超晶格
超导电性
凝聚态物理
费米能量
石墨烯
电子
异常(物理)
热力学平衡
电流(流体)
费米气体
材料科学
物理
量子力学
热力学
作者
Alexey I. Berdyugin,Na Xin,Haoyang Gao,Sergey Slizovskiy,Zhiyu Dong,Shubhadeep Bhattacharjee,Piranavan Kumaravadivel,Shuigang Xu,Л. А. Пономаренко,Matthew Holwill,D. A. Bandurin,Minsoo Kim,Yang Cao,M. T. Greenaway,Kostya S. Novoselov,I. V. Grigorieva,Kenji Watanabe,Takashi Taniguchi,Vladimir I. Fal’ko,Leonid Levitov
出处
期刊:Science
[American Association for the Advancement of Science]
日期:2022-01-27
卷期号:375 (6579): 430-433
被引量:60
标识
DOI:10.1126/science.abi8627
摘要
In thermodynamic equilibrium, current in metallic systems is carried by electronic states near the Fermi energy whereas the filled bands underneath contribute little to conduction. Here we describe a very different regime in which carrier distribution in graphene and its superlattices is shifted so far from equilibrium that the filled bands start playing an essential role, leading to a critical-current behavior. The criticalities develop upon the velocity of electron flow reaching the Fermi velocity. Key signatures of the out-of-equilibrium state are current-voltage characteristics resembling those of superconductors, sharp peaks in differential resistance, sign reversal of the Hall effect, and a marked anomaly caused by the Schwinger-like production of hot electron-hole plasma. The observed behavior is expected to be common for all graphene-based superlattices.
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