Suturina Elizaveta A, Nehrkorn Joscha, Zadrozny Joseph M, Liu Junjie, Atanasov Mihail, Weyhermüller Thomas, Maganas Dimitrios, Hill Stephen, Schnegg Alexander, Bill Eckhard, Long Jeffrey R, Neese Frank
Max Planck Institute for Chemical Energy Conversion , Stiftstraße 34-36, Mülheim an der Ruhr 45470, Germany.
Novosibirsk State University , Pirogova 2, 630090 Novosibirsk, Russia.
Inorg Chem. 2017 Mar 6;56(5):3102-3118. doi: 10.1021/acs.inorgchem.7b00097. Epub 2017 Feb 22.
The magnetic properties of pseudotetrahedral Co(II) complexes spawned intense interest after (PPh)[Co(SPh)] was shown to be the first mononuclear transition-metal complex displaying slow relaxation of the magnetization in the absence of a direct current magnetic field. However, there are differing reports on its fundamental magnetic spin Hamiltonian (SH) parameters, which arise from inherent experimental challenges in detecting large zero-field splittings. There are also remarkable changes in the SH parameters of [Co(SPh)] upon structural variations, depending on the counterion and crystallization conditions. In this work, four complementary experimental techniques are utilized to unambiguously determine the SH parameters for two different salts of [Co(SPh)]: (PPh)[Co(SPh)] (1) and (NEt)[Co(SPh)] (2). The characterization methods employed include multifield SQUID magnetometry, high-field/high-frequency electron paramagnetic resonance (HF-EPR), variable-field variable-temperature magnetic circular dichroism (VTVH-MCD), and frequency domain Fourier transform THz-EPR (FD-FT THz-EPR). Notably, the paramagnetic Co(II) complex [Co(SPh)] shows strong axial magnetic anisotropy in 1, with D = -55(1) cm and E/D = 0.00(3), but rhombic anisotropy is seen for 2, with D = +11(1) cm and E/D = 0.18(3). Multireference ab initio CASSCF/NEVPT2 calculations enable interpretation of the remarkable variation of D and its dependence on the electronic structure and geometry.
在(PPh)[Co(SPh)]被证明是首个在无直流磁场情况下显示出磁化强度缓慢弛豫的单核过渡金属配合物之后,假四面体Co(II)配合物的磁性引发了强烈关注。然而,关于其基本磁自旋哈密顿量(SH)参数存在不同的报道,这源于检测大零场分裂时固有的实验挑战。[Co(SPh)]的SH参数也会随着结构变化而发生显著变化,这取决于抗衡离子和结晶条件。在这项工作中,利用四种互补的实验技术明确确定了[Co(SPh)]两种不同盐的SH参数:(PPh)[Co(SPh)](1)和(NEt)[Co(SPh)](2)。所采用的表征方法包括多场超导量子干涉仪磁强计、高场/高频电子顺磁共振(HF-EPR)、变场变温磁圆二色性(VTVH-MCD)和频域傅里叶变换太赫兹EPR(FD-FT THz-EPR)。值得注意的是,顺磁性Co(II)配合物[Co(SPh)]在1中表现出很强的轴向磁各向异性,D = -55(1) cm且E/D = 0.00(3),但在2中则表现出菱形各向异性,D = +11(1) cm且E/D = 0.18(3)。多参考从头算CASSCF/NEVPT2计算能够解释D的显著变化及其对电子结构和几何形状的依赖性。