澳门太阳集团网站入口
网站地图
加入收藏
中文
English
澳门太阳集团网站入口
中心概况
研究队伍
科学研究
交流合作
人才培养
人才招聘
当前位置:
澳门太阳集团网站入口
-
交流合作
-
专题学术讲座
- 正文
大师讲堂
专题学术讲座
学术会议
中心报告会
专题学术讲座
物理系学术报告:Fermi surface(s) and superconducting gap(s) in bulk SrTiO3
报告题目:
Fermi surface(s) and superconducting gap(s) in bulk SrTiO3
报 告 人:
Prof. Kamran Behnia Ecole Superieure de physique et de Chimie Industrielles (ESPCI), Paris
报告时间:
2013-7-3 10:30
报告地点:
理科楼B406会议室
摘要:
SrTiO3 is a large-gap insulator, which upon the introduction of n-type carriers undergoes a superconducting transition below 1 K. Discovered in 1964, it has been the first member of a loose family of semiconducting superconductors, which now includes column-IV elements. Recent attention has focused on the interface between SrTiO3 and other insulators or vacuum, a two-dimensional metal with a superconducting ground state. The origin of superconductivity in the bulk system is a mystery, since the non-monotonous variation of the critical temperature with carrier concentration defies the expectations of the crudest version of the BCS theory.
We have found that down to concentrations as low as 5.5 X 1017 cm-3, the system has both a sharp Fermi surface and a superconducting ground state. This is by far the most dilute superconductor currently known. Surprisingly, the normal state of this superconductor is a metal whose Fermi energy is as little as 1.1 meV on top of a band gap as large as 3 eV. We argue that the large Bohr radius is the key factor in pulling down the threshold of superconductivity and metallicity in this system. The survival of superconductivity in such a dilute metal with a Fermi temperature much smaller than Debye temperature puts strong constraints for the identification of the pairing mechanism.
With further doping, additional bands are filled and the metal becomes multi-band. Analysis of quantum-oscillations leads to a solid determination of the critical doping for the occupation of each band. In this doping range, the superconducting state has multiple gaps according to visible signatures detectable in its thermal transport.
版权所有 量子物质科学协同创新中心
本页已经浏览
次