Department of Chemistry and Centre for Laser, Atomic and Molecular Science, University of New Brunswick, Fredericton, NB, Canada.
Magn Reson Chem. 2010 Dec;48 Suppl 1:S122-31. doi: 10.1002/mrc.2649.
The g tensor components of the 4,5-dihydro-1,3,2-dithiazolyl (H2DTA•) radical, which is a basic building block for molecular magnets and spintronic devices, is calculated by the coupled-perturbed Kohn-Sham (CPKS) hybrid density functional (HDF) and multireference configuration interaction-sum over states (MRCI-SOS) techniques. In both methods, the diagonalized g tensor principal axes are found to be aligned with the radical's inertial axes. The tensor components are in very good agreement with those determined experimentally by electron paramagnetic resonance (EPR) spectroscopy. The MRCI technique produced g tensor components that are more accurate than those obtained by the CPKS-HDF method. Nonetheless, to get reasonable MRCI results, one must include the in-plane and out-of-plane interactions in an unbiased way. The minimum reference space that satisfies these conditions is generated from a complete active space of nine electrons in six orbitals [CAS(9,6)] and contains a(1), a(2), b(1) and b(2) type orbitals. In addition, the number of roots in the MRCI-SOS g tensor expansion should include all excited states that range from 0 to 56,000 cm(-1). The most accurate results are obtained using an MRCI-SOS/CAS(13,9) calculation. These g tensor components are within the experimental accuracy range of 1000 ppm. The one- and two-electron contributions to the g tensor components are separated and individually analyzed. The very good agreement with experiment opens the door for further accurate calculations of spin Hamiltonian tensors of larger DTA• radicals.
4,5-二氢-1,3,2-二噻唑基(H2DTA•)自由基的 g 张量分量是通过耦合微扰 Kohn-Sham(CPKS)杂化密度泛函(HDF)和多参考组态相互作用-态求和(MRCI-SOS)技术计算的,它是分子磁体和自旋电子器件的基本构建块。在这两种方法中,对角化的 g 张量主轴与自由基的惯性轴一致。张量分量与电子顺磁共振(EPR)光谱实验测定的结果非常吻合。MRCI 技术产生的 g 张量分量比 CPKS-HDF 方法更准确。尽管如此,要获得合理的 MRCI 结果,必须以无偏的方式包括平面内和平面外相互作用。满足这些条件的最小参考空间是从九个电子六个轨道的完整活性空间[CAS(9,6)]中生成的,包含 a(1)、a(2)、b(1)和 b(2)类型轨道。此外,MRCI-SOS g 张量展开中的根数量应包括从 0 到 56,000 cm(-1)的所有激发态。使用 MRCI-SOS/CAS(13,9)计算可获得最准确的结果。这些 g 张量分量在实验精度范围 1000 ppm 内。将 g 张量分量的单电子和双电子贡献分开并分别进行分析。与实验非常吻合,为进一步准确计算更大 DTA•自由基的自旋哈密顿张量开辟了道路。