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铁(II)铼(IV)氰化物单链磁体家族中的磁结构相关性:密度泛函理论与从头算计算

Magneto-structural correlations in a family of Fe(II)Re(IV)(CN)2 single-chain magnets: density functional theory and ab initio calculations.

作者信息

Zhang Yi-Quan, Luo Cheng-Lin, Wu Xin-Bao, Wang Bing-Wu, Gao Song

机构信息

College of Chemistry and Molecular Engineering, Peking University , Beijing 100871, P. R. China.

出版信息

Inorg Chem. 2014 Apr 7;53(7):3503-10. doi: 10.1021/ic402945j. Epub 2014 Mar 27.

DOI:10.1021/ic402945j
PMID:24673387
Abstract

Until now, the expressions of the anisotropic energy barriers Δξ and ΔA, using the uniaxial magnetic anisotropy D, the intrachain coupling strength J, and the high-spin ground state S for single-chain magnets (SCMs) in the intermediate region between the Ising and the Heisenberg limits, were unknown. To explore this relationship, we used density functional theory and ab initio methods to obtain expressions of Δξ and ΔA in terms of D, J, and S of six R4Fe(II)-Re(IV)Cl4(CN)2 (R = diethylformamide (1), dibutylformamide (2), dimethylformamide (3), dimethylbutyramide (4), dimethylpropionamide (5), and diethylacetamide (6)) SCMs in the intermediate region. The ΔA value for compounds 1-3 was very similar to the magnetic anisotropic energy of a single Fe(II), while the value of Δξ was predicted using the exchange interaction of Fe(II) with the neighboring Re(IV), which could be expressed as 2JSReSFe. Similar to compounds 1-3, the anisotropy energy barrier ΔA of compounds 4 and 5 was also equal to (Di - Ei)SFe(2), but the correlation energy Δξ was closely equal to 2JSReSFe(cos 98.4 - cos 180) due to the reversal of the spins on the opposite Fe(II). For compound 6, one unit cell of Re(IV)Fe(II) was regarded as a domain wall since it had two different Re(IV)-Fe(II) couplings. Thus, the Δξ of compound 6 was expressed as 4J″SRe1Fe1SRe2Fe2, where J″ was the coupling constant of the neighboring unit cells of Re1Fe1 and Re2Fe2, and ΔA was equal to the anisotropic energy barrier of one domain wall given by DRe1Fe1(S(2)Re1Fe1 - 1/4).

摘要

到目前为止,在伊辛极限和海森堡极限之间的中间区域,利用单轴磁各向异性D、链内耦合强度J以及单链磁体(SCMs)的高自旋基态S来表示各向异性能垒Δξ和ΔA的表达式尚不清楚。为了探究这种关系,我们使用密度泛函理论和从头算方法,得到了六种R4Fe(II)-Re(IV)Cl4(CN)2(R = 二乙酰胺(1)、二丁酰胺(2)、二甲基甲酰胺(3)、二甲基丁酰胺(4)、二甲基丙酰胺(5)和二乙酰胺(6))SCMs在中间区域的Δξ和ΔA关于D、J和S的表达式。化合物1 - 3的ΔA值与单个Fe(II)的磁各向异性能非常相似,而Δξ值是利用Fe(II)与相邻Re(IV)的交换相互作用预测的,其可表示为2JSReSFe。与化合物1 - 3类似,化合物4和5的各向异性能垒ΔA也等于(Di - Ei)SFe(2),但由于相反Fe(II)上自旋的反转,相关能Δξ近似等于2JSReSFe(cos 98.4 - cos 180)。对于化合物6,由于其具有两种不同的Re(IV)-Fe(II)耦合,一个Re(IV)Fe(II)晶胞被视为一个畴壁。因此,化合物6的Δξ表示为4J″SRe1Fe1SRe2Fe2,其中J″是Re1Fe1和Re2Fe2相邻晶胞的耦合常数,而ΔA等于由DRe1Fe1(S(2)Re1Fe1 - 1/4)给出的一个畴壁的各向异性能垒。

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