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Prediction of high-Tc superconductivity in ternary actinium beryllium hydrides at low pressure

Kun Gao, Wenwen Cui, Jingming Shi, Artur P. Durajski, Jian Hao, Silvana Botti, Miguel A. L. Marques, Yinwei Li

DOI 10.1103/PhysRevB.109.014501 · Physical Review B

T1

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Abstract

Hydrogen-rich superconductors are promising candidates to achieve room-temperature superconductivity. However, the extreme pressures needed to stabilize these structures significantly limit their practical applications. An effective strategy to reduce the external pressure is to add a light element M that binds with H to form MHx units, acting as a chemical precompressor. We exemplify this idea by performing ab initio calculations of the Ac–Be–H phase diagram, proving that the metallization pressure of Ac–H binaries, for which critical temperatures as high as 200 K were predicted at 200 GPa, can be significantly reduced via beryllium incorporation. We identify three thermodynamically stable (AcBe2H10, AcBeH8, and AcBe2H14) and four metastable compounds (fcc AcBeH8, AcBeH10, AcBeH12 and AcBe2H16). All of them are superconductors. In particular, fcc AcBeH8 remains dynamically stable down to 10 GPa, where it exhibits a superconducting-transition temperature Tc of 181 K. The Be–H bonds are responsible for the exceptional properties of these ternary compounds and allow them to remain dynamically stable close to ambient pressure. Our results suggest that high-Tc superconductivity in hydrides is achievable at low pressure and may stimulate experimental synthesis of ternary hydrides.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
AcBe2H10

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—200 GPaunknown
AcBeH8

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—200 GPaunknown
AcBe2H14

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—200 GPaunknown
AcBe2H16

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150200 GPaunknown
AcBeH10

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165300 GPaunknown
AcBeH8

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18110 GPaunknown
SH3

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

200155 GPaunknown
LaH10

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260170 GPaunknown
CaH6

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

215160 GPaunknown
YH6

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220166 GPaunknown
YH9

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

243182 GPaunknown
Li2MgH16

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473250 GPaunknown
YCeH20

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246350 GPaunknown
LaCeH20

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233250 GPaunknown
(La,Y)H10

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253183 GPaunknown
CaBeH8

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254210 GPaunknown
LaBeH8

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11080 GPaunknown
(La,Ce)H9

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

4892 GPaunknown
(La,Nd)H10

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

148180 GPaunknown
LaBH8

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

12650 GPaunknown
YBeH8

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

249100 GPaunknown
AcH16

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

241150 GPaunknown

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