Aharonov-Bohm effect for the quantum Hall conductivity on a disordered lattice.

Aharonov-Bohm effect for the quantum Hall conductivity on a disordered lattice.
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无序晶格上量子霍尔电导率的阿哈罗诺夫-玻姆效应。

DOI:
10.1103/physrevlett.55.1136
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发表时间:
1985
影响因子:
8.6
通讯作者:
Aoki
Aoki
中科院分区:
物理与天体物理1区
文献类型:
--
作者:
Aoki

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The Hall conductivity (${\ensuremath{\sigma}}_{\mathrm{xy}}$) on a lattice with disorder has been calculated in torus geometry to test the quantum Hall effect for finite magnetic fields $H$. It is shown that the quantum Hall effect persists independent of degree of disorder even away from the quantum ($H\ensuremath{\rightarrow}\ensuremath{\infty}$) limit, and that the Hall effect characteristic of periodic systems is not destroyed by disorder. The value of ${\ensuremath{\sigma}}_{\mathrm{xy}}$ for finite systems has a deviation from quantization, which depends on the Aharonov-Bohm flux $\ensuremath{\Phi}$ and disappears as the size is increased.
The Hall conductivity (${\ensuremath{\sigma}}_{\mathrm{xy}}$) on a lattice with disorder has been calculated in torus geometry to test the quantum Hall effect for finite magnetic fields $H$. It is shown that the quantum Hall effect persists independent of degree of disorder even away from the quantum ($H\ensuremath{\rightarrow}\ensuremath{\infty}$) limit, and that the Hall effect characteristic of periodic systems is not destroyed by disorder. The value of ${\ensuremath{\sigma}}_{\mathrm{xy}}$ for finite systems has a deviation from quantization, which depends on the Aharonov-Bohm flux $\ensuremath{\Phi}$ and disappears as the size is increased.