← Back to search

Distinct pressure evolution of superconductivity and charge density wave in kagome superconductor CsV3Sb5 thin flakes

Ge Ye, Mengwei Xie, Chufan Chen, Yanan Zhang, Dongting Zhang, Xin Ma, Xiangyu Zeng, Fanghang Yu, Yi Liu, Xiaozhi Wang, Guanghan Cao, Xiaofeng Xu, Xianhui Chen, Huiqiu Yuan, Chao Cao, Xin Lu

DOI 10.1103/PhysRevB.109.054501 · Physical Review B

T1

Active bibliographic source — not scientific approval

Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.

Abstract

It is intriguing to explore the coexistence and (or) competition between charge density wave (CDW) and superconductivity (SC) in many correlated electron systems, such as cuprates [M. Hücker et al., Phys. Rev. B 83, 104506 (2011); Q. Li et al., Phys. Rev. Lett. 99, 067001 (2007), and J. Fink et al., Phys. Rev. B 79, 100502(R) (2009)], organic superconductors [Y. Ihara et al., Phys. Rev. B 100, 060505(R) (2019) and N. Morinaka et al., Phys. Rev. B 80, 092508 (2009)], and dichacolgenides [X. Xi et al., Nat. Nanotechnol. 10, 765 (2015) and J. A. Galvis et al., Phys. Rev. B 87, 094502 (2013)]. Among them, the recently discovered Z2 topological kagome metals AV3Sb5 (A=K, Rb, Cs) serve as an ideal platform to study the intricate relation between them. Here, we report the electrical resistance measurements on CsV3Sb5 thin flakes (≈60 nm) under hydrostatic pressure up to 2.12 GPa to compare its pressure phase diagram of CDW and SC with its bulk form. Even though the CDW transition temperature (TCDW) in CsV3Sb5 thin flakes is still monotonically suppressed under pressure and totally vanishes at P2=1.83 GPa similar to the bulk, the superconducting transition temperature (Tc) shows an initial decrease and consequent increase up to its maximum ∼8.03 K at P2, in sharp contrast with the M-shaped double domes in the bulk CsV3Sb5. Our results suggest the important role of reduced dimensionality on the CDW state and its interplay with the SC, offering a new perspective to explore the exotic nature of CsV3Sb5.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
CsV3Sb5

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

4.4Pressure unresolvedonset
CsV3Sb5

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

3.8Pressure unresolvedzero_resistance
CsV3Sb5

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

8.031.83 GPaonset
CsV3Sb5

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

2.5Pressure unresolvedunknown
RbV3Sb5

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

0.92Pressure unresolvedunknown
KV3Sb5

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

0.93Pressure unresolvedunknown

Similar papers