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. 2002 Feb 12;99(4):1836–1841. doi: 10.1073/pnas.042664399

Table 1.

Data collection and structure determination

Data set APSR-red APSR-sulfite APSR-phas* Thim1 Thim2 Thim3 Thim4
Wavelength 1.06 1.06 1.07 1.005 1.009 1.733 1.740
Resolution, Å 1.6 2.5 2.5 2.6 2.5 2.7 2.6
Completeness, % 92.6 79.2 96.5 91.1 90.7 95.3 88.9
Multiplicity 3.3 2.6 3.1 5.9 6.1 6.2 6.0
Rsym, % 6.3 8.0 3.2 4.6 4.8 6.2 5.2
Phasing power§ −/− 0.3/0.3 2.1/3.2 1.5/2.4
(centrics/acentrics) [ano] −/2.2 −/2.2 −/2.7 −/2.4
Rcullis, % −/− 0.6/0.6 0.4/0.3 0.5/0.4
(centrics/acentrics) [ano] −/0.7 −/0.7 −/0.6 −/0.7
Rcryst, % 17.6 16.0
Rfree, %** 19.8 19.9
rms deviation bond length, Å 0.010 0.008
rms deviation bond angles, Å 1.4 1.5
*

APSR-phas, native data set used for phase determination. 

Thim, thimerosal, 0.5 mM, 24 h. The cryobuffer was used for heavy-atom soaking experiments. 

Rsym = ∑hkli|Ii − 〈I〉|/∑〈I〉. Ii, intensity of the ith measurement per reflection hkl; 〈I〉, average intensity for a reflection. 

§

Phasing power = rms. F(H)/E, F(H) is the heavy-atom structure factor amplitudes, and E is the lack of closure error. 

Rcullis = ∑hkl(|FPH(obs)| − |FPH(calc)|)/∑hkl(|FPH(obs)| − |FP(obs)|). 

Rcryst = ∑hkl(|F(obs)| − |F(calc)|)/∑hkl|F(obs)|. 

**

Rfree = ∑hkl(|F(obs)| − |F(calc)|)/∑hkl|F(obs)|, where 5% of the observed structure factor amplitudes are not used for refinement.