Crystal structure evolution and superconductivity of the ternary hydride CSH3 under pressure
Kai Hu, Qingjun Tong, Li-Min Guan, Dahui Wang, Jinqing Yu
DOI 10.1103/PhysRevB.105.094108 · Physical Review B
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Abstract
Under high-pressure conditions, the changes of atomic arrangement and stacking of the lattice structures lead to enhanced electronic correlation effect and even superconductivity. Motivated by a recent experimental demonstration of pressure-induced superconductivity in a C-S-H system, in this work, we construct a CSH3 system via simple combining of H3S and C to study the crystal structural evolution and possible superconductivity at high pressure using first-principles calculations. We predicted the trigonal and orthorhombic crystal structures of CSH3 under pressure, with the space groups R−3m, Pbcm, and Pmmn, respectively. We find that the trigonal R−3m phase transform to the orthorhombic Pbcm phase at 210 GPa, at which the volume of CSH3 phases drops by ∼7%. Due to large the electronic density of states of the H component near the Fermi level, the Tc is higher in the Pbcm and the Pmmn phases than in the R−3m phase. A Tc as high as 98 K is found for the Pbcm phase at 250 GPa.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| CSH3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 98 | 250 GPa | unknown |
| CSH3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 63 | 250 GPa | unknown |
| H3SXe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 89 | 240 GPa | unknown |
| H6SSe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 195 | Pressure not reported | unknown |
| YSH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 95 | Pressure not reported | unknown |
| KScH12 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 122 | Pressure not reported | unknown |
| GaAsH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 98 | Pressure not reported | unknown |
| CH4Mg Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 84 | Pressure not reported | unknown |
| LiPH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 150 | Pressure not reported | unknown |
| Li5MoH11 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6.5 | Pressure not reported | unknown |
| BaReH9 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 7 | Pressure not reported | unknown |
| CH4K Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 12 | Pressure not reported | unknown |
| CS2H10 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 155 | 150 GPa | unknown |
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