义梯度近似(GGA)的第一性原理计算了高温高压下金属化合物Co_2Zr和Co_2Ti的结构和热力学性质.Co_2Zr和Co_2Ti均为立方晶体,且结构类型为Cu2Mg结构.通过计算得出的晶格参数跟实验值符合较好.用准谐德拜模型计算了Co_2Zr和Co_2Ti的热力学性质.在0~100 GPa的压强和0~1500 K的温度作用下,两种物质的德拜温度Θ,热容CV,热膨胀系数α随压强和温度的变化而变化.随着压强的增大,德拜温度单调的增加;相同压强下,Co_2Ti的德拜温度始终大于Co_2Zr.热容CV和热膨胀系数α均随温度的增加而增加,增大压强时反而减小,说明减小温度和增大压强对CV以及α有相同的影响. 相似文献
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The magnetic anisotropy energy (MAE) of 3d transition-metal wires, stripes, and films is calculated self-consistently as a function of stripe width and film thickness. The magnetization-reorientation transitions in stripes are determined along the crossover from the mono-atomic one-dimensional chain to the two-dimensional monolayer. It is shown that the MAE oscillates as a function of stripe width and depends strongly on the considered transition metal. The reorientation transitions in Co films deposited on a highly polarizable substrate such as Pd are discussed. A local analysis of the layer-resolved MAEs provides new insights into the off-plane magnetization observed in Pd-capped Co films on Pd(111). The interfaces responsible for the stability of the off-plane easy axis are characterized microscopically. An unexpected internal magnetic structure of the Co–Pd interfaces is revealed in which the magnetic moments and spin–orbit interactions at Pd atoms play a crucial role. The nature of the reorientation transition from perpendicular to in-plane magnetization with increasing film thickness is studied by means of full-vectorial calculations. The existence of a spin-canted phase at intermediate film thickness is demonstrated. 相似文献
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Eun-Ju KimYong-Hoon Jeong Han-Cheol Choe William A. Brantley 《Applied Surface Science》2012,258(6):2083-2087
Surface phenomena of HA/TiN coatings on the nanotubular-structured beta Ti-29Nb-5Zr alloy for biomaterials have been investigated by several experimental methods. The nanotubular structure was formed by anodizing the Ti-29Nb-5Zr alloy in 1 M H3PO4 electrolytes with 1.0 wt.% NaF at room temperature. Hydroxyapatite (HA)/titanium nitride (TiN) films were deposited on Ti-29Nb-5Zr alloy specimens using a magnetron sputtering system. The HA target was made of human tooth-ash by sintering at 1300 °C for 1 h, and the HA target had an average Ca/P ratio of 1.9. The HA/TiN depositions were performed, using the pure HA target, on Ti-29Nb-5Zr alloy following the initial deposition of a TiN buffer layer coating. Microstructures and nanotubular morphology of the coated alloy specimens were examined by FE-SEM, EDX, XRD, and XPS. The Ti-29Nb-5Zr alloy substrate had small grain size and preferred orientation along the drawing direction. The HA/TiN coating was stable with a uniform morphology at the tips of the nanotubes. 相似文献
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基于密度泛函理论(DFT)采用第一性原理的全势能线性缀加平面波(FLAPW)的能带计算方法研究了强磁性Heusler合金Co2TiSn和Co2ZrSn的电子能带结构,在计算中考虑了自旋-轨道藕合(SOC)的修正.计算结果表明两种合金在费米面附近的能带结构是一个d-d电子杂化作用形成的能带.分析计算结果发现Co原子对磁矩有主要的贡献,两种Heusler合金的磁矩是由于Co原子3d eg的自旋劈裂形成的,3deg的自旋向下分量是合金的电子态密度(DOS)的主要来源.由能带计算得到Co2TiSn和Co2ZrSn的自旋磁矩分别为1.97μB和1.96μB,其中Co原子在上述两种合金中的自旋磁矩分别是1.01μB和1.02μB,轨道磁矩分别为0.041μB和0.051μB. 相似文献
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Zhipeng HouWenquan Wang Shifeng XuJinbao Zhang Chunji WuFeng Su 《Physica B: Condensed Matter》2012,407(7):1047-1050
The phases and magnetic properties of Co-Zr-Ti melt-spun ribbons were studied by XRD analysis and magnetic measurements. The optimal magnetic properties of Ms=59.0 emu/g, Mr=4.0 kG, Hc=2.9 kOe, and (BH)max=3.0 MGOe were obtained in Co82Zr14Ti4 ribbons produced at a wheel speed of 30 m/s. In this work, we found that Ti was one of the few large atomic radius elements, which could improve hard magnetic properties of Co-Zr alloy. 相似文献