Abstract

The research on the superconductivity of hydrogen-rich compounds has become a hot research topic in the field of high-temperature superconductors in recent years and yttrium hydride YH<sub>9+x</sub> has been experimentally confirmed to have high temperature superconductivity (near room temperature (Tc = 262 K)), following behind the research of H<sub>3</sub>S (Tc = 200 K) and LaH<sub>10</sub> (Tc = 260 K). The theoretical study of binary hydrogen-rich systems is relatively mature, while the structural characteristics and superconductivity of ternary or quaternary hydrogen-rich compounds are still under exploration. In this paper, nLiH + YH<sub>3</sub>→Li<sub>n</sub>YH<sub>n+3</sub> (<i>n</i> = 1–3) is the synthesis way to explore the stable configuration of ternary hydride LinYH<sub>n+3</sub> in a pressure range of 0–300 GPa. The crystal structure, electronic structure, thermodynamic and kinetic stability of LiYH<sub>4</sub>, Li<sub>2</sub>YH<sub>5</sub> and Li<sub>3</sub>YH<sub>6</sub> in the pressure range of 0–300 GPa are studied based on the structure prediction by particle swarm optimization algorithm and first-principles calculation. The CALYPSO method is used to search for 1–4 times molecular formula structures for Li-Y-H ternary systems with different stoichiometric ratios in the pressure range of 0–300 GPa in steps of 50 GPa. The results show that LiYH<sub>4</sub>-<i>P</i>4/<i>nmm</i>, Li<sub>2</sub>YH<sub>5</sub>-<i>I</i>4/<i>mmm</i>, and Li<sub>3</sub>YH<sub>6</sub>-P4/nmm can be respectively synthesized with a certain ratio between LiH and YH<sub>3</sub> respectively in a pressure range of 169–221 GPa, 141–300 GPa and 166–300 GPa. The Li<sub>2</sub>YH<sub>5</sub> has the lowest stable pressure and widest range which can be the possible choice in experiment. The results can provide the data support for the superconductivity research and experimental synthesis of hydrides in Li-Y-H ternary system.

Highlights

  • The results show that LiYH4-P4/nmm, Li2YH5-I4/mmm, and Li3YH6-P4/nmm can be respectively synthesized with a certain ratio between LiH and YH3 respectively in a pressure range of 169–221 GPa, 141–300 GPa and 166–300 GPa

  • 1) (Science and Technology on Surface Physics and Chemistry Laboratory, Mianyang 621907, China) 2) (Institute of Atomic and Molecular Physics, Sichuan University, Chengdu 610065, China) ( Received 30 April 2021; revised manuscript received 7 September 2021 )

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Summary

17 GPa 25 GPa

图 3 考虑零点能 (ZPE) 修正后不同 LiYH4 结构的焓值在 (a) 0−35 GPa 范围内和 (b) 290−325 GPa 范围内随压力的变化关系. 图 4 不同 LiYH4 结构 (a) P21/m (1 atm), (b) P4/nmm (150 GPa) 和 (c) Cmmm (300 GPa) 的等值面值为 0.5 的三维电子局域 函数 (ELF). 弱的相互作用 (图 4(c)), 实际上, H1 和 H6 原子之 间相交的区域 (绿色区域)ELF 数值较小, 不足 0.5, 不能判断它们之间是否形成了共价键; 而如图 4(a) 和 4(b) 所示, 当 ELF 图的等值面值设置为 0.5 时, 低压相 P21/m 和 P4/nmm 中 H 原子之间不存在 相互作用, 在 3.5 节中 Bader 电荷分析 P4/nmm 结构中 H 呈离子性, 进一步说明该结构中 H 原子 之间没有共价相互作用

Li2YH5
GPa Cmc21 with ZPE Pmmn with ZPE
Li3YH6
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