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石墨中激子玻色-爱因斯坦凝聚的临界点。

Critical point for Bose-Einstein condensation of excitons in graphite.

作者信息

Wang Jinhua, Nie Pan, Li Xiaokang, Zuo Huakun, Fauqué Benoît, Zhu Zengwei, Behnia Kamran

机构信息

Wuhan National High Magnetic Field Center, Huazhong University of Science and Technology, Wuhan 430074, China.

School of Physics, Huazhong University of Science and Technology, Wuhan 430074, China.

出版信息

Proc Natl Acad Sci U S A. 2020 Dec 1;117(48):30215-30219. doi: 10.1073/pnas.2012811117. Epub 2020 Nov 16.

Abstract

An exciton is an electron-hole pair bound by attractive Coulomb interaction. Short-lived excitons have been detected by a variety of experimental probes in numerous contexts. An excitonic insulator, a collective state of such excitons, has been more elusive. Here, thanks to Nernst measurements in pulsed magnetic fields, we show that in graphite there is a critical temperature (T = 9.2 K) and a critical magnetic field (B = 47 T) for Bose-Einstein condensation of excitons. At this critical field, hole and electron Landau subbands simultaneously cross the Fermi level and allow exciton formation. By quantifying the effective mass and the spatial separation of the excitons in the basal plane, we show that the degeneracy temperature of the excitonic fluid corresponds to this critical temperature. This identification would explain why the field-induced transition observed in graphite is not a universal feature of three-dimensional electron systems pushed beyond the quantum limit.

摘要

激子是由吸引性库仑相互作用束缚的电子 - 空穴对。在众多情况下,通过各种实验探针已检测到短寿命激子。激子绝缘体,即此类激子的一种集体状态,却更难以捉摸。在此,借助脉冲磁场中的能斯特测量,我们表明在石墨中存在一个用于激子玻色 - 爱因斯坦凝聚的临界温度(T = 9.2 K)和临界磁场(B = 47 T)。在这个临界场中,空穴和电子朗道子带同时穿过费米能级并允许激子形成。通过量化激子在基面中的有效质量和空间分离,我们表明激子流体的简并温度对应于这个临界温度。这一认定将解释为何在石墨中观察到的场致转变并非超出量子极限的三维电子系统的普遍特征。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfda/7720211/1c5ee4c0710b/pnas.2012811117fig01.jpg

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