化合物半导体-绝缘体界面的界面态(续)

 三、界面态连续体的动态响应和分布多年来的大量研究结果表明把界面态处理为局域在半导体界面平面处的经典理论完全不能够解释化合物半导体-绝缘体界面的行为特点,从而使人们逐渐认识到界面态的空间分布特征.图3为半导体界面的能带结构示意图.在实际的I-S界面上,界面态是在绝缘体-半导体界面附近,在能量上和空间上的连续分布体(如图中点所示). 这里以n型半导体为例,通过绝缘体中的界面态对电子的捕获和发射过程说明界面态动态响应的特点.由于势垒△Ec的存在,空间分布的界面态与电子的作用只能依介量子力学的隧道效应得以进行.     

核内核子-核子弹性散射截面

通过对标量、矢量介子场引入动量-密度相关的耦合常数,能够同时重现核物质饱和态性质、能量依赖的相对论光学势以及核内核子平均自由程的实验结果.并用这套耦合常数计算了核内核子-核子弹性散射截面,结果表明,在某些能量区域密度依赖很明显而必须加以考虑.     

Hill统计量的渐近正态性

的正整数。此后,统计量γ_n的渐近性质被广泛地加以研究。Mason证明了γ_n是弱相容的,同时指出:如果k_n=[n~β],0<β<1,那末γ_n也是γ的强相容估计。[3]和[4]讨论了γ_n的渐近正态性;作为正则变化函数性质的一个应用,[5]中对此亦有讨论。本文将在d.f.F连续这一假定下,揭露γ_n的分布与一个条件iid的rv阵列行和的     

一种新的奇偶非线性相干态及其量子统计性质

定义了一种新的奇偶非线性相干态即算符B2[B=af(N)]的两个正交归一本征态,利用数值计算方法研究了它们的量子统计性质.结果表明,与通常的奇偶相干态不同,在参数|β|变化的某些范围内,只有偶非线性相干态可以存在压缩效应,而振幅平方压缩和反聚束效应在这两个态中均可以呈现 关键词： 新的奇偶非线性相干态 压缩 振幅平方压缩 反聚束效应     

单线态氧(~1O_2)与咪唑1,4-环加成反应的理论研究

本文用量子化学从头计算方法对单线态氧(~O_2)与咪唑环加成反应的机理进行了理论研究.用能量梯度法优化获得了实验上尚未检测到的侧式桥环过氧化物(endoperoxde)的结构,并在势能面上确定了单线态氧与咪唑1,4-环加成反应的过渡态.通过对过渡态的结构特征,虚振动方向,电荷分布情况以及轨道相互作用的分析,说明这个反应的机理是同步和协同的;正反应的活化势垒为69.5kJ·mol~(-1),逆反应的活化势垒为140.4kJ·mol~(-1)(6-31G的结果).     

磁场对氩原子ArI5p[3/2]2能态碰撞消激发与碰撞消取向的影响

在空心阴极放电激光诱导荧光实验中，当加强外磁场于观察方向，采用“魔角”激发，对氩原子ArI5p［3/2］₂能态，外磁场强度越强，则碰撞消激发速率越快，而碰撞消取向速率反而越慢，其总的效果是导致弛豫曲线的衰减速率随磁场强度增强而变缓．ArI5p［3/2］₂的自然能级寿命在不加外磁场情况下为120±5ns． 关键词：     

随机删失半参数回归模型中估计的渐近性质

设Y是表示生存时间并遵从下面半参数模型Y=Xβ+g(T)+ε的随机变量,(X,T)是取值于R×[0,1]上的随机变量,β是未知参数,g(·)是[0,1]上的未知回归函数,ε是随机误差。当Y因受某种随机干扰而被随机右删失时,就删失分布未知的情形分别定义了β与g(·)的估计^{^}β_n与^{^}g_n(·),在一定条件下证明了^{^}β_n的渐近正态性,并得到了^{^}g_n(·)的最优收敛速度。     

Realization of Greenberg-Horne-Zeilinger （GHZ） and W Entangled States with Multiple Superconducting Quantum-Interference Device Qubits in Cavity QED

An alternative scheme is proposed for generating the Greenberg-Horne-Zeilinger （GHZ） and W types of the entangled states with multiple superconducting quantum-interference device （SQUID） qubits in a single-mode microwave cavity field. In this scheme, there is no transfer of quantum information between the SQUIDs and the cavity, the cavity is always in the vacuum and thus the requirement on the quality of cavity is greatly loosened. In addition, during the process of the generation of the W entangled state, the present method does not involve a real excitation of intermediate levels. Thus, decoherence due to energy relaxation of intermediate levels is minimized.     

Controlled Bidirectional Quantum Direct Communication by Using a GHZ State

A controlled bidirectional quantum secret direct communication scheme is proposed by using a Greenberger- Horne-Zeilinger （GHZ） state. In the scheme, two users can exchange their secret messages simultaneously with a set of devices under the control of a third party. The security of the scheme is analysed and confirmed.     

Double-Humped Transverse Density Profile in Two-Dimensional Chute Flow with Rough Sidewalls

We study a two-dimensional granular rapid flow with rough sidewalls stuck with the same size discs by molecular dynamics simulation. A transient state of the double-humped density profile in the flowing process has been found, which appears and moves as travelling wave and is the same as the phenomena in the recent experiments [Acta Phys. Sin. 53 （2004） 3389 （in Chinese）]. Our simulation shows that the rough sidewalls play an important role in the converting momentum of boundary discs from the vertical direction to the horizontal one through particle collisions to form this profile and the good elasticity of discs ensures this effect. The appearance of the double-humped profile may be a precursor, which determines if the whole flow will be far repulsed from the boundary and become dilute eventually.