High- superconductivity in CsC compounds governed by local Cs-C Coulomb interactions
arXiv:1703.03350 · doi:10.1088/1361-648X/aa5dbd
Abstract
Unique among alkali-doped C fullerene compounds, the A15 and fcc forms of CsC exhibit superconducting states varying under hydrostatic pressure with highest transition temperatures at = 38.3 and 35.2 K, respectively. Herein it is argued that these two compounds under pressure represent the optimal materials of the C family, and that the C-associated superconductivity is mediated through Coulombic interactions with charges on the alkalis. A derivation of the interlayer Coulombic pairing model of high- superconductivity employing non-planar geometry is introduced, generalizing the picture of two interacting layers to an interaction between charge reservoirs located on the C and alkali ions. The optimal transition temperature follows the algebraic expression, = (12.474 nm K)/, where relates to the mean spacing between interacting surface charges on the C and is the average radial distance between the C surface and the neighboring Cs ions. Values of for the measured cation stoichiometries of CsC with x 0 are found to be 38.19 and 36.88 K for the A15 and fcc forms, respectively, with the dichotomy in transition temperature reflecting the larger and structural disorder in the fcc form. In the A15 form, modeled interacting charges and Coulomb potential e/ are shown to agree quantitatively with findings from nuclear-spin relaxation and mid-infrared optical conductivity. In the fcc form, suppression of below is ascribed to native structural disorder. Phononic effects in conjunction with Coulombic pairing are discussed.
14 pages, 3 figures (Updated Metadata to correct typographical errors, 12 March 2017)
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