s±-wave superconductivity in pressurized La4Ni3O10

被引:2
|
作者
Zhang, Ming [1 ]
Sun, Hongyi [2 ,3 ]
Liu, Yu-Bo [4 ]
Liu, Qihang [5 ,6 ,7 ]
Chen, Wei-Qiang [5 ,6 ,7 ]
Yang, Fan [4 ]
机构
[1] Zhejiang Sci Tech Univ, Dept Phys, Zhejiang Key Lab Quantum State Control & Opt Field, Hangzhou 310018, Zhejiang, Peoples R China
[2] Southern Univ Sci & Technol, Shenzhen Inst Quantum Sci & Engn, Shenzhen 518055, Peoples R China
[3] Int Quantum Acad, Shenzhen 518048, Peoples R China
[4] Beijing Inst Technol, Sch Phys, Beijing 100081, Peoples R China
[5] Southern Univ Sci & Technol, Dept Phys, Shenzhen 518055, Peoples R China
[6] Southern Univ Sci & Technol, Guangdong Basic Res Ctr Excellence Quantum Sci, Shenzhen 518055, Peoples R China
[7] Southern Univ Sci & Technol, Shenzhen Key Lab Adv Quantum Funct Mat & Devices, Shenzhen 518055, Peoples R China
基金
国家重点研发计划;
关键词
PHASE; ORDER;
D O I
10.1103/PhysRevB.110.L180501
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Recently, evidence of superconductivity (SC) has been reported in pressurized La4Ni3O10. Here we study its possible pairing mechanism and pairing symmetry. Through fitting the density-functional-theory band structure, we provide a six-orbital tight-binding model. In comparison with the band structure of La3Ni2O7, the additional nonbonding dz2 band is important to the pairing mechanism here. When the multiorbital Hubbard interactions are included, our random-phase-approximation based study yields an s +/--wave SC. The dominant Fermi-surface nesting with vector Q1 approximate to (n, n) is between the gamma pocket contributed by the bonding dz2 band top and the alpha 1 pocket contributed by the nonbonding dz2 band bottom, leading to the strongest pairing amplitude and opposite gap signs within the two regimes. The dominant real-space pairing is the interlayer dz2-orbital pairing. This s +/--wave pairing pattern is insensitive to the band details. Upon electron doping, the Tc would increase promptly before the system enters the N & eacute;el-ordered spin-density-wave phase.
引用
收藏
页数:9
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