Topological electronic states, superconductivity, and ferromagnetism in two-dimensional ScXS2 (X=Rh, Ta, Mo) monolayers
Haifei Qin, Hong Sun
DOI 10.1103/pnry-ysbl · Physical Review B
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
The two-dimensional (2D) materials with coexistence of Dirac points and Van Hove singularities (VHSs) provide a promising platform for seeking topological superconductivity or ferromagnetism at high critical temperatures. However, ideal examples combining electronic topological properties with superconductivity or ferromagnetism are scarce. Here, through structural search, we identify 2D ScXS2 (X = Rh, Ta, Mo) monolayers with simple square or rectangular lattices, where VHSs lie near Dirac points close to the Fermi levels. Using first-principles calculations, Bardeen-Cooper-Schrieffer theory, and Monte Carlo simulations, we found that all the three monolayers exhibit nontrivial topological electronic properties. Moreover, ScRhS2 is intrinsically superconducting with Tc = 1.36 K; ScTaS2 shows tunable superconductivity reaching Tc = 2.21 K under 6% uniaxial tensile strain which also displays ferroelasticity induced by the Jahn-Teller effect; and ScMoS2 hosts a topological ferromagnetic half-metal ground state with a giant anomalous Hall effect and Curie temperature of 329 K stabilized by a high magnetic anisotropy energy of 1.837 meV/Mo. These results establish ScXS2 monolayers as a versatile 2D material family for exploring exotic mixtures of topological states, superconductivity, and half-metal ferromagnetism, offering potential for novel electronic and spintronic applications.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| UTe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1.6 | Pressure not reported | unknown |
| FeTe0.5Se0.5 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 15 | Pressure not reported | unknown |
| ScRhS2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1.36 | Pressure not reported | unknown |
| ScTaS2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2.21 | Pressure not reported | unknown |
Similar papers
Spatial variation of the two-fold anisotropic superconducting gap in a monolayer of FeSe0.5Te0.5 on a topological insulator
similarity 0.96A. Kamlapure et al.
Source status unknown — claims are unverified
UTe2: A narrow-band superconductor
similarity 0.94Martin Sundermann et al.
Source status unknown — claims are unverified
Effect of impurity substitution on band structure and mass renormalization of the correlated FeTe0.5Se0.5 superconductor
similarity 0.94S. Thirupathaiah et al.
Source status unknown — claims are unverified
Change of superconducting character in UTe2 induced by magnetic field
similarity 0.94K. Kinjo et al.
Source status unknown — claims are unverified
Correlation between Fermi surface reconstruction and superconductivity in pressurized FeTe0.55Se0.45
similarity 0.94Gongchang Lin et al.
Source status unknown — claims are unverified
Effect of doping on electrical, magnetic, and superconducting properties of KxFe2−yS2
similarity 0.94Jiangang Guo et al.
Source status unknown — claims are unverified