金属小粒子的电子热容特性

考虑了金属小粒子电子数奇偶性、能级分离对电子热容的影响，采用随机矩阵理论对能级间距分别为等能级分布、泊松分布、正交系综分布、么正系综分布、辛系综分布的情况，详细计算了金属小粒子的电子热容，并对其高低温特点作了简单分析．     

金属小粒子的超导电性

文章利用BCS理论的推广,对金属小粒子的超导电性进行了探索.得出金属小粒子的尺寸对其超导电性产生了强烈的影响,金属小粒子的能隙不再仅是温度的函数,同时也是小粒子尺寸或者电子能间距的函数。     

金属小粒子超导电性的增强与减弱效应

用无规矩阵理论对BCS理论进行修正,得到一种处理金属小粒子超导电性的新方法,用这种方法我们发现：对于自旋s=1/2的金属小粒子,仅具有超导减弱效应;而处于s=0态的金属小粒子,同时具有超导增强和超导减弱效应,并且,金属小粒子超导电性能隙与转变的 关系与宏观金属中的非常类似。     

能级统计与金属小粒子电子比热的研究

利用随机矩阵理论，在能级间距分别为等能级分布、泊松分布、正交系综分布、么正系综分布及辛系综分布的情况下，对含电子数为奇数和偶数的金属小粒子的电子比热进行了理论计算；并对其高低温特点作了讨论．     

高斯正交系综中金属小粒子的超导电性

利用推广的BCS场理论，考虑随机矩阵理论的能级统计，得到了适合奇偶两种电子数的金属小粒子能隙和超导转变温度的统一公式．计算结果表明，对于总自旋为零的、服从高斯正交系(GOE)的金属小粒子，可以从理论上定性再现其随其尺寸变小，所出现的超导电性先增强后衰减到零、连续变化的实验现象，说明了此类现象与库仑堵塞和能谱统计有关。     

金属小粒子超导电性的尺寸效应及其形成机制

利用推广的BCS平均场理论, 考虑随机矩阵理论所给予的能级统计和关联, 推导得出了适合奇偶两种电子数宇称的统一公式, 将公式用到3个Gauss系综的计算结果表明, 对于总自旋为零的Gauss正交系综(GOE)和Gauss幺正系综(GUE)中的金属小粒子, 可以从理论上再现金属小粒子随其尺寸变小, 所出现的超导电性先增强后衰减到零连续变化的实验现象, 而对Gauss辛系综(GSE)中的金属小粒子, 只有超导电性逐步衰减到零的现象. 经分析发现, 金属小粒子的超导增强现象来自于电子配对、轨道自旋耦合强度与外磁场强度的平衡, 而后者只有在计算中考虑系综的能谱统计特征才能体现.     

金属小粒子超导电性研究

摘要用统计系综理论对遵从高斯正交系综的所有金属小粒子的不同自旋态S     

金属小粒子超导电性研究

用统计系统理论对遵从高斯正交系统的所有金属小粒子的不同自旋态SZ＝0,1／2,1,3／2,2,5／2…进行了研究,发现以上各态均存在临界能间距dc/△（0）＝13．81,1．85,0．81,0．50,0．36,0．28…随着粒子尺寸的减小,其超导电性终究会消失;金属小粒子自旋态越高,临界能间距dc越小,对自旋SZ＝0的态,确实存在超导增强效应。     

金属小粒子磁场下的电子热容特性

考虑金属小粒子在磁场下。应用随机矩阵理论对能间距分别为正交系综分布、么正系综分布、辛系综分布等情况，考虑了奇偶效应，计算了几个典型温度下金属小粒子电子热容，并对电子热容随磁场变化做了简单的分析．     

磁场中的超导金属小粒子

将平均场方法同无规矩阵理论结合用于研究外加磁场对不同自旋s基态金属小粒子超导电性的影响。我们发现，超导电性仍然会随着粒子尺寸的减小而衰减；外加磁场的存在将会使得除s＞0任何态产生超导增强效应。而对s=0，超导增强效应总是存在的。     

自旋轨道耦合与自旋霍尔效应?

从巨磁阻效应正式拉开自旋电子学的序幕开始,如何控制和操纵电子的自旋自由度在学术界和工业界掀起了巨大的研究浪潮,如何产生并测量自旋流也是自旋电子学面临的重大挑战.自旋轨道耦合为自旋电子学提供了利用全电学来控制自旋的物理基础,由自旋轨道耦合引起的自旋霍尔效应则为自旋电子学提供了产生较大纯自旋流的方法.本文从1879年Edwin Hall发现的那个迷人的效应谈起,同时从自旋轨道耦合的起源来认识自旋霍尔效应,进一步探讨了如何利用其逆效应来探测自旋霍尔效应及自旋流,并简单总结了与自旋霍尔效应相关的部分新效应及新应用.     

用重整化群流方程研究铁氧体的自旋波模型

采用重整化群的方法研究铁氧体的自旋波模型,导出一组非线性流方程,并求出铁氧体自旋波模型的能谱表达式,当双子格的自旋相等时,铁氧体自旋波模型的能谱表达式退化为反铁磁自旋波模型的能谱表达式.     

