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在电荷密度波材料1T-TiSe₂中观察到的非相干到相干的转变 。 (注:原文中“1T-TiSe”应该是“1T-TiSe₂”,这里按照正确的化学式进行了补充翻译)

Incoherence-to-coherence crossover observed in charge-density-wave material 1T-TiSe.

作者信息

Ou Yi, Chen Lei, Xin Ziming, Ren Yujing, Yuan Penghao, Wang Zhengguo, Zhu Yu, Chen Jingzhi, Zhang Yan

机构信息

International Center for Quantum Materials, School of Physics, Peking University, 100871, Beijing, China.

Collaborative Innovation Center of Quantum Matter, 100871, Beijing, China.

出版信息

Nat Commun. 2024 Oct 24;15(1):9202. doi: 10.1038/s41467-024-53647-x.

Abstract

Analogous to the condensation of Cooper pairs in superconductors, the Bose-Einstein condensation (BEC) of electron-hole pairs in semiconductors and semimetals leads to an emergence of an exotic ground state - the excitonic insulator state. In this paper, we study the electronic structure of 1T-TiSe utilizing angle-resolved photoemission spectroscopy and alkali-metal deposition. Alkali-metal adatoms are deposited in-situ on the sample surface, doping the system with electrons. The conduction bands of 1T-TiSe are thereby pushed down below the Fermi energy, which enables us to characterize its temperature dependence with precision. We found that the formation of the charge density wave (CDW) in 1T-TiSe at ~ 205 K is accompanied by a significant increase of the band gap, supporting the existence of excitonic pairing in the CDW state of 1T-TiSe. More importantly, by analyzing the linewidth of the single-particle excitation spectrum, we unveiled an incoherence-to-coherence crossover at 165 K, which could be attributed to a possible exciton condensation that occurs beneath the CDW transition in 1T-TiSe. Our results not only explain the exotic transport properties of 1T-TiSe, but also highlight the possible existence of an excitonic condensate in this semiconducting material.

摘要

类似于超导体中库珀对的凝聚,半导体和半金属中电子 - 空穴对的玻色 - 爱因斯坦凝聚(BEC)导致一种奇异基态的出现——激子绝缘体态。在本文中,我们利用角分辨光电子能谱和碱金属沉积研究了1T - TiSe的电子结构。碱金属吸附原子原位沉积在样品表面,用电子对系统进行掺杂。由此,1T - TiSe的导带被压低至费米能级以下,这使我们能够精确地表征其温度依赖性。我们发现,1T - TiSe中在约205 K时电荷密度波(CDW)的形成伴随着带隙的显著增加,这支持了1T - TiSe的CDW态中激子配对的存在。更重要的是,通过分析单粒子激发谱的线宽,我们揭示了在165 K时从不相干到相干的转变,这可能归因于1T - TiSe中CDW转变之下发生的一种可能的激子凝聚。我们的结果不仅解释了1T - TiSe的奇异输运性质,还突出了这种半导体材料中可能存在激子凝聚体。

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