Table 1.
Data set
|
|||
---|---|---|---|
λ1 | λ2 | λ3 | |
Wavelength, Å | 0.9791 | 0.9789 | 0.9686 |
Resolution, Å | 20.0–2.3 | 20.0–2.3 | 20.0–2.3 |
No. of observations | 184,409 | 180,695 | 168,715 |
No. of unique reflections | 27,098 | 30,005 | 29,499 |
Completeness (%)* | 89.1 (92.6) | 98.6 (99.8) | 97.6 (99.5) |
Rsym (%)*† | 5.8 (37.5) | 5.7 (32.9) | 4.8 (32.0) |
Phasing (F/σ(F) ≥ 1.0) | |||
Resolution, Å | 2.7 | 2.4 | 2.3 |
Phasing Power‡ | 1.62 | 2.54 | — |
Figure of merit | 0.49 for 23,123 phased reflections | ||
0.79 post-solvent flattening | |||
Refinement statistics (λ3 data set) | |||
No. of reflections (F/σ(F) ≥ 2.0) | |||
Working | 25,681 | ||
Test | 1,343 | ||
R (Rfree)§ | 22.1% (27.5%) | ||
No. of protein atoms | 3,666 | ||
No. of waters | 204 | ||
〈B-factor〉, Å2 | |||
Monomer A | 55.0 | ||
Monomer B | 54.1 | ||
Water | 57.1 | ||
r.m.s.d. from ideality | |||
Bond lengths, Å3 | 0.0118 | ||
Angles, deg | 1.62 |
Values in parentheses refer to statistics for data in the 2.38–2.30 Å resolution shell.
Rsym = ∑|I − 〈I〉|/∑〈I〉.
Phasing power: FHC/E for the isomorphous case and 2FHC"/E for the anomalous case, where FHC is the calculated heavy atom structure factor and E is the rms lack of closure.
R = ∑|FO − FC|∑FO; Rfree computed using randomly selected 5% of the data that were excluded throughout the refinement.