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Design Principles for High-Temperature Superconductors with a Hydrogen-Based Alloy Backbone at Moderate Pressure
Zihan Zhang, Tian Cui, Michael J. Hutcheon, Alice M. Shipley, Hao Song, Mingyang Du, Vladimir Z. Kresin, Defang Duan, Chris J. Pickard, and Yansun Yao
Phys. Rev. Lett. 128, 047001 – Published 28 January 2022
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Abstract
Hydrogen-based superconductors provide a route to the long-sought goal of room-temperature superconductivity, but the high pressures required to metallize these materials limit their immediate application. For example, carbonaceous sulfur hydride, the first room-temperature superconductor made in a laboratory, can reach a critical temperature () of 288K only at the extreme pressure of 267GPa. The next recognized challenge is the realization of room-temperature superconductivity at significantly lower pressures. Here, we propose a strategy for the rational design of high-temperature superconductors at low pressures by alloying small-radius elements and hydrogen to form ternary H-based superconductors with alloy backbones. We identify a “fluorite-type” backbone in compositions of the form , which exhibit high-temperature superconductivity at moderate pressures compared with other reported hydrogen-based superconductors. The phase of , with a fluorite-type H-Be alloy backbone, is predicted to be thermodynamically stable above 98GPa, and dynamically stable down to 20GPa with a high . This is substantially lower than the synthesis pressure required by the geometrically similar clathrate hydride (170GPa). Our approach paves the way for finding high- ternary H-based superconductors at conditions close to ambient pressures.
- Received 15 May 2021
- Revised 28 September 2021
- Accepted 24 December 2021
DOI:https://doi.org/10.1103/PhysRevLett.128.047001
© 2022 American Physical Society
Physics Subject Headings (PhySH)
- Research Areas
Chemical bondingCrystal structureImpurities in superconductorsPressure effectsSuperconducting phase transition
- Physical Systems
Crystal structuresHigh-temperature superconductorsHydrides
- Techniques
Density functional theoryMethods in superconductivity
Condensed Matter, Materials & Applied Physics
Authors & Affiliations
Zihan Zhang1, Tian Cui2,1,*, Michael J. Hutcheon3, Alice M. Shipley3, Hao Song1, Mingyang Du1, Vladimir Z. Kresin4, Defang Duan1,†, Chris J. Pickard5,6, and Yansun Yao7
- 1State Key Laboratory of Superhard Materials, College of Physics, Jilin University, Changchun 130012, China
- 2Institute of High Pressure Physics, School of Physical Science and Technology, Ningbo University, Ningbo 315211, China
- 3Theory of Condensed Matter Group, Cavendish Laboratory, University of Cambridge, J. J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom
- 4Lawrence Berkeley Laboratory, University of California, Berkeley, California 94720, USA
- 5Department of Materials Science & Metallurgy, University of Cambridge, 27 Charles Babbage Road, Cambridge CB3 0FS, United Kingdom
- 6Advanced Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba, Sendai 980-8577, Japan
- 7Department of Physics and Engineering Physics, University of Saskatchewan, Saskatoon, Saskatchewan S7N 5E2, Canada
- *Corresponding author.cuitian@nbu.edu.cn
- †Corresponding author.duandf@jlu.edu.cn
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Issue
Vol. 128, Iss. 4 — 28 January 2022
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Images
Figure 1
(a)The crystal structure of with [] cubic units. The U ions are shown in black and the H ions in pink. (b)The crystal structure of , in which La ions are shown in green. The backbone in consists of cubic-unit H atoms (pink) and tetrahedron-center H atoms (gray). (c)The crystal structure of , with [] cubic centers shown as red balls. (d)The crystal structure of fluorite , the Ca cations are shown in dark blue, and the F ions in light blue. (e)The crystal structure of . The backbone in consists of tetrahedral-unit H atoms (pink) and cubic-center Be atoms (blue). (f)The fluorite-type cage of .
Figure 2
Calculated enthalpy of fluorite-type hydrides . (a)The radius of atom is plotted on the axis and the radius of atom on the axis. Dynamically unstable systems are shown as black crosses. Metastable phases are shown as circles, colored according to the calculated enthalpy above the convex hull. Thermodynamically stable phases are shown as carmine squares. (b)Calculated enthalpy as a function of pressure for La-Be-H structures relative to the phase of , where structures of , , and H are from Refs.[9, 10, 11, 38, 54], respectively.
Figure 3
Pressure dependence of s for typical superconductors. The orange circles are s of fluorite-type backbone hydrides at the lowest pressure where they become dynamically stable. The red circle is at the lowest pressure where becomes thermodynamically stable (98GPa), and the suggested synthesis pressure range for cubic is highlighted in yellow. The blue squares are s of clathrate binary hydrides at the lowest pressures reported in Refs.[6, 9, 10, 39, 55]. The purple stars are s of well-known superconductors from experiment [7, 12, 24, 55]. The background is shaded according to the figure of merit used to evaluate the significance of a particular superconductor [55]. The dotted line is the pressure limit of Kawai-type multianvil presses (KMAPs) [56].
Figure 4
(a)The polarization vectors of bonds in [] backbone; in these bonds the positive charge is located at H atoms (pink) and negative charge is located at S atoms (yellow). (b)The polarization vectors of bonds in [] backbone converge, leading to a concentration of charge at the hydrogen atoms. In these bonds the positive charge is located at Be atoms (green) and the negative charge is located at H atoms (pink).