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Origin of superconductivity of CaC 6 and of other intercalated graphites
Author(s) -
Calandra Matteo,
Mauri Francesco
Publication year - 2006
Publication title -
physica status solidi (b)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.51
H-Index - 109
eISSN - 1521-3951
pISSN - 0370-1972
DOI - 10.1002/pssb.200669206
Subject(s) - superconductivity , condensed matter physics , fermi surface , graphite , phonon , fermi level , intercalation (chemistry) , materials science , coupling (piping) , electron , physics , quantum mechanics , composite material , metallurgy
By intercalation of donor the low conductivity of graphite can be enhanced and a superconducting state can occur at low temperature. The first discovered superconductors were alkali‐intercalated compounds, with a critical temperatures ( T c ) of the order of 1 K. In 2005 we learned with surprise that Ca intercalated graphite (CaC 6 ) is a superconductor with the sizable T c of 11.5 K. Using density functional theory we demonstrate that superconductivity in CaC 6 is phonon‐mediated with an electron–phonon coupling λ equal to 0.83 and a phonon‐frequency logarithmic‐average equal to 25 meV. Superconductivity is mostly due C vibrations perpendicular and Ca vibrations parallel to the graphite layers. A non zero electron–phonon coupling for these modes can not be associated to the Fermi surface of the graphite pi bands but requires the presence of a second Fermi surface associated to the intercalant atoms. This result suggests a general mechanism for the occurrence of superconductivity in intercalated graphite. In order to stabilize a superconducting state it is necessary to have an intercalant Fermi surface since the simple doping of the π bands in graphite does not lead to a sizeable electron–phonon coupling. This condition occurs if the intercalant band is partially occupied, i.e. when the intercalant is not fully ionized. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)