量子 SK 自旋玻璃的 GT 相图

研究了量子Ｓｈｅｒｒｉｎｇｔｏｎ－Ｋｉｒｋｐａｔｒｉｃｋ自旋玻璃模型．数值计算了不同自旋值的Ｇａｂａｙ－Ｔｏｕｌｏｕｓｅ相图,并讨论了相应的自旋自相互作用及玻璃序参数．     

Al2O3：Ni^2＋晶体的自旋哈密顿参量和光谱精细结构

本文用完全对角化方法计算了Ａｌ２Ｏ３：Ｎｉ＾２＋的光谱精细结构的ＥＰＲ参量，得到了与实验相符合的结果。同时，本文首次考虑了自旋－自旋相互作用对Ｎｉ＾２＋离子的ＥＰＲ参量和光谱精细结构的影响。     

TRANSFER-MATRIX METHOD FOR SURFACE SPIN WAVES IN A SEMI-INFINITE MAGNETIC SUPERLATTICE WITH A SINGLE-ION ANISOTROPY

Surface spin waves in a semi-infinite magnetic super lattice with a single-ion uniaxial anisotropy are investigated through the transfer matrix method. The dispersion equations of surface spin waves are obtained. We find that not all the magnetic superlattice structures can excite the surface spin waves, and that the anisottropy term need not be favorable to the excitation of surface spin waves, but surely influences the values of the energy of the excited surface spin waves.     

Triplet-singlet spin relaxation via nuclei in a double quantum dot

The spin of a confined electron, when oriented originally in some direction, will lose memory of that orientation after some time. Physical mechanisms leading to this relaxation of spin memory typically involve either coupling of the electron spin to its orbital motion or to nuclear spins. Relaxation of confined electron spin has been previously measured only for Zeeman or exchange split spin states, where spin-orbit effects dominate relaxation; spin flips due to nuclei have been observed in optical spectroscopy studies. Using an isolated GaAs double quantum dot defined by electrostatic gates and direct time domain measurements, we investigate in detail spin relaxation for arbitrary splitting of spin states. Here we show that electron spin flips are dominated by nuclear interactions and are slowed by several orders of magnitude when a magnetic field of a few millitesla is applied. These results have significant implications for spin-based information processing.     

Spin electromagnetic field and dipole: A localized and quantized field

This paper investigates the structure of a spin electromagnetic (EM) field and its various physical properties. A spin EM field is an intrinsic mode of free space, which satisfies the spin equations derived from Maxwell equations. A spin mode has two basic properties: the spin along its axis and the localization of electromagnetic field. The source and EM structure of this electric and magnetic mode are described in detail in this paper. The distributed charge and current of a spin mode can be integrated to obtain the electric and magnetic moment, and they can be treated as the electromagnetic dipole. A spin mode possesses both wave and particle properties: a wave number, angular frequency and characteristic speed are its wave parameters; an intrinsic radius, energy and angular momentum are its dynamic parameters. The former is analogous to an EM resonant mode; the latter is similar to the behavior of a particle with intrinsic spin. There are two kinds of electric modes present, one can be expressed through a pair of charges, and the other can be expressed by a magnetic current. They both have the same electric moment, but have different divergence properties.     

自旋三重态超导

超导体中的库珀对通常是由一对自旋相反总自旋为零(自旋单态)的电子组成.然而,在某些特殊情况下,超导体中的库珀对可以是自旋三重态,这类超导体被称之为自旋三重态超导体.自旋三重态超导是非常罕见的量子现象,在已经发现的上万种超导体中,仅有几个超导体可能具有三重态配对.近几年,随着拓扑物态研究的深入,三重态超导体因为可能是拓扑超导的载体而越来越多地引起关注.本文简要地总结了几类可能的自旋三重态超导体的物理性质.     

Electrical detection of spin precession in a metallic mesoscopic spin valve

To study and control the behaviour of the spins of electrons that are moving through a metal or semiconductor is an outstanding challenge in the field of 'spintronics', where possibilities for new electronic applications based on the spin degree of freedom are currently being explored. Recently, electrical control of spin coherence and coherent spin precession during transport was studied by optical techniques in semiconductors. Here we report controlled spin precession of electrically injected and detected electrons in a diffusive metallic conductor, using tunnel barriers in combination with metallic ferromagnetic electrodes as spin injector and detector. The output voltage of our device is sensitive to the spin degree of freedom only, and its sign can be switched from positive to negative, depending on the relative magnetization of the ferromagnetic electrodes. We show that the spin direction can be controlled by inducing a coherent spin precession caused by an applied perpendicular magnetic field. By inducing an average precession angle of 180 degrees, we are able to reverse the sign of the output voltage.     

基于玻色约瑟夫森结的自旋压缩的相干控制

提出了利用人造原子-基于约瑟夫森结的超导量子比特产生自旋压缩的电路模型,给出了系统的有效哈密顿量.在海森堡绘景下,利用冷冻自旋近似方法得到近似解析解,进而分析了系统自旋压缩效应的调控方法.研究表明,通过调节系统粒子数或者耦合强度与有效非线性相互作用强度的比例,均可有效地调控系统的自旋压缩程度和处于自旋压缩态的时间.外场越弱,粒子数越多,系统的自旋压缩程度越强,处于自旋压缩态的时间越长.