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1. 兰州理工大学理学院, 甘肃兰州 730050
2. 内蒙古大学理学院, 内蒙古呼和浩特 010021
3. 中国地震局兰州地震研究所, 甘肃兰州 730000
收稿日期:2005-01-25,
修回日期:2005-06-20,
纸质出版日期:2005-11-20
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元丽华, 王旭, 安张辉, 马军. 抛物量子阱中束缚极化子的极化势和结合能[J]. 发光学报, 2005,26(6): 709-713
YUAN Li-hua, WANG Xu, AN Zhang-hui, MA Jun. Polarization Potential and the Binding Energy of a Bound Polaron in a Parabolic Quantum Well[J]. Chinese Journal of Luminescence, 2005,26(6): 709-713
利用改进的Lee-Low-Pines(LLP)方法
用变分法计算了无限深抛物量子阱中同时考虑与体纵光学声子和界面纵光学声子相互作用的束缚极化子的极化势和结合能.数值计算得出:阱宽较大时极化势很小
阱宽较小时极化势较大
所以对于较窄的抛物阱必须考虑极化势.对于给定阱宽的抛物阱
随着远离阱中心极化势迅速减小
当到达阱的界面附近极化势又开始增大.阱宽较小时
束缚极化子的结合能随着阱宽L的增大而急剧减小;阱宽较大时
结合能减小的非常缓慢
最后接近体材料中的三维值.
The effect of the electron-phonon interaction on an electron bound to an impurity in a parabolic quantum well(PQW) has been studied theoretically in the past
but similar studies calculating the pola-rization potential in a PQW have not been reported.In this paper
the polarization potential and the binding energy of the bound polaron in the PQW are investigated.The study has taken the effect of bulk longitudinal optical(LO) phonons and the interface longitudinal optical(IO) phonons into account.By using the method of modified Lee-Low-Pines(LLP) variational method
the polarization potential and the binding energy of the bound polaron in the GaAs/Al
x
Ga
1-x
As PQW are obtained.The contribution of the impurity-phonon interaction to the total electron energy can be eliminated by the first canonical transformation
and the effect of this displacement on the lattice polarization leads to the polarization potential which partially compensates the electron-impurity Coulomb interaction.By the second canonical transformation
the ground state energy of the bound polaron in the infinite parabolic quantum well is worked out
and then the binding energy of the bound polaron can be gained by further calculations.The research results indicate that
the polarization potential is much smaller in the wider wells
but it is larger in the narrow wells
therefore
the polarization potential should not be neglected in the very narrow wells.For a given well width
the polarization potential decreases rapidly with increasing |
z
| and gets a minimum
then it increases with increasing |
z
| near the interface of the well.The contribution of the polarization potential to the ground state energy of the bound polaron decreases rapidly with increasing the well width(
L
) at first
and then decreases slowly with increasing
L
and approaches zero at large
L
.The binding energy of the bound polaron decreases rapidly with increasing
L
at the beginning
then decreases very slowly with increasing
L
and finally closes to the value of three-dimensional GaAs.In summary
the polarization potential should not be eliminated in a narrow PQW.
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