Anomalous enhancement of charge density wave in kagome superconductor CsV3Sb5 approaching the 2D limit
The recently discovered kagome metals AV 3 Sb 5 (A = Cs, Rb, K) exhibit a variety of intriguing phenomena, such as a charge density wave (CDW) with time-reversal symmetry breaking and possible unconventional superconductivity. Here, we report a rare non-monotonic evolution of the CDW temperature ( T...
Gespeichert in:
Veröffentlicht in: | Nature communications 2023-04, Vol.14 (1), p.2492-2492, Article 2492 |
---|---|
Hauptverfasser: | , , , , , , , , , , , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | The recently discovered kagome metals AV
3
Sb
5
(A = Cs, Rb, K) exhibit a variety of intriguing phenomena, such as a charge density wave (CDW) with time-reversal symmetry breaking and possible unconventional superconductivity. Here, we report a rare non-monotonic evolution of the CDW temperature (
T
CDW
) with the reduction of flake thickness approaching the atomic limit, and the superconducting transition temperature (
T
c
) features an inverse variation with
T
CDW
.
T
CDW
initially decreases to a minimum value of 72 K at 27 layers and then increases abruptly, reaching a record-high value of 120 K at 5 layers. Raman scattering measurements reveal a weakened electron-phonon coupling with the reduction of sample thickness, suggesting that a crossover from electron-phonon coupling to dominantly electronic interactions could account for the non-monotonic thickness dependence of
T
CDW
. Our work demonstrates the novel effects of dimension reduction and carrier doping on quantum states in thin flakes and provides crucial insights into the complex mechanism of the CDW order in the family of AV
3
Sb
5
kagome metals.
The kagome superconductor CsV
3
Sb
5
exhibits a charge density wave (CDW) as well as superconductivity (SC). Here, the authors find that the CDW transition temperature decreases with decreasing sample thickness to 72 K at 27 atomic layers, but then unexpectedly increases to 120 K at 5 layers, an opposite trend to SC. |
---|---|
ISSN: | 2041-1723 2041-1723 |
DOI: | 10.1038/s41467-023-38257-3 |