Rajaraman Gopalan, Totti Federico, Bencini Alessandro, Caneschi Andrea, Sessoli Roberta, Gatteschi Dante
Università degli Studi di Firenze, INSTM, Polo Scientifico, Dipartimento di Chimica, via della Lastruccia 3, 50019, Sesto F.no, Italy.
Dalton Trans. 2009 May 7(17):3153-61. doi: 10.1039/b817540c. Epub 2009 Mar 13.
Density functional calculations have been performed on a [Gd(iii)Cu(ii)] complex [L(1)CuGd(O(2)CCF(3))(3)(C(2)H(5)OH)(2)] () (where L(1) is N,N'-bis(3-ethoxy-salicylidene)-1,2-diamino-2-methylpropanato) with an aim of assessing a suitable functional within the DFT formalism to understand the mechanism of magnetic coupling and also to develop magneto-structural correlations. Encouraging results have been obtained in our studies where the application of B3LYP on the crystal structure of yields a ferromagnetic J value of -5.8 cm(-1) which is in excellent agreement with the experimental value of -4.42 cm(-1) (H = JS(Gd).S(Cu)). After testing varieties of functional for the method assessment we recommend the use of B3LYP with a combination of an effective core potential basis set. For all electron basis sets the relativistic effects should be incorporated either via the Douglas-Kroll-Hess (DKH) or zeroth-order regular approximation (ZORA) methods. A breakdown approach has been adopted where the calculations on several model complexes of have been performed. Their wave functions have been analysed thereafter (MO and NBO analysis) in order to gain some insight into the coupling mechanism. The results suggest, unambiguously, that the empty Gd(iii) 5d orbitals have a prominent role on the magnetic coupling. These 5d orbitals gain partial occupancy via Cu(ii) charge transfer as well as from the Gd(iii) 4f orbitals. A competing 4f-3d interaction associated with the symmetry of the complex has also been observed. The general mechanism hence incorporates both contributions and sets forth rather a prevailing mechanism for the 3d-4f coupling. The magneto-structural correlations reveal that there is no unique parameter which the J values are strongly correlated with, but an exponential relation to the J value found for the O-Cu-O-Gd dihedral angle parameter is the most credible correlation.
已对[Gd(iii)Cu(ii)]配合物[L(1)CuGd(O₂CCF₃)₃(C₂H₅OH)₂]( )(其中L(1)为N,N'-双(3-乙氧基水杨醛)-1,2-二氨基-2-甲基丙烷)进行了密度泛函计算,目的是在密度泛函理论形式体系内评估一种合适的泛函,以理解磁耦合机制,并建立磁结构相关性。在我们的研究中获得了令人鼓舞的结果,其中在晶体结构上应用B3LYP得到铁磁J值为-5.8 cm⁻¹,这与实验值-4.42 cm⁻¹(H = JS(Gd).S(Cu))非常吻合。在测试了各种用于方法评估的泛函后,我们建议使用B3LYP并结合有效核势基组。对于所有电子基组,应通过Douglas-Kroll-Hess(DKH)或零阶正则近似(ZORA)方法纳入相对论效应。采用了一种分解方法,对 的几个模型配合物进行了计算。此后对它们的波函数进行了分析(MO和NBO分析),以便深入了解耦合机制。结果明确表明,空的Gd(iii) 5d轨道在磁耦合中起重要作用。这些5d轨道通过Cu(ii)电荷转移以及Gd(iii) 4f轨道获得部分占据。还观察到与配合物对称性相关的竞争4f - 3d相互作用。因此,一般机制包含了这两种贡献,并提出了一种相当普遍的3d - 4f耦合机制。磁结构相关性表明,没有与J值强烈相关的唯一参数,但对于O - Cu - O - Gd二面角参数发现的与J值的指数关系是最可靠的相关性。