Harnessing quantum transport by transient chaos

被引:18
|
作者
Yang, Rui [1 ]
Huang, Liang [1 ,2 ,3 ]
Lai, Ying-Cheng [1 ,4 ,5 ]
Grebogi, Celso [5 ]
Pecora, Louis M. [6 ]
机构
[1] Arizona State Univ, Sch Elect Comp & Energy Engn, Tempe, AZ 85287 USA
[2] Lanzhou Univ, Inst Computat Phys & Complex Syst, Lanzhou 730000, Gansu, Peoples R China
[3] Lanzhou Univ, Key Lab Magnetism & Magnet Mat MOE, Lanzhou 730000, Peoples R China
[4] Arizona State Univ, Dept Phys, Tempe, AZ 85287 USA
[5] Univ Aberdeen, Univ London Kings Coll, Inst Complex Syst & Math Biol, Sch Nat & Comp Sci, Aberdeen AB24 3UE, Scotland
[6] USN, Res Lab, Washington, DC 20375 USA
基金
英国生物技术与生命科学研究理事会;
关键词
FRACTAL CONDUCTANCE FLUCTUATIONS; SCATTERING; SOFT;
D O I
10.1063/1.4790863
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
Chaos has long been recognized to be generally advantageous from the perspective of control. In particular, the infinite number of unstable periodic orbits embedded in a chaotic set and the intrinsically sensitive dependence on initial conditions imply that a chaotic system can be controlled to a desirable state by using small perturbations. Investigation of chaos control, however, was largely limited to nonlinear dynamical systems in the classical realm. In this paper, we show that chaos may be used to modulate or harness quantum mechanical systems. To be concrete, we focus on quantum transport through nanostructures, a problem of considerable interest in nanoscience, where a key feature is conductance fluctuations. We articulate and demonstrate that chaos, more specifically transient chaos, can be effective in modulating the conductance-fluctuation patterns. Experimentally, this can be achieved by applying an external gate voltage in a device of suitable geometry to generate classically inaccessible potential barriers. Adjusting the gate voltage allows the characteristics of the dynamical invariant set responsible for transient chaos to be varied in a desirable manner which, in turn, can induce continuous changes in the statistical characteristics of the quantum conductance-fluctuation pattern. To understand the physical mechanism of our scheme, we develop a theory based on analyzing the spectrum of the generalized non-Hermitian Hamiltonian that includes the effect of leads, or electronic waveguides, as self-energy terms. As the escape rate of the underlying non-attracting chaotic set is increased, the imaginary part of the complex eigenenergy becomes increasingly large so that pointer states are more difficult to form, making smoother the conductance-fluctuation pattern. (C) 2013 American Institute of Physics. [http://dx.doi.org/10.1063/1.4790863]
引用
收藏
页数:9
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