Fujiwara Emiko, Kobayashi Akiko, Fujiwara Hideki, Kobayashi Hayao
Research Centre for Spectrochemistry, Graduate School of Science, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan.
Inorg Chem. 2004 Feb 9;43(3):1122-9. doi: 10.1021/ic034670s.
To contribute to the development of single-component molecular metals, several nickel complexes with cyclohexeno-condensed or ethylenedioxy-substituted TTF (tetrathiafulvalene) dithiolate ligands, (R(4)N)(n)[Ni(chdt)(2)] [R = Me, n = 2 (1); R = (n)Bu, n = 1 (2); n = 0 (3)] and (R(4)N)(n)[Ni(eodt)(2)] [R = Me, n = 2 (4); R = (n)Bu, n = 1 (5); n = 0 (6)], were prepared. X-ray structures were determined on the monoanionic species 2 and 5. The tetra-n-butylammonium complex of the monoanionic [Ni(chdt)(2)] (2) with a 1:1 composition revealed that its magnetic susceptibility gave a good agreement with the Bonner-Fisher model (J/k(B) = -28 K), which was derived from the one-dimensional chains of anions with a regular interval. On the other hand, the magnetic susceptibility of the tetra-n-butylammonium complex of the monoanionic [Ni(eodt)(2)] (5) showed the Curie-Weiss behavior (C = 0.376 K.emu.mol(-1) and Theta = -4.6 K). Both of the monoanionic species 2 and 5 indicate that they belong to the S = 1/2 magnetic system and have relatively large and anisotropic g-values, suggesting the contribution of the nickel 3d orbital. Electrical resistivity measurements were performed on the compressed pellets of the neutral species 3 and 6. Fairly large conductivities were obtained (sigma(rt) = 1-10 S.cm(-1)). In addition, despite the measurements on the compressed pellets of powder samples, the neutral species 6 showed metallic behavior down to ca. 120 K and retained high conductivity even at 0.6 K [sigma(0.6 K)/sigma(rt) approximately 1/30], suggesting the crystal to be essentially metallic down to very low temperature. The electrical behavior and Pauli paramagnetism of 6 indicate the system to be a new single-component metal.
为推动单组分分子金属的发展,制备了几种含有环己烯稠合或乙二氧基取代的四硫富瓦烯(TTF)二硫醇盐配体的镍配合物,即(R(4)N)(n)[Ni(chdt)(2)] [R = 甲基,n = 2 (1);R = 正丁基,n = 1 (2);n = 0 (3)] 和 (R(4)N)(n)[Ni(eodt)(2)] [R = 甲基,n = 2 (4);R = 正丁基,n = 1 (5);n = 0 (6)]。测定了单阴离子物种2和5的X射线结构。单阴离子[Ni(chdt)(2)]的四正丁基铵配合物(2),其组成比为1:1,结果表明其磁化率与邦纳 - 费舍尔模型(J/k(B) = -28 K)吻合良好,该模型源自具有规则间隔的一维阴离子链。另一方面,单阴离子[Ni(eodt)(2)]的四正丁基铵配合物(5)的磁化率表现出居里 - 外斯行为(C = 0.376 K·emu·mol⁻¹,θ = -4.6 K)。单阴离子物种2和5均表明它们属于S = 1/2磁体系,并且具有相对较大且各向异性的g值,这表明镍3d轨道有贡献。对中性物种3和6的压缩颗粒进行了电阻率测量。获得了相当大的电导率(σ(rt) = 1 - 10 S·cm⁻¹)。此外,尽管是对粉末样品的压缩颗粒进行测量,但中性物种6在约120 K以下表现出金属行为,甚至在0.6 K时仍保持高电导率[σ(0.6 K)/σ(rt)约为1/30],这表明该晶体在非常低的温度下本质上是金属性的。6的电学行为和泡利顺磁性表明该体系是一种新型的单组分金属。