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讨论了电子—狄喇克双子束缚态解的宇称性质,指出:当q≠0(即磁荷存在)时,解的宇称确定性遭到破坏,因此破坏宇称守恒的△j=0的跃迁是允许的。从而产生了不同于通常类氢原子的线性斯塔克效应。还计算了该系统的斯塔克效应的能级分裂,指出了它不同于类氢原子的诸多特点。It is discussed that the parity conservation is not true when q≠0, i.e., the magnetic charge g≠0 for the electron-Dirac dyon bound system, so that the transitions are not forbiden when △j = 0 and the linear Stark effect may occur. The splitting of this effect is calculated. The features different from hydrogen-like atoms are also briefly discussed.
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