TY - JOUR
T1 - Electronic structure calculation and superconductivity in λ-(BETS)2GaCl4
AU - Aizawa, Hirohito
AU - Koretsune, Takashi
AU - Kuroki, Kazuhiko
AU - Seo, Hitoshi
N1 - Funding Information:
Acknowledgments The authors acknowledge D. P. Sari and I. Watanabe for valuable discussions. HA is grateful to S. Yasuzuka and S. Imajo for useful discussions. This work is supported by the Japan Society for the Promotion of Science KAKENHI Grants No. 16K17754, 18K03442, and 26400377, Grants-in-Aid from the Yokohama Academic Foundation, and the RIKEN iTHES Project.
Publisher Copyright:
©2018 The Physical Society of Japan.
PY - 2018
Y1 - 2018
N2 - Quasi-two-dimensional molecular conductor λ-(BETS)2GaCl4 shows superconductivity (SC) below 5.5 K, neighboring the dimer-type Mott insulating phase. To elucidate the origin of SC and its gap function, we carry out first-principles band calculation and derive a four-band tight-binding model from the maximally localized Wannier orbitals. Considering the spin-fluctuation-mediated mechanism by adding the Hubbard U-term to the model, we analyze the SC gap function by applying the random phase approximation. We show that the SC gap changes its sign four times along the Fermi surface (FS) in the unfolded Brillouin zone, suggestive of a d-wave-like SC gap, which only has two-fold symmetry because of the low symmetry of the crystal structure. By decomposing the SC gap into the pairing functions along the crystal axes, we compare the result to similar analyses of the well-studied κ-type molecular conductors and to the experiments.
AB - Quasi-two-dimensional molecular conductor λ-(BETS)2GaCl4 shows superconductivity (SC) below 5.5 K, neighboring the dimer-type Mott insulating phase. To elucidate the origin of SC and its gap function, we carry out first-principles band calculation and derive a four-band tight-binding model from the maximally localized Wannier orbitals. Considering the spin-fluctuation-mediated mechanism by adding the Hubbard U-term to the model, we analyze the SC gap function by applying the random phase approximation. We show that the SC gap changes its sign four times along the Fermi surface (FS) in the unfolded Brillouin zone, suggestive of a d-wave-like SC gap, which only has two-fold symmetry because of the low symmetry of the crystal structure. By decomposing the SC gap into the pairing functions along the crystal axes, we compare the result to similar analyses of the well-studied κ-type molecular conductors and to the experiments.
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U2 - 10.7566/JPSJ.87.093701
DO - 10.7566/JPSJ.87.093701
M3 - Article
AN - SCOPUS:85052394663
SN - 0031-9015
VL - 87
SP - 937011
EP - 937015
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 9
ER -