Crystals (Nov 2012)

Magnetism and Pressure-Induced Superconductivity of Checkerboard-Type Charge-Ordered Molecular Conductor β-(meso-DMBEDT-TTF)2X (X = PF6 and AsF6)

  • Yutaka Nishio,
  • Yoshiya Uwatoko,
  • Kazuyuki Matsubayashi,
  • Hiroyuki Tajima,
  • Motoi Kimata,
  • Youichi Murakami,
  • Kensuke Kobayashi,
  • Hironori Nakao,
  • Reiji Kumai,
  • Akiko Nakao,
  • Kazuyuki Takahashi,
  • Akira Ueda,
  • Takayuki Isono,
  • Sanguchul Lee,
  • Tatsuya Shimokawa,
  • Takahisa Shikama,
  • Koji Kajita,
  • Hatsumi Mori

DOI
https://doi.org/10.3390/cryst2041502
Journal volume & issue
Vol. 2, no. 4
pp. 1502 – 1513

Abstract

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The metallic state of the molecular conductor β-(meso-DMBEDT-TTF)2X (DMBEDT-TTF = 2-(5,6-dihydro-1,3-dithiolo[4,5-b][1,4]dithiin-2-ylidene)-5,6-dihydro-5,6-dimethyl-1,3-dithiolo[4,5-b][1,4]dithiin, X = PF6, AsF6) is transformed into the checkerboard-type charge-ordered state at around 75–80 K with accompanying metal-insulator (MI) transition on the anisotropic triangular lattice. With lowering temperatures, the magnetic susceptibility decreases gradually and reveals a sudden drop at the MI transition. By applying pressure, the charge-ordered state is suppressed and superconductivity appears in β-(meso-DMBEDT-TTF)2AsF6 as well as in the reported β-(meso-DMBEDT-TTF)2PF6. The charge-ordered spin-gapped state and the pressure-induced superconducting state are discussed through the paired-electron crystal (PEC) model, where the spin-bonded electron pairs stay and become mobile in the crystal, namely the valence-bond solid (VBS) and the resonant valence bonded (RVB) state in the quarter-filled band structure.

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