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Ab Initio Size-Consistent Calculations of Effective Exchange Interactions in Mesoscopic Magnetic Clusters Composed of Triplet Methylenes and Quartet Nitrogen Atoms

机译:由三重态亚甲基和四方氮原子组成的介观磁簇中的有效交换相互作用的从头算大小一致的计算

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The electronic structures of linear magnetic clusters composed of eleven triplet methylenes eleven quartet nitrogen atoms, and five triplet methylenes plus six quartet nitrogen atoms were investigated by the unrestricted Hartree-Fock (UHF), post UHF and their spin-projected wavefunctions in combination with the Heisenberg model. The effective exchange integrals (J_(ab)) in the Heisenberg model were calculated by the difference between the total energies of the highest spin (HS) and lowest spin (LS) UHF-based wavefunction of the clusters. The J_(ab) values by the UHF-based and spin-polarized DFT methods were compared with those of the SO-Cl, MRSDCI, CASSCF, CAST2, and MRMP2 calculations in the case of small linear clusters, such as a triplet methylene dimer. The spin-polarized density functional (BLYP and B3LYP) calculations followed by the size-consistent spin projection were carried out for dimer, trimer, and clusters with eleven magnetic sites to obtain the J_(ab) values, since the DFT methods were heavily utilized in solid state physics. It was found that all of the methods, except for DFT, provide similar J_(ab) values in the magnetic region of the dimer, where the interatomic distance is longer than 3.0 A. However, the spin crossover from the LS state to the HS state occurs at a larger distance in the cases of MRSDCI and MRMP2. The spin projection for LS spin-polarized wavefunctions becomes less important in the case of long linear clusters, such as (CH_2)_(11). The DFT results are generally biased to stabilize the low-spin states. The implications of the calculated results are discussed in relation to the molecular magnetisms in mesoscopic molecular aggregates.
机译:通过无限制Hartree-Fock(UHF),后UHF及其结合自旋投影波函数研究了由11个三重态亚甲基,11个四重氮原子,5个三重亚甲基加6个四重氮原子组成的线性磁团簇的电子结构。海森堡模型。根据簇的最高自旋(HS)和最低自旋(LS)UHF波函数的总能量之差,计算出海森堡模型中的有效交换积分(J_(ab))。在小型线性簇(例如三联体亚甲基二聚体)的情况下,将基于UHF和自旋极化DFT方法的J_(ab)值与SO-Cl,MRSDCI,CASSCF,CAST2和MRMP2计算的J_(ab)值进行了比较。 。对自旋极化密度泛函(BLYP和B3LYP)进行计算,然后对具有11个磁性位点的二聚体,三聚体和簇进行尺寸一致的自旋投影,以获得J_(ab)值,因为DFT方法被大量利用在固态物理学中发现除DFT以外,所有方法在二聚体的磁性区域(原子间距离均大于3.0 A)提供相似的J_(ab)值。但是,从LS状态到HS的自旋交叉在MRSDCI和MRMP2的情况下,状态会以较大的距离出现。在诸如(CH_2)_(11)之类的长线性簇的情况下,用于LS自旋极化波函数的自旋投影变得不太重要。 DFT结果通常偏向稳定低旋转状态。关于介观分子聚集体中的分子磁性,讨论了计算结果的含义。

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