Spin-Dependent Scattering and Giant Magnetoresistance in Magnetic Granular Films

Based on a macroscopic theory in which the spin-dependent interface scattering and the bulk scattering are included, the transport properties in systems of cylindrical magnetic granules are investigated analytically. It is shown that the giant magnetoresistance as well as the resistivities of these systems depend strongly on the size of the granules.     

磁电子学讲座 第九讲 金属磁性多层膜的结构及其对巨磁电阻效应的影响

介绍了金属磁性多层膜的微结构和磁结构的研究进展,简要综述了磁性多层膜的结构与巨磁电阻（ＧＭＲ）之间的关系     

On a random graph with immigrating vertices: Emergence of the giant component

A randomly evolving graph, with vertices immigrating at rate n and each possible edge appearing at rate 1/n, is studied. The detailed picture of emergence of giant components with O(n^2/3) vertices is shown to be the same as in the Erdős–Rényi graph process with the number of vertices fixed at n at the start. A major difference is that now the transition occurs about a time t=π/2, rather than t=1. The proof has three ingredients. The size of the largest component in the subcritical phase is bounded by comparison with a certain multitype branching process. With this bound at hand, the growth of the sum‐of‐squares and sum‐of‐cubes of component sizes is shown, via martingale methods, to follow closely a solution of the Smoluchowsky‐type equations. The approximation allows us to apply results of Aldous [Brownian excursions, critical random graphs and the multiplicative coalescent, Ann Probab 25 (1997), 812–854] on emergence of giant components in the multiplicative coalescent, i.e., a nonuniform random graph process. © 2000 John Wiley & Sons, Inc. Random Struct. Alg., 17: 79–102, 2000     

三明治结构与同轴电缆结构磁性材料巨磁阻抗效应的理论研究

根据两种具有巨磁阻抗（GMI）效应的磁性材料实验样品，提出了两种理论模型（同轴电缆结构——Cu丝外覆软磁材料的圆柱形；三明治结构——Cu或Ag为中间层外包软磁层的三明治膜），利用Maxwell方程和Landau_Lifshitz方程对其GMI效应的机理进行了理论研究.证明了两种模型的差别仅仅是形状因子的不同，从而由理论上证实了两种结构GMI效应增强的内在一致性.证实了在同种磁性材料情况下，双层结构具有结构方面的优越性.并对照实验数据讨论了参数的影响，得到与实验定性相符的结果. 关键词： 巨磁阻抗效应 三明治膜 Maxwell方程 Landau_Lifshit     

Study of the first-excited K π=0+ and 2+ bands in 228Th in the 226Ra(α,2n) reaction

Excited bands of ²²⁸Th were studied in the ²²⁶Ra(α,2n) reaction by gamma-ray and conversion-electron spectroscopy. The first-excited K ^π=0⁺ and 2⁺ bands were identified up to I ^π= 12⁺ and 10⁺, respectively. The spin dependence of the moments of inertia is discussed. The experimental data indicate a structural change of these bands from ²²⁸Th to ²³⁰Th and ²³²Th. Received: 11 August 1997 / Revised version: 19 September 1997     

射频溅射功率对FeZrBCu软磁合金薄膜巨磁阻抗效应的影响

用射频溅射法制备了FeZrBCu软磁合金薄膜.研究了不同溅射功率对FeZrBCu薄膜软磁特性和巨磁阻抗效应的影响.用电子探针显微镜测量发现，当溅射功率为240W时，薄膜样品中Fe的原子含量为8732%，Cu的原子含量为29%.这种样品的矫顽力最小，为68A/m，饱和磁化强度约为111×105⁵A/m，软磁性能最佳，巨磁阻抗效应最大，溅态膜在 13MHz最大巨磁阻抗比纵向为17%，横向为11%.重点分析了阻抗的电阻、电感分量及横向有 效磁导率随频率的变化，得到在低频下主要是磁电感 关键词： 铁基合金 薄膜 巨磁阻抗效应     

核电荷半径的同位旋相关性及其微观诠释

原子核电荷半径R_c所有的实验数据都表明, R_c系统偏离A^1/3律, 即随A增大R_c/A^1/3系统地递减, 而R_c/Z^1/3则比较接近于一个常量. 原子核巨单极共振能量E_x ∝ R^－1的大量实验数据也支持这一结论. 根本原因在于A^1/3律与同位旋无关, 而Z^1/3律已部分反映了同位旋的影响. 基于壳模型, 给出了Z^1/3律的微观诠释. 壳模型中质子和中子谐振子势强度参数ω_p和ω_n的差异, 可以用Z^1/3律说明. 基于与Wigner的原子核同位旋多重态质量公式(IMME)相似的理论考虑, 提出了核电荷半径改进的Z^1/3律.     

巨单极共振和对称能

基于带有混合同位旋标量-矢量非线性耦合的有效拉格朗日量, 在完全自洽的相对论无规位相近似的框架内, 通过单极压缩模式讨论了核物质的不可压缩性. 比较核²⁰⁸Pb,¹⁴⁴Sm,¹¹⁶Sn和⁹⁰Zr实验和计算的巨单极共振能量, 给出了核物质不可压缩系数的取值范围. 新的同位旋标量-矢量非线性耦合软化核物质的对称能, 但无损于基态性质与实验的一致性. 讨论了对称能的软化对巨单极共振的影响.     

On tree census and the giant component in sparse random graphs

For each of the two models of a sparse random graph on n vertices, G(n, # of edges = cn/2) and G(n, Prob (edge) = c/n) define t_n(k) as the total number of tree components of size k (1 ≤ k ≤ n). the random sequence {[t_n(k) - nh(k)]n^?1/2} is shown to be Gaussian in the limit n →∞, with h(k) = k^k?2c^k?1e^?kc/k! and covariance function being dependent upon the model. This general result implies, in particular, that, for c> 1, the size of the giant component is asymptotically Gaussian, with mean nθ(c) and variance n(1 ? T)^?2(1 ? 2Tθ)θ(1 ? θ) for the first model and n(1 ? T)^?2θ(1 ? θ) for the second model. Here Te^?T = ce^?c, T<1, and θ = 1 ? T/c. A close technique allows us to prove that, for c < 1, the independence number of G(n, p = c/n) is asymptotically Gaussian with mean nc^?1(β + β²/2) and variance n[c^?1(β + β²/2) ?c^?2(c + 1)β²], where βe^β = c. It is also proven that almost surely the giant component consists of a giant two-connected core of size about n(1 ? T)β and a “mantle” of trees, and possibly few small unicyclic graphs, each sprouting from its own vertex of the core.     

Thermal Stability of Ni-Fe/Co/Au/Co GMR Pseudo-Spin-Valves

Pseudo-spin-valves (PSV) structures, Ni₈₃Fe₁₇-3 nm / Co-2.5 nm / Au-t _Au / Co-2.5 nm, with 2.4t _Au3.2 nm were deposited by UHV magnetron sputtering. The weak ferromagnetic coupling J2×10^-6 J/m² between Ni-Fe/Co and Co layers and GMR effect 3% was found at RT. The GMR amplitude decreases monotonically from 5% at -100°C to 1% at 200°C. However, the slope of R(H) curve, i.e., GMR field sensitivity, is equal to about 1.5%/Oe and remains almost constant in the entire investigated temperature range. Additionally, our PSV display a good thermal stability, with no significant changes of magnetic and transport properties after annealing up to 250°C.