Lawrence J, Yang E-C, Hendrickson D N, Hill S
Department of Physics, University of Arizona, Tucson, Arizona 85721, USA.
Phys Chem Chem Phys. 2009 Aug 21;11(31):6743-9. doi: 10.1039/b908460f. Epub 2009 Jun 29.
Multi-dimensional high-field/frequency electron paramagnetic resonance (HFEPR) spectroscopy is performed on single-crystals of the high-symmetry spin S = 4 tetranuclear single-molecule magnet (SMM) Ni(hmp)(dmb)Cl, where hmp(-) is the anion of 2-hydroxymethylpyridine and dmb is 3,3-dimethyl-1-butanol. Measurements performed as a function of the applied magnetic field strength and its orientation within the hard-plane reveal the four-fold behavior associated with the fourth order transverse zero-field splitting (ZFS) interaction, (1/2)B(S + S), within the framework of a rigid spin approximation (with S = 4). This ZFS interaction mixes the m(s) = +/-4 ground states in second order of perturbation, generating a sizeable (12 MHz) tunnel splitting, which explains the fast magnetic quantum tunneling in this SMM. Meanwhile, multi-frequency measurements performed with the field parallel to the easy-axis reveal HFEPR transitions associated with excited spin multiplets (S < 4). Analysis of the temperature dependence of the intensities of these transitions enables determination of the isotropic Heisenberg exchange constant, J = -6.0 cm(-1), which couples the four spin s = 1 Ni(II) ions within the cluster, as well as a characterization of the ZFS within excited states. The combined experimental studies support recent work indicating that the fourth order anisotropy associated with the S = 4 state originates from second order ZFS interactions associated with the individual Ni(II) centers, but only as a result of higher-order processes that occur via S-mixing between the ground state and higher-lying (S < 4) spin multiplets. We argue that this S-mixing plays an important role in the low-temperature quantum dynamics associated with many other well known SMMs.
对高对称性自旋(S = 4)的四核单分子磁体(SMM)([Ni(hmp)(dmb)Cl]_4)的单晶进行了多维高场/高频电子顺磁共振(HFEPR)光谱研究,其中(hmp^-)是2 - 羟甲基吡啶的阴离子,(dmb)是3,3 - 二甲基 - 1 - 丁醇。在硬平面内作为外加磁场强度及其取向的函数进行的测量揭示了与四阶横向零场分裂(ZFS)相互作用((1/2)B(S + S))相关的四重行为,该相互作用在刚性自旋近似((S = 4))的框架内。这种ZFS相互作用在二阶微扰中混合了(m_s = \pm4)的基态,产生了相当大的(12 MHz)隧道分裂,这解释了该SMM中的快速磁量子隧穿。同时,在磁场平行于易轴的情况下进行的多频测量揭示了与激发自旋多重态((S < 4))相关的HFEPR跃迁。对这些跃迁强度的温度依赖性分析能够确定各向同性海森堡交换常数(J = -6.0 cm^{-1}),它耦合了簇内的四个自旋(s = 1)的(Ni(II))离子,以及对激发态内ZFS的表征。综合实验研究支持了最近的工作,表明与(S = 4)态相关的四阶各向异性起源于与单个(Ni(II))中心相关的二阶ZFS相互作用,但这仅是通过基态与更高激发态((S < 4))自旋多重态之间的(S)混合发生的高阶过程的结果。我们认为这种(S)混合在与许多其他著名SMM相关的低温量子动力学中起着重要作用。