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Superconductivity in dense scandium-based phosphides

Kaixuan Zhao, Qianyi Wang, Honggang Li, Bo Gao, Shubo Wei, Li Zhu, Haiyang Xu, Hanyu Liu, Shoutao Zhang

DOI 10.1103/PhysRevB.108.174513 · Physical Review B

T1

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Abstract

The recent achievement of room-temperature superconductivity at near-ambient pressure in nitrogen-doped lutetium hydride further boosts enthusiasm for the pursuit of high-temperature superconductors. Transition-metal phosphides (TMPs) have attracted substantial attention due to their fascinating properties encompassing superconductivity. Nevertheless, the superconducting scandium-based phosphides with high scandium concentration are not well comprehended. Towards this end, our work focuses on the rational design of scandium-rich phosphides via the first-principles swarm structure calculations under pressure. Strikingly, several metallic phases, viz., ScP, Sc2P, and Sc3P, are unambiguously uncovered wherein P atoms exhibit captivating configurations from ladder, linear chain, and eventually to isolated atom. Further electron-phonon coupling simulations elucidate that P6/mmm Sc2P, isostructural to MgB2, possesses a remarkable superconducting transition temperature, Tc, of ∼20 K at 100 GPa, mainly deriving from the large acoustic phonon softening in the low-frequency region. Tetragonal I4/mmm Sc3P is revealed to host a high phonon-mediated superconductivity of 20.5 K at 140 GPa, which is chiefly attributed to the significant coupling between the low-frequency softened acoustic and optical phonon modes associated with the Sc-dominated vibrations and Sc 3d electronic states around the Fermi energy. This study paves the way for discovering distinguished superconductors in transition metal-based phosphide systems.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Sc2P

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20100 GPaunknown
Sc2P

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19.8100 GPaunknown
Sc3P

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20.5140 GPaunknown
H3S

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203155 GPaunknown
CaH6

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215172 GPaunknown
CaH6

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210160 GPaunknown
LaH10

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250170 GPaunknown
LaH10

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260188 GPaunknown
MnP

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1Pressure not reportedunknown
Mo3P

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5.5Pressure not reportedunknown
Nb2P5

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2.6Pressure not reportedunknown
YP2

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9.5Pressure not reportedunknown
Y3P

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12.1Pressure not reportedunknown
LaP2

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22.211 GPaunknown
Sc

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36260 GPaunknown
Sc

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32283 GPaunknown
ScH12

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313Pressure not reportedunknown
ScP4

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1150 GPaunknown

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