Superconductivity of cubic MB6 (M = Na, K, Rb, Cs).

Previous studies have shown that NaB₆, KB₆, and RbB₆ adopting Pm 3 ̄ m are superconductors with a relatively high T_c under ambient conditions. In this paper, we conducted systematic structural and related properties research on CsB₆ through a genetic evolution algorithm and total energy calculations based on density functional theory between 0 and 20 GPa. Our results reveal a cubic Pm 3 ̄ m CsB₆, which is dynamically stable under the pressures we studied. We systematically calculated the formation enthalpies, electronic properties, and superconducting properties of Pm 3 ̄ m MB₆ (M = Na, K, Rb, Cs). They all exhibit metallic features, and boron has high contributions to band structures, density of states, and electron–phonon coupling (EPC). The calculated results about the Helmholtz free energy difference of Pm 3 ̄ m CsB₆ at 0, 10, and 20 GPa indicate that it is stable upon chemical decomposition (decomposition to simple substances Cs and B) from 0 to 400 K. The phonon density of states indicates that boron atoms occupy the high frequency area. The EPC results show that Pm 3 ̄ m CsB₆ is a superconductor with T_c = 11.7 K at 0 GPa, close to NaB₆ (13.1 K), KB₆ (11.7 K), and RbB₆ (11.3 K) at 0 GPa in our work, which indicates that boron atoms play an essential role in superconductivity: vibrations of B₆ regular octagons lead to the high T_c of Pm 3 ̄ m MB₆. Our work about Pm 3 ̄ m hexaborides provides a supplementary study on the borides of the group IA elements (without Fr and Li) and has an important guiding significance for the experimental synthesis of CsB₆. [ABSTRACT FROM AUTHOR]