Skip to main content
. Author manuscript; available in PMC: 2013 Jun 24.
Published in final edited form as: Structure. 2004 Oct;12(10):1901–1907. doi: 10.1016/j.str.2004.08.003

Table 1.

Data Collection and Refinement Statistics

Data Collection Statistics
Peak (λ = 1.2831 Å) Inflection Point (λ = 1.2837 Å)
Space group and unit cell (Å) P3121a = b = 115.3 c = 106.4
Resolution (Å)a 50.0–1.97 (2.05–1.97) 30.0–1.97 (2.05–1.97)
Total reflections 460,699 543,743
Unique reflections 124,827 (12,464) 124,854 (12,466)
Redundancy 3.7 (3.7) 4.4 (4.3)
Completeness (%)a 100 (100) 100 (100)
Rsyma,b (%) 5.0 (51.2) 4.2 (35.2)
I/σ (I)a,b 24.57 (2.64) 34.7 (4.1)

Phasing Statistics
Resolution (Å) 50.0–2.50
Anomalous phasing power acentricc 0.34
Anomalous Rcullisd 0.81
Figure of merit 0.28

Refinement Statistics
Resolution (Å) 20.0–1.97
Reflections (working) 56,615
Reflections (test) 1,186
Rwork (%)e 19.7
Rfree (%)e 22.4
Number of protein atoms 4,382
Number of waters 277
Number of acetate ions 6
Number of Zn ions 2
Rms deviations
 Bond lengths (Å) 0.025
 Bond angles (°) 1.849
Average B factor (Å2)
 Main chain 36.0
 Side chain 40.6
 Waters 39.2
a

Values in parentheses correspond to the last shell.

b

Rsym = Σ|Ii − <I>|/ΣI, where Ii is the intensity of the i-th observation, and <I> is the mean intensity of the reflections. The values are for unmerged Friedel pairs.

c

Phasing power = rms (|Fh|/E), where |Fh| is the heavy atom structure factor amplitude, and E is residual lack of closure error.

d

Rcullis = Σ||Fh.obs| − |Fh.calc||/Σ|Fh| for acentric reflections, where |Fh.obs| is the observed heavy atom structure factor amplitude, and |Fh.calc| is the calculated heavy atom structure factor amplitude.

e

Rwork = Σ||Fobs| − |Fcalc||/Σ|Fobs|, crystallographic R factor, and Rfree = Σ||Fobs| − |Fcalc||/Σ|Fobs|, where all reflections belong to a test set of randomly selected data.