金属互连结构的电迁移失效分析新算法

综合考虑了电子风、温度梯度、应力梯度和原子密度梯度四种电迁移驱动机制, 基于ANSYS软件平台和FORTRAN程序提出一种新的电迁移失效分析算法．通过ANSYS电－热－结构耦合分析获得模型的电流密度分布、温度分布和应力分布, 基于FORTRAN编写的原子密度重分布算法获得不同时刻的原子密度, 依据空洞生成和扩展失效准则进行电迁移动态空洞演化模拟并得到失效寿命．最后, SWEAT结构与CSP结构的应用算例验证了算法的精度．     

Preparation of Entanglement and Schrodinger Cat States of Superconducting Quantum Interference Devices Qubits via Coupling to a Microwave Cavity

An alternative scheme is proposed for the generation of n-qubit W states of superconducting quantum interference devices （SQUID） in cavity QED. In this scheme, Raman coupling of two lower flux states of SQUID system is achieved via a microwave pulse and the cavity mode. Conditioned on no photon leakage from the cavity, the n-qubit W state can be generated whether the effective coupling parameters of the SQUID to cavity mode and classical microwave fields are the same or different. Our strictly numerical simulations of the time evolution of the system including decay show that the success probability of our scheme is almost unity and the interaction time is on the order of 10-9 s. The scheme can also be used to generate the Schrodinger cat states of multi-SQUID.     

Teleportation of Entangled States through Divorce of Entangled Pair Mediated by a Weak Coherent Field in a High-Q Cavity

We propose a scheme to partially teleport an unknown entangled atomic state. A high-Q cavity, supporting one mode of a weak coherent state, is needed to accomplish this process. By partial teleportation we mean that teleportation will occur by changing one of the partners of the entangled state to be teleported. The entangled state to be teleported is composed by one pair of particles, we called this surprising characteristic of maintaining the entanglement, even when one of the particle of the entangled pair being teleported is changed, of divorce of entangled states.     

冲击条件下含纳米空洞的单晶铜的塌缩

利用分子动力学方法研究了单晶铜中不同大小的球形空洞在冲击波下的演化过程.模拟结果表明不同大小空洞的塌缩过程不同.模拟中冲击波由空洞左边扫向空洞右边.在较大尺寸的空洞塌缩过程中会产生系列的位错环.当空洞半径较小时，先在空洞的右侧形成位错环，当空洞半径增大到某一临界大小时，在空洞左右两侧同时产生位错环，当空洞半径较大时，先在空洞左侧形成位错环.当空洞左右两侧的位错环均形成以后，其右侧位错环前端的生长速度大于其左侧的.空洞半径增大，相应的位错环前端的生长速度变化不大.当空洞半径增大时，空洞中心指向位错源的矢量方     

受有两级空洞损伤时韧性材料的力学行为

本文利用大应变有限元方法研究了两级空洞对韧性材料的损伤作用.模型是以轴对称圆柱基体作为胞元,内含一初始的球型空洞.基体内的应力/应变随胞元外载的增大而达到临界状态,从而在围绕初级空洞的基体内将萌生次级空洞.后者是由空单元实现的.两级空洞的交互作用被证明将促进材料中的空洞化现象从而加速损伤并导至材料的总体弹性模量值在临近破断时急剧下降.     

板材成型中的分叉和断裂及其空洞扩展效应

用平面应力有限元方法分析空洞模型以模拟一种双相钢板材在成型过程中所遇到的微空洞损伤,经试算可使模型的总体和局部的响应与已有的实验相一致,由此可提供描述该材料的损伤本构参数并研究局部剪切带和扩散型颈缩等分叉现象,临界应变值的分布形成了成型极限图中的下限曲线,当空洞模型的总体应力急剧下降或微裂纹开始出现,其相应的总体应变值提供了上限曲线。     

双稳系统在周期激励及噪声干扰作用下的数值模拟研究

利用Monte Carlor方法(MCM),对周期激励及噪声干扰作用下双稳系统的性态进行研究.获得了系统周期形式的非平稳概率分布及位移-速度联合分布.发现它们与系统势能的某些拓扑关系,在鞍点及力场零点附近的空洞(hole),在时间方向上的分叉.对跳跃和信号强度随参数变化的关系也进行了探讨.     

考虑空洞效应的共晶钎料合金粘塑性-损伤本构模型

在温度298K～398K和恒应变率10-5/s～10-3/s范围内进行一系列的拉伸实验,研究共晶焊料的力学行为,揭示空洞成核和生长变形机理的存在.提出一种考虑孔洞效应的粘塑性-损伤模型,基于Guron-Tvergaard-Needleman思想和正交法则,引入孔洞体积分数作为损伤变量以描述共晶钎料的力学特性.与实验数据比较,验证粘塑性-损伤模型对锡铅合金在恒应变率和稳态塑性流动条件下应力应变行为的预测能力.结果表明,该模型能够有效描述共晶焊料的本构行为:非线性、应变率敏感性、空洞损伤演化,并可用于分析电子封装中焊点的可靠性问题.     

Entangling Mesoscopic Squeezed Vacuum States and Mesoscopic Coherent States in Dissipative Cavity QED System

A scheme has been proposed for generating the macroscopic entanglement between the mesoscopic squeezed vacuum states and mesoscopic coherent states by considering both the two-photon interaction and the single photon interaction of N two-level atoms in cavities with high quality factor assisted by a strong driving field. Moreover, we derive the dissipative interaction models for single photon interaction and two-photon interaction, respectively. The corresponding analytical expressions of the fidelities can be given. Our scheme can be realized in the current techniques on the cavity QED.     

Scheme for Entanglement Generation of Two Atoms in Two Bad Cavities

We present a scheme for generation of two-atomic entangled state by using the interference of polarized photons. The scheme does not require complete mapping between the atomic state and the photonic state, nor does it require the establishment of maximal entanglement between the atom and the cavity. And the atom-cavity coupling strength is smaller than the cavity decay rate. This greatly relaxes the requirement on the cavity quality. The scheme is for non-post-selection results and all the steps of the scheme are within the current technologies.