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141.
142.
在二维正方Heisenberg铁磁系统的基础上建立了磁振子-声子相互作用模型. 利用松原格林函数理论研究了系统的声子衰减,计算了布里渊区的主要对称点线上的声子衰减曲线. 发现在第一布里渊区,在Δ线上,横向声频支声子无衰减,在Z线上,纵向声频支声子无衰减;横向声频支声子衰减比纵向声频支声子衰减至少大一个数量级,并讨论了各项参数的变化对横向声频支声子衰减与纵向声频支声子衰减的影响. 根据声子衰减与声子寿命的关系,声子衰减与声子态密度的关系,可以讨论横向声频支声子与纵向声频支声子的寿命与态密度.
关键词:
磁振子-声子相互作用
横向声频支声子衰减
纵向声频支声子衰减
声子寿命 相似文献
143.
制备了Nd28Fe66B6/Fe50Co50多层纳米复合磁性薄膜,对溅射态和650℃退火处理15 min试样的相成分分析和微结构的观察显示,溅射态薄膜呈非晶态,经650℃退火处理15 min后,薄膜主要相成分为硬磁性Nd2Fe14B相和软磁性相FeCo(110)相.Nd2Fe14B相呈柱状,其易磁化c轴垂直于膜面,尺寸约10 nm.在硬磁性相和软磁性相之间存在少量富Nd相和非晶态,富Nd相大小约7 nm.磁性测量和分析表明,1)该系列薄膜退火态具有垂直于膜面的磁晶各向异性.2)对于固定厚度(10 nm)层Nd-Fe-B和不同厚度(tFeCo=1—100 nm)层FeCo多层纳米复合膜,剩磁随软磁相FeCo 厚度的增加快速增加,而矫顽力则减小.当tFeCo=5 nm时,最大磁能积达到200 kJ/m3. 3)硬磁相Nd-Fe-B层和软磁相FeCo层之间交换耦合导致剩磁和磁能积增强.
关键词:
Nd-Fe-B/FeCo多层纳米复合膜
交换耦合
磁各向异性 相似文献
144.
采用多晶材料趋近饱和定律研究了非晶Fe39.4-xCo40Si9B9Nb2.6Cux(x=0.5,1,1.5) 合金在不同温度纳米晶化后的有效磁各向异性常数〈K〉.结果表明, Cu含量较低(x=0.5)时,纳米晶粒较大并且在较低的退火温度(550℃)下析出硬磁相,〈K〉随退火温度Ta升高显著增加;随着Cu含量的增加,有效地细化了晶粒,并且抑制了硼化物的析出,〈K〉明显减小.讨论了〈K〉与晶粒尺寸D及初始磁导率的关系.
关键词:
纳米晶
有效磁各向异性
磁导率
FeCo基合金 相似文献
145.
Karen B. Paul 《Central European Journal of Physics》2007,5(1):11-24
Fe(2 ML)/V(y ML) and interleaved Fe(2 ML)/V(y ML)/Fe(3 ML)/V(y ML) superlattice systems with spacer thicknesses, y, (4 ≤ y ≤ 17) were investigated macro-magnetically to estimate the coupling strength and the magnetoresistance in these materials,
and particularly in the antiferromagnetically coupled monolayers. The results from the magnetic and magnetoresistive measurements
indicate that adding one monolayer of Fe increases the antiferromagnetic coupling and the magnetoresistivity ratio from 0.0075
mJ/m2 at 20 K and 2 % at 10 K for Fe(2 ML)/V(y ML), to 0.05 mJ/m2 and 2.5 % for Fe(2 ML)/V(y ML)/Fe(3 ML)/V(y ML) at the same temperatures. Both systems exhibit in-plane magnetic and magnetoresistive isotropy, therefore the increase
of the conferred physical parameters is attributed mainly to the stresses at the interface as governing mechanisms over the
magnetoelastic forces.
相似文献
146.
