Table 1.
Native | White line, λ1 | Inflection point, λ2 | Remote, λ3 | |
---|---|---|---|---|
Data collection | ||||
Wavelength, Å | 0.87 | 0.9790 | 0.9792 | 0.935 |
Resolution, Å | 15–1.9 | 20–2.3 | 20–2.3 | 20–2.3 |
Unique reflections | 19,245 | 10,977 | 10,990 | 11,006 |
Multiplicity, % | 4.7 | 4.2 | 3.9 | 4.0 |
Completeness, %* | 96.9 (98.2) | 99.2 (98.5) | 99.3 (99.3) | 99.6 (99.6) |
Rmerge, %*† | 5.4 (22.6) | 4.1 (17.8) | 3.9 (20.0) | 4.2 (25.6) |
Intensity/σ* | 8.1 (2.9) | 12.1 (3.9) | 13 (3.5) | 10.3 (2.7) |
Phasing, 10–2.5 Å | ||||
RCullis, centric/acentric‡ | 0.80/0.79 | 0.62/0.67 | ||
RCullis, anomalous§ | 0.49 | 0.61 | 0.68 | |
Phasing power, centric/acentric¶ | 0.78/1.12 | 1.18/1.71 | ||
Mean figure of merit | 0.69 | |||
Refinement, 15–1.9 Å | ||||
R factor, %‖ | 21.7 | |||
Rfree, %‖ | 27.1 | |||
rmsd bond lengths, Å | 0.009 | |||
rmsd bond angles, ° | 1.363 | |||
rmsd B factors, Å2 | 1.901 |
Values in parentheses refer to the highest resolution bin.
Rmerge = ΣhΣi|Ii(h) − 〈I(h)〉|/ΣhΣiIi(h), where Ii(h) is the ith measurement of reflection h and 〈I(h)〉 is the weighted mean of all measurements of I(h).
RCullis is defined as the isomorphous lack-of-closure over the isomorphous difference.
RCullis (anomalous) is calculated as the anomalous lack-of-closure over the anomalous difference.
The phasing power is defined as (rms Fh/rms lack-of-closure) summed over all reflections used in the heavy atom refinement.
R factor = Σh|Fobs − Fcalc|/ΣhFobs, where Fobs and Fcalc are the observed and calculated structure factors.