Superconducting gap evolution of kagome metal CsV3Sb5 under pressure

被引:5
作者
Zhang, Dongting [1 ,2 ]
Chen, Chufan [1 ,2 ]
Yin, Lichang [1 ,2 ]
Huang, Yan'En [1 ,2 ]
Shi, Fengrui [1 ,2 ]
Liu, Yi [3 ]
Xu, Xiaofeng [3 ]
Yuan, Huiqiu [1 ,2 ,4 ,5 ,6 ]
Lu, Xin [1 ,2 ,4 ,6 ]
机构
[1] Zhejiang Univ, Ctr Correlated Matter, Hangzhou 310058, Peoples R China
[2] Zhejiang Univ, Dept Phys, Hangzhou 310058, Peoples R China
[3] Zhejiang Univ Technol, Dept Appl Phys, Key Lab Quantum Precis Measurement Zhejiang Prov, Hangzhou 310023, Peoples R China
[4] Zhejiang Univ, Dept Phys, Zhejiang Prov Key Lab Quantum Technol & Device, Hangzhou 310058, Peoples R China
[5] Zhejiang Univ, State Key Lab Silicon Mat, Hangzhou 310058, Peoples R China
[6] Collaborat Innovat Ctr Adv Microstruct, Nanjing 210093, Peoples R China
基金
国家重点研发计划; 中国国家自然科学基金;
关键词
high pressure; point contact spectroscopy; multiband; CsV3Sb5;
D O I
10.1007/s11433-022-1979-y
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Kagome superconductors AV(3)Sb(5) (A=Cs, V, Sb) have served as an ideal platform to unveil the intriguing competitions between charge-density-wave (CDW), superconductivity and possible nontrivial topological states. We report soft point-contact spectroscopy (SPCS) studies on CsV3Sb5 under pressure up to 2.5 GPa. Its superconducting transition temperature T-c and gaps for SPCS at pressure P = 0.1 GPa suggest the absence of the adverse local strain effect as observed in point-contacts at ambient pressure, while the SPCS-determined T-c under hydrostatic pressure deviates from the reported double dome feature below 2.5 GPa. Three distinct gap values in CsV3Sb5 are proposed to exist through the whole pressure range with 2 delta(1)/k(B)T(c)<= 1, 2 delta(2)/k(B)T(c)similar to 2.3 -3.0 and 2 delta(3)/k(B)T(c)> 3.5. The two smaller gaps for 2 delta(1)/k(B)T(c)<= 1 and 2 & UDelta;(2)/k(B)T(c)similar to 2.3-3.0 are robust under pressure, while there is no trace of the largest gap 2 delta(3)/k(B)T(c)> 3.5 for SPCS in the c direction with P <= P-1 = 0.7 GPa and P >= P-2 = 2.0 GPa and it becomes observable in the pressure range of (P-1, P-2), suggesting a complex relation between CDW and superconductivity between (P-1, P-2).
引用
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页数:6
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