Bridonneau Nathalie, Rigamonti Luca, Poneti Giordano, Pinkowicz Dawid, Forni Alessandra, Cornia Andrea
Dipartimento di Scienze Chimiche e Geologiche, Università degli Studi di Modena e Reggio Emilia and INSTM RU of Modena and Reggio Emilia, via G. Campi 103, 41125 Modena, Italy.
Laboratory of Molecular Magnetism (LAMM), Dipartimento di Chimica 'Ugo Schiff', Università degli Studi di Firenze and INSTM RU of Firenze, via della Lastruccia 3-13, 50019 Sesto Fiorentino (FI), Italy.
Dalton Trans. 2017 Mar 21;46(12):4075-4085. doi: 10.1039/c7dt00248c.
The molecular structures and magnetic properties of homoleptic iron(ii) compounds Fe(bpp-COOMe) (1) and Fe(bpp-triolH) (2) have been investigated to ascertain their spin crossover (SCO) behaviour. In these hexacoordinated complexes, the bpp (2,6-bis(pyrazol-1-yl)pyridine) ligands adopt a mer-mer coordination mode and carry COOMe or C(O)NHC(CHOH)para substituents, respectively, on the central pyridyl ring. In spite of the almost equal donor power of the ligands to the iron(ii) centre, the two compounds feature different spin state configurations at room temperature. Compound 1 displays a highly-distorted octahedral environment around the iron(ii) centre, which adopts a high spin (HS) state at all temperatures, even under an external applied pressure up to 1.0 GPa. By contrast, 2 is characterized by a more regular octahedral coordination around the metal ion and exhibits a low spin (LS) configuration at or below room temperature. However, it shows a thermally-induced SCO behaviour at T > 400 K, along with Light-Induced Excited Spin State Trapping (LIESST) at low temperature, with T = 38 K. Since DFT (U)M06/6-311+G(d) geometry optimizations in vacuo indicate that both complexes should adopt a HS state and a highly-distorted coordination geometry, the stabilization of a LS configuration in 2 is ultimately ascribed to the effect of intermolecular hydrogen bonds, which align the [Fe(bpp-triolH)] cations in 1D chains and impart profound differences in the geometric arrangement of the ligands.
已对同配铁(II)化合物Fe(bpp - COOMe)(1)和Fe(bpp - triolH)(2)的分子结构和磁性进行了研究,以确定它们的自旋交叉(SCO)行为。在这些六配位配合物中,bpp(2,6 - 双(吡唑 - 1 - 基)吡啶)配体采用面 - 面配位模式,并且在中心吡啶环上分别带有COOMe或C(O)NHC(CHOH)对位取代基。尽管配体对铁(II)中心的给电子能力几乎相等,但这两种化合物在室温下具有不同的自旋态构型。化合物1在铁(II)中心周围呈现高度扭曲的八面体环境,在所有温度下均采用高自旋(HS)态,即使在高达1.0 GPa的外部施加压力下也是如此。相比之下,化合物2的特征是金属离子周围的八面体配位更规则,并且在室温及以下呈现低自旋(LS)构型。然而,它在T > 400 K时表现出热诱导的SCO行为,以及在低温(T = 38 K)下的光诱导激发自旋态捕获(LIESST)。由于真空中的DFT(U)M06/6 - 311 + G(d)几何优化表明这两种配合物都应采用HS态和高度扭曲的配位几何结构,因此化合物2中LS构型的稳定最终归因于分子间氢键的作用。分子间氢键使[Fe(bpp - triolH)]阳离子排列成一维链,并在配体的几何排列上产生了显著差异。