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. 2017 Sep 11;7:11184. doi: 10.1038/s41598-017-11474-9

Table 1.

Data collection, MAD phasing, and refinement statistics.

Native Se-Met (Hsp104MMM)
Data Collection Statistics
Space group P 6522 P 6522
Unit Cell a = 179.1 Å, b = 179.1 Å, c = 69.7 Å a = 179.5 Å, b = 179.5 Å, c = 69.1 Å
α = 90°, β = 90°, γ = 120° α = 90°, β = 90°, γ = 120°
Source NSLS-X25 NSLS-X25
Wavelength (Å) λ = 1.10 λ1 = 0.9789 λ2 = 0.9792 λ3 = 1.0024
Resolution (Å) 41.53–2.82 44.8–3.5 44.8–3.5 44.8–3.8
Completeness (%)a 84.2 (12.7) 99.8 (100) 99.8 (99.5) 99.9 (99.9)
Redundancy 14.7 (1.7) 6.9 (6.8) 6.9 (6.5) 6.7 (6.9)
Rsym a,b 0.076 (0.386) 0.086 (0.393) 0.091 (0.497) 0.088 (0.320)
I/σc 17.6 12.9 11.1 10.7
MAD Phasing Statistics
Riso d 0.222 0.044 0.053
RCullis e 0.62 0.72
Phasing Powerf 2.38 2.07 1.16
Figure of Meritg 0.63 (centric) 0.60 (acentric)
Refinement Statistics
Resolution (Å) 41.53–2.82
No. reflections 14036
Rcryst/Rfree 0.210/0.279
No. atoms 2725
Protein 2721
Water 4
B-factors 94.1
Protein 94.1
Water 74.3
rmsd bond (Å) 0.002
rmsd angle (°) 0.399
Ramachandran
Favored (%) 97.1
Outliers (%) 0.0

aValues for the highest resolution shell are given in parentheses. bRsym = Σhkl|I(hkl) − < I(hkl) > |/ΣhklI(hkl), where <I(hkl)> is the mean of the symmetry equivalent reflections of I(hkl). cBased on unmerged data. dRiso = Σ|FPH − FP|/ΣFp, where Fp is the peak (λ1), and FPH are the inflection (λ2), low energy remote (λ3) or native structure factor amplitudes. eRCullis = Σ||FPH ± FP| − FH calc|/Σ|FPH ± FP| for centric reflections only. fIsomorphous phasing power = Σ|FH|/Σ||FPH obs| − |FPH calc||; anomalous phasing power = Σ|F″H|/Σ||ADobs| − |ADcalc||. gFigure of Merit = weighted mean of the cosine of the deviation from αbest.