给出了具有椭球边界量子棒经过坐标变换成球形边界的哈密顿量.采用线性组合算符和幺正变换的方法研究了在非均匀抛物限制势下量子棒中强耦合磁极化子的性质.导出了量子棒中强耦合磁极化子的振动频率和声子平均数随磁场的回旋频率、电子-声子耦合强度、椭球的纵横比和横向和纵向有效受限长度的变化关系.结果表明:振动频率和声子平均数随电子-声子耦合强度和磁场的回旋频率的增加而增加,随横向和纵向有效受限长度的减小而迅速增大.当e'>1时,振动频率和声子平均数随椭球的纵横比增加而增加. e'<1时,随着椭球的纵横比减少,振动频率和声子平均数都增大.当e'=1时,振动频率和声子平均数取极小值.
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