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. 2010 May 15;66(Pt 6):741–744. doi: 10.1107/S0907444910012436

Table 2. Summary scaling statistics for three data sets, comparing the conventional approach of background rejection with the new approach of ice-ring subtraction.

The first two data sets were collected from C222 crystals of human acidic fibroblast growth factor mutants (Lee et al., 2008). ‘FGF-d’ was used for the structure determination of mutant L26N/D28A (PDB code 3ba7). ‘FGF-e’ was an ice-affected data set for mutant K112N/N114A that was replaced prior to structure determination (PDB code 3bag). ‘Sxa63’ is a data set from a P222 crystal of the Pyrococcus furiosus box C/D ribonucleoprotein particle that was also replaced prior to structure determination (Li et al., submitted work). Resolution shells affected by ice rings where the new procedure improves the completeness are shown in bold.

FGF-d FGF-e Sxa63
  Background rejection Ice-ring subtraction   Background rejection Ice-ring subtraction   Background rejection Ice-ring subtraction
Resolution (Å) Rmerge Completeness (%) Rmerge Completeness (%) Resolution (Å) Rmerge Completeness (%) Rmerge Completeness (%) Resolution (Å) Rmerge Completeness (%) Rmerge Completeness (%)
∞–4.00 0.049 94 0.050 95 ∞–5.12 0.048 100 0.047 100 ∞–6.79 0.070 100 0.076 100
4.00–3.18 0.075 70 0.071 99 5.12–4.08 0.062 100 0.062 100 6.79–5.42 0.088 100 0.088 100
3.18–2.78 0.083 96 0.083 97 4.08–3.57 0.117 37 0.147 98 5.42–4.75 0.097 100 0.099 100
2.78–2.52 0.091 87 0.091 87 3.57–3.24 0.130 65 0.125 100 4.75–4.32 0.102 100 0.102 100
2.52–2.34 0.096 76 0.097 76 3.24–3.01 0.143 99 0.120 98 4.32–4.01 0.111 100 0.116 100
2.34–2.20 0.128 51 0.142 76 3.01–2.83 0.171 95 0.135 95 4.01–3.78 0.170 72 0.165 100
2.20–2.09 0.120 74 0.113 76 2.83–2.69 0.201 92 0.153 92 3.78–3.59 0.404 47 0.346 100
2.09–2.00 0.159 77 0.159 77 2.69–2.57 0.277 92 0.214 91 3.59–3.43 0.233 100 0.229 100
2.00–1.93 0.190 77 0.174 78 2.57–2.48 0.274 91 0.205 90 3.43–3.30 0.243 100 0.258 100
1.93–1.86 0.204 69 0.226 78 2.48–2.39 0.325 89 0.233 89 3.30–3.19 0.273 100 0.327 100
1.86–1.80 0.244 77 0.236 77 2.39–2.32 0.418 89 0.244 88 3.19–3.09 0.339 100 0.398 100
1.80–1.75 0.280 77 0.283 77 2.32–2.25 0.595 33 0.645 87 3.09–3.00 0.387 100 0.439 99
∞–1.75 0.081 77 0.081 83 ∞–2.25 0.124 82 0.122 94 ∞–3.00 0.119 93 0.125 100