Computational Design of Novel Hydrogen-Rich YS–H Compounds
Author(s) -
Ju Chen,
Wenwen Cui,
Jingming Shi,
Meiling Xu,
Jian Hao,
A.P. Durajski,
Yinwei Li
Publication year - 2019
Publication title -
acs omega
Language(s) - Uncategorized
Resource type - Journals
SCImago Journal Rank - 0.779
H-Index - 40
ISSN - 2470-1343
DOI - 10.1021/acsomega.9b02094
Subject(s) - ternary operation , superconductivity , ambient pressure , crystal structure prediction , hydrogen , fermi level , metallic hydrogen , stoichiometry , crystal structure , crystal (programming language) , diamond anvil cell , materials science , crystallography , hydrogen storage , chemical physics , metal , chemistry , condensed matter physics , high pressure , thermodynamics , electron , metallurgy , physics , organic chemistry , quantum mechanics , computer science , programming language
The recent successful findings of H 3 S and LaH 10 compressed above 150 GPa with a record high T c (above 200 K) have shifted the focus on hydrogen-rich materials for high superconductivity at high pressure. Moreover, some studies also report that transition-metal ternary hydrides could be synthesized at a relatively low pressure (∼10 GPa). Therefore, it is highly desirable to investigate the crystal structures of ternary hydrides compounds at high pressure since they have been long considered as promising superconductors and hydrogen-storage materials with a high T c , and can be possibly synthesized at low pressure as well. In this work, combining state-of-the-art crystal structure prediction and first-principles calculations, we have performed extensive simulations on the crystal structures of YSH n ( n = 1-10) compounds from ambient pressure to 200 GPa. We uncovered three thermodynamically stable compounds with stoichiometries of YSH, YSH 2 , and YSH 5 , which became energetically stable at ambient pressure, 143, and 87 GPa, respectively. Remarkably, it is found that YSH contains monoatomic H atoms, while YSH 2 and YSH 5 contain a mixture of atomlike and molecular hydrogen units. Upon compression, YSH, YSH 2 , and YSH 5 undergo a transition from a semiconductor to a metallic phase at pressures of 168, 143, and 232 GPa, respectively. Unfortunately, electron-phonon coupling calculations reveal that these compounds possess a weak superconductivity with a relatively low T c (below 1 K), which mainly stem from the low value of density of states occupation at the Fermi level ( E F ). These results highlight that the crystal structures play a critical role in determining the high-temperature superconductivity.
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