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Superconducting dense lithium-based germanides with electride states

Qianyi Wang, Jiahui Wei, Ting Zhong, Jiance Sun, Bo Gao, Li Zhu, Hanyu Liu, Shoutao Zhang

DOI 10.1103/PhysRevB.110.144523 · Physical Review B

T1

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Abstract

Lithium-based electrides with interstitial anionic electrons (IAEs) have recently garnered a great deal of attention, since these materials were found to host intriguing properties such as multiple IAE arrangements and potential superconductivity. In this study, we here conducted comprehensive simulations on the pressure-induced stable Li-abundant germanides leveraging the advanced first-principles structure predictions. As a consequence, our simulations identified several metallic Li-Ge electride phases with robust stability, i.e., Li5Ge, Li6Ge, Li7Ge, Li8Ge, and Li10Ge. Strikingly, the evolution from connected one-dimensional (1D) to zero-dimensional (0D) electride states of Li5Ge was identified concurrent with an orthorhombic Cmcm to triclinic C2/c phase transition on account of compression-induced volume reduction, whereas Li10Ge possesses the unusual coexistent 0D and 1D IAEs. Electron-phonon coupling (EPC) calculations uncover that the superconductivity of Cmcm Li5Ge is superior to that of C2/c Li5Ge at 50 GPa, which is due to the larger EPC strength, higher density of states at the Fermi level, and more pronounced softened phonon modes of Cmcm Li5Ge. Remarkably, Li10Ge was calculated to have the highest superconducting critical temperature (Tc) of 8.5 K below 50 GPa compared to other lithium-carbon family electrides, which is ascribed to the fact that the Li 2p electron states near the Fermi energy are strongly coupled with phonon modes associated with the vibrations of Li atoms. Our findings provide insights into lithium-bearing electride systems with implications for the pursuit of distinguished electride superconductors.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Li5Ge

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—50 GPaunknown
Li5Ge

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—50 GPaunknown
Li10Ge

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8.550 GPaunknown
H3S

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203155 GPaunknown
CaH6

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215172 GPaunknown
LaH10

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255188 GPaunknown
LaBeH8

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11080 GPaunknown
Li5He2

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26210 GPaunknown
Li5C

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48.3210 GPaunknown
Li6C

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1080 GPaunknown
Li5Si

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1.1Pressure unresolvedunknown
Li5Si

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7.2100 GPaunknown
Li5C

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5.795 GPaunknown
Ge

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5Pressure not reportedunknown

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