Family of binary transition metal pnictide superconductors
Zheng-Wei Liao, Xin-Wei Yi, Jing-Yang You, Bo Gu, Gang Su
DOI 10.1103/PhysRevB.108.014501 · 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
Superconductivity in transition metal nitrides (TMNs) has been investigated for a long time, such as zirconium nitride (ZrN) with a superconducting transition temperature Tc of 10 K. Recently, a phase diagram has been revealed in ZrNx with different nitrogen concentrations, which is very similar to that of high-temperature copper oxide superconductors. Here, we study the TMNs with a face-centered cubic lattice where ZrN and HfN have been experimentally obtained and predict eight new stable superconductors by the first-principles calculations. We find that CuN has a high Tc of 30 K with a very strong electron-phonon coupling (EPC) strength. In contrast to ZrN, CuN has softening acoustic phonons at the high-symmetry point L, which accounts for its much stronger EPC. In addition, the highly symmetrical structure leads to topological nodal points and lines, such as the hourglass Weyl loop on the kx/y/z=0 plane and Weyl points on the kx/y/z=2π/a plane, as well as quadratic band touch at the Γ point. CuN could be a topological superconductor. Our results expand the transition metal nitrides superconductor family and would be helpful to guide the search for high-temperature topological superconductors.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| CdN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 19.86 | Pressure unresolved | unknown |
| CdP Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 11.64 | Pressure unresolved | unknown |
| CdAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 10.29 | Pressure unresolved | unknown |
| CuN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 29.64 | Pressure unresolved | unknown |
| CuSb Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6.03 | Pressure unresolved | unknown |
| HfN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 9.1 | Pressure unresolved | unknown |
| HfN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8.8 | Pressure not reported | unknown |
| HfP Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 4.74 | Pressure unresolved | unknown |
| HgSb Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.57 | Pressure unresolved | unknown |
| ZnSb Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 9.81 | Pressure unresolved | unknown |
| ZrN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 10.65 | Pressure unresolved | unknown |
| ZrN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 10 | Pressure not reported | unknown |
| CuN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 29.28 | 1 GPa | unknown |
| CuN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 29.01 | 2 GPa | unknown |
| CuN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 28.5 | 3 GPa | unknown |
| CuN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 28.01 | 4 GPa | unknown |
| CuN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 27.5 | 5 GPa | unknown |
| ZrN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 10.8 | 1 GPa | unknown |
| ZrN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 10.66 | 2 GPa | unknown |
| ZrN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 10.5 | 3 GPa | unknown |
| ZrN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 10.39 | 4 GPa | unknown |
| ZrN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 10.26 | 5 GPa | unknown |
Similar papers
Electronic structure of superconducting layered zirconium and hafnium nitride
similarity 0.93Izumi Hase & Yoshikazu Nishihara
Source status unknown — claims are unverified
Thermodynamics of ferromagnetic superconductors with spin-triplet electron pairing
similarity 0.92Diana V. Shopova & Dimo I. Uzunov
Source status unknown — claims are unverified
Spin-fluctuation-mediated d+id′ pairing mechanism in doped β−MNCl (M=Hf,Zr) superconductors
similarity 0.91Kazuhiko Kuroki
Source status unknown — claims are unverified
Ni3AlB: A bridge between superconductivity and ferromagnetism
similarity 0.91Izumi Hase
Source status unknown — claims are unverified
Longitudinal Spin Fluctuations and Superconductivity in Ferromagnetic ZrZn2 from Ab Initio Calculations
similarity 0.91G. Santi et al.
Source status unknown — claims are unverified
Pressure-induced superconductivity in Bi2−xSbxTe3−ySey
similarity 0.91Tong He et al.
Source status unknown — claims are unverified