Electron g-factor in coupled quantum wells CdTe and CdMnTe

被引:0
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作者
Afanasiev, M. M. [1 ]
Kozyrev, N. V. [1 ]
Kirstein, E. [2 ]
Kalevich, V. K. [1 ]
Zhukov, E. A. [1 ,2 ]
Mantsevich, V. N. [3 ,4 ]
Krivenko, I. S. [5 ]
Karczewski, G. [6 ]
Yakovlev, D. R. [1 ,2 ]
Kusraev, Yu G. [1 ]
Bayer, M. [1 ]
机构
[1] Ioffe Inst, St Petersburg 194021, Russia
[2] Tech Univ Dortmund, Expt Phys 2, D-44221 Dortmund, Germany
[3] Lomonosov Moscow State Univ, Phys Dept, Chair Semicond & Cryoelect, Moscow 119991, Russia
[4] Lomonosov Moscow State Univ, Phys Dept, Quantum Technol Ctr, Moscow 119991, Russia
[5] Univ Michigan, Dept Phys, Ann Arbor, MI 48109 USA
[6] Polish Acad Sci, Inst Phys, PL-02668 Warsaw, Poland
来源
关键词
BEATS;
D O I
10.1088/1742-6596/1400/6/066023
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
In tunnel-coupled quantum wells (QWs) CdTe (20 nm wide) and CdMnTe (8 nm wide) separated by Cd0.88Mg0.Te-12 barrier with a thickness of L-B = 5, 7, 9, and 11 monolayers (MLs), the dependence of electron g-factor on the barrier thickness and temperature is investigated by means of the pump-probe Kerr rotation technique. The renormalization of the electron g-factor occurs due to the s-d exchange interaction of electrons with manganese ions in a magnetic QW. The most change of the electron g-factor value Delta g = 0.25 is registered at the least barrier width of 5 MLs and temperature T = 5 K. In this case, the penetration of the electron wave function from the nonmagnetic QW into the magnetic one is estimated to be 0.6%.
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页数:5
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