Chiral d-wave superconductivity in a triangular surface lattice mediated by long-range interaction

被引:14
|
作者
Cao, Xiaodong [1 ]
Ayral, Thomas [2 ,3 ]
Zhong, Zhicheng [1 ,4 ]
Parcollet, Olivier [3 ]
Manske, Dirk [1 ]
Hansmann, Philipp [1 ,5 ]
机构
[1] Max Planck Inst Festkorperforsch, Heisenbergstr 1, D-70569 Stuttgart, Germany
[2] Rutgers State Univ, Phys & Astron Dept, Piscataway, NJ 08854 USA
[3] CEA, CNRS, Inst Phys Theor IPhT, UMR 3681, F-91191 Gif Sur Yvette, France
[4] Chinese Acad Sci, Ningbo Inst Mat Technol & Engn, Ningbo 315201, Zhejiang, Peoples R China
[5] Eberhard Karls Univ Tubingen, Inst Theoret Phys, Morgenstelle 14, D-72076 Tubingen, Germany
关键词
MEAN-FIELD THEORY; SYSTEMS;
D O I
10.1103/PhysRevB.97.155145
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Adatom systems on the Si(111) surface have recently attracted an increasing attention as strongly correlated systems with a rich phase diagram. We study these materials by a single band model on the triangular lattice, including 1/r long-range interaction. Employing the recently proposed TRILEX method, we find an unconventional superconducting phase of chiral d-wave symmetry in hole-doped systems. Contrary to usual scenarios where charge and spin fluctuations are seen to compete, here the superconductivity is driven simultaneously by both charge and spin fluctuations and crucially relies on the presence of the long-range tail of the interaction. We provide an analysis of the relevant collective bosonic modes and predict how a cumulative charge and spin paring mechanism leads to superconductivity in doped silicon adatom materials.
引用
收藏
页数:5
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