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. 2016 Feb 4;61(3):434–448. doi: 10.1016/j.molcel.2015.12.017

Table 1.

The Statistics of Structures

Crystals BRCT-Ab1p_short BRCT-Ab2p
X-ray source Diamond Light Source Beamline I03 Diamond Light Source Beamline I04-1
Wavelength (Å) 0.9793 0.9200
Space group P3221 P212121
Cell dimensions a, b, c (Å) and α, β, γ (°) 63.8, 63.8, 93.4, 90, 90, and 120 86.8, 183.7, 190.5, 90, 90, and 90
Resolution (Å) 47.6-2.5 95.3-3.5
Rsyma 0.051 (0.498)b 0.096 (0.701)
I / σ 24 (5.1) 16.4 (2.6)
Wilson B factor 58.6 97.2
Completeness (%) 99.9 (99.8) 99.8 (98.8)
Redundancy 9.3 (9.4) 7.4 (7.8)
Refinement
Resolution (Å) 47.6-2.5 (2.6-2.5) 95.3-3.5 (3.7-3.5)
No. unique reflections 8,000 39,170
Rcrystc 0.215 (0.356) 0.235 (0.319)
Rfreed 0.252 (0.374) 0.298 (0.341)
No. protein atoms 1,701 14,092
No. copy number of complex in ASU 1 8
Ramachandran favored (%) 97.7 97.1
Average B-factor (Å2) 66.68 114.6
Rmsds
Bond lengths (Å) 0.007 0.007
Bond angles (°) 0.823 0.900
a

Rsym = Σh|Ih − < I > |/ΣhIh, where Ih is the intensity of reflection h and < I > is the mean intensity of all symmetry-related reflections.

b

The statistics in parenthesis are for the highest resolution shell.

c

Rcryst = Σ||Fobs|−|Fcalc||/Σ|Fobs|, Fobs and Fcalc are observed and calculated structure factor amplitudes.

d

Rfree as for Rcryst using a random subset of the data (about 10% for BRCT-Ab1p_short and 5% for BRCT-Ab2p) excluded from the refinement.