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1.
李华  姜寿亭  梅良模  高汝伟 《物理学报》1993,42(7):1179-1185
本文根据Nd2Fe14B化合物中存有少量巡游电子的基本实验事实,提出了在Nd2Fe14B中配位子所产生的晶场和巡游电子所产生的电场共同造成了Nd离子磁晶各向异性的理论模型。提出并解决了计算巡游电子同中心Nd离子相互作用的理论方法。在同时考虑Nd离子所受配位子的晶场和巡游电子的电场的作用情况下,用单离子模型计算了Nd2Fe14B中Nd离子所产生的磁晶各向异性及其随温度的变化。所 关键词:  相似文献   

2.
杨白  沈保根  赵同云  孙继荣 《物理学报》2007,56(6):3527-3532
采用快淬方法制备了纳米晶复合Pr2Fe14B/α-Fe永磁薄带,研究了不同淬火速率对薄带织构和磁性的影响.通过改善快淬工艺,使得薄带中Pr2Fe14B相的晶粒在薄带的自由面形成显著的织构,Pr2Fe14B相晶粒易轴沿垂直于带面方向取向.分析了快淬凝固过程中Pr2Fe14B相的晶粒取向过程和机理,以及晶粒的大小和薄带结构的均匀性对薄带磁性的影响.对自由面有显著取向的薄带,进行酸蚀和打磨减薄处理,去除贴辊面未取向的部分,剩余部分为具有Pr2Fe14B相晶粒取向的各向异性薄带,Pr2Fe14B相取向使薄带的剩磁得到增强,矫顽力也有所提高. 关键词: 快淬 2Fe14B/α-Fe永磁薄带')" href="#">纳米晶复合Pr2Fe14B/α-Fe永磁薄带 织构 磁性能  相似文献   

3.
赵铁松  金汉民 《物理学报》1990,39(6):163-168
基于单离子模型,详细分析了Ho2Fe14B化合物在T=0K沿[100],[110]和[001]轴磁化时,Ho和Fe次晶格的磁化过程。预测了该化合物在T=0K高达2000 kOe的磁场中沿主晶轴的磁化曲线。 关键词:  相似文献   

4.
陈宪锋 《物理学报》2005,54(8):3856-3861
针对低温下各向同性Pr2Fe14B永磁材料的最小形核场问题,用数值 计算法和近似解 析解研究了第二磁晶各向异性常数K2对最小形核场的影响.研究发现,尽管对于 Nd2 Fe14B永磁材料一级近似的解析解与数值计算结果很接近,但是对于低温下各向 同性P r2Fe14B永磁材料则至少要用二级近似下的解析解才能与数值计算 结果相接近.用有 关最小形核场的计算结果很好地解释了低温时各向同性Pr2Fe14B永 磁材料的矫顽力与最小形核场的关系. 关键词: 第二磁晶各向异性常数 形核场 矫顽力  相似文献   

5.
吴文霞  郭永权  李安华  李卫 《物理学报》2008,57(4):2486-2492
应用固体与分子经验电子理论计算了Nd2Fe14B的价电子结构、磁矩和居里温度,计算结果与实验值相符.计算表明:该合金的磁性与3d磁电子数成正比.从Fe(c)晶位到Fe(k2)晶位磁矩增加,其机理源于价电子、哑对电子和3d磁电子之间的转化,有78%的哑对电子和18%的3d共价电子转化成了磁电子.居里温度和磁矩与Fe原子配位数成正比,与加权等同键数Iσ成反比,Nd原子 关键词: 2Fe14B')" href="#">Nd2Fe14B 价电子结构 居里温度  相似文献   

6.
构造了立方和不规则形状晶粒的各向异性纳米晶单相Pr2Fe14B磁体 .利用微磁学的有限元法,模拟计算了样品的磁滞回线.计算结果表明,随着磁体晶粒易轴取向度的变差, 磁体的剩磁、矫顽力均随之下降.不同晶粒尺寸的纳米晶单相Pr2Fe14B磁体,其磁 性能随取向度的变化快慢不同,原因在于磁体中的晶间交换作用 (IGEC) 的强弱不同.随着 晶粒取向度的提高,纳米晶单相磁体的矫顽力逐渐增加,这完全不同于烧结磁体. 关键词: 纳米晶磁体 矫顽力 剩磁  相似文献   

