Superconductivity in atom-intercalated quaternary hydrides under ambient pressure
Bo-Wen Yao, Zhenfeng Ouyang, Xiao-Qi Han, Chang-Jiang Wu, Peng-Jie Guo, Ze-Feng Gao, Zhong-Yi Lu
DOI 10.1103/rltl-vgzj · Physical Review B
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Abstract
Multinary hydrides offer great promise for achieving high-temperature conventional superconductivity under ambient pressure. However, the rich variety of structural configurations in hydrides poses a formidable challenge for searching their immense phase space. In this work, we used our developed artificial intelligence (AI) search engine (InvDesFlow) to perform extensive investigations regarding ambient stable superconducting hydrides. We assessed the thermodynamic stability of hydrides by our AI model. For K2GaCuH6, the AI-predicted formation energy difference along the synthesis path is 0.146 eV/atom, closely matching the density functional theory result of 0.137 eV/atom. This agreement confirms the thermodynamic stability of hydrides and validates the reliability of AI method. Several quaternary hydrides with high superconducting temperature (Tc) are predicted. In particular, the superconducting Tc of K2GaCuH6 and K2LiCuH6 are calculated to be 68 and 53 K under ambient pressure, respectively, which shows a significant enhancement in comparison with that of K2CuH6 (Tc∼18K). We also find that intercalating atoms could cause phonon softening and induce more phonon modes with strong electron-phonon coupling. Hence, we propose that intercalating atoms is a feasible approach in searching for superconducting quaternary hydrides.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| K2GaCuH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 68 | Pressure unresolved | unknown |
| K2LiCuH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 53 | Pressure unresolved | unknown |
| K2CuH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 18 | Pressure unresolved | unknown |
| MgB2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 39 | Pressure unresolved | unknown |
| CaH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 205 | 172 GPa | unknown |
| H3S Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 203 | 220 GPa | unknown |
| LaH10 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 250 | 170 GPa | unknown |
| LaBeH8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 110 | 80 GPa | unknown |
| Mg2IrH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 160 | Pressure unresolved | unknown |
| Li2AuH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 140 | Pressure unresolved | unknown |
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