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. 2000 Mar 1;19(5):831–842. doi: 10.1093/emboj/19.5.831

Table III. Data collection and phasing statistics.

  Native Erλ1 Erλ2 Erλ3 A221V
Data collectiona          
Space group C2221   C2221   P21
Cell constants (Å) a = 60.6   a = 56.8   a = 58.2
  b = 107.5   b = 106.5   b = 255.7 β = 118.2°
  c = 256.6   c = 256.6   c = 60.4
Resolution range (Å) 30.0–2.50   30.0–2.50   30.0–2.04
Wavelength (Å) 1.5418 1.4834 1.4840 1.1000 1.1000
Observed reflections 94 388 189 030 95 680 87 407 187 495
Unique reflections 24 839 25 204 23 902 22 321 96 350
Whole range          
 completeness (%) 94.9 96.3 91.3 85.3 99.4
Rmergeb 8.3 5.2 4.4 4.3 4.0
Iσ(I) 11.4 28.7 21.1 27.9 20.8
Last shell          
 resolution range (Å) 2.55–2.5 2.55–2.5 2.55–2.5 2.55–2.5 2.07–2.04
 completeness (%) 88.7 92.4 90.5 83.3 99.2
Rmerge 30.3 25.7 22.3 22.0 26.9
Iσ(I) 3.3 7.1 5.0 7.3 4.3
Phasing (15.0–2.5Å)          
 phasing power (iso)   0.80 0.87  
 phasing power (ano)   0.98 0.90 0.66  
Rcullis (iso)c   0.87 0.80  
Rcullis (ano)   0.74 0.80 0.81  
Figure of merit (before/after solvent flattening) 0.444/0.786        

aThe data for the native crystals were obtained at 298 K in-house, while those for the heavy atom derivatives and A221V mutant form were cryo collected (100 K) at BW6, DESY, Hamburg, Germany.

bRmerge = Σ∣I – <I>∣/ΣI.

cRcullis = <phase integrated lack of closure>/∣FPHFP