Symmetry change of d-wave superconductivity in κ-type organic superconductors
被引:13
作者:
Imajo, S.
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Osaka Univ, Grad Sch Sci, Toyonaka, Osaka 5600043, Japan
Univ Tokyo, Inst Solid State Phys, Kashiwa, Chiba 2778581, JapanOsaka Univ, Grad Sch Sci, Toyonaka, Osaka 5600043, Japan
Imajo, S.
[1
,2
]
Kindo, K.
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Univ Tokyo, Inst Solid State Phys, Kashiwa, Chiba 2778581, JapanOsaka Univ, Grad Sch Sci, Toyonaka, Osaka 5600043, Japan
Kindo, K.
[2
]
Nakazawa, Y.
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Osaka Univ, Grad Sch Sci, Toyonaka, Osaka 5600043, JapanOsaka Univ, Grad Sch Sci, Toyonaka, Osaka 5600043, Japan
Nakazawa, Y.
[1
]
机构:
[1] Osaka Univ, Grad Sch Sci, Toyonaka, Osaka 5600043, Japan
[2] Univ Tokyo, Inst Solid State Phys, Kashiwa, Chiba 2778581, Japan
Magnetic-field-angle-resolved heat capacity of dimer-Mott organic superconductors kappa-(BEDT-TTF)(2)X is reported (BEDT-TTF and X represent bis(ethylenedithio)tetrathiafulvalene and a monovalent anion, respectively). Temperature and field dependence of heat capacity indicates that the superconductivity has line nodes on the Fermi surface, which is a typical feature of d-wave superconductivity. In-plane field-angle dependence exhibits fourfold oscillations as well as twofold oscillations due to anisotropy of superconducting gap functions. From analyses of the fourfold term, the gap symmetry is determined as d(x2-y2) + s(+/-) for X = Cu[N(CN)(2)]Br and d(xy) for X = Ag(CN)(2)H2O. We suggest that the symmetry difference comes from the competition of d(xy) and d(x2-y2) antiferromagnetic fluctuations depending on lattice geometry.