Open quantum dots: Physics of the non-Hermitian Hamiltonian

被引:7
|
作者
Ferry, D. K. [1 ]
Akis, R. [1 ]
Burke, A. M. [1 ,5 ]
Knezevic, I. [2 ]
Brunner, R. [3 ]
Meisels, R. [3 ]
Kuchar, F. [3 ]
Bird, J. P. [4 ]
机构
[1] Arizona State Univ, Sch Elect Comp & Energy Engn, Tempe, AZ 85287 USA
[2] Univ Wisconsin, Dept Elect Engn, Madison, WI 53706 USA
[3] Univ Leoben, Inst Phys, A-8700 Leoben, Austria
[4] SUNY Buffalo, Dept Elect Engn, Buffalo, NY 14260 USA
[5] Univ New S Wales, Sch Phys, Sydney, NSW, Australia
来源
关键词
Semiconductor quantum dots; classical to quantum transition; projection algebra; dissipation; WEAK-LOCALIZATION; CONDUCTANCE FLUCTUATIONS; PHASE BREAKING; NUMERICAL-ANALYSIS; LEVEL SPECTRUM; TRANSPORT; DECOHERENCE; SELECTION; PROBE;
D O I
10.1002/prop.201200065
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Quantum dots provide a natural system in which to study both classical and quantum features of transport, as they possess a very rich set of eigenstates.When coupled to the environment through a pair of quantum point contacts, these dots possess a mixed phase space which yields families of closed, regular orbits as well as an expansive sea of chaos. In this latter case, many of the eigenstates are decohered through interaction with the environment, but many survive and are referred to as the set of pointer states. These latter states are described by a projected, non-Hermitian Hamiltonian which describes their dissipation through many-body interactions with particles in the external environment. (C) 2013 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
引用
收藏
页码:291 / 304
页数:14
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