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. 2018 Jul 20;293(38):14926–14936. doi: 10.1074/jbc.RA118.002560

Table 1.

Data collection and refinement statistics

PvdPapo PvdPTyr PvdPSeMet
Data collection statistics
    Beamline PETRAIII P11 BESSYII 14.2 SLS X06DA/PETRAIII P11
    No. of crystals 1 1 3
    Wavelength (Å) 0.9794 1.282 0.9779/0.9794
    Space group P21 P21 P21
    Unit cell dimensions
        a, b, c (Å) 97.35, 107.79, 107.94 77.33, 109.14, 82.51 96.19, 108.41, 108.41
        α, β, γ (°) 90, 99.97, 90 90, 95.55, 90 90, 99.70, 90
    Resolution range (Å) (highest shell) 48.07–2.09 (2.26–2.09) 48.09–2.70 (3.03–2.70) 48.34–3.50 (3.70–3.50)
    Ellipsoidala resolution (Å) (direction)b 2.84 (0.988 a* − 0.152 c*) 3.73 (0.718 a* − 0.696 c*) n.a.c
2.19 (b*) 2.7 (b*) n.a.
2.09 (−0.032 a* + 0.999 c*) 2.93 (0.64 a* + 0.768 c*) n.a.
    Total no. of reflections (ellipsoidal)d 578,302 (27,712) 229,383 (8,710) 2,663,558 (404,486)
    No. of unique reflections (ellipsoidala)d 85,942 (4,285) 23,084 (1,154) 54,434 (8,374)
    Average multiplicityd 6.7 (6.5) 9.9 (7.5) 48.9 (48.3)
    Completenessd (%) 66.3 (16.0) 61.5 (10.5) 99.9 (100.0)
    Completeness (ellipsoidala)d,e (%) 93.2 (76.7) 92.1 (56.5) n.a.
    I/σ(I) (ellipsoidala)d 10.7 (1.6) 8.6 (1.6) 18.1 (10.6) (spherical)
    Rmeasd,f 0.13 (1.28) 0.32 (1.49) 0.27 (0.54)
    Rpimd,g 0.051 (0.50) 0.10 (0.54) NDh
    CC½i 0.99 (0.54) 0.99 (0.51) 0.99 (0.99)

Refinement statistics
    Resolution (Å) 45.61–2.09 48.09–2.70
    No. of reflections used 85,901 22,962
    Rworkj (%) 21.41 20.46
    Rfreek (%) 24.10 26.18
    No. of residues
        Protein 1,889 916
        Water 513 24
        Zn2+ 4
        l-Tyrosine 2
    Mean B-factorl2) 48 34
        All protein residues 48 34
        Ligands 36
        Water molecules 38 20
    r.m.s.d.
        Bond length (Å)m 0.002 0.002
        Bond angle (°)m 0.495 0.460
    Ramachandran plot (%)
        Favored regionsm 96.82 96.6
        Allowed regionsm 100 100
        Outliersm 0 0
    MolProbity scorem 1.00 0.95

PDB code 6EYS 6EYV

a Statistics refer to data truncated by STARANISO to remove weak reflections affected by anisotropy (46).

b The resolution limits for three directions in reciprocal space (a*, b*, c*) are indicated here. To accomplish this, STARANISO computed an ellipsoid postfitted by least squares to the cutoff surface, removing points where the fit was poor. Note that the cutoff surface is unlikely to be perfectly ellipsoidal, so this is only an estimate.

c n.a., not applicable.

d Values in parentheses are for the highest-resolution shell.

e The anisotropic completeness was obtained by least squares fitting an ellipsoid to the reciprocal lattice points at the cutoff surface defined by a local mean I/σ(I) threshold of 1.5, rejecting outliers in the fit due to spurious deviations (including any cusp) and calculating the fraction of observed data lying inside the ellipsoid so defined. Note that the cutoff surface is unlikely to be perfectly ellipsoidal, so this is only an estimate.

f Rmeas = Σhkl{N(hkl)/[N(hkl) − 1]}1/2 × Σi|Ii(hkl) − 〈I(hkl)〉|/ΣhklΣi Ii(hkl).

g Rpim = Σhkl{1/[N(hkl) − 1]}1/2 × Σi|Ii(hkl) − 〈I(hkl)〉|/ΣhklΣiIi(hkl).

h Not determined.

i CC1/2 = Σ(x − 〈x〉)(y − 〈x〉)/[Σ(x − 〈x〉)2Σ(y − 〈y〉)2]1/2.

j Rwork = (ΣhklFobs| − k|Fcalc‖)/(Σhkl|Fobs|).

k Rfree is the same as Rwork with 5% of reflections chosen at random and omitted from refinement.

l B-factors calculated with Moleman2 (55).

m Statistics calculated with the MolProbity web server (56) (http://molprobity.biochem.duke.edu/) (Please note that the JBC is not responsible for the long-term archiving and maintenance of this site or any other third party-hosted site.).