共查询到17条相似文献,搜索用时 140 毫秒
1.
2.
3.
讨论了利用分子场近似结合中子衍射或X射线衍射的实验结果计算R2Fe17型稀土过渡族化合物中稀土磁矩与过渡族磁矩之间交换耦合常量的方法,并据此计算了R2Fe17-xAlx(R=Tb,Dy,Ho,Er,Gd,x=7或8)化合物中稀土磁矩与过渡族磁矩之间的交换耦合常量.计算结果与实验值符合较好.
关键词:
2Fe17-xAlx化合物')" href="#">R2Fe17-xAlx化合物
交换耦合常量 相似文献
4.
通过X射线衍射和磁性测量等手段研究了(Nd1-xGdx)3Fe27.31Ti1.69(0≤x≤0.6)化合物的结构和磁性.X射线衍射测量结果表明Gd替代后并未改变Nd3(Fe,Ti)29化合物的晶体结构,但引起了晶胞体积收缩.随着Gd含量的增加,化合物的居里温度TC和室温磁晶各向异性场Ba单调增加,而自旋重取向
关键词:
1-xGdx)3Fe27.31Ti1.69化合物')" href="#">(Nd1-xGdx)3Fe27.31Ti1.69化合物
磁晶各向异性
自旋重取向
磁相图 相似文献
5.
本文对Nd-Fe-Si三元系富铁区域相的结构和磁性进行了研究。结果表明,Nd-Fe-Si三元系富铁区域(Fe>40at%),除出现NdFe2Si2三元金属间化合物外(Si>20at%),同时只出现Nd2(Fe,Si)17赝二元金属间化合物,其中Si取代9d位的Fe原子,而不能形成类似于Nd2Fe14B的三元金属间化合物,Si取代Nd2Fe17中的9d位Fe原子后,使晶胞体积缩小;使饱和磁化强度减小;同时使Fe次晶格的铁磁相互作用增强,导致居里温度增高;还使得Fe次晶格的易面各向异性减弱,造成室温下各向异性场减小。
关键词: 相似文献
6.
研究了处于永磁体强磁场中Mn1.2Fe0.8P1-xSix 系列化合物的热磁发电性能, 采用高性能球磨和固相烧结合成方法制备了Mn1.2Fe0.8P1-xSix 系列化合物, 并对该系列化合物的物相结构、磁性和热磁发电性能进行了测量. 结果表明: Mn1.2Fe0.8P0.37Si0.63和Mn1.2Fe0.8P0.35Si0.65化合物是具有Fe2P型六角结构的一级相变软磁性材料, 两者居里温度分别为334 K和348 K, 处于工业余热温区. 根据一级相变磁性材料在居里温度磁化强度发生突变这一特性, 研制热磁发电演示装置, 测量了Mn1.2Fe0.8P0.37Si0.63和Mn1.2Fe0.8P0.35Si0.65这两种材料铁磁相变产生感应电流大小与线圈匝数、热磁发电材料质量、表面积、表面上温度梯度的关系. 研究结果表明, Mn1.2Fe0.8P1-xSix系列化合物具有很好的热磁发电性能, 有望成为热磁发电候选材料. 相似文献
7.
研究了Mn42Al50-xFe8+x合金的结构、磁性和磁热效应. 通过成分调节, 居里温度TC在室温附近一宽温区连续可调, 分别为270 K (Mn42Al42Fe16), 341 K (Mn42Al40Fe18)和370 K(Mn42Al38Fe20). 磁化强度在相变温度处发生一陡降, 热磁曲线和等温磁化曲线均未观察到热和磁的滞后, 表明发生一可逆的二级相变. 在各自居里温度附近, 0-5 T的外磁场变化下磁熵变峰值分别为2.48, 2.52和2.40 J·kg-1·K-1. Mn50-xAl50-yFex+y合金的磁熵变峰值虽然与许多优良的磁制冷材料相比并不大, 但是制备该化合物的原材料价格非常低廉, 制备工艺简单, 加工成型也较容易, 化合物本身耐腐蚀性、延展性较好, 且在居里温度附近发生的是可逆的二级相变, 无晶格或结构的变化, 有利于制冷剂的多次循环使用.
关键词:
磁性
磁热效应
二级相变 相似文献
8.
9.
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
10.
11.
