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. Author manuscript; available in PMC: 2013 Jul 14.
Published in final edited form as: Dalton Trans. 2012 Mar 20;41(26):7984–7993. doi: 10.1039/c2dt30147d

Table 2.

Selected EXAFS fits to the NO-bound and Fe(II)–unligated states of Tt H-NOX.a

Tt H-NOX Fe(II)–NO

fit 1 fit 2 fit 3 fit 4
shell r σ 2 shell r σ 2 shell r σ 2 shell r σ 2




1 Fe-NO 1.75 5.1 1 Fe-NO 1.73 3.0 1 Fe-NO 1.74 5.4
4 Fe-Np 1.99 3.9 4 Fe-Np 1.97 3.3 4 Fe-Np + 1 Fe-
NHis
1.97 5.1 4 Fe-Np 1.97 3.4
1 Fe-NHis 2.32 6.5
8 Fe••Cα 3.01 3.3 8 Fe••Cα 2.99 3.6 8 Fe••Cα 2.99 3.6 8 Fe••Cα 2.99 3.5
16 Fe••Cα/Np 3.18 6.8 16 Fe••Cα/Np 3.16 7.2 16 Fe••Cα/Np 3.16 7.2 16 Fe••Cα/Np 3.16 7.1
4 Fe••Ch 3.10 37.5 4 Fe••Ch 3.34 4.9 4 Fe••Ch 3.34 4.9 4 Fe••Ch 3.35 4.5
8 Fe••Cβ 4.36 6.3 8 Fe••Cβ 4.31 5.5 8 Fe••Cβ 4.31 5.4 8 Fe••Cβ 4.31 5.5
16 Fe••Cβ/Np 4.39 12.6 16 Fe••Cβ/Np 4.34 11.0 16 Fe••Cβ/Np 4.33 10.8 16 Fe••Cβ/Np 4.33 11.0




F 0.369 F 0.286 F 0.315 F 0.270
ΔE0 8.40 ΔE0 3.76 ΔE0 3.43 ΔE0 3.48





Tt H-NOX Fe(II)–unligated

fit 5 fit 6 fit 7 fit 8
shell r σ 2 shell r σ 2 shell r σ 2 shell r σ 2




4 Fe-Np 2.02 7.2 4 Fe-Np + 1
Fe-NHis
2.02 10.0 4 Fe-Np 2.02 7.2 4 Fe-Np + 1
Fe-NHis
2.03 10.3
1 Fe-NHis/O 2.69 2.6 1 Fe-O 2.38 3.2
8 Fe••Cα 3.11 13.4 8 Fe••Cα 3.12 15.9 8 Fe••Cα 3.09 15.0 8 Fe••Cα 3.12 14.2
4 Fe••Ch 3.40 −0.3 4 Fe••Ch 3.40 −0.4 4 Fe••Ch 3.40 −0.5 4 Fe••Ch 3.40 −0.8
8 Fe••Cβ 4.39 3.7 8 Fe••Cβ 4.39 4.0 8 Fe••Cβ 4.39 3.8 8 Fe••Cβ 4.39 3.3
16 Fe••Cβ/Np 4.42 7.5 16 Fe••Cβ/Np 4.42 8.0 16 Fe••Cβ/Np 4.42 7.7 16 Fe••Cβ/Np 4.42 6.7




F 0.381 F 0.436 F 0.362 F 0.411
ΔE0 4.95 ΔE0 4.94 ΔE0 4.98 ΔE0 4.98




a

r is in units of Å; σ2 is in units of 10−3 Å2; ΔE0 is in units of eV. All fits are to unfiltered data. F represents a goodness-of-fit parameter. Fourier transform ranges: k = 2.0 – 13.85 Å−1 (resolution = 0.134 Å) for Tt H-NOX Fe(II)–NO; k = 2.0 – 12.0 Å−1 (resolution = 0.157 Å) for Tt H-NOX Fe(II)–unligated. Values of r for the Fe••Cα single scattering and Fe••Cα/Np multiple scattering paths were constrained to a constant difference from one another, while σ2 for the multiple scattering path was constrained to be twice that of the single scattering path. A similar constraint was placed on the Cβ and Cβ/Np combination. Inclusion of the Fe••Cα/Np multiple scattering paths was not required for fits of Fe(II)-unligated data.