极化子单激发态的反向极化研究

通过对有机高分子中极化子的单激发态进行研究，发现该态在外电场下呈现反向极化特征，极化规律与双激子态类似.在强电场下，反向极化消失，极化子单激发态解离为一个单极化子和一个双极化子态. 关键词： 极化子态 激子态 反向极化     

介质极化磁化的进一步讨论

证明了Ｍ与Ｐ只能构成两个独立的洛伦兹不变量。     

极化强度矢量与磁化强度矢量的相对论变换

本文推出了磁化强度矢量与极化强度矢量的相对论变换关系，证明了Ｍ和Ｐ可构成两个洛伦兹不变量，从面可加深对Ｍ和Ｐ的理解。     

浅海矢量声场极化特性的深度分布规律

海洋波导环境中声场的极化特性可为水下目标探测提供新思路,因此对极化特性进行研究很有意义.本文将Stokes参数扩展到宽带形式,利用非平稳相位近似方法对公式进行简化,降低了理论推导的复杂性,并揭示了极化特性在声源深度及声源对称深度具有显著变化特性的物理机理.数值仿真结果表明:使用非平稳相位近似进行简化后的公式是有效的,可以较好地表征出极化特性的深度分布规律;同时,通过对宽带Stokes参数归一化,可以去除水平距离对极化特性深度分布规律的影响;随后,以归一化宽带Stokes参数为研究对象,分析了声源频率、声源深度、声速剖面及海水深度等参数对极化特性深度分布规律的影响.通过RHUMRUM实验数据处理结果验证了非平稳相位近似的有效性和归一化宽带Stokes参数的距离无关性质.相关结论可为基于矢量场极化特性的被动目标深度估计提供理论依据.     

胶子的极化态与ξ(2230)的胶子球解释

本文讨论了当胶子只有横极化分量时对ξ(2230)胶子球解释的影响.     

Z→3γ及相关过程的解析手征振幅和极化矢量的讨论

给出了Z→3γ及相关过程的解析手征振幅.结果与Glover等的结果不同,虽然手征振幅的这种差别并不影响总几率的计算,但它有直接的物理意义,并可为实验检验.同时对极化矢量的定义进行了讨论,并指出Glover文章之错误.     

电子与双声子相互作用对Holstein极化子的影响

在量子化的Holstein模型的基础上再考虑电子与双声子相互作用，运用相干态展开法，得到了一维分子晶体模型处于基态的极化子满足的非线性薛定谔方程及其定态孤子解、基态能量、晶格位移. 关键词： 相干态 极化子 孤立子 非线性薛定谔方程     

一维分子晶体中的极化子

本文从量子化的Holstein模型出发,运用相干态展开法和能量极小原理,通过实施连续近似得到了一维分子晶体模型处于基态的极化子满足的非线性薛定谔方程及其定态孤子解、基态能量、晶格位移,其结果与Holstein T[1].从半经典理论所得的结果完全一致,因此相干态展开方法在处理与极化子有关的其他物理问题中是一种非常有效的方法.     

声子色散对抛物量子点中极化子基态能量的影响

在声子色散影响下利用压缩态变分法计算了抛物量子点中弱耦合极化子的基态能量。采用的变分方法是基于逐次正则并且利用单模压缩态变换处理通常被我们所忽略的在第一次幺正变换中产生的声子产生湮灭算符的双线性项。计算得出了在考虑声子色散的情况下抛物量子点中弱耦合极化子的基态能量的数学表达式。讨论了抛物量子点中在电子-声子弱耦合情况下,受限长度,电子-声子耦合常数,色散系数与极化子基态能量之间的依赖关系。     

声子和磁场对量子环中极化子性质的影响

采用求解能量本征方程、幺正变换和变分相结合的方法,研究声子和磁场对量子环中极化子性质的影响. 对KBr量子环的数值计算表明,电子或极化子的基态能量随量子环频率(或平均半径)的增大而增大,极化子基态能移随量子环频率的增大(或平均半径的减小)而减小,极化子中的平均声子数随量子环频率的增大(或平均半径的减小)而增大. 当有垂直磁场时,极化子基态能量和基态能移与外磁场及电子转动状态有关. 随着磁场强度的增大,基态能量出现简并且呈现非周期性振荡;能移随磁场强度的增大(或转动量子数绝对值的减小)而减小.     

Feynman propagator for an arbitrary half—integral spin

Based on the solution to Bargmann－Wigner equation for a particle with arbitrary half-integral spin, a direct derivation of the projection operator and propagator for a particle with arbitrary half-integral spin is worked out. The projection operator constructed by Behrends and Fronsdal is re-deduced and confirmed and simplified, the general commutation rules and Feynman propagator with additional non-covariant terms for a free particle with arbitrary half-integral spin are derived, and explicit expressions for the propagators for spins 3/2, 5/2 and 7/2 are provided.     