The magnetic properties (magnetic ordering temperature, magnetization) of the ferrimagnetic compounds R
2Fe17 and RFe11Ti, as well as of their hydrides and nitrides, were studied. The hydrogenation-and nitrogenation-induced variation of the
exchange fields acting on the rare-earth (RE) ions from both the Fe sublattice and other RE ions was determined, and the dependence of the Curie temperatures of the starting compounds, their hydrides, and nitrides
on the de Gennes factor was revealed. It was found that incorporation of light atoms (H, N) into the crystal lattices of RFe11Ti and R
2Fe17 increases the Curie temperature T
C substantially, increases the Fe-Fe exchange coupling, and decreases the R-R exchange interactions, as well as increases the R-Fe intersublattice exchange under hydrogenation and decreases it under nitrogenation, an effect that can be understood as
resulting from the attendant changes in the electronic structure of these compounds and in the indirect exchange interactions.
__________
Translated from Fizika Tverdogo Tela, Vol. 45, No. 10, 2003, pp. 1850–1856.
Original Russian Text Copyright ? 2003 by Nikitin, Tereshina. 相似文献
12.
Haiying Chen Yan ZhangJingzhi Han Honglin DuChangsheng Wang Yingchang Yang 《Journal of magnetism and magnetic materials》2008
A series of R2Fe17 (R=Sm, Gd, Tb, Dy, Er) have been synthesized. The magnetocaloric effect (MCE) of these compounds has been investigated by means of magnetic measurements in the vicinity of their Curie temperature. The Curie temperature of Er2Fe17 is 294 K. The maximum magnetic entropy change of Er2Fe17 under 5 T magnetic field is ∼3.68 J/kg K. In the R2Fe17 (R=Sm, Gd, Tb, Dy, Er) system, the maximum magnetic entropy change under 1.5 T magnetic field is 1.72, 0.89, 1.32, 1.59, 1.68 J/kg K corresponding to their Curie temperature (400, 472, 415, 364, 294 K), respectively. 相似文献
13.
14.
通过x射线衍射及磁测量手段研究了Y2(Fe1-y-x,Coy,C rx)17化合物的结 构及居里温度.研究结果表明Y2(Fe1-y-x,Coy,Crx)17化合物具有六 角相的Th2Ni17型结构.随着x的增加,Y2(Fe
关键词:
2(Fe1-y-x')" href="#">Y2(Fe1-y-x
y')" href="#">Coy
x)1 7化合物')" href="#">Crx)1 7化合物
x射线衍射
居里温度 相似文献
15.
In this paper the values of the crystalline-electric-field
parameters Anm for R2Fe17 and
R2Fe17H3 (R=Tb,Ho,Er) are evaluated by fitting
calculations to the magnetization curves measured on the single
crystal at several temperatures. The fitted Anm for
R2Fe17 are strikingly different from those for the
corresponding R2Fe17H3. The energy gaps between the
lowest four energy levels for Ho ions in Ho2Fe172 can be
reproduced by using the fitted Anm and exchange field
2μBHex, which estimated from the fit of the
temperature dependence of the spontaneous magnetization combined
with inelastic neutron scattering experiment. 相似文献
16.
The structural stability of the intermetallic compounds R2Co17 and R2Co17T (T=Be, C) is tested by many means including random atom shifts, global deformations and high temperature disturbances under the control of the pair potentials. The structure type and crystal constants of R2Co17 and R2Co17Be are close to experimental results. The addition of Be and C in the interstice of R2Co17 causes a decrease of the cohesive energy, and Be and C only occupies the 9e interstitial site with the Th2Zn17-type structure or the 6h interstitial site with the Th2Ni17-type structure. All the above results indicate that the potentials are valid for studying the structural properties of these kinds of anisotropy materials. 相似文献
17.
The crystal and magnetic structures of Nd2Fe14Si3 at room temperature were refined by Rietveld analysis of neutron-powder-diffraction data. It was found that silicon atoms occupy preferentially both 18h and 18f of Th2Zn17-type structure with occupancies 0.36 and 0.14, respectively, The Fe-Fe bond-lengths computed with the refined crystallographic parameters have optimum values, as compared with those of Nd2Fe17 compounds, which can explain well why the Curie temperature rises strongly when the unit cell volume reduces with the substitution of silicon for iron in Nd2Fe17. 相似文献