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Complexes with Fe<sup>III</sup><sub>2</sub>(μ-O)(μ-OH), Fe<sup>III</sup><sub>2</sub>(μ-O)<sub>2</sub>, and [Fe<sup>III</sup><sub>3</sub>(μ<sub>2</sub>-O)<sub>3</sub>] Cores:  Structures, Spectroscopy, and Core Interconversions

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journal contribution
posted on 1999-03-02, 00:00 authored by Hui Zheng, Yan Zang, Yanhong Dong, Victor G. Young, Lawrence Que
We have synthesized the first complexes with bis(μ-oxo)diiron(III) and (μ-oxo)(μ-hydroxo)diiron(III) cores (<b>1</b> and <b>2</b>, L = TPA (<b>a</b>), 5-Et<sub>3</sub>-TPA (<b>b</b>), 6-Me<sub>3</sub>-TPA (<b>c</b>), 4,6-Me<sub>6</sub>-TPA (<b>d</b>), BQPA (<b>e</b>), BPEEN (<b>f</b>), and BPMEN (<b>g</b>)) and found them to have novel structural properties. In particular, the presence of two single-atom bridges in these complexes constrains the Fe−Fe distances to 2.7−3.0 Å and the Fe−μ-O−Fe angles to 100° or smaller. The significantly acute Fe−O−Fe angles (e.g., 92.5(2)° for <b>1c</b> and 100.2(2)° for<b> 2f</b>) enforced by the Fe<sub>2</sub>O<sub>2</sub>(H) core endow these complexes with UV−vis, Raman, and magnetic properties quite distinct from those of other (μ-oxo)diiron(III) complexes. Complex <b>1c</b> exhibits visible absorption bands at 470 (ε = 560 M<sup>-1</sup> cm<sup>-1</sup>) and 760 nm (ε = 80 M<sup>-1</sup> cm<sup>-1</sup>), while complexes <b>2</b> show features at ca. 550 (ε ≈ 800 M<sup>-1</sup> cm<sup>-1</sup>) and ca. 800 nm (ε ≈ 70 M<sup>-1</sup> cm<sup>-1</sup>), all of which are red shifted compared to those of other (μ-oxo)diiron(III) complexes. These complexes also exhibit distinct ν<sub>Fe-O</sub><sub>-</sub><sub>Fe</sub> vibrations at ca. 600 and ca. 670 cm<sup>-1</sup> assigned to the ν<sub>sym</sub> and the ν<sub>asym</sub> of the Fe−O−Fe units, respectively. The relative intensities of the ν<sub>sym</sub> and ν<sub>asym</sub> bands are affected by the symmetry of the Fe−O−Fe units; an unsymmetric core enhances the intensity of the ν<sub>asym</sub>. Complexes <b>2</b> exhibit another band at ca. 500 cm<sup>-1</sup>, which is assigned to the Fe−(OH)−Fe stretching mode due to its sensitivity to both H<sub>2</sub><sup>18</sup>O and <sup>2</sup>H<sub>2</sub>O. Magnetic susceptibility studies reveal <i>J</i> = 54 cm<sup>-1</sup> for <b>1c</b> and ca. 110 cm<sup>-1</sup> for <b>2 </b>(<b>H</b> =<i> J</i><b>S</b><sub>1</sub>·<b>S</b><sub>2</sub>), values smaller than those for the antiferromagnetic interactions found in (μ-oxo)diiron(III) complexes. This weakening arises from the longer Fe−μ-O bonds and the smaller Fe−μ-O−Fe angles in the Fe<sub>2</sub>O<sub>2</sub>(H) diamond core structure. These spectroscopic signatures can thus serve as useful tools to ascertain the presence of such core structures in metalloenzyme active sites. These two core structures, Fe<sub>2</sub>(μ-O)<sub>2</sub> (<b>1</b>) and Fe<sub>2</sub>(μ-O)(μ-OH) (<b>2</b>), can also be interconverted by protonation equilibria with p<i>K</i><sub>a</sub>'s of 16−18 in CH<sub>3</sub>CN. Furthermore, the Fe<sub>2</sub>(μ-O)<sub>2</sub> core (<b>1</b>) isomerizes to the Fe<sub>3</sub>(μ<sub>2</sub>-O)<sub>3</sub> core (<b>7</b>), while the Fe<sub>2</sub>(μ-O)(μ-OH) core (<b>2</b>) exhibits aquation equilibria to the Fe<sub>2</sub>(μ-O)(μ-H<sub>3</sub>O<sub>2</sub>) core (<b>5</b>), except for L = 6-Me<sub>3</sub>-TPA and 4,6-Me<sub>6</sub>-TPA. It is clear from these studies that electronic and steric properties of the ligands significantly affect the various equilibria, demonstrating a rich chemistry involving water-derived ligands alone.

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