完整系统Appell方程的Lie-Mei对称性与守恒量

研究了完整系统Appell方程的Lie-Mei对称性与守恒量.在完整系统Appell方程的基础上,给出了Appell方程的Lie-Mei对称性的定义和判据,得到了Appell方程的Lie-Mei对称性导致的Hojman守恒量和Mei守恒量.举例说明结果的应用.     

2008年高考物理试题对称性问题赏析

人们早就知道,麦克斯韦优美的电磁理论之所以有力量,之所以优美,在很大程度上要归功于该理论的数学描述中所显示出来的平衡和对称。     

Lie symmetrical perturbation and adiabatic invariants of generalized Hojman type for Lagrange systems

Based on the invariance of differential equations under infinitesimal transformations of group, Lie symmetries, exact invariants, perturbation to the symmetries and adiabatic invariants in form of non-Noether for a Lagrange system are presented. Firstly, the exact invariants of generalized Hojman type led directly by Lie symmetries for a Lagrange system without perturbations are given. Then, on the basis of the concepts of Lie symmetries and higher order adiabatic invariants of a mechanical system, the perturbation of Lie symmetries for the system with the action of small disturbance is investigated, the adiabatic invariants of generalized Hojman type for the system are directly obtained, the conditions for existence of the adiabatic invariants and their forms are proved. Finally an example is presented to illustrate these results.     

利用破坏对称性的超导人造原子制备χ型四比特纠缠态

提出了利用在一维传输线共振器中的破坏对称性的超导人造原子来制备χ型四比特纠缠态的方案. 方案中所用到的Δ型三能级人造原子不同于自然的原子, 它可以产生循环跃迁. 经过适当时间的相互作用和简单的操作, 可以得到想要制备的纠缠态. 由于人造原子的激发态和光子态被绝热消除, 所以该方案对于人造原子的自发辐射和传输线共振器的衰减是鲁棒的.     

曲线曲面积分中利用对称性及曲线曲面方程化简

证明了曲线曲面积分中有关对称性的两个命题,并举例说明了命题结论在一些特殊类型曲线曲面积分计算中的应用.还探讨了在对坐标的曲线积分及曲面积分中利用曲线方程或曲面方程化简的问题.     

用高斯定理求电场的条件是满足环路定理

通过举例说明用高斯定理求电场的条件是:仅由对称性分析就能得出满足环路定理的电场形式.     

De-excitation Energy of Superdeformed Secondary Minima of Odd-Odd Au Isotopes and Its Sensitivity to the Density Dependence of Symmetry Energy

The de-excitation energy of superdeformed secondary minima of odd-odd Au isotopes is investigated using the relativistic mean field model with the inclusion of the isoscalar-isovector coupling. It is shown that the de-excitation energies of superdeformed secondary minima relative to the ground states can serve as a significant probe to the density dependence of the symmetry energy.     

Clebsch-Gordan系数的对称性

利用Schur引理确定了角动量耦合的Clebsch-Gordan系数按照其定义所允许的任意程度,然后利用正交归一关系和相位知识,导出了Clebsch-Gordan系数的对称性.     

广义对称性在积分计算中的应用

设f（P）是对称区域Ω上的连续函数,其中P∈Ω.若f（P）在Ω中各对称点处函数值的绝对值相等且符号相反时,∫Ωf（P）dΩ=0;当f（P）在Ω中各对称点处的函数值相等时,Ω∫f（P）dΩ=2Ω∫1f（P）dΩ,其中Ω1为Ω＂对称的一半＂.此结论称为积分的广义对称性.通过实例说明了利用此结论可以简化很多积分的计算.