Nucleon octet in a relativistic logarithmic potential

A simple independent-quark-model based on the Dirac equation with logarithmic potential is used to calculate several properties of octet baryons such as magnetic moment, the axial vector coupling constantg _A (n) for neutronβ-decay and the charge radius of the proton. In view of the simplicity of the model, the results obtained are quite good.     

LD泵浦的Nd：YAG调Q激光器腔内倍频研究

DPL的调Q倍频是获得高重复率绿光输出的有效方法,本文研究了这种激光器的动态特性,提出存在使转换效率最高的最佳非线性耦合系数,它是调Q时反转粒子数超阈值倍数的函数.实验用国产200mWR的MQW—LDA泵浦Nd:YAG激光器,声光调Q,KTP腔内倍频,输出0.4μJ的倍频光,脉宽70ns,峰功率6W.     

非线性Schrōdinger方程和非线性Klein-Gordon方程耦合组Cauchy问题整体经典解的存在唯一性

本文讨论非线性Schrōdinger方程和非线性Klein-Gordon方程耦合组的Cauchy问题,对初值和空间维数以及非线性项加以适当限制,在Sobolev空间框架下,得到了整体经典解的存在唯一性。     

青藏高压东侧偏北大风对梅雨暴雨影响的合成分析

利用常规观测资料对1991～1996年江淮地区梅雨大暴雨期的高、低层流场进行合成诊断分析,结果表明,梅雨期暴雨时,在对流层上部,由于青藏高原向东扩、在高压东侧出现偏北大风轴,由此构成的高空辐射区随着高压的东移而东移,它常常位于低空急流前端的上空、形成上层东北风,下层西南风的特殊耦合关系。     

基于线计算的全加器设计

随着集成电路特征尺寸的不断缩小, 互连线在芯片内部占的比重越来越大, 但是互连线仅用于数据传输, 芯片计算能力仍然需要依靠晶体管开关实现. 如何在有限的硬件资源内进一步提高芯片的计算能力, 已经成为当前集成电路设计的核心问题. 本文通过研究金属互连线间电容耦合效应, 采用互连线串扰现象完成逻辑运算的思想, 提出一种基于线计算的全加器设计方案. 该方案首先建立线计算模型, 通过调整反相器阈值和不同干扰线与受扰线之间电容耦合强度匹配技术, 采用相同线计算电路结构实现不同功能的逻辑门电路; 然后, 在逻辑门的基础上实现基于线计算的全加器; 最后, 在TSMC 65nm CMOS工艺下仿真验证. 结果表明, 所设计的线计算电路具有正确逻辑功能, 与传统设计方法相比, 线计算逻辑门具有更低开销, 且线计算电路具有抗逆向工程能力.     

Single quantum dot nanolaser

Recent theoretical and experimental progress on nanolasers is reviewed with a focus on the emission properties of devices operating with a few or even an individual semiconductor quantum dot as a gain medium. Concepts underlying the design and operation of these devices, microscopic models describing light‐matter interaction and semiconductor effects, as well as recent experimental results and lasing signatures are discussed. In particular, a critical review of the “self‐tuned gain” mechanism which gives rise to quantum‐dot mode coupling in the off‐resonant case is provided. Furthermore recent advances in the modeling of single quantum dot lasers beyond the artificial atom model are presented with a focus on the exploration of similarities and differences between the atomic and semiconductor systems.     

Large coercivity and unconventional exchange coupling in manganese-oxide-coated manganese gallium nanoparticles

The microstructures and magnetic properties of nanoparticles, each composed of an antiferromagnetic （AFM） manganese-oxide shell and a ferromagnetic-like core of manganese-gallium （MnGa） compounds, are studied. The coreshell structure is confirmed by transmission electron microscope （TEM）. The ferromagnetic-like core contains three kinds of MnGa binary compounds, i.e., ferrimagnetic （FI） DO22-type MnaGa, ferromagnetic （FM） Mn8Gas, and AFM DO19-type Mn3Ga, of which the first two correspond respectively to a hard magnetic phase and to a soft one. Decoupling effect between these two phases is found at low temperature, which weakens gradually with increasing temperature and disappears above 200 K. The exchange bias （EB） effect is observed simultaneously, which is caused by the exchange coupling between the AFM shell and FM-like core. A large coercivity of 6.96 kOe （1Oe = 79.5775 A·m^-1） and a maximum EB value of 0.45 kOe are achieved at 300 K and 200 K respectively.     

Persistent spin current in a quantum wire with weak Dresselhaus spin——orbit coupling

The spin current in a parabolically confined semiconductor heterojunction quantum wire with Dresselhaus spin--orbit coupling is theoretically studied by using the perturbation method. The formulae of the elements for linear and angular spin current densities are derived by using the recent definition for spin current based on spin continuity equation. It is found that the spin current in this Dresselhaus spin--orbit coupling quantum wire is antisymmetrical, which is different from that in Rashba model due to the difference in symmetry between these two models. Some numerical examples for the result are also demonstrated and discussed.     

Spin–orbit stiffness of the spin‐polarized electron gas

In a spin‐polarized electron gas, Coulomb interaction couples the spin and motion degrees of freedom to build propagating spin waves. The spin wave stiffness S_sw quantifies the energy cost to trigger such excitation by perturbing the kinetic energy of the electron gas (i.e. putting it in motion). Here we introduce the concept of spin–orbit stiffness, S_so, as the energy necessary to excite a spin wave with a spin polarization induced by spin–orbit coupling. This quantity governs the Coulombic enhancement of the spin–orbit field acting of the spin wave. First‐principles calculations and electronic Raman scattering experiments carried out on a model spin‐polarized electron gas, embedded in a CdMnTe quantum well, demonstrate that S_so = S_sw. Through optical gating of the structure, we demonstrate the reproducible tuning of S_so by a factor of 3, highlighting the great potential of spin–orbit control of spin waves in view of spintronics applications. (© 2016 WILEY‐VCH Verlag GmbH &Co. KGaA, Weinheim)