β"-(F-T)3(MnCl4)(1,1,2-C2H3Cl3) (ET = bis(ethylenedithio)tetrathiafulvalene);: a pressure-sensitive new molecular conductor with localized spins

被引:31
|
作者
Naito, T [1 ]
Inabe, T
Takeda, K
Awaga, K
Akutagawa, T
Hasegawa, T
Nakamura, T
Kakiuchi, T
Sawa, H
Yamamoto, T
Tajima, H
机构
[1] Hokkaido Univ, Grad Sch Sci, Div Chem, Sapporo, Hokkaido 0600810, Japan
[2] Univ Tokyo, Dept Basic Sci, Tokyo, Japan
[3] Hokkaido Univ, Res Inst Elect Sci, Sapporo, Hokkaido 060, Japan
[4] Chiba Univ, Dept Phys, Chiba 260, Japan
[5] Univ Tokyo, Inst Solid State Phys, Tokyo, Japan
关键词
D O I
10.1039/b102786g
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
An electrolysis of bis(ethylenedithio)tetrathiafulvalene (ET) and a Mn-cluster in a 1,1,2-trichloroethane solution containing 10% (vol/vol) of ethanol yields black lustrous single crystals, beta"-(ET)(3)(MnCl4)(1,1,2-C2H3Cl3) based on the X-ray structural study. The crystal structure can be characterized as alternating two-dimensional donor sheets and insulating sheets made of isolated [MnCl4](2-) ions and the 1,1,2-C2H3Cl3 molecules. Every pair of the neighbouring donor molecules has a large displacement along both short and long molecular axes. A tight-binding band calculation suggests that this arrangement should lead to a weak but isotropic intermolecular interaction in the donor sheets, and this in turn should lead to a marginally metallic or semiconducting electronic structure. Although the polarized reflectance spectra and the temperature-dependent spin susceptibility derived from the EPR spectra on the single crystal indicate metallic nature, the electrical behaviour under atmospheric pressure is semiconductive with room temperature conductivity of 35 S cm(-1) and apparent activation energy of 0.023 eV. It exhibits a resistive hump with hysteresis at around 60 K, which could be associated with a structural transition demonstrated by a series of low temperature X-ray oscillation photographs. The magnetic susceptibility at 4.5-300 K does not exhibit any anomaly and is well reproduced by the Curie-Weiss model with Curie constant C/emu K mol(-1) = 3.89 and Weiss temperature theta /K = -0.10. This magnetic behaviour can be quantitatively understood as the sum of Pauli paramagnetism of the pi -electrons and the contribution from the local spins on the Mn(II) ions with d(5)-configuration S = 5/2). High pressure easily suppresses the increase in resistivity at low temperature, and the electrical behaviour is particularly sensitive to the first 3-5 kbar.
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收藏
页码:2221 / 2227
页数:7
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