Table 6.
EXAFS Curve-Fitting Results for Oxidized DFscE11D.a
fit no. | R (Å) | σ2 × 105 (Å2) | ΔE0 | Fb | |
---|---|---|---|---|---|
10 | 5 O/N | 2.02 | 970 | −4.3 | 0.308 |
11 | 6 O/N | 2.02 | 1170 | −4.5 | 0.315 |
12 | 5 Fe–O/Nc | 2.02 | 960 | −4.4 | 0.232 |
2 Fe–C | 2.97 | 530 | |||
2 Fe–C | 3.34 | 720 | |||
4 Fe–N–C/Nd | 4.18 | 740 | |||
13 | 6 Fe–O/Nc | 2.02 | 1160 | −4.8 | 0.239 |
2 Fe–C | 2.97 | 530 | |||
2 Fe–C | 3.33 | 740 | |||
4 Fe–N–C/Nd | 4.17 | 650 | |||
14 | 0.5 Fe–O | 1.89 | 450 | −5.0 | 0.226 |
5 Fe–O/N | 2.03 | 870 | |||
2 Fe–C | 2.97 | 550 | |||
2 Fe–C | 3.33 | 750 | |||
4 Fe–N–C/Nd | 4.17 | 640 |
All fits were performed over the k range of 2-13 Å-1. The estimated uncertainty in R is ± 0.02 Å for the first shell and ± 0.05 Å for outer shells; the uncertainty in N is ~25%.
The goodness of the fit is defined as F = [Σ(k6(χexptl – χcalcd)2)/(Σk6χexptl2)]½.
Scatterers differing by Z ± 1 are not distinguishable in an EXAFS fit. The first element in a pair indicates the type of atom used to model the backscattered wave in the FEFF calculation.
Modeled as the Fe-N-C path of 158° of an imidazole ring.