Weller Ruth, Atanasov Mihail, Demeshko Serhiy, Chen Ting-Yi, Mohelsky Ivan, Bill Eckhard, Orlita Milan, Meyer Franc, Neese Frank, Werncke C Gunnar
Department of Chemistry, Philipps-University Marburg, Hans-Meerwein-Straße 4, 35043Marburg, Germany.
Max-Planck-Institut für Kohlenforschung, Kaiser-Wilhelm-Platz 1, 45470Mülheim an der Ruhr, Germany.
Inorg Chem. 2023 Feb 20;62(7):3153-3161. doi: 10.1021/acs.inorgchem.2c04050. Epub 2023 Feb 6.
The rational design of 3d-metal-based single-molecule magnets (SMM) requires a fundamental understanding of their intrinsic electronic and structural properties and how they translate into experimentally observable features. Here, we determined the magnetic properties of the linear iron(I) silylamides K{crypt}[FeL] and [KFeL] (L = -N(Dipp)SiMe; crypt = 4,7,13,16,21,24-Hexaoxa-1,10-diazabicyclo[8.8.8]hexacosan). For the former, slow-relaxation of the magnetization with a spin reversal barrier of = 152 cm as well as a closed-waist magnetic hysteresis and magnetic blocking below 2.5 K are observed. For the more linear [KFeL], in which the potassium cation is encapsulated by the aryl substituents of the amide ligands, the relaxation barrier and the blocking temperature increase to = 184 cm and = 4.5 K, respectively. The increase is rationalized by a more pronounced axial anisotropy in [KFeL] determined by dc-SQUID magnetometry. The effective relaxation barrier of [KFeL] is in agreement with the energy spacing between the ground and first-excited magnetic states, as obtained by field-dependent IR-spectroscopy (178 cm), magnetic measurements (208 cm), as well as theoretical analysis (212 cm). In comparison with the literature, the results show that magnetic coercivity in linear iron(I) silylamides is driven by the degree of linearity in conjunction with steric encumbrance, whereas the ligand symmetry is a marginal factor.
基于3d金属的单分子磁体(SMM)的合理设计需要对其内在的电子和结构性质以及它们如何转化为实验可观测特征有基本的了解。在此,我们测定了线性铁(I)硅烷基酰胺K{crypt}[FeL]和[KFeL](L = -N(Dipp)SiMe;crypt = 4,7,13,16,21,24 - 六氧杂 - 1,10 - 二氮杂双环[8.8.8]二十六烷)的磁性。对于前者,观察到磁化强度的缓慢弛豫,其自旋反转势垒为 = 152 cm,以及在2.5 K以下的闭腰磁滞和磁阻塞现象。对于更线性的[KFeL],其中钾阳离子被酰胺配体的芳基取代基所包围,弛豫势垒和阻塞温度分别增加到 = 184 cm和 = 4.5 K。通过直流超导量子干涉仪磁强计测定,[KFeL]中更明显的轴向各向异性解释了这种增加。[KFeL]的有效弛豫势垒与基态和第一激发磁态之间的能量间距一致,这是通过场依赖红外光谱(178 cm)、磁性测量(208 cm)以及理论分析(212 cm)得到的。与文献相比,结果表明线性铁(I)硅烷基酰胺中的磁矫顽力是由线性程度与空间位阻共同驱动的,而配体对称性是一个次要因素。