具连续p(x)-增长条件的变分积分的极小点的正则性

本文研究积分泛函的局部极小点的正则性，其中是连续函数且是正常数。证明了：若是J的局部极小点，则问当p（x）满足条件在某些附加条件下有     

Anti-function solution of uniaxial anisotropic Stoner-Wohlfarth model

The anti-trigonometric function is used to strictly solve the uniaxial anisotropic Stoner-Wohlfarth (SW) model, which can obtain the relation of the angle α (θ) between the magnetization (the anisotropy field) and the applied magnetic field. Using this analytic solution, the hysteresis loops of uniaxial anisotropic SW particles magnetized in typical directions could be numerically calculated. Then, the hysteresis loops are obtained in randomly distributed SW particle ensembles while ignoring the dipole interaction among them with the analytic solution. Finally, the correctness of the analytic solution is verified by the exact solutions of remanence, switching field, and coercivity from the SW model. The analytic solution provides an important reference for understanding the magnetizing and magnetization reversal processes of magnetic materials.     

自旋-轨道耦合二分量玻色-爱因斯坦凝聚系统的孤子解

在旋量玻色-爱因斯坦凝聚体中,孤子态作为宏观量子效应的典型状态,可以通过自旋-轨道耦合进行调控,这使得对自旋-轨道耦合玻色-爱因斯坦凝聚体中孤子的研究成为近年来超冷原子领域研究的重要课题之一.本文研究了描述一维自旋-轨道耦合二分量玻色-爱因斯坦凝聚体Gross-Pitaevskii方程的精确求解,利用直接假设及可积约化方法,给出了系统多种类型的孤子解,讨论了相应的孤子动力学以及自旋-轨道耦合效应对系统的量子磁化和自旋-极化态的影响.     

动力学群微分表示的计算:以Lorentz群 SO(3,1) 为例

该文给出了动力学群在群参数空间以及陪集空间上的右、左微分表示和伴随微分表示的符号计算方法.作为例子, 计算了Lorentz 群SO(3,1)的6 -参数和3 -参数的右、左及伴随微分表示,这些表示是旋转群SO(3)关于欧拉角和极角的微分表示的相对论性推广.特别,作者给出了伴随微分表示的两种不同的3 -参数形式,同时也得到了Wigner小群SO(2,1) 和 SO(3)$的6 -参数和3 -参数的相应表示.这些表示在相对论性量子陀螺的研究中可得到应用.     

Exact soliton solutions in anisotropic ferromagnetic wires with Dzyaloshinskii–Moriya interaction

We theoretically investigate the exact soliton solutions of anisotropic ferromagnetic wires with Dzyaloshinskii–Moriya interaction. For example, we give the bright and black soliton solutions. From these results we find that the Dzyaloshinskii–Moriya interaction affects the existence region of soliton, spin-wave transport, and soliton dynamic properties. As the Dzyaloshinskii–Moriya interaction grows, the soliton width is widened, which provides a way to control the soliton dynamics.