7.
郝红飞  王静  孙锋  张澜庭 《物理学报》2013,62(11):117501-117501
基于第一性原理投影缀加波和梯度矫正局域密度近似(PAW-GGA), 研究了Nd2Fe14B和Dy2Fe14B的基态晶格属性, 进而对Dy在Nd2Fe14B晶格中的掺杂进行了研究, 并采用GGA+U的方式进行了原子磁矩计算, 并与自旋轨道耦合 (SOI) 计算结果进行了对照. 置换计算表明, Dy原子倾向于置换Nd2Fe14B晶格中4f位的稀土原子. 磁矩计算表明, 在R2Fe14B (R: 稀土元素) 晶格中, 4f位的稀土元素与Fe原子作用更强, 对磁性能的影响更大. 稀土原子与Fe的作用与距离呈正相关. 关键词: 2Fe14B')" href="#">Nd2Fe14B 晶格占位 形成能 原子磁矩  相似文献   

8.
运用微磁学方法结合物质参数探究了垂直取向Nd2Fe14B/α-Fe磁性三层膜的磁化反转过程,计算出成核场、钉扎场以及磁滞回线随s(软磁相厚度)的变化,并与相关的实验和理论数据进行比较.由于考虑了退磁能量项,垂直取向的成核场比平行取向时低,在外磁场还没有反向时就发生了成核.随着软磁相厚度的增加,理论矫顽力从等于成核场(同时也等于钉扎场),到等于钉扎场,再到小于钉扎场,矫顽力机理由成核变为钉扎. 关键词: 成核场 钉扎场 矫顽力 磁滞回线  相似文献   

9.
本文在1.5—300K温度范围内测量了R2Fe14B(R=Ce,Pr,Gd)各向异性常数K1,K2和各向异性场HA随温度的变化。同时用单离子模型计算了Pr3+离子对Pr2Fe14B磁晶各向异性的贡献,得到与实验值半定量符合的结果。 关键词:  相似文献   

10.
基于单离子晶场模型 ,提出了计算稀土 Fe(Co)金属间化合物取向多晶样品磁化曲线的方法 .用此方法计算了取向Pr2 Fe14 B和Nd2 Fe14 B多晶的高场磁化曲线 ,计算中使用了拟合化合物单晶磁化曲线得到的交换场与晶场参数 .计算曲线与实验曲线相符合 .  相似文献   

11.
Static magnetic measurements have been carried out on single crystals of Er2Fe14B and Tm2Fe14B in a temperature range between 77 and 590 K. Spin reorientation phenomena have been found in both compounds slightly above room temperature. In Er2Fe14B, the easy direction of magnetization changes from [100] to [001] at 316 K as temperature increases, and Tm2Fe14B from [100] to [001] at 310 K. Anomalously large anisotropy in the saturation magnetization has been detected around the spin reorientation temperature.  相似文献   

12.
冯维存  高汝伟  李卫  韩广兵  孙艳 《中国物理》2005,14(8):1649-1652
本文采用统计平均方法研究了软、硬磁性晶粒尺寸及相分布对Nd2Fe14B/α-Fe纳米复合永磁材料矫顽力的影响。计算结果表明:对于单相纳米硬磁材料,磁体矫顽力随着硬磁性晶粒尺寸的减小而降低;对于软、硬两磁性相组成的Nd2Fe14B/a-Fe纳米复合永磁材料,两相的随机分布将导致磁体矫顽力随硬磁性晶粒尺寸的减小呈现极大值。本文的计算结果还表明当硬磁性晶粒尺寸大于软磁性晶粒的最佳尺寸时(15nm),具有多层膜结构的Nd2Fe14B/a-Fe纳米复合永磁材料将比两相随机分布时具有更大的矫顽力。  相似文献   