自旋为任意整数的传播子

以自旋为任意整数的自由粒子的波函数(Bargmann-Wigner方程的解)为基础，进一步研究了 自旋为任意整数的投影算符和传播子.证明了Behrends和Fronsdal所构造的投影算符是正确 的.导出了自旋为任意整数的场的一般对易规则和费恩曼传播子的一般表达式. 关键词： 整数自旋 投影算符 对易规则 费恩曼传播子     

Flexible Manipulation of the Polarization Conversions in a Structured Vector Field in Free Space

The conversion between different polarizations generally requires an optical element or an optical system. We demonstrate, theoretically and experimentally, that the conversion between different states of polarization (SoP) can be flexibly manipulated in a structured optical field by itself. During the structured optical field propagation in free space, any two orthogonal polarizations can be generated and auto‐focus at any desired propagation positions by purposely designing the initial SoP distribution and a caustic phase in the field cross‐section. The experiment arrangement combines a caustic‐based approach and a 4f optical system. This approach provides a way to flexibly manipulate the polarization conversions in free space propagation by the optical field itself (without any physical element along the propagation path), may lead to more complex and flexible vectorial manipulations of an optical field scenarios and potential applications in corresponding areas.     

高能重离子非对心碰撞中的整体夸克极化

There exists a large local relative orbital angular momentum between produced partons along the direction opposite to the reaction plane in the early stage of non-central heavy-ion collisions. This initial local orbital angular momentum can lead to quark polarization along the same direction due to spin-orbital coupling in QCD. We present the quark polarization by using hard thermal loop gluon propagator for quark-quark scattering in quark-gluon plasma and compare it with the result obtained from the static potential model.     

γγ→γZ过程高能总截面的数值计算

给出了γγ→γZ过程,质心系总能量在91.2—2000GeV的总截面.结果表明在总能量大于140GeV时,W玻色子图的贡献比起费米子图的贡献要大,当总能量在750GeV左右,截面达到极大值220fb(|cosθ|33cm^－2·sec^－1,每年在总能量750GeV处可观察到6000多个γγ→γZ事例,用它可以进一步验证标准模型,特别是其中规范粒子的三顶角和四顶角相互作用.     

Gasser-Leutwyler Coefficients of Chiral Lagrangian for Pseudoscalar Goldstone Bosons

Based on the Dyson-Schwinger equations in rainbow approximation for quark propagator with an effective gluon propagator, and on the parametrized fully dressed quark propagator proposed by us, the unknown Gasser-Leutwyler coefficients of the chiral Lagrangian for pseudoscalar Goldstone bosons, Li, are predicted respectively. The predicted values of Li in the two different ways are not only in reasonable agreement each other but also in agreement with empirical values used widely in literature and the values predicted by many other theoretical models with QCD characteristics. The compatible results of Gasser-Leutwyler coefficients predicted by our parameterized quark propagator,in turn, clearly verify its extensive validity.     

Gasser-Leutwyler Coefficients of Chiral Lagrangian for Pseudoscalar Goldstone Bosons

Based on the Dyson-Schwinger equations in raAnbow approximation for quark propagator with an effective gluon propagator, and on the parametrized fully dressed quark propagator proposed by us, the unknown GasserLeutwyler coeiticients of the chiral Lagrangian for pseudoscalar Goldstone bosons, Li, are predicted respectively. The predicted values of Li in the two different ways are not only in reasonable agreement each other but also in agreement with empirical values used widely in literature and the values predicted by many other theoretical models with QCD characteristics. The compatible results of Gasser-Leutwyler coefficients predicted by our parameterized quark propagator, in turn, clearly verify its extensive validity.     

Dirac Particle Polarization in Uniform Magnetic Field

For Dirac particles in a uniform magnetic field, the polarization operator projections onto three directions remain unchanged. If the orbital angular moment of particles is large with respect to 1, then the spin of moving particles retain the fixed orientation relative to the axes of the cylindrical coordinate system.     

偏振模色散的偏振主态旋转补偿法

提出一种用以补偿一阶偏振模色散的方法通过理论分析,说明了使用偏振分离器和加入光学延迟来抑制光纤中的PMD的方法以及其存在的由于延迟偏差造成的过补偿或欠补偿由理论分析可知,通过调整输入信号偏振态的方向,可以有效改善补偿效果模拟实验证明了该方法的可行性.