Swain Abinash, Sen Asmita, Rajaraman Gopalan
Department of Chemistry, Indian Institute of Technology Bombay, Powai, Mumbai - 400076, India.
Dalton Trans. 2021 Nov 16;50(44):16099-16109. doi: 10.1039/d1dt02256c.
Lanthanide based single-molecule magnets are gaining wide attention due to their potential applications in emerging technologies. One of the main challenges in this area is quenching quantum tunnelling of magnetisation (QTM), which often undercuts the magnetisation reversal barrier. Among the several strategies employed, enhancing exchange coupling has been studied in detail, with large exchanges resulting in stronger quenching of QTM effects. Lanthanides, however, suffer from weak exchanges offered by the deeply buried 4f orbitals and the numerous attempts to enhance the exchange coupling in the {3d-4f} pairs have not exceeded values larger than 30 cm. In this work, using a combination of DFT and the CASSCF/RASSI-SO method, we have explored lanthanide-transition metal direct bonds as a tool to quench QTM effects. In this direction, we have modelled [PyCpLnMCp(CO)] (Ln = Gd(III), Dy(III), and Er(III) and M = V(0), Mn(0), Co(0) and Fe(I) and here PyCp = [2,6-(CHCH)CHN] using [PyCpDyFeCp(CO)] as an example as reported by Nippe (C. P. Burns, X. Yang, J. D. Wofford, N. S. Bhuvanesh, M. B. Hall and M. Nippe, , 2018, , 8144). Bonding analysis reveals a dative Ln-TM bond with a donation of π(V/Mnd-π*CO) to 5d (Gd) in the case of Gd-V and Gd-Mn and 4s(Co) to 5d/5d (Gd) for Gd-Co with the transition metal ion being found in the low-spin = ½ configurations in all the cases. B3LYP/TZV (Gd;CSDZ) calculations on [PyCpGdMCp(CO)] yield = -46.1 cm, = -57.1 cm, = +55.3 cm, = +13.9 cm, = -162.1 cm and = -343.9 cm and unveiling record-high values for {3d-4f} complexes. The mechanism of magnetic coupling is developed, which discloses the dominating presence of strong 3d-4f orbital overlaps in most of the cases studied, leading to antiferromagnetic exchange. When these overlaps are weaker and 3d to Gd(5d), charge transfer dominates, yielding a ferromagnetic coupling for the Gd-Co/Gd-Fe complexes. Calculations performed on the anisotropic Dy(III) and Er(III) complexes reveal that the ground state axis lies along the Cp-Ln-Cp axis and the Ln-TM bonds, respectively. Thus the Ln-TM bond hinders the single-ion anisotropy of Dy(III) by offering equatorial ligation and lowering the = ±½ state energy, and at the same time, helping in enhancing the axiality of Er(III). When strong {3d-4f} exchange couplings are introduced, record-high barrier heights as high as 229 cm were accomplished. Furthermore, the exchange coupling annihilates the QTM effects and suggests the lanthanide-transition metal direct bond as a viable alternative to enhance exchange coupling to bring {3d-4f} complexes back in the race for high-blocking SMMs.
基于镧系元素的单分子磁体因其在新兴技术中的潜在应用而受到广泛关注。该领域的主要挑战之一是抑制磁化量子隧穿(QTM),这常常削弱磁化反转势垒。在采用的几种策略中,增强交换耦合已得到详细研究,较大的交换作用会导致更强的QTM效应淬灭。然而,镧系元素因深埋的4f轨道提供的交换作用较弱,且在{3d - 4f}对中增强交换耦合的众多尝试尚未超过30 cm的值。在这项工作中,我们结合密度泛函理论(DFT)和完全活性空间自洽场/限制活性空间态相互作用 - 自旋轨道(CASSCF/RASSI - SO)方法,探索了镧系 - 过渡金属直接键作为淬灭QTM效应的一种工具。在此方向上,我们以[PyCpDyFeCp(CO)]为例(如Nippe所报道,C. P. Burns、X. Yang、J. D. Wofford、N. S. Bhuvanesh、M. B. Hall和M. Nippe,2018,8144)对[PyCpLnMCp(CO)](Ln = Gd(III)、Dy(III)和Er(III),M = V(0)、Mn(0)、Co(0)和Fe(I),此处PyCp = [2,6 - (CHCH)CHN])进行了建模。键合分析表明,在Gd - V和Gd - Mn的情况下存在一个给体Ln - TM键,有π(V/Mnd - π*CO)向5d(Gd)的电子给予,而对于Gd - Co则是4s(Co)向5d/5d(Gd)的电子给予,所有情况下过渡金属离子均处于低自旋S = ½构型。对[PyCpGdMCp(CO)]进行的B3LYP/TZV(Gd;CSDZ)计算得出J = -46.1 cm⁻¹、J = -57.1 cm⁻¹、J = +55.3 cm⁻¹、J = +13.9 cm⁻¹、J = -162.1 cm⁻¹和J = -343.9 cm⁻¹,并揭示了{3d - 4f}配合物创纪录的高J值。我们推导了磁耦合机制,该机制表明在大多数研究案例中,强3d - 4f轨道重叠占主导,导致反铁磁交换。当这些重叠较弱且是从3d到Gd(5d)时,电荷转移占主导,使得Gd - Co/Gd - Fe配合物产生铁磁耦合。对各向异性的Dy(III)和Er(III)配合物进行的计算表明,基态S轴分别沿着Cp - Ln - Cp轴和Ln - TM键。因此,Ln - TM键通过提供赤道配位并降低S = ±½态能量来阻碍Dy(III)的单离子各向异性,同时有助于增强Er(III)的轴向性。当引入强{3d - 4f}交换耦合时,实现了高达229 cm⁻¹的创纪录高势垒高度。此外,交换耦合消除了QTM效应,并表明镧系 - 过渡金属直接键是增强交换耦合的可行替代方案,使{3d - 4f}配合物在高阻挡单分子磁体的竞争中重新占据优势。