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1. 中国石油大学, 数理系 北京,102249
2. 内蒙古民族大学, 物理与机电学院, 内蒙古, 通辽, 028043
收稿日期:2004-08-25,
修回日期:2004-11-24,
纸质出版日期:2006-01-20
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张鹏, 周广刚, 宝日玛, 肖景林. 极性晶体中强耦合表面磁极化子特性[J]. 发光学报, 2006,27(1): 23-26
ZHANG Peng, ZHOU Guang-gang, BAO Ri-ma, XIAO Jing-lin. Properties of the Strong Coupling Surface Magnetopolaron in Polar Crystal[J]. Chinese Journal of Luminescence, 2006,27(1): 23-26
研究极性晶体中表面磁极化子的特性。采用Huybrechts线性组合算符和幺正变换方法
导出了晶体中强耦合表面磁极化子处于基态的振动频率和有效哈密顿量
讨论了坐标z的两种极限情况
对RbCl晶体进行了数值计算。结果表明:振动频率和平行有效哈密顿量随磁场的增加而增大。
In the past dozens of years
with the development of magneto-optical technology
the properties of the polaron in a magnetic field have been widely studied both experimentally and theoretically. However
the properties of magnetopolaron have not been investigated by Huybrechts method so far. The excitation energy of the strong coupling surface polaron have been calculated using Huybrechts method by the present authors and co-workers. The properties of the surface magnetopolaron in polar crystals were studied. The ground state vibration frequency and the effective Hamiltonian of surface magnetopolaron were derived by using the linear combination operator and the unitary transformation method. Two limiting cases of the coordinate z for the electron-SO phonon and electron-LO phonon system are discussed. Numerical calculations
for the RbCl crystal as an example
are performed. We find that due to the existence of the surface optical (SO) phonons
the electrons move more close to the surface
the interactions between the electrons and the SO phonons become more strong. When the electron infinitely close to the surface
the contribution of the LO phonon can be neglected. On the other hand
the contribution of the bulk LO phonon will increase with the increase of the distance between electron and the surface. At this moment
the contribution of the bulk LO phonon is much greater than SO phonon's
and then we can omit the SO phonon. The results show that the vibration frequency and the parallel effective Hamiltonian of surface magnetopolaron will be increased with increasing magnetic field. The reason is that with the increase of magnetic field the location of the magnetopolaron will be enhanced.
Larsen D M.Perturbation theory for the two-dimensional polaron in a magnetic field[J].Phys.Rev.,1986,B33:799-806.
Wu X G,Peeters F M,Pevreese J T.Two-dimensional polaron in a magnetic field[J].Phys.Rev.,1985,B32:7964-7969.
Peeters F M,Wu X G,Devreese J T.Landau levels above the optical-phonon continuum in two and three dimensions[J].Phys.Rev.,1986,B33:4338-4340.
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Wei B H,Yu K W.Self-energy of a magnetopolaron at the interface of polar crystals[J].J.Phys.:Condens.Matter.,1995,7:1059-1067.
Xiao J L,Xiao W.Influence of the interaction between phonons on the properties of the surface magnetopolaron in polar crystals[J].Phys.Rev.,1998,B58:1678-1688.
Xiao J L,Eerdunchaolu,Xiao W.Magnetic field and temperature dependence of the mass of a surface polaron in polar crystals[J].J.Phys.Soc.Jpn.,2002,71(5):1332-1338.
Huybrechts W J.Internal excited state of the optical polaron[J].J.Phys.,1977,C10:3761-3768.
Zhang P,Xiao J L.The excitation energy of the strong coupling surface polaron[J].Chin.J.Lumin.(发光学报),2003,24(1):33-38 (in Chinese).
Zhang P,Li Z J,Xiao J L.The influence of the interaction between phonons on the induced potential of the surface polaron in magnetic field[J].Chin.J.Lumin.(发光学报),1998,19(4):300-305 (in Chiense).
Kartheuser E.Polarons in Ionic Crystals and Polar Semiconductors[M].North-Holland Publ.Co.,Amsterdam,1972.
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