Graduate School of Pure and Applied Sciences, University of Tsukuba, Tennodai 1-1-1, Tsukuba, Ibaraki 305-8571, Japan.
J Am Chem Soc. 2011 Mar 16;133(10):3592-600. doi: 10.1021/ja109721w. Epub 2011 Feb 22.
A series of cyanide bridged Fe-Co molecular squares, Co(2)Fe(2)(CN)(6)(tp*)(2)(dtbbpy)(4)(2)·2MeOH (1), Co(2)Fe(2)(CN)(6)(tp*)(2)(bpy)(4)(2)·2MeOH (2), and Co(2)Fe(2)(CN)(6)(tp)(2)(dtbbpy)(4)(2)·4H(2)O (3) (tp = hydrotris(pyrazol-1-yl)borate, tp* = hydrotris(3,5-dimethylpyrazol-1-yl)borate, bpy =2,2'-bipyridine, dtbbpy =4,4'-di-tert-butyl-2,2'-bipyridine), were prepared by the reactions of Fe(CN)(3)(L) (L = tp or tp*) with Co(2+) and bidentate ligands (bpy or dtbbpy) in MeOH. In the molecular squares, Fe and Co ions are alternately bridged by cyanide ions, forming macrocyclic tetranuclear cores. Variable temperature X-ray structural analyses and magnetic susceptibility measurements confirmed that 1 exhibits two-step charge-transfer induced spin transitions (CTIST) centered at T(1/2) = 275 and 310 K in the solid state. The Fe and Co ions in 1 are the low-spin (LS) Fe(III) and high-spin (HS) Co(II) ions, described here in the high-temperature (HT) phase ([Fe(III)(LS2)Co(II)(HS2)]) at 330 K, while a low-temperature (LT) phase ([Fe(II)(LS2)Co(III)(LS2)]) with LS Fe(II) and Co(III) ions was dominant below 260 K. X-ray structural analysis revealed that in the intermediate (IM) phase at 298 K 1 exhibits positional ordering of [Fe(III)(LS2)Co(II)(HS2)] and [Fe(II)(LS2)Co(III)(LS2)] species with the 2:2 ratio. In photomagnetic experiments on 1, light-induced CTIST from the LT to the HT phase was observed by excitation of Fe(II) → Co(III) intervalence charge transfer (IVCT) band at 5 K and the trapped HT phase thermally relaxed to the LT phase in a two-step fashion. On the other hand, 2 and 3 are in the HT and LT phases, respectively, throughout the entire temperature range measured, and no CTIST was observed. UV-vis-NIR absorption spectral measurements and cyclic voltammetry in solution revealed that the different electronic states in 1-3 are ascribable to the destabilization of iron and cobalt ion d-orbitals by the introduction of methyl and tert-butyl groups to the ligands tp and bpy, respectively. Temperature dependence of UV-vis-NIR spectra confirmed that 1 exhibited a one-step CTIST in butyronitrile, of which T(1/2) varied from 227 to 280 K upon the addition of trifluoroacetic acid.
一系列氰桥联的 Fe-Co 分子正方形,Co(2)Fe(2)(CN)(6)(tp*)(2)(dtbbpy)(4)(2)·2MeOH(1),Co(2)Fe(2)(CN)(6)(tp*)(2)(bpy)(4)(2)·2MeOH(2)和Co(2)Fe(2)(CN)(6)(tp)(2)(dtbbpy)(4)(2)·4H(2)O(3)(tp = 三(吡唑基)硼氢化盐,tp* = 三(3,5-二甲基吡唑基)硼氢化盐,bpy = 2,2'-联吡啶,dtbbpy = 4,4'-二叔丁基-2,2'-联吡啶),通过[Fe(CN)(3)(L)]- (L = tp 或 tp*)与 Co(2+)和双齿配体(bpy 或 dtbbpy)在 MeOH 中的反应制备。在分子正方形中,Fe 和 Co 离子被氰化物离子交替桥接,形成大环四核核。变温 X 射线结构分析和磁化率测量证实,1 在固态中在 T(1/2)=275 和 310 K 处表现出两步电荷转移诱导自旋转变(CTIST)。1 中的 Fe 和 Co 离子是低自旋(LS)Fe(III)和高自旋(HS)Co(II)离子,在 330 K 时在高温(HT)相中描述为[Fe(III)(LS2)Co(II)(HS2)],而在 260 K 以下主要是低温(LT)相[Fe(II)(LS2)Co(III)(LS2)]中的 LS Fe(II)和 Co(III)离子。X 射线结构分析表明,在 298 K 的中间(IM)相中,1 表现出[Fe(III)(LS2)Co(II)(HS2)]和[Fe(II)(LS2)Co(III)(LS2)]物种的位置有序,比例为 2:2。在 1 的光磁实验中,通过在 5 K 时激发 Fe(II)→Co(III)间隔电荷转移(IVCT)带观察到从 LT 到 HT 相的光诱导 CTIST,并且捕获的 HT 相以两步方式热松弛到 LT 相。另一方面,2 和 3 在整个测量温度范围内分别处于 HT 和 LT 相,并且没有观察到 CTIST。溶液中的紫外可见近红外吸收光谱测量和循环伏安法表明,1-3 中不同的电子态归因于配体 tp 和 bpy 中引入甲基和叔丁基分别使铁和钴离子 d 轨道失稳。紫外可见近红外光谱的温度依赖性证实,1 在丁腈中表现出一步 CTIST,其 T(1/2)在加入三氟乙酸时从 227 到 280 K 变化。