超导电性
凝聚态物理
布里渊区
物理
电子能带结构
带隙
BCS理论
库珀对
费米面
配对
作者
Junjie 俊杰 Jia 贾,Yadong 亚东 Gu 谷,Chaohui 超辉 Yin 殷,Yingjie 英杰 Shu 束,Yiwen 逸雯 Chen 陈,Jumin 聚民 Shi 史,Xing 杏 Zhang 张,Hao 浩 Chen 陈,Taimin 泰民 Miao 苗,Xiaolin 晓琳 Ren 任,Bo 波 Liang 梁,Wenpei 文培 Zhu 朱,Neng 能 Cai 蔡,Fengfeng 丰丰 Zhang 张,Shenjin 申金 Zhang 张,Feng 峰 Yang 杨,Tao Wang,Qinjun 钦军 Peng 彭,Zuyan 祖彦 Xu 许,Hanqing 寒青 Mao 毛
标识
DOI:10.1088/1674-1056/ad51f9
摘要
Abstract In iron-based superconductor Fe(Se,Te), a flat band-like feature near the Fermi level was observed around the Brillouin zone center in the superconducting state. It is under debate whether this is the evidence on the presence of the BCS–BEC [Bardeen–Cooper–Schrieffer (BCS), Bose–Einstein condensation (BEC)] crossover in the superconductor. High-resolution laser-based angle-resolved photoemission measurements are carried out on high quality single crystals of FeSe 0.45 Te 0.55 superconductor to address the issue. By employing different polarization geometries, we have resolved and isolated the d yz band and the topological surface band, making it possible to study their superconducting behaviors separately. The d yz band alone does not form a flat band-like feature in the superconducting state and the measured dispersion can be well described by the BCS picture. We find that the flat band-like feature is formed from the combination of the d yz band and the topological surface state band in the superconducting state. These results reveal the origin of the flat band-like feature and rule out the presence of BCS-BEC crossover in Fe(Se,Te) superconductor.
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