Boltzmann-transport equation is analytically solved for two-component magnetoplasma using Chapman-Enskog analysis to include
collisional diffusion transport having anisotropies in both streaming velocity and temperature components. The modified collisional
integrals are analytically solved with flux integrals and perturbed kinetic equation to arrive at drift diffusion velocity
and resulting transport coefficients which are markedly affected by both streaming and temperature anisotropy. The early isotropic
results are recovered in the limit V
0 = 0 and T
‖ = T
⊥ which reduce to eqs (11.30) and (11.31) of [1] and eqs (2.7) and (2.13) of [2]. The electrical resistivity (η⊥) diminishes sharply in fusion temperature limit kT
⊥ = 1 keV. The shape of the curves for both electrical resistivity and thermal conductivity is rectangular hyperbolic. However,
for low thermal ratio (T
‖/T
⊥ < 1), the curves are raised up and for high thermal ratio (T
‖/T
⊥ > 1), they are lowered down the isotropic case (T
‖/T
⊥ > 1), showing comparatively diminished magnitudes of the quantities.
相似文献
147.
晶粒间界相对纳米Nd_2Fe_(14)B各向异性和矫顽力的影响 总被引:1,自引:0,他引:1
本文采用立方晶粒结构模型研究了晶粒间界相对纳米硬磁材料各向异性和矫顽力的影响.结果表明:晶粒间界相减弱了交换耦合作用.当晶粒尺寸D为定值时,随着晶粒间界相厚度d的增加,晶粒平均各向异性单调增加,而材料的有效各向异性Keff、矫顽力单调减小.我们计算的矫顽力随晶粒尺寸的变化与相关理论和实验结果基本一致. 相似文献
148.
M. Patra K. De S. Majumdar S. Giri 《The European Physical Journal B - Condensed Matter and Complex Systems》2007,58(4):367-371
We observe the negative shift of the magnetic hysteresis loop at 5 K, while the sample is cooled in external magnetic field
in case of 30% of Fe substitution in LaMnO3. The negative shift and training effect of the hysteresis loops indicate the phenomenon of exchange bias. The cooling field
dependence of the negative shift increases with the cooling field below 7.0 kOe and then, decreases with further increase
of cooling field. The temperature dependence of the negative shift of the hysteresis loops exhibits that the negative shift
decreases sharply with increasing temperature and vanishes above 20 K. Temperature dependence of dc magnetization and ac susceptibility
measurements show a sharp peak (Tp) at 51 K and a shoulder (Tf) around 20 K. The relaxation of magnetization shows the ferromagnetic and glassy magnetic components in the relaxation process,
which is in consistent with the cluster-glass compound. 相似文献
149.
M. C. Desjonquères C. Barreteau G. Autès D. Spanjaard 《The European Physical Journal B - Condensed Matter and Complex Systems》2007,55(1):23-27
We show that considerable orbital magnetic moments and magneto-crystalline anisotropy energies are obtained for a Fe monatomic
wire described in a tight-binding method with intra-atomic electronic interactions treated in a full Hartree Fock (HF) decoupling
scheme.
Even though the use of the orbital polarization ansatz with simplified Hamiltonians leads to fairly good results when the
spin magnetization is saturated this is not the case of unsaturated systems. We conclude that the full HF scheme is necessary
to investigate low dimensional systems. 相似文献
150.
Summary Exact solutions are obtained in the framework of the classical theory of laminates subjected to the action of normal moments,
double forces, double moments or momentless double dipoles. Seven cases of such loads are considered and completed by considering
the case of given transversal discontinuity of normal deflection. It is shown that, in contrast to the case of infinite straight
dislocations in a pure in-plane problem, the energy of this eighth solution depends on the discontinuity orientation. Some
numerical examples are presented. Besides the formal value, the obtained double-force and double-moment solutions, as well
as dimensionless double dipoles, can be used to construct kernels of additional boundary integral equations (BIE). Due to
the coupling phenomena in the BIE system for the region with a corner point, additional variable such as corner forces appear
and require the mentioned equation.
Received 22 June 1999; accepted for publication 6 March 2000 相似文献