Enhanced superconductivity of stoichiometric ternary superhydride YScH8 at high pressure
Weihao Jia, Xindeng Lv, Yu Huang, Qinghong Gu, Dawei He, Kaiping Hu, Xingbin Zhao, Zihan Zhang, Yanping Huang, Tian Cui
DOI 10.1103/tjqv-vxrz · Physical Review B
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Abstract
The pursuit of room-temperature superconductivity has generated growing interest in hydrogen-rich materials. However, the limited structural and compositional diversity of traditional binary superhydrides hinders further progress in this field. Ternary hydrides, with their enhanced structural flexibility and synergistic intermetallic interactions, provide a promising route to overcome these limitations. In this study, using YH4 as the parent material, we successfully synthesized two Y-Sc-H ternary hydrides by controlling laser-heating temperature and scandium doping concentration: the substitutionally doped stoichiometric P4/mmm−YScH8 and nonstoichiometric I4/mmm−(Y,Sc)H4. Electrical transport measurements revealed that P4/mmm−YScH8 exhibits a superconducting transition temperature (Tc) of 113 K at 191.7 GPa, representing a 41% enhancement over YH4 (79 K at 179 GPa), with structural stability retained down to at least 160 GPa. In contrast, I4/mmm−(Y,Sc)H4 induces only a slight modification of the Tc of the parent YH4, which is consistent with the Anderson theorem. Electronic structure calculations reveal that the band structure of P4/mmm−YScH8 is substantially reconstructed due to the introduction of Sc 3d orbitals. This shifts the van Hove-like features closer to the Fermi level, increases the density of states at the Fermi level, and consequently enhances the electron-phonon coupling, ultimately leading to an elevated superconducting transition temperature Tc. These findings demonstrate the effectiveness of elemental synergy strategies in designing high-Tc superhydrides.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| YScH8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 113 | 191.7 GPa | onset |
| YH4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 79 | 179 GPa | onset |
| LaH10 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 255 | 170 GPa | unknown |
| YH9 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 243 | 201 GPa | unknown |
| YH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 220 | 166 GPa | unknown |
| YH4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 88 | 155 GPa | unknown |
| YScH8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 110 | 140 GPa | unknown |
| (Y,Sc)H4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 124 | 100 GPa | unknown |
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