Effects of tunneling coupling on plasmon modes in asymmetric double-quantum-well structures

被引:0
作者
Xin-Hai Liu
Xue-Hua Wang
Ben-Yuan Gu
机构
[1] Institute of Physics,
[2] Chinese Academy of Sciences,undefined
[3] PO Box 603,undefined
[4] Beijing 100080,undefined
[5] PR China,undefined
[6] CCAST (World Laboratory),undefined
[7] PO Box 8730,undefined
[8] Beijing 100080,undefined
[9] PR China and Institute of Physics,undefined
[10] Chinese Academy of Sciences,undefined
[11] PO Box 603,undefined
[12] Beijing 100080,undefined
[13] PR China,undefined
来源
The European Physical Journal B - Condensed Matter and Complex Systems | 2001年 / 24卷
关键词
PACS. 73.21.-b Electron states and collective excitations in multilayers, quantum wells, mesoscopic, and nanoscale systems;
D O I
暂无
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摘要
The collective charge density excitations in asymmetric double-quantum-well (DQW) structures with different tunneling strengths are systematically studied. In particular, the damping properties of the plasmon modes in various tunneling strengths are investigated in detail. It is shown that plasmon modes in asymmetric DQW structures are quite different from those in symmetric DQW systems. In weak tunneling regime, an intra-subband mode ω- with an acoustic-like dispersion relation which is damped in symmetric DQW structures arises and coexists with the optical-like mode ω+ while the inter-subband mode ω10 is highly damped. With the tunneling strength being increased, the ω10 branch gradually becomes undamped and emerges out of the (1-0) single-particle continuum, whereas the ω- branch gradually approaches the (0-0) single-particle continuum. In intermediate coupling regime, these three branches of modes coexist undamped. In strong tunneling regime, ω- enters the (0-0) single-particle continuum and becomes damped. Consequently, only the ω+ and ω10 modes exist in this regime.
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页码:37 / 41
页数:4
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