(nBu4N)[Ni(dmstfdt)2]:: A planar nickel coordination complex with an extended-TTF ligand exhibiting metallic conduction, metal-insulator transition, and weak ferromagnetism

被引:17
作者
Fujiwara, Emiko
Yamamoto, Kimiko
Shimamura, Mina
Zhou, Biao
Kobayashi, Akiko [1 ]
Takahashi, Kazuyuki
Okano, Yoshinori
Cui, Hengbo
Kobayashi, Hayao
机构
[1] Univ Tokyo, Grad Sch Sci, Res Ctr Spectrochem, Bunkyo Ku, Tokyo 1130033, Japan
[2] Univ Tokyo, Grad Sch Sci, Bunkyo Ku, Tokyo 1130033, Japan
[3] Nihon Univ, Coll Humanities & Sci, Dept Chem, Setagaya Ku, Tokyo 1568550, Japan
[4] CREST, Inst Mol Sci, Okazaki, Aichi 4448585, Japan
[5] CREST, JST, Okazaki, Aichi 4448585, Japan
关键词
D O I
10.1021/cm062131q
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The 1:1 tetrabutylammonium salt of a nickel complex with an extended-TTF ligand, ((Bu4N)-Bu-n)[Ni(dmstfdt)(2)] (dmstfdt = dimethyldiselenadithiafulvalenedithiolate) (1) is a unique ambivalent molecular system exhibiting weakly metallic conduction above room temperature and a weak ferromagnetism at low temperature. Its X-ray structure consists of two independent [Ni(dmstfdt)(2)](-) (A and B) and two (Bu4N+)-Bu-n in the unit cell. The pseudo-planar anions are arranged in a zigzag -ABA'B'- manner along the molecular side-by-side direction with a dihedral angle of the molecular planes of 42.6 degrees. The tight-binding band structure calculation, based on transfer integrals estimated by the extended HUckel approximation, presents both three-dimensional electron and hole Fermi surfaces, which is consistent with the observed weakly metallic conduction around room-temperature despite the 1:1 stoichiometry of the complex. At 147 K, 1 shows a sharp insulating transition associated with the localization of one electron on each nickel complex below 160 K. The chi T values of 1 increase linearly from 0.129 to 0.383 emu K mol(-1) with decreasing temperature (160-340 K), suggesting a gradual electron localization with lowering the temperature. In the range of temperature of 80-150 K, chi follows the Curie-Weiss law: chi = C/(T - theta); C = 0.383 emu K mol(-1); and theta = -4 K. Weak ferromagnetism sets in below 20 K. The coercive field is +/- 1.3 kOe at 2.0 K.
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页码:553 / 558
页数:6
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