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Spin Coupling in Roussin’s Red and Black Salts

机译:鲁辛红盐和黑盐中的自旋耦合

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摘要

Although DFT calculations have provided a first-order electronic-structural description for Roussin’s red and black salts, a detailed study of spin coupling in these species has yet to be reported. Such an analysis is presented here for the first time, based on broken-symmetry density functional theory (DFT, chiefly OLYP/STO-TZP) calculations. Both the Noodleman and Yamaguchi formulas were used to evaluate the Heisenberg coupling constants (J). Three nitrosylated binuclear clusters were studied: [Fe2(NO)2(Et-HPTB)(O2CPh)]2+ (1; Et-HPTB=N,N,N',N'-tetrakis-(N-ethyl-2-benzimidazolylmethyl)-2-hydroxy-1,3-diaminopropane), [Fe(NO)2{Fe(NO)(NS3)}-S,S'] (2), and Roussin’s red salt anion [Fe2(NO)4(μ-S)2]2− (3). Although the Heisenberg J for 1 is small (≈102 cm−1), 2 and 3 exhibit J values that are at least an order of magnitude higher (≈103 cm−1), where the J values refer to the following Heisenberg spin Hamiltonian: =JSASB. For Roussin’s black salt anion, [Fe4(NO)73-S)3]− (4), the Heisenberg spin Hamiltonian describing spin coupling between the {FeNO}7 unit (SA=3/2) and the three {Fe(NO)2}9 units (SB=SC=SD=1/2) in [Fe4(NO)73-S)3]− was assumed to have the form: =J12(SASB+SASC+SASD)+J22(SBSC+SBSD+SCSD), in which J12 corresponds to the interaction between the apical iron and a basal iron, and J22 refers to that between any two basal iron centers. Although the basal–basal coupling constant J22 was found to be small (≈102 cm−1), the apical–basal coupling constant J12 is some forty times higher (≈4000 cm−1). Thus, the nitrosylated iron–sulfur clusters feature some exceptionally high J values relative to the non-nitrosylated {2Fe2S} and {4Fe4S} clusters. An analysis of spin-dependent bonding energies shed light on this curious feature. In essence, the energy difference between the high-spin (i.e., ferromagnetically coupled iron sites) and low-spin (i.e., maximum spin coupling) states of Roussin’s salts are indeed rather similar to those of analogous non-nitrosylated iron–sulfur clusters. However, the individual Fe(NO)x (x=1, 2) site spins are lower in the nitrosylated systems, resulting in a smaller denominator in both the Noodleman and Yamaguchi formulas for J, which in turn translates into the very high J values.
机译:尽管DFT计算提供了鲁辛红盐和黑盐的一阶电子结构描述,但尚未报道这些物种自旋耦合的详细研究。这种分析是首次基于破碎对称密度泛函理论(DFT,主要是OLYP / STO-TZP)计算得出。 Noodleman和Yamaguchi公式均用于评估Heisenberg耦合常数(J)。研究了三个亚硝化双核簇:[Fe 2 (NO) 2 (Et-HPTB)(O 2 CPh)] 2 + (1; Et-HPTB = N,N,N',N'-四-(N-乙基-2-苯并咪唑基甲基)-2-羟基-1,3-二氨基丙烷),[Fe(NO) 2 {Fe(NO)(NS 3 )}-S,S'](2)和鲁辛的红盐阴离子[Fe 2 (NO) 4 (μ-S) 2 ] 2-(3)。尽管1的Heisenberg J很小(≈10 2 cm -1 ),但是2和3的J值至少高一个数量级(≈10< sup> 3 cm −1 ),其中J值引用以下Heisenberg自旋哈密顿量:= JS A S B 。对于鲁辛的黑盐阴离子,[Fe 4 (NO) 7 (μ 3 -S) 3 ] < sup>-(4),海森堡自旋哈密顿量描述{FeNO} 7 单元(S A = 3/2)与三个{Fe(NO) 2 } 9 单位(S B = S C = S D < / sub> = 1/2)在[Fe 4 (NO) 7 (μ 3 -S) 3 ] -假定为以下格式:= J 12 (S A S B + S A S C + S A S D )+ J 22 (S B S C + S B S D + S C S D ),其中J 12 对应于顶端铁和基底铁之间的相互作用,J 22 指任意两个基底铁中心之间的相互作用。尽管发现基底-基底耦合常数J 22 很小(≈10 2 cm -1 ),但顶部-基底耦合常数J 12 高40倍(≈4000cm -1 )。因此,相对于未亚硝化的{2Fe2S}和{4Fe4S}簇,亚硝化的铁硫簇具有一些特别高的J值。对自旋相关键能的分析揭示了这种奇怪的特征。本质上,鲁辛盐的高自旋状态(即铁磁耦合的铁位点)和低自旋状态(即最大的自旋耦合)之间的能量差确实与类似的非亚硝化铁硫簇相似。但是,亚硝化系统中的单个Fe(NO)x x (x = 1,2)位点自旋较低,导致J的Noodleman和Yamaguchi公式中的分母都较小,这反过来又转换为非常高的J值。

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