Table 1.
Two-sided plane group | Phase residual (degrees)a | Number of comparisons | Target residual (degrees)b |
---|---|---|---|
p1 | 27.8c | 434 | |
p2 | 40.8d | 217 | 40.8 |
p12_b | 73.7 | 113 | 29.3 |
p12_a | 74.0 | 111 | 29.0 |
p121_b | 76.6 | 113 | 29.3 |
p121_a | 72.4 | 111 | 29.0 |
c12_b | 73.7 | 113 | 29.3 |
c12_a | 74.0 | 111 | 29.0 |
p222 | 59.0 | 441 | 34.2 |
p2221_b | 58.4 | 441 | 34.2 |
p2221_a | 62.2 | 441 | 34.2 |
p22121 | 69.3 | 441 | 34.2 |
c222 | 59.0 | 441 | 34.2 |
p4 | 30.0d | 525 | 33.2 |
p422 | 51.3 | 998 | 30.6 |
p4212 | 61.6 | 998 | 30.6 |
Internal phase residuals were determined using the program ALLSPACE (Valpuesta et al., 1994) from spots of IQ1 to IQ5 to 7 Å resolution. Only plane groups compatible with the sbpA lattice are shown.
Phase residual versus other spots (90° random).
Target residual based on statistics taking Friedel weight into account.
Note that in space group p1 no phase comparison is possible, so the numbers given here are theoretical phase residuals based on the signal-to-noise ratio of the observed diffraction spots.
Within 20% of target residual.