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. 2016 Jan 22;72(Pt 2):139–144. doi: 10.1107/S2053230X16000212

Table 3. Data collection and processing.

Values in parentheses are for the outermost shell.

  State III State IV
Diffraction source Rigaku MICROSTAR copper rotating-anode generator Rigaku MICROSTAR copper rotating-anode generator
Wavelength (Å) 1.5418 1.5418
Temperature (K) 100 100
Detector Rigaku R-AXIS IV++ image plate Rigaku R-AXIS IV++ image plate
Crystal-to-detector distance (mm) 200 200
Rotation range per image (°) 1 1
Total rotation range (°) 180 180
Exposure time per image (s) 300 300
Space group P21 P21
a, b, c (Å) 31.61, 120.21, 61.26 30.81, 111.16, 62.74
α, β, γ (°) 90, 102.92, 90 90, 103.07, 90
Mosaicity (°) 1.06 1.84
Resolution range (Å) 59.71–3.00 (3.16–3.00) 55.58–2.60 (2.74–2.60)
Total No. of reflections 28708 (3610) 32753 (4559)
No. of unique reflections 8613 (1168) 9779 (1328)
Completeness (%) 96.1 (88.9) 77.8 (73.2)
Multiplicity 3.3 (3.1) 3.3 (3.4)
I/σ(I)〉 10.3 (2.5) 11.9 (2.5)
R r.i.m. 0.066 (0.532) 0.061 (0.451)
Overall B factor from Wilson plot (Å2) 85.1 60.5

The state IV crystal was anisotropic, resulting in the low completeness of the diffraction data. Although we tried many crystals, it was difficult to collect a data set with higher completeness.