TABLE 3.
Shell I | Distance vector | Coordination number/per Mn Ni | Distance/Å Ri | Debye-Waller parameter/Å2 2 σi2 |
---|---|---|---|---|
I | Mn–O/N | 3.92 ± 0.82* (5.5)† 3.44§ | 1.853 ± 0.003* 1.853§ | 0.0186 ± 0.0050* (0.0276)† 0.0156§ |
II | Mn–O | 0.31 ± 0.35* (0.0) 0.06§ | 2.164 ± 0.002* 2.163§ | 0.0124 ± 0.0020* 0.0110§ |
6.21‡ ± 0.40* (6.0) | ||||
III | Mn–Mn | 1.02 ± 0.06* (1.0) 1.23§ | 2.709 ± 0.002* 2.715§ | 0.0046 ± 0.0020* 0.0065§ |
IV | Mn–Mn | 0.43 ± 0.18* (0.5) | 3.083 ± 0.020* | 0.0027 ± 0.0025 |
V | Mn–Ca/Mn | 0.45 ± 0.14* (0.5) | 3.295 ± 0.020* | 0.0027 ± 0.0025 |
VI | Mn–O/N/C | 2.86 ± 0.55* (3.0) | 3.637 ± 0.010* | 0.0080 ± 0.0025 |
The values of Ri and σi of the eight spectra were coupled to yield equal numbers in all spectra (joint-fit approach); in addition the values of σIV and σV were fixed (no variation during the individual fit session). The averaged RF value of the eight spectra was 11%. The shown Ni values refer to the intact Mn complex of PSII (no heating, 0 min) and, for shell II, also to the state resulting from 180 min of heat exposure; the resulting Ni for the other heating periods are shown in Fig. 5 (solid circles).
Indicated is the range of values obtained for variations in the values of σIV and σV (σIV = σV = 0.0002, 0.0027, 0.0052) and in the k-weighting (either k2- or k3-weighting for all three values of σIV and σV). This range represents the robustness of the fit with respect to variations in details of the fit approach, but not a confidence interval.
The values in parentheses were used for the calculation of the model spectra shown in Fig. 4.
Coordination number as obtained for samples exposed to 180 min of heating.
Results of a three-shell simulation of the eight spectra (Fig. 5, open circles); Ri and 2σ2 were coupled to yield identical values for all eight spectra; RF was 25.0%.