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Transport-Coefficient Dependence of Current-Induced Cooling Effect in a Two-Dimensional Electron Gas

机译:二维电子气体中电流致冷效应的输运系数依赖性

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摘要

The dependence of the current-induced cooling effect on the electron mobility (mu)_(e) is explored for a two-dimensional electron gas (2DEG) subjected to a perpendicular magnetic field. We calculate the distributions of the electrochemical potentials and the temperatures under a magnetic field, fully taking account of thermoelectric and thermomagnetic phenomena. Whereas the electrochemical potential and the electric current remain qualitatively unchanged, the temperature distribution exhibits drastic mobility dependence. The lower-mobility system has cold and hot areas at opposite corners, which results from the heat current brought about by the Ettingshausen effect in the vicinity of the adiabatic boundaries. The cooling effect is intensified by an increase in (mu)_(e). Intriguingly, the cold and hot areas change places with each other as the mobility (mu)_(e) is further increased. This is because the heating current on the adiabatic edges due to the Righi-Leduc effect exceeds that due to the Ettingshausen effect in the opposite direction.
机译:对于经受垂直磁场的二维电子气(2DEG),探索了电流感应冷却效应对电子迁移率μ_(e)的依赖性。我们在充分考虑热电和热磁现象的情况下,计算磁场下电化学势和温度的分布。尽管电化学势和电流在质量上保持不变,但是温度分布表现出剧烈的迁移率依赖性。低流动性系统在相对的拐角处有冷热区域,这是由绝热边界附近的埃廷斯豪森效应所产生的热流引起的。通过增加μ_(e)来增强冷却效果。有趣的是,随着迁移率μ_(e)进一步增加,冷区和热区彼此改变位置。这是因为在相反方向上,由于Righi-Leduc效应而在绝热边缘上的加热电流超过了由于Ettingshausen效应而在绝热边缘上的加热电流。

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