激光场中正电子对反质子的辐射复合反应

在软光子近似下, 计算了激光场中正电子对反质子的辐射复合过程. 辐射场作为经典场处理, 入射正电子态用Coulomb-Volkov波函数描述, 末道形成的反氢缀饰态由含时间微扰论给出. 理论结果显示激光背景明显削弱了反氢生成截面.     

Coulomb-Volkov近似下电子在激光场中对核的相对论散射

本文在Coulomb-Volkov近似下,研究了激光场中电子对核的相对论散射.电子出射与入射态分别用Volkov波函数和Coulomb-Volkov波函数来描述.数值计算给出了辐射场修正的散射截面及其对激光强度和频率的依赖关系,并与相应的Born近似结果进行了比较.     

激光场中正电子对氢原子的电离反应

本文在一级Bom近似下，研究了激光场中正电子对基态氢原子的碰撞电离反应，并与入射粒子为电子的（e，2e）反应进行了对比．激光场中正电子态和敲出电子态分别采用Volkov波函数和Coulomb-Volkov波函数，靶原子的缀饰波函数由含时微扰论给出．计算结果显示激光缀饰的三重电离截面明显依赖于入射粒子电荷符号．激光越强，二者差距越大．     

应用迈克耳孙干涉仪研究压电陶瓷的特性

简述了应用迈克耳孙干涉仪测量压电陶瓷压电常量的原理及实验结果分析.简单介绍了研究压电陶瓷振动特性的方法.     

Delocalization of Quantum Kicked Rotator with a Large Denominator

We use the iterative unitary matrix multiplication method to calculate the long-time behaviour of the resonant quantum kicked rotator with a large denominator. The delocalization time is an exponential function of the denominator. The wave function delocalizes through degenerate states. We also construct a nonresonant quantum kicked rotator with delocalization.     

激光辅助的快质子对氢原子的碰撞电离

在质心参考系中研究了激光场中1 MeV质子对基态氢原子的碰撞电离过程. 靶原子的缀饰波函数由含时间微扰论给出, 末道出射电子态用双中心Coulomb-Volkov波函数描述. 计算表明辐射场使出射电子的双重微分截面变小. 敲出电子的能量越高, 截面减小越明显, 但截面中CTC峰的位置基本不受辐射场的影响.     

A Modified Protocol of Quantum Key Distribution Based on Entanglement Swapping

By comparing Cabello＇s addendum to his quantum key distribution protocol [Phys. Rev. A 64 （2001） 024301], we propose a more convenient modified protocol based on the entanglement swapping which is secure against the eavesdropping strategy addressed by Zhang et al. [Phys. Rev. A 63 （2001）036301] and other existing types of attack.     

激光场中正电子对氢原子的电离反应

本文在一级Born近似下,研究了激光场中正电子对基态氢原子的碰撞电离反应,并与入射粒子为电子的(e,2e)反应进行了对比.激光场中正电子态和敲出电子态分别采用Volkov波函数和Coulomb-Volkov波函数,靶原子的缀饰波函数由含时微扰论给出.计算结果显示激光缀饰的三重电离截面明显依赖于入射粒子电荷符号.激光越强,二者差距越大.     

Positron-Impact Ionization of Atomic Hydrogen in a Bichromatic Laser Field in the Second Born Approximation

The positron impact-ionization of atomic hydrogen in the presence of a linearly polarized bichromatic field is investigated in the second Born approximation. The field is composed of a fundamental frequency and its second harmonic. The state of positron in the field is described by the Volkov wavefunction, and the continuum state of the ejected electron is described by the Coulomb—Volkov wavefunction. The dressed ground state of target is a first order time-dependent perturbative wavefunction. The triple differential cross sections and their dependencies on laser field parameters are discussed. Numerical results demonstrate that the second-order effect plays a crucial role in understanding the laser-assisted positron scattering process.     

缀饰原子的简化波函数(英文)

作为含时薛定谔方程的微扰近似解,在速度规范下给出了激光场中缀饰原子的一个波函数.利用平均激发能近似和完备关系,可将此波函数简化为一个含时的相乘算符作用于无场时的"裸原子"态上.在软光子近似下,平均激发能仅出现在光场频率的一阶和二阶项上.此波函数适用于计算激光辅助的散射过程,特别是重排过程. A wave function for laser dressed atom is derived as a perturbative solution of the time dependent Schrdinger equation in the velocity gauge. With the use of the average excitation energy approximation and the closure approximation, the solution is reduced to a time dependent operator acting on the "bare" atomic state. In soft photon approximation, the average excitation energy only appears in the first and second order terms of field frequency. Such a simplified dressed wave function is useful in...