Table 1.
Data collection | ||||
Data set | Parent | Mersalyl | Me3PbAC | EtHgCl |
X-ray source | NSLS X4a | Laboratory | CHESS-A1 | CHESS-A1 |
Wavelength | 1.0397 Å | 1.54 Å | 0.91 Å | 0.91 Å |
Resolution | 50-2.8 Å | 40-3.5 Å | 40-3.0 Å | 40-4.0 Å |
Unique refl | 33,401 | 8,827 | 14,560 | 6,029 |
Completeness | 99.1% | 97.9% | 99.3% | 97.1% |
Rsym | 6.8% | 10.5% | 7% | 6.1% |
Reagent conc.* | 1 mM | 2.5 mM | 1 mM | |
Soaking time* | 6 h | 6 h | 5 h | |
Number of sites | 4 | 8 | 7 | 8 |
Phasing power† | 1.45 | 1.11 | 1.1 | |
Anomalous phasing power† | 0.5 | |||
Mean f.o.m. 0.45 acentric/0.59 centric | ||||
Refinement 50-2.8 Å (2σ data) | ||||
Working R factor: 22.3% Free R factor: 27.4% | ||||
Rms deviations Bond lengths 0.014 Å Bond angles 1.68° |
Rsym = Σ|Ih− 〈Ih〉|/Σ Ih, where 〈Ih〉 is the average intensity over Friedel and symmetry equivalents. Phasing power = Σ|FH|/Σ∥FPHobs |−|FPHcalc∥. Anomalous phasing power Σ|FH|/Σ∥ADobs|−|ADcalc ∥, where AD is the Bijvoet difference. NSLS is the National Synchrotron Light Source at Brookhaven National Laboratory, and CHESS is the Cornell High Energy Synchrotron Source.
See the Materials and Methods section for full details.
Acentric.