Hilgar J D, Bernbeck M G, Flores B S, Rinehart J D
Department of Chemistry and Biochemistry , University of California - San Diego , La Jolla , CA 92093 , USA . Email:
Chem Sci. 2018 Jul 31;9(36):7204-7209. doi: 10.1039/c8sc01361f. eCollection 2018 Sep 28.
Synthetic control of the crystal field has elevated lanthanides to the forefront of single-molecule magnet (SMM) research, yet the resultant strong, predictable single-ion anisotropy has thus far not translated into equally impressive molecule-based magnets of higher dimensionality. This roadblock arises from the dual demands made of the crystal field: generate anisotropy and facilitate magnetic coupling. Here we demonstrate that particular metal-ligand pairs can dominate the single-ion electronic structure so fully that the remaining coordination sphere plays a minimal role in the magnitude and orientation of the magnetic anisotropy. This Metal-Ligand Pair Anisotropy (MLPA) effectively separates the crystal field into discrete components dedicated to anisotropy and magnetic coupling. To demonstrate an MLPA building unit, we synthesized four new mononuclear complexes that challenge the electronic structure of the iconic lanthanocene ([Ln(COT)]; COT = cyclooctatetraene dianion) complex which is known to generate strong anisotropy with Ln = Er. Variation in symmetry and coordination strength for Er(COT)I(THF) (THF = tetrahydrofuran) (), Er(COT)I(Py) (Py = pyridine) (), Er(COT)I(MeCN) (MeCN = acetonitrile) (), and Er(COT)(Tp*) (Tp* = tris(3,5-dimethyl-1-pyrazolyl)borate) () shows that the Er-COT unit stabilizes anisotropy despite deliberate de-optimization. All four half-sandwich complexes display SMM behavior with effective energy barriers of = 95.6(9), 102.9(3.1), 107.1(1.3), and 133.6(2.2) cm for by a multi-relaxation-process fitting. More importantly, the basic state splittings remain intact and the anisotropy axes are within several degrees of normal to the COT ring according to complete active space self-consistent field (CASSCF) calculations. Further investigation of the MLPA conceptual framework is warranted as it can provide building units with well-defined magnetic orientation and strength. We envision that the through-barrier processes observed herein, such as quantum tunneling, can be mitigated by formation of larger clusters and molecule-based materials.
对晶体场的合成控制已将镧系元素提升到单分子磁体(SMM)研究的前沿,然而,由此产生的强大、可预测的单离子各向异性迄今为止尚未转化为同样令人印象深刻的高维分子基磁体。这一障碍源于对晶体场的双重要求:产生各向异性并促进磁耦合。在这里,我们证明特定的金属-配体对可以完全主导单离子电子结构,以至于其余的配位球在磁各向异性的大小和取向上所起的作用极小。这种金属-配体对各向异性(MLPA)有效地将晶体场分离为专门用于各向异性和磁耦合的离散成分。为了展示一个MLPA构建单元,我们合成了四种新的单核配合物,它们挑战了标志性的镧茂([Ln(COT)];COT = 环辛四烯二价阴离子)配合物的电子结构,已知该配合物在Ln = Er时会产生很强的各向异性。Er(COT)I(THF)(THF = 四氢呋喃)()、Er(COT)I(Py)(Py = 吡啶)()、Er(COT)I(MeCN)(MeCN = 乙腈)()和Er(COT)(Tp*)(Tp* = 三(3,5-二甲基-1-吡唑基)硼酸根)()的对称性和配位强度的变化表明,尽管经过刻意的去优化,Er-COT单元仍能稳定各向异性。通过多弛豫过程拟合,所有四种半夹心配合物都表现出SMM行为,有效能垒分别为 = 95.6(9)、102.9(3.1)、107.1(1.3)和133.6(2.2) cm。更重要的是,根据完全活性空间自洽场(CASSCF)计算,基态分裂保持不变,各向异性轴与COT环法线的夹角在几度之内。由于MLPA概念框架可以提供具有明确磁取向和强度的构建单元,因此有必要对其进行进一步研究。我们设想,本文中观察到的诸如量子隧穿等穿越势垒过程,可以通过形成更大的簇和分子基材料来缓解。