Maximum Tc at the verge of a simultaneous order-disorder and lattice-softening transition in superconducting CaC6
A. Gauzzi, N. Bendiab, M. d’Astuto, B. Canny, M. Calandra, F. Mauri, G. Loupias, N. Emery, C. Hérold, P. Lagrange, M. Hanfland, M. Mezouar
DOI 10.1103/PhysRevB.78.064506 · Physical Review B
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Abstract
In order to account for the large drop of superconducting critical temperature, Tc, and for the dramatic increase in residual resistivity, ϱ0, previously reported in CaC6 at Pcr≈9 GPa, we studied the room-temperature crystal structure of bulk CaC6 samples as a function of pressure up to 13 GPa by means of synchrotron x-ray diffraction in diamond anvil cells. At Pcr, we found no change of the trigonal R3¯m space group symmetry, but a large increase in isothermal compressibility, κ, from −0.0082 GPa−1 to −0.0215 GPa−1, accompanied by a large broadening of Bragg peaks. With both effects being reversible, it follows that superconductivity in CaC6 is maximized at the verge of a peculiar order-disorder phase transition concomitant to a large lattice softening. Space group symmetry considerations supported by ab initio calculations of the relaxed structure within the density functional theory lead us to conclude that the disordered phase is presumably characterized by a random off-centering of the Ca atoms in the ab plane with respect to the C honeycomb layers.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| CaC6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 11.5 | Pressure unresolved | unknown |
| CaC6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 15.1 | 7.5 GPa | onset |
| CaC6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5 | 9 GPa | unknown |
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