Magnetism and Pressure-Induced Superconductivity of Checkerboard-Type Charge-Ordered Molecular Conductor #946;-(meso-DMBEDT-TTF)2X (X = PF6 and AsF6)

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&am...

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Veröffentlicht in:Crystals (Basel) 2012-11, Vol.2 (4), p.1502-1513
Hauptverfasser: 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
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Sprache:eng
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Zusammenfassung: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.
ISSN:2073-4352
2073-4352
DOI:10.3390/cryst2041502