Boudalis Athanassios K, Sanakis Yiannis, Dahan Françoise, Hendrich Michael, Tuchagues Jean-Pierre
Laboratoire de Chimie de Coordination du CNRS, UPR 8241, Toulouse, France.
Inorg Chem. 2006 Jan 9;45(1):443-53. doi: 10.1021/ic051652x.
A new asymmetrically coordinated bis-trinuclear iron(III) cluster containing a Fe(3)O core has been synthesized and structurally, magnetically, and spectroscopically characterized. Fe(6)Na(2)O(2)(O(2)CPh)(10)(pic)(4)(EtOH)(4)(H(2)O)(2)(2).2EpsilontOH (1.2EpsilontOH) crystallizes in the P space group and consists of two symmetry-related {Fe(3)O](7+) subunits linked by two Na(+) cations. Inside each Fe(3)O subunit, the iron(III) ions are antiferromagnetically coupled, and their magnetic exchange is best described by an isosceles triangle model with two equal (J) and one different (J ') coupling constants. On the basis of the H = -2SigmaJ(ij)S(i)S(j) spin Hamiltonian formalism, the two best fits to the data yield solutions J = -27.4 cm(-1), J ' = -20.9 cm(-1) and J = -22.7 cm(-1), J ' = -31.6 cm(-1). The ground state of the cluster is S = (1)/(2). X-band electron paramagnetic resonance (EPR) spectroscopy at liquid-helium temperature reveals a signal comprising a sharp peak at g approximately 2 and a broad tail at higher magnetic fields consistent with the S = (1)/(2) character of the ground state. Variable-temperature zero-field and magnetically perturbed Mössbauer spectra at liquid-helium temperatures are consistent with three antiferromagnetically coupled high-spin ferric ions in agreement with the magnetic susceptibility and EPR results. The EPR and Mössbauer spectra are interpreted by assuming the presence of an antisymmetric exchange interaction with |d| approximately 2-4 cm(-1) and a distribution of exchange constants J(ij).
一种含有Fe(3)O核心的新型不对称配位双三核铁(III)簇合物已被合成,并通过结构、磁性和光谱进行了表征。Fe(6)Na(2)O(2)(O(2)CPh)(10)(pic)(4)(EtOH)(4)(H(2)O)(2)(2).2EpsilontOH (1.2EpsilontOH)在P空间群中结晶,由两个通过两个Na(+)阳离子连接的对称相关的{Fe(3)O](7+)亚基组成。在每个Fe(3)O亚基内部,铁(III)离子反铁磁耦合,其磁交换最好用具有两个相等(J)和一个不同(J ')耦合常数的等腰三角形模型来描述。基于H = -2ΣJ(ij)S(i)S(j)自旋哈密顿形式,对数据的两个最佳拟合得到解J = -27.4 cm(-1),J ' = -20.9 cm(-1)和J = -22.7 cm(-1),J ' = -31.6 cm(-1)。簇合物的基态为S = (1)/(2)。液氦温度下的X波段电子顺磁共振(EPR)光谱显示出一个信号,该信号在g约为2处有一个尖锐峰,在更高磁场处有一个宽尾,这与基态的S = (1)/(2)特征一致。液氦温度下的变温零场和磁扰动穆斯堡尔光谱与三个反铁磁耦合的高自旋铁离子一致,这与磁化率和EPR结果相符。通过假设存在|d|约为2 - 4 cm(-1)的反对称交换相互作用和交换常数J(ij)的分布来解释EPR和穆斯堡尔光谱。