时间反演对称性引起的自旋宇称效应

推广关于由有限重轴旋转对称性导致的自旋宇称效应的纯量子力学理论 ,建立了源于时间反演对称性的自旋宇称效应 .所涉及的量子系统既可以是单自旋的 ,也可以是多自旋的 ;所涉及的状态可以是自旋在任意轴上的投影的任意一对具有反号本征值的本征态 ;所涉及的自旋可以有任意的量子数 .结果还清楚地表明 :上述两种对称性所引起的自旋宇称效应互为补充 ,但并不等价     

SPECIFIC HEAT OF A HEISENBERG SYSTEM WITH FINITE SIZE

Based upon the spin wave theory, the influence of the size of a three-dimensional Heisenberg system on its thermodynamic properties was studied. It is found that the specific heat increases due to the finite size and free surface of the system. For a magnetic film with finite thickness, the interaction of spin waves was also discussed. There exist three additional scattering processes, namely, the scattering between spin waves with wave-vectors parallel to the surface of the film (two-dimensional spin wave), the scattering between two and three-dimensional waves, and the scattering between those waves with the same component in the direction along the thickness of the film. As a result, the T⁴ term, arising from the coupling of spin waves, in the expression of the specific heat of the system, splite into three parts proportional to T^5/2,T^7/2 and T⁴, respectively. Here T is the temperature.     

INTERLAYER EXCHANGE COUPLING IN COMPLEX MAGNETIC MULTILAYERS

We extend the hole confinement model of Edwards et al. to the problem of two kinds of complex magnetic sandwich structures. One is the magnetic sandwich covered on both sides by nonmagnetic films(case 1) and the other is that covered by magnetic films(case 2). The interlayer exchange coupling and the angular dependence of coupling energy in the two cases are investigated systematically. For case 1, our results show that the magnetic and outer nonmagnetic films influence significantly the oscillation behavior of exchange coupling and the appearance of noncollinear exchange coupling is very sensitive to the thickness of magnetic and outer nonmagnetic layers. Our results also show that the nonoscillatory component of the coupling generally varies with the thickness of magnetic(outer nonmagnetic) films and the results in the case where the thickness of both magnetic(outer nonmagnetic) films vary simultaneously are significantly different from that in the case where the thickness of one of the two magnetic(outer nonmagnetic) films is fixed while the other is varied, which is qualitatively in agreement with the experimental measurements. For case 2, the exponential dependence of exchange coupling on the thickness of the intermagnetic layer has been obtained, similar to the Parkin's experimental results for giant magnetoresistance.     

关于磁性物质的自旋位形的某些问题

本文用Lyons-Kaplan的方法,讨论了具有一种磁性离子组成的布拉维点阵的自旋位形在外磁场作用下的变化及磁晶各向异性时它的影响。存在有一个反铁磁-铁磁性结构转变的临界磁场,外磁场大于临界磁场时一切反铁磁结构都消失。磁场(小于临界磁场)和各向异性都使自旋位形的简并部分消失。最后还讨论了所得到的自旋位形的稳定性。     

反磁化形核行为的微磁学研究

本文指出,在对称情况下,微磁学中的反磁化形核问题是一个典型的分歧问题。利用对分歧问题的研究结果,在详细分析Brown方程分歧解的稳定性之后,得到的结论是:形核场是Brown方程的最大分歧点,Brown,Frei,Aharoni和Shtrikman等人用线性化方法获得的结果,包含在本文的笫一级微扰近似的结果中。不局限于线性化近似,文中还得到了形核场近旁的反磁化行为,它们或者连续地沿分歧解进行,或者是一个不连续跃变;同时,还给出了连续和不连续形核的判据。     

有限铁磁—反铁磁线链中的自旋波谱及其激发

本文研究了由交换作用耦合起来的有限长铁磁和反铁磁链组成的自旋系统。计算了系统的自旋波的波谱及其在微波场中的激发强度。在所得结果的基础上,讨论了具有反铁磁氧化层的铁磁薄膜的自旋波共振。阐明了等效地使用唯象普遍边界条件的可能性。根据理论,对等效的表面各向异性能作了估计,得到的数值与实验值很好地符合。     

高次幂交换作用的低维磁性系统相变不存在的证明

本文严格证明了各向同性高次幂海森堡模型在一维和二维的情况下不出现长程序。 关键词：     

圆柱状铁磁体中的偶极-交换自旋波

对于轴向磁化的圆柱状铁磁体,同时考虑偶极作用和交换作用,得到了偶极-交换自旋波的本征方程,给出了频谱的数值结果。当自旋波波矢β较小,即偶极能起主要作用时,相当于静磁模的结果,β较大,即交换能起主要作用时,过渡到宏观自旋波交换模理论的结果。     

外磁场中单畴反铁磁颗粒的宏观量子效应

用瞬子方法研究了外加磁场对单畴双轴反铁磁颗粒宏观量子效应的影响. 当外磁场沿易磁化方向时,简并基态中的一个能量抬高,变为亚稳态,其隧穿衰变率随外磁场增大;当外磁场沿中间磁化方向时,能级的隧穿劈裂随外磁场的变化而振荡.从而提出一种观察单畴反铁磁颗粒中宏观量子相干和隧穿现象的实验方法.     

怀念优秀的青年物理学家孟宪振

在整个中华民族蒙灾受难的“十年动乱”中 ,我国物理学也遭受了种种损失 .2 0年前 ,已经初露锋芒的青年实验物理学家和热忱的科学组织者孟宪振同志含冤离去 ,就是至今思之犹痛的损失之一 .孟宪振 ,1931年生于北平 ,194 9年考入清华大学气象系 ,1952年从物理系毕业后分配到中国科学院应用物理研究所 (后改称物理研究所 ) .1953年我国开始实行第一个国民经济五年计划 ,全国上下都在为开展大规模的经济建设而奋斗 .应用物理研究所集中主要力量 ,解决经济建设提出的迫切课题 .孟宪振等在前辈磁学家施汝为、潘孝硕、向仁生指导下 ,参加铝镍钴磁性…