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. Author manuscript; available in PMC: 2010 Jan 13.
Published in final edited form as: Biochemistry. 2009 Jan 13;48(1):59–73. doi: 10.1021/bi8016087

Table 4.

First-shell EXAFS Curve-Fitting Results for Biferrous DFsc, Biferrous DFscY51L, and Biferrous DFscE11D.a

DFsc DFscY51L DFscE11D

fit no. 1 2 3 4 5 6 7 8 9
Fe–O/Nb N 5 2 2 5 2 2 5 2 2
R (Å) 2.07 2.02 2.03 2.07 2.02 2.03 2.07 2.01 2.02
σ2 × 1052) 1230 370 390 1040 470 530 1140 500 540

Fe–O/Nb N 3 3 3 3 3 3
R (Å) 2.16 2.16 2.14 2.14 2.13 2.14
σ2 × 1052) 650 700 670 810 710 820

Fe–C N 1 1 1
R (Å) 2.55 2.55 2.54
σ2 × 1052) 470 200 400

Fe–C N 2 2 2 2 2 2 2 2 2
R (Å) 2.96 3.00 3.00 2.96 2.99 2.99 2.96 3.01 3.01
σ2 × 1052) 590 390 430 730 460 570 1000 760 810

ΔE0, eV −9.1 −6.0 −5.7 −8.4 −6.0 −5.9 −7.1 −4.6 −4.4

Fc 0.433 0.393 0.391 0.345 0.333 0.309 0.270 0.255 0.233
a

All fits were performed over the k range of 2-15 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%.

b

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.

c

The goodness of the fit is defined as F = [Σ(k6(χexptlχcalcd)2)/(Σk6χexptl2)]½.