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首页> 外文期刊>Journal of the American Chemical Society >Controlled Intramolecular Electron Transfers in Cyanide-Bridged Molecular Squares by Chemical Modifications and External Stimuli
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Controlled Intramolecular Electron Transfers in Cyanide-Bridged Molecular Squares by Chemical Modifications and External Stimuli

机译:通过化学修饰和外部刺激控制氰化物桥连的分子正方形中的分子内电子转移

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摘要

A series of cyanide bridged Fe-Co molecular squares, [Co_2Fe_2(C-N)_6(tp*)_2(dtbbpy)_4](PF_6)_2·2M_eOH (l), [Co_2Fe_2(CN)_6(tp*)_2(bpy)_4](PF_6)_2 •2M_eOH (2), and [Co_2Fe_2(CN)_6(tp)_2(dtbbpy)_4](PF_6)_2-4H_2O (3) (tp = hydrotris(pyrazol-l-yl)borate, tp* = hydrotris(3,5-dimethylpyrazol-l-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 T1/2 = 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 ([FeⅢ_(LS2)CoⅡ_(HS2)]) at 330 K, while a low-temperature (LT) phase ([FeⅡ_(LS2)CoⅢ_(LS2)]) with LS Fe(ll) and Co(IIl) 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 [FeⅢ_(LS2)CoⅡ_(Hs2)] and [FeII_(LS2)CoⅢ_(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 terf-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 T1/2 varied from 227 to 280 K upon the addition of trifluoroacetic acid.
机译:一系列由氰化物桥接的Fe-Co分子正方形[Co_2Fe_2(CN)_6(tp *)_ 2(dtbbpy)_4](PF_6)_2·2M_eOH(l),[Co_2Fe_2(CN)_6(tp *)_ 2(bpy) )_4](PF_6)_2•2M_eOH(2)和[Co_2Fe_2(CN)_6(tp)_2(dtbbpy)_4](PF_6)_2-4H_2O(3)(tp =氢化三(吡唑-1-基)硼酸盐制备tp * =氢三(3,5-二甲基吡唑-1-基)硼酸酯,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+)和二齿配体(bpy或dtbbpy)在MeOH中的反应进行反应。在分子方块中,Fe和Co离子被氰化物离子交替桥接,形成大环四核核。可变温度X射线结构分析和磁化率测量结果证实,在固态下1表现出以T1 / 2 = 275和310 K为中心的两步电荷转移诱导的自旋跃迁(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,在此处以高温(HT)相描述([FeⅢ_(LS2)CoⅡ_ (HS2)])在330 K时,而具有LS Fe(II)和Co(IIl)离子的低温(LT)相([FeⅡ_(LS2)CoⅢ_(LS2)])在260 K以下占主导。X-射线结构分析表明,在298 K 1的中间(IM)相中,[FeⅢ_(LS2)CoⅡ_(Hs2)]和[FeII_(LS2)CoⅢ_(LS2)]的位置顺序为2:2。在1的光磁实验中,通过在5 K激发Fe(II)→Co(III)间隔电荷转移(IVCT)带,观察到了从LT到HT相的光诱导CTIST,并且捕获的HT相热弛豫到LT阶段分为两步。另一方面,在整个测量温度范围内,2和3分别处于HT和LT相,并且未观察到CTIST。溶液中的UV-vis-NIR吸收光谱测量和循环伏安法表明,通过将甲基和叔丁基引入配体tp中,1-3中的不同电子态可归因于铁和钴离子d轨道的失稳和bpy分别。 UV-vis-NIR光谱的温度依赖性证实1在丁腈中表现出一步式CTIST,在添加三氟乙酸后,T1 / 2在227至280 K之间变化。

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  • 来源
    《Journal of the American Chemical Society》 |2011年第10期|p.3592-3600|共9页
  • 作者单位

    Graduate School of Pure and Applied Sciences, University of Tsukuba, Tennodai 1-1-1, Tsukuba, Ibaraki 305-8571, Japan;

    Graduate School of Pure and Applied Sciences, University of Tsukuba, Tennodai 1-1-1, Tsukuba, Ibaraki 305-8571, Japan;

    Graduate School of Pure and Applied Sciences, University of Tsukuba, Tennodai 1-1-1, Tsukuba, Ibaraki 305-8571, Japan;

    Graduate School of Pure and Applied Sciences, University of Tsukuba, Tennodai 1-1-1, Tsukuba, Ibaraki 305-8571, Japan;

    Photon Factory and Condensed Matter Research Center, Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan;

    Photon Factory and Condensed Matter Research Center, Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan;

    Photon Factory and Condensed Matter Research Center, Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan;

    Graduate School of Pure and Applied Sciences, University of Tsukuba, Tennodai 1-1-1, Tsukuba, Ibaraki 305-8571, Japan;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);美国《化学文摘》(CA);
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