Hydrogen bond conversion and near room temperature superconductivity in oxygen hydrides
Si-Yuan Liu, Pei-Ying Huo, Wei-Zhou Jiang, Rong-Yao Yang, Yan-Hui Liu
DOI 10.1103/PhysRevB.109.104514 · Physical Review B
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Abstract
The discovery of hydrogen-rich high Tc superconducting materials, such as H3S and LaH10 under the ultrahigh pressures of more than one million atmospheres is constantly refreshing the record of superconducting critical temperature, ushering the era of room temperature superconductivity. Herein, we investigate the role of the hydrogen bond in the superconductivity of the superhydrides of oxygen, as the hydrogen bond reflects an electronic structure of oxygen in terms of the polarity of the lone pair of electrons. In an extensive exploration of the structures and superconductivity in oxygen hydrides, we predict a high Tc superconducting transition in Im−3m phase of H3O with first-principles calculations combined with swarm-structure search. A high Tc of 301.5 K is obtained, as the Im−3m phase of H3O is dynamically stabilized at the pressure as high as 670 GPa. It is found that a significant contribution to superconduction arises from the oxygen s-state electrons. With increasing the pressure, the orbital hybridization brings the essential rise of the coordination unsaturation that is favorable for the emergence of the superconductivity, whereas the superhydride compound reaches the stability at a much higher pressure than that for the isoelectric compounds of the sulfur, selenium, and tellurium due to the difficulty in orbital hybridization for the larger energy-level spacing in oxygen. Considering the difference in the hydrogen bond, we also investigate the isotope effect and obtain Tc values up to 247 K for D3O. Our work deepens the understanding of the relationship between superconductivity and coordination unsaturation in the presence of the strong hydrogen bond and can be instructive for the design of superconducting materials under pressurization.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| H3O Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 301.5 | 670 GPa | unknown |
| D3O Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 247 | 670 GPa | unknown |
| CaH6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 215 | 172 GPa | unknown |
| LaH10 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 255 | Pressure not reported | unknown |
| H3S Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 203 | 155 GPa | unknown |
| HSe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 40 | Pressure not reported | unknown |
| H3Se Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 110 | Pressure not reported | unknown |
| H4Te Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 104 | Pressure not reported | unknown |
| H5Te2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 58 | Pressure not reported | unknown |
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