Theoretical Explanation of Superconductivity in C6Ca
Overview
Authors
Affiliations
Using density functional theory, we demonstrate that superconductivity in C6Ca is phonon mediated with lambda = 0.83 and phonon frequency (omega)log = 24.7 meV. The calculated isotope exponents are alpha(Ca) = 0.24 and alpha(C) = 0.26. Superconductivity is due mostly to C vibrations perpendicular and Ca vibrations parallel to the graphite layers. Since the electron-phonon couplings of these modes are activated by the presence of an intercalant Fermi surface, the occurrence of superconductivity in graphite intercalated compounds requires a noncomplete ionization of the intercalant.
Charge stripes in the graphene-based materials.
Grozic P, Keran B, Kadigrobov A, Radic D Sci Rep. 2023; 13(1):18931.
PMID: 37919346 PMC: 10622548. DOI: 10.1038/s41598-023-46157-1.
Pressure-induced phase transitions and superconductivity in magnesium carbides.
Kim S, Kim K, Koo J, Lee H, Min B, Kim D Sci Rep. 2019; 9(1):20253.
PMID: 31882982 PMC: 6934831. DOI: 10.1038/s41598-019-56497-6.
Preparation and characterization of a new graphite superconductor: CaSrC.
Nishiyama S, Fujita H, Hoshi M, Miao X, Terao T, Yang X Sci Rep. 2017; 7(1):7436.
PMID: 28785117 PMC: 5547157. DOI: 10.1038/s41598-017-07763-y.
Phonon-mediated high-T superconductivity in hole-doped diamond-like crystalline hydrocarbon.
Lian C, Wang J, Duan W, Chen C Sci Rep. 2017; 7(1):1464.
PMID: 28469256 PMC: 5431101. DOI: 10.1038/s41598-017-01541-6.
Synthesis and superconducting properties of CaC.
Emery N, Herold C, Mareche J, Lagrange P Sci Technol Adv Mater. 2016; 9(4):044102.
PMID: 27878015 PMC: 5099629. DOI: 10.1088/1468-6996/9/4/044102.