Książek Maria, Weselski Marek, Kaźmierczak Marcin, Tołoczko Aleksandra, Siczek Miłosz, Durlak Piotr, Wolny Juliusz A, Schünemann Volker, Kusz Joachim, Bronisz Robert
Institute of Physics, University of Silesia, 75 Pułku Piechoty 1, 41-500, Chorzów, Poland.
Faculty of Chemistry, University of Wrocław, F. Joliot-Curie 14, 50-383, Wrocław, Poland.
Chemistry. 2020 Nov 11;26(63):14419-14434. doi: 10.1002/chem.202002460. Epub 2020 Oct 1.
Reaction of 1,2-di(tetrazol-2-yl)ethane (ebtz) with Fe(BF ) ⋅6 H O in different nitriles yields one-dimensional coordination polymers Fe(ebtz) (RCN) ⋅nRCN (n=2 for R=CH (1) and n=0 for R=C H (2) C H (3), C H (4), CH Cl (5)) exhibiting spin crossover (SCO). SCO in 1 and 3-5 is complete and occurs above 160 K. In 2, it is shifted to lower temperatures and is accompanied by wide hysteresis (T =78 K, T =123 K) and proceeds extremely slowly. Isothermal (80 K) time-resolved single-crystal X-ray diffraction studies revealed a complex nature for the HS→LS transition in 2. An initial, slow stage is associated with shrinkage of polymeric chains and with reduction of volume at 77 % (in relation to the difference between cell volumes V -V ) whereas only 16 % of iron(II) ions change spin state. In the second stage, an abrupt SCO occurs, associated with breathing of the crystal lattice along the direction of the Fe-nitrile bonds, while the nitriles reorient. HS→LS switching triggered by light (808 nm) reveals the coupling of spin state and nitrile orientation. The importance of this coupling was confirmed by studies of Fe(ebtz) (C H CN/C H CN) mixed crystals (2 a, 2 b), showing a shift of T to higher values and narrowing of the hysteresis loop concomitant with an increase of the fraction of butyronitrile. This increase reduces the capability of nitrile molecules to reorient. Density functional theory (DFT) studies of models of 1-5 suggest a particular possibility of 2 to adopt a low (140-145°) value of its Fe-N-C(propionitrile) angle.
1,2-二(四唑-2-基)乙烷(ebtz)与Fe(BF₄)₂·6H₂O在不同腈类溶剂中反应,生成一维配位聚合物Fe(ebtz)₂(RCN)₂₂·nRCN(R = CH₃时n = 2,R = C₂H₅(2)、C₃H₇(3)、C₄H₉(4)、CH₂Cl(5)时n = 0),这些聚合物表现出自旋交叉(SCO)现象。1以及3 - 5中的SCO是完全的,且发生在160 K以上。在2中,SCO温度移向更低温度,伴有宽滞后现象(T₁ = 78 K,T₂ = 123 K),且进行得极其缓慢。等温(80 K)时间分辨单晶X射线衍射研究揭示了2中从高自旋(HS)到低自旋(LS)转变的复杂本质。初始的缓慢阶段与聚合物链的收缩以及体积减少77%(相对于晶胞体积V₁ - V₂的差值)相关,而只有16%的亚铁离子改变自旋态。在第二阶段,伴随着晶格沿Fe - 腈键方向的呼吸以及腈类分子的重新取向,发生了突然的SCO。光(808 nm)触发的HS→LS转变揭示了自旋态与腈类取向的耦合。对Fe(ebtz)₂(C₂H₅CN/C₃H₇CN)₂₂混合晶体(2a、2b)的研究证实了这种耦合的重要性,研究表明随着丁腈比例的增加,T₁移向更高值且滞后回线变窄。这种增加降低了腈类分子重新取向的能力。对1 - 5模型的密度泛函理论(DFT)研究表明,2特别有可能采用低的(140 - 145°)Fe - N - C(丙腈)角值。