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. 1999 Oct 26;96(22):12379–12383. doi: 10.1073/pnas.96.22.12379

Table 1.

Data collection and refinement statistics for cowpox vCCI

I II III
Data collection
 Diffraction data Native 1 Native 2 Gd3+ SeMet SeMet + Gd3+
 Space group C2221 C2221 C2221 C2221 C2221
 Resolution, Å 2.82 1.85 3.60 3.40 3.40
 Total observations 54,518 176,998 23,305 31,592 53,803
 Unique reflections 11,986 46,769 5,037 7,094 7,098
 Completeness, % 97.7  (98.5) 87.7  (66.6) 80.9  (85.9) 99.1  (95.4) 99.0  (98.3)
Rsym, % 9.2  (23.1) 6.5  (15.0) 6.2  (7.0) 74  (11.1) 7.6  (11.4)
Rderiv, % 14.9  (14.8) 11.7  (18.0) 17.4  (20.2)
 Phasing power 1.48  (0.98) 1.23  (0.78) 1.57  (1.08)
 Figure of merit 0.62  (a) 0.74  (c)
Refinement statistics
 Resolution range, Å 20–1.85
 No. reflections in working set 45,823
Rcryst 0.212
Rfree 0.244
 rms deviation from ideal geometry
  Bond length, Å 0.007
  Bond angles, ° 1.43
Average B factors
 Protein atoms, Å2 26.7
 Solvent molecules, Å2 39.2
 Anisotropic B factor, Å2 B11 = 2.291, B22 = −5.156, B33 = 2.86
 Bulk solvent correction B = −3.603 Å2k = 0.38 e/Å3

Rsym = ΣhΣi|Ii(h) − 〈I(h〉)|ΣhΣiIi(h), where Ii(h) is the ith measurement and 〈I(h)〉 is the weighted mean of all measurements of I(h). Rderiv = Σh| |Fderiv(h)| − |Fnative1(h)| |/Σh|Fnative1(h)|. Phasing power = 〈|FH|〉/E, where 〈|FH|〉 is the structure factor amplitude for the heavy atom and E is the estimated lack-of-closure error. Rcryst and Rfree = Σh| |F(h)obs| − |F(h)calc| |/Σh|F(h)obs| for reflections in the working and test sets, respectively. Numbers in parentheses are for final shell.