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Superconductivity near 70 K in boron-carbon clathrates MB2C8 (M=Na, K, Rb, Cs) at ambient pressure

Bin Li, Yulan Cheng, Cong Zhu, Jie Cheng, and Shengli Liu
Phys. Rev. B 109, 184517 – Published 22 May 2024

Abstract

Inspired by the first boron-carbon (B-C) clathrate SrB3C3 and the ternary borohydride KB2H8 [Miao et al., Phys. Rev. B 104, L100504 (2021)], we have performed first-principles density functional theory calculations of the electronic and phonon band structures for B-C compounds MB2C8 (M = Na, K, Rb, Cs). Our calculations reveal that these materials are dynamically stable and can potentially exhibit superconductivity at ambient pressure. However, only the K, Rb, and Cs compounds exhibit thermodynamic stability below 50 GPa, while NaB2C8 remains thermodynamically unstable at all pressures considered. Based on the Allen and Dynes modified McMillan equation, we predict the superconducting transition temperature Tc of these compounds to be over 65 K at ambient pressure, with Tc decreasing under higher pressures. Remarkably, we find CsB2C8 possesses the highest predicted Tc of 68.76 K. Our findings demonstrate the possibility of high temperature superconductivity in cubic MB2C8 at ambient pressure, expanding the B-C clathrate superconductor family. These results provide valuable insights to guide the identification of new atmospheric pressure superconductors.

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  • Received 11 March 2024
  • Revised 1 May 2024
  • Accepted 14 May 2024

DOI:https://doi.org/10.1103/PhysRevB.109.184517

©2024 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Bin Li1,2,*, Yulan Cheng3, Cong Zhu3, Jie Cheng1,2,†, and Shengli Liu1

  • *libin@njupt.edu.cn
  • chengj@njupt.edu.cn

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Issue

Vol. 109, Iss. 18 — 1 May 2024

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Images

  • Figure 1
    Figure 1

    (a) The top view and (b) side view of the crystal structure of MB2C8, where M refers to an alkali metal. The blue, pink, and gray spheres represent the M, boron, and carbon atoms, respectively. (c) The B8C24 cage with M in the center.

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  • Figure 2
    Figure 2

    Calculated enthalpy change (ΔH) as a function of pressure for MB2C8 compounds with M = Na, K, Rb, Cs. ΔH is referenced relative to the enthalpy of decomposition into standard elemental phases decompositions at the corresponding pressure. Other possible decomposition enthalpies were also considered. More negative ΔH indicates greater thermodynamic stability. Figures (a)–(d) show ΔH plots for NaB2C8, KB2C8, RbB2C8, and CsB2C8, respectively.

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  • Figure 3
    Figure 3

    (a)–(c) Phonon dispersion curves showing the phonon frequencies (ωqν) with a color scale representing the phonon linewidths (λqνωqν), the phonon density of states (PHDOS) projected onto individual atoms, the Eliashberg spectral function α2F(ω), and the electron-phonon coupling strength λ(ω) at 40 GPa for (a) KB2C8, (b) RbB2C8, and (c) CsB2C8. In the PHDOS plots, the projections onto the K, Rb, Cs (red), B (yellow), and C (blue) atoms are shown in different colors to distinguish the contributions of different atoms.

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  • Figure 4
    Figure 4

    Electronic band structures and partial density of states (DOS) projected on individual atomic species for MB2C8 (M = K, Rb, Cs) at 40 GPa pressure for KB2C8, (b) RbB2C8, and (c) CsB2C8. In the DOS plots, the projections onto the M (K/Rb/Cs), B, and C atoms are shown in yellow, blue, and red colors, respectively. The Fermi energy is set to zero on the energy scale.

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  • Figure 5
    Figure 5

    (a) Electronic band structures of CsB2C8 at 40 GPa. (b) The three Fermi surfaces (FS#1, FS#2, FS#3) derived from bands crossing the Fermi level in (a). The FS contours are colored according to the Fermi velocities.

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  • Figure 6
    Figure 6

    (a) Calculated electron-phonon coupling constant λ, and (b) logarithmic average of phonon frequency ωlog for MB2C8 (M = Na, K, Rb, Cs) as a function of pressure.

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