| Literature DB >> 25166909 |
Logan J Giles1, Christian Ruppelt, Jing Yang, Ralf R Mendel, Florian Bittner, Martin L Kirk.
Abstract
Mo K-edge X-ray absorption spectroscopy has been used to probe as-isolated structures of the MOSC family proteins pmARC-1 and HMCS-CT. The Mo K-edge near-edge spectrum of HMCS-CT is shifted ~2.5 eV to lower energy compared to the pmARC-1 spectrum, which indicates that as-isolated HMCS-CT is in a more reduced state than pmARC-1. Extended X-ray absorption fine structure analysis indicates significant structural differences between pmARC-1 and HMCS-CT, with the former being a dioxo site and the latter possessing only a single terminal oxo ligand. The number of terminal oxo donors is consistent with pmARC-1 being in the Mo(VI) oxidation state and HMCS-CT in the Mo(IV) state. These structures are in accord with oxygen-atom-transfer reactivity for pmARC-1 and persulfide bond cleavage chemistry for HMCS-CT.Entities:
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Year: 2014 PMID: 25166909 PMCID: PMC4164224 DOI: 10.1021/ic5015863
Source DB: PubMed Journal: Inorg Chem ISSN: 0020-1669 Impact factor: 5.165
Figure 1Mo K-edge XANES spectra of as-isolated HMCS-CT (black) and as-isolated pmARC-1 (red). Inset: Complete k = 18 spectra.
Figure 2Mo EXAFS of pmARC-1 (black) and the corresponding FT of fit 1-1 (green). Inset: (top) Mo=O (red) and Mo–S (purple) scattering paths that contribute to the overall fit; (middle) k-space data for pmARC-1 (black) and fit 1-1 (green); (bottom) residual (blue).
EXAFS Curve-Fitting Results for MOSC Proteins
| Mo≡O | Mo–S | Mo–O | ||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| fit | σ2 | σ2 | σ2 | Δ | ||||||||
| pmARC-1 | fit 1-1 | 2.0 | 1.76 | 0.002 | 3.0 | 2.47 | 0.013 | –3.76 | 8.79 | |||
| fit 1-2 | 3.0 | 1.76 | 0.005 | 2.0 | 2.45 | 0.009 | –5.48 | 15.79 | ||||
| fit 1-3 | 3.0 | 1.76 | 0.005 | 3.0 | 2.45 | 0.013 | –5.78 | 13.38 | ||||
| fit 1-4 | 1.0 | 1.76 | 0.001 | 3.0 | 2.43 | 0.010 | 1.0 | 2.43 | 0.001 | –6.94 | 33.98 | |
| model 1-1 | 2 | 1.71 | 3 | 2.46 | ||||||||
| HMCS-CT | fit 2-1 | 1.0 | 1.71 | 0.002 | 3.0 | 2.38 | 0.006 | 1.0 | 2.49 | 0.004 | –8.97 | 5.51 |
| fit 2-2 | 1.0 | 1.71 | 0.002 | 3.0 | 2.37 | 0.006 | –7.97 | 6.66 | ||||
| fit 2-3 | 2.0 | 1.72 | 0.008 | 2.0 | 2.37 | 0.006 | –7.24 | 12.09 | ||||
| model 2-1 | 1 | 1.69 | 3 | 2.36 | 1 | 2.31 | ||||||
| model 2-2 | 1 | 1.70 | 3 | 2.34 | ||||||||
The σ2 value was fixed to 0.001 to avoid negative σ2 values.
Geometry-optimized model structure consistent with fit 1-1.
Geometry-optimized model structure consistent with fit 2-1.
Geometry-optimized model structure consistent with fit 2-2. Details on the model calculations are given in the Supporting Information.
Figure 4Possible structures for as-isolated pmARC-1 (A) and HMCS-CT (B) determined from XAS. (C) Internal redox conversion of the molybdenum(IV) persulfide to form a MoVI=S species and uncoordinated cysteine.
Figure 3Mo EXAFS for HMCS-CT (black) and the corresponding FT of fit 2-1 (green). Inset: (top) Mo≡O (red), Mo–O (orange), and Mo–S (purple) scattering paths that contribute to the overall fit; (middle) k-space data for HMCS-CT (black) and fit 2-1 (green); (bottom) residual (blue).