Geometric and Electronic Structure of the Heme-Peroxo-Copper Complex [(FTPP)Fe-(O)-Cu"(TMPA)](CIO).

The geometric and electronic structure of the untethered heme–peroxo–copper model complex [(FTPP)Fe–(O)–Cu(TMPA)](ClO) (1) has been investigated using Cu and Fe K-edge EXAFS spectroscopy and density functional theory calculations in order to describe its geometric and electronic structure. The Fe an...

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Published in:Journal of the American Chemical Society Vol. 127; no. 34; pp. 11969 - 11979
Main Authors: del RíO, Diego, Sarangi, Ritimukta, Chufän, Eduardo E., Karlin, Kenneth D., Hedman, Britt, Hodgson, Keith O., Solomon, Edward I.
Format: Article
Published: American Chemical Society 8/31/2005
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Online Access:View this record in EBSCOhost
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      dt: 8/31/2005
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      pub: American Chemical Society
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        18186835
        10.1021/ja043374r
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        atl: Geometric and Electronic Structure of the Heme-Peroxo-Copper Complex [(FTPP)Fe-(O)-Cu"(TMPA)](CIO).
      aug:
        au:
          del RíO, Diego
          Sarangi, Ritimukta
          Chufän, Eduardo E.
          Karlin, Kenneth D.
          Hedman, Britt
          Hodgson, Keith O.
          Solomon, Edward I.
        affil:
          Department of Chemistry, Stanford University.
          Department of Chemistry, Johns Hopkins University.
          Stanford Synchrotron Radiation Laboratory.
      su:
        Electronic structure
        Extended X-ray absorption fine structure
        Spectrum analysis
        Density functionals
        Copper
        Particles (Nuclear physics)
      sug:
        subj:
          Electronic structure
          Extended X-ray absorption fine structure
          Spectrum analysis
          Density functionals
          Copper
          Particles (Nuclear physics)
      ab: The geometric and electronic structure of the untethered heme–peroxo–copper model complex [(FTPP)Fe–(O)–Cu(TMPA)](ClO) (1) has been investigated using Cu and Fe K-edge EXAFS spectroscopy and density functional theory calculations in order to describe its geometric and electronic structure. The Fe and Cu K-edge EXAFS data were fit with a CuߪFe distance of ∼3.72 Å. Spin-unrestricted DFT calculations for the S = 2 spin state were performed on [(P)Fe–(O)–Cu(TMPA)] as a model of 1. The peroxo unit is bound end-on to the copper, and side-on to the high-spin iron, for an overall μ-η¹; η² coordination mode. The calculated CuߪFe distance is ∼0.3 Å longer than that observed experimentally. Fleoptimization of [(P)Fe–(O)–Cu(TMPA)] with a 3.7 Å CuߪFe constrained distance results in a similar energy and structure that retains the overall μ-η¹η²-peroxo coordination mode. The primary bonding interaction between the copper and the peroxide involves electron donation into the half-occupied Cu d orbital from the peroxide π* orbital. In the case of the Fe––peroxide η² bond, the two major components arise from the donor interactions of the peroxide π* and π* orbitals with the Fe d and d orbitals, which give rise to σ and δ bonds, respectively. The π* interaction with both the half-occupied d orbital on the copper (η¹) and the d orbital on the iron (η²), provides an effective superexchange pathway for strong antiferromagnetic coupling between the metal centers.
      pubtype: Academic Journal
      doctype: Article
      src: R
    language: English
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