论文标题
高 - $ t \ rm_ {c} $ clathrate的超导率y $ _ {3} $ euh $ _ {24} $
High-$T\rm_{c}$ superconductivity of clathrate Y$_{3}$EuH$_{24}$
论文作者
论文摘要
三元超水的理论预测及其随后的实验确认的最新进展使我们引入了新一代的超导体,有可能实现最期待的室温超导体的综合。由于最近对YH $ _6 $和EUH $ _6 $的高压实验的动机,我们理论上通过混合两种化合物来研究了稳定性以及超导性。在这里,我们确定了四个阶段,能够在150-300 GPA的压力范围内保持热力学稳定性,即$ fm \ bar {3} m $ -y $ -y $ _ $ _ {3} $ euh $ _ {24} $,$ cmmm $ -cmmm $ -yeuh $ _ {12} $, $ cmmm $ -yeu $ _ {3} $ h $ _ {24} $,$ immm $ -yeu $ _ {3} $ h $ _ {24} $。其中,只有$ fm \ bar {3} m $ -y $ _ {3} $ euh $ _ {24} $可以在搜索的压力范围内保持动态稳定性。 Allen-Dynes修改后的McMillan公式用于进一步检查此阶段的超导性,结果表明,y $ _ {3} $ _ {3} $ euh $ _ $ _ {24} $的预测超导过渡温度$ t \ rm_ {c} $在200 gpa处接近220 k。 $ fm \ bar {3} m $ -y $ _ {3} $ euh $ _ {24} $具有几乎相同的对数平均声子频率$ $ω__{log} $ to yh $ _ {6} $,但其电子量(EPC)常数$ yh yhy y yh y yh yh yh yh y yh y ys y ys y ys 2. 6 y $在较低的终极$ t_ {c} $ value中。
Recent progress on theoretical predictions of ternary superhydrides and their subsequent experimental confirmations have introduced us with a new generation of superconductors, having the potential to realize the synthesis of the most anticipated room temperature superconductors. Motivated by the recent high pressure experiment on YH$_6$ and EuH$_6$, we have theoretically examined the stability as well as superconductivity by mixing the two compounds. Here we identified four phases capable of maintaining thermodynamic stability in the pressure range of 150-300 GPa, namely $Fm\bar{3}m$-Y$_{3}$EuH$_{24}$, $Cmmm$-YEuH$_{12}$, $Cmmm$-YEu$_{3}$H$_{24}$,$Immm$-YEu$_{3}$H$_{24}$. Among them, only $Fm\bar{3}m$-Y$_{3}$EuH$_{24}$ can maintain dynamically stability in the searched pressure range. The Allen-Dynes modified McMillan formula was used to further check the superconductivity of this phase, and the results reveal that the predicted superconducting transition temperature $T\rm_{c}$ of Y$_{3}$EuH$_{24}$ is approaching 220 K at 200 GPa. $Fm\bar{3}m$-Y$_{3}$EuH$_{24}$ has a nearly identical logarithmic average phonon frequency $ω_{log}$ to YH$_{6}$, but its electron-phonon coupling (EPC) constant $λ$ is somewhat smaller than YH$_{6}$'s 2.56, resulting in a lower ultimate $T_{c}$ value.