13.
Y2Fe14B and Nd2Fe14B are ferromagnets in which 3d interactions are dominant. In Y2Fe14B, the
-axis of the quadraticque est de magnetization. The 3d anisotropy is an order of magnitude weaker than in YCo5. In agreement with point-charge model, CEF potential in Nd2Fe14B favours the
-axis at 300 K. At low temperature, the magnetization reorientation observed results from competition between exchange and anisotropy.  相似文献   

14.
The magnetic properties of Nd4.5Fe77−xMnxB18.5 (x=0, 1 and 2) nanocomposites prepared by the crystallization of amorphous precursors were investigated. Addition of Mn is found to decrease the crystallization temperature of the amorphous ribbons. The intrinsic coercivity iHc and maximum energy product (BH)max increase from 2.6 kOe and 9.1 MGOe for x=0 to 3.1 kOe and 10.3 MGOe for x=1, respectively, and the remanence ratio Mr/Ms increases from 0.70 to 0.72. The effect of Mn on Curie temperature TC and the thermal stability of Mr and iHc were also studied. 57Fe Mössbauer spectra have been recorded for x=0, 1 and 2 ribbons at room temperature and site preference of the Mn atoms in Fe3B and Nd2Fe14B phases is discussed using the Mössbauer spectroscopy.  相似文献   

15.
It is difficult to obtain the crystallographic alignment for stoichiometric Nd2Fe14B alloys by applying the melt-spun and subsequent hot-pressing and hot-deformation techniques. However, the enhanced alignment and magnetic properties of die-upset nano-crystal Nd2Fe14B magnets have been obtained by Nb addition in the present paper. The magnetic properties studies show that Nb addition leads to the remarkable increase of remanence Br and intrinsic coercivity Hci, which is due to the improvement of c-axis texture and refinement of microstructure. Microstructure studies using transmission electron microscopy (TEM) and X-ray diffraction (XRD) reveal that Nb atoms are enriched at grain boundary and the NbFeB phase is observed with increasing Nb content. Since some Fe atoms in the Nd2Fe14B phase participate in the formation of NbFeB phase, the excessive Nd atoms may be enriched at grain boundary, which may improve the physical property of grain boundary and provide a mass transport pass for preferential growth of oriented Nd2Fe14B grains, thus leading to the enhanced alignment and magnetic properties.  相似文献   

16.
In this paper, compact bulk nanocomposite Nd2Fe14B/α-Fe magnetic materials were prepared by hot extrusion of amorphous and nanocrystalline powders, which were prepared by high-energy ball-milling (HEBM) of the Nd2Fe14 B-type hard magnetic phase with 20 vol% of α-Fe as soft magnetic phase. The extrusion temperature has important influence on magnetic properties and microstructure of magnetic materials. The results show that the grain size of Nd2Fe14B and α-Fe phase increases steadily with increasing extrusion temperature. Furthermore, optimal extrusion temperature of 1223 K occurs, at which the highest magnetic properties and relative density can be obtained.  相似文献   

17.
The lean rare-earth Pr4.5Fe77−xTixB18.5 (x=0, 1, 4, 5) nanocomposite alloys were prepared by melt spinning method and subsequent thermal annealing. The effect of Ti content and annealing temperature on the magnetic properties and the microstructure of these magnets were investigated. The enhancing coercivity Hc from 211.4 to 338.2 kA/m has been observed at the optimal annealing temperature of 700 °C by the addition of 5 at% Ti in Pr2Fe14B/Fe3B alloys. It was also found that increasing Ti content leads to marked grain refinement in the annealed alloys, resulting in strong exchange-coupling interaction between the hard and the soft phases in these ribbons. In addition, the magnetization reversal behaviors of Pr2Fe14B/Fe3B nanocomposites were discussed in detail.  相似文献   

18.
胡伯平  张寿恭 《物理学报》1987,36(10):1364-1370
本文对Si加入Nd2Fe14B四方相后所形成的合金相的结构和磁性进行了研究。结果表明,Si加入Nd2Fe14B四方相后并不破坏它的结构(Si的含量可达B的两倍),而形成Nd2(Fe,Si)14B赝三元金属间化合物。随着Si含量的增加,晶格常数和饱和磁化强度随之减小,但居里温度则随之增加。Si的加入,并不改变Nd2Fe14B的室温各向 关键词:  相似文献   

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