Ahmed Ahmed, Hall Amy, Vasili Hari Babu, Kulmaczewski Rafal, Kulak Alexander N, Cespedes Oscar, Pask Christopher M, Brammer Lee, Roseveare Thomas M, Halcrow Malcolm A
School of Chemistry, University of Leeds, Woodhouse Lane, Leeds, UK, LS2 9JT.
School of Natural Sciences, College of Science and Engineering, University of Galway, H91 TK 33, Galway, Ireland.
Angew Chem Int Ed Engl. 2025 Jan 27;64(5):e202416924. doi: 10.1002/anie.202416924. Epub 2024 Dec 17.
Polycrystalline [FeL][BF] (L=2,6-di(pyrazol-1-yl)isonicotinonitrile) exhibits an abrupt hysteretic spin transition near 240 K, with a shoulder on the warming branch whose appearance depends on the sample history. The freshly isolated material is a ca 60 : 40 mixture of triclinic (HS1) and tetragonal (HS2) high-spin polymorphs, which are structurally closely related. Both HS1 and HS2 undergo a high→low-spin transition on cooling at 230±10 K. HS1 transforms to a new triclinic low-spin phase with a doubled unit cell volume (LS3), while HS2 forms a monoclinic low-spin phase (LS4) with similar unit cell dimensions to HS2. Single crystals of LS3 and LS4 both convert to HS1 on rewarming. The low→high-spin transition for LS4 is ca 10 K higher in temperature than for LS3, explaining the asymmetric thermal hysteresis. Powder diffraction, calorimetry and magnetic data show that multiple cycling about the spin-transition leads to slow enrichment of the HS1 and LS3 phases at the expense of HS2 and LS4. That is consistent with the HS2/LS4 fraction of the polycrystalline sample undergoing rare, bifurcated HS2→(LS3+LS4) and LS4→(HS1+HS2) phase transitions. The rate of enrichment of HS1/LS3 differed between these experiments, implying it is sample and/or measurement-dependent. Three other salts of this iron(II) complex and the coordination polymer [Ag(μ-L)]BF are also briefly described.
多晶型物[FeL][BF](L = 2,6 - 二(吡唑 - 1 - 基)异烟腈)在240 K附近表现出突然的滞后自旋转变,升温分支上有一个肩部,其出现取决于样品历史。新分离的材料是三斜(HS1)和四方(HS2)高自旋多晶型物的约60:40混合物,它们在结构上密切相关。HS1和HS2在230±10 K冷却时都经历高→低自旋转变。HS1转变为一种新的三斜低自旋相,其晶胞体积加倍(LS3),而HS2形成一种单斜低自旋相(LS4),其晶胞尺寸与HS2相似。LS3和LS4的单晶在重新升温时都转变为HS1。LS4的低→高自旋转变温度比LS3高约10 K,这解释了不对称的热滞现象。粉末衍射、量热法和磁性数据表明,围绕自旋转变的多次循环导致HS1和LS3相缓慢富集,而HS2和LS4相减少。这与多晶样品的HS2/LS4部分经历罕见的、分叉的HS2→(LS3 + LS4)和LS4→(HS1 + HS2)相变一致。这些实验中HS1/LS3的富集速率不同,这意味着它取决于样品和/或测量。还简要描述了这种铁(II)配合物的另外三种盐以及配位聚合物[Ag(μ - L)]BF。