格点Chern-Simons理论的量子化

讨论了Chern-Simons理论的naive格点化,并就其中最简单的一种情形用Dirac约束体系量子化方法进行量子化.由此显示naive格点化的缺陷,找出了克服这一困难的办法.求出了anyon产生算符.     

量子化电磁场中的非经典电子波包:电子与光子的纠缠

文中研究了量子化电磁场中非经典电子波包的运动。当初始光子态是Fock态时，随着电子和光子所组成系统的演化，初台可分离的电子态和光子态会互相纠缠，而且电子几率密度的时间演化呈非经典的分岔和汇合的现象。基到这些非经典特征，电子可以在光子场中被加速和减速，而系统保持能量守恒。     

重离子融合反应入射道效应的动力学研究

运用微观输运模型-改进的量子分子动力学模型(ImQMD), 研究了弹靶质量对称体系⁷⁴Ge+⁷⁴Ge与弹靶质量不对称体系⁴⁸Ti+¹⁰⁰Mo的重离子融合反应入射道效应及其动力学机制, 并分析了复合体系的均方根半径〈r²〉^1/2和形变参量β随时间的演化过程, 结果表明质量对称的反应体系比不对称体系更容易产生形变较大的Gd, 则说明重离子融合反应中的动力学效应对大形变核的产额有很大的影响.     

Segal－Bargmann－Hall Transform and Geometric Quantization

Using geometric methods, Hall has proved that the Segal-Bargmann transform for a con-nected Lie group K of compact type is an isometric isomorphism [H1] and is unique when Kis simply connected [H7]. Furthermore, Hall considered geometric quantization of T~*(K), K'scotangent bundle [H9]. Using the vertical polarization and a natural Khler polarization obtainedby identifying T~*(K) with the complexified group KC, Hall concluded that the pairing map be-tween the two Hilbert Spaces induced by these two polarizations coincides with the generalizedSegal-Bargmann transform C_t (up to constant).     

原子的吸收光谱和发射光谱的演示

介绍了利用光学多道分析仪和投影仪在课堂上实时演示原子的吸收光谱和发射光谱的实验方法。     

取样平均法提高CCD多道探讨器信噪比

应用取样平均法有效地提高了ＣＣＤ光学多道探测器信噪比，当采样次数为ｍ时，信噪比提高√ｍ倍，应用于实验得到了高信噪比的各种光谱谱图。     

光抽运双光子激光朗之万量子理论

本文采用朗之万量子理论获得光抽运双光子激光具有双光子损耗时的朗之万方程,进一步获得稳态平均光子数、频率牵引、线宽和动态斯塔克效应,对激光增益来源的分析表明,非相干抽运仅有单双光子两步过程有贡献,而相干抽运,除上述过程外还有单双光子一步过程有贡献,而且,上述两个过程都受到负反馈和饱和因子的制约,线宽与稳态平均光子数无关。 关键词：     

组合Bose场的分数自旋和分数统计性

对组合Bose子场，采用FS (Faddeev-Senjanovic) 路径积分量子化方法进行量子化.从量子Noether定理出发，给出量子分数自旋和分数统计性质. 关键词： 路径积分量子化 分数自旋 分数统计     

Field Quantization and Spontaneous Emission in Left-handed Material

Recently, research on left-handed materials （LHMs） has attracted considerable attentions. The LHMs are a kind of man-made metameterials which have negative permittivity and negative permeability. These metameterials have many novel properties such as inverse light pressure, and reverse Doppler effect, which lead to many potential applications of LHMs such as superlenses which, in principle, can achieve arbitrary subwavelength resolution. However, though the properties mentioned above are seen to be classical, the quantum phenomena in LHMs have also attracted attentions such as the modified spontaneous emission of atoms in LHME.