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. 2003 Jun 13;100(13):7889–7894. doi: 10.1073/pnas.1330742100

Table 1. Crystallographic data.

Crystal λ, Å Resolution, Å II* Rm, % Multiplicity Completeness, %§ PhP
P. aeruginosa SulA, space group P212121, a = 79.7 Å, b = 91.7 Å, c = 92.3 Å
    OCMP 0.8638 3.5 12.9 (4.4) 0.095 (0.274) 3.9 99.8 (99.8) 1.3 1.4
    K2OsO4 0.8638 4.0 13.3 (4.4) 0.103 (0.217) 3.8 94.8 (94.8) 0.7 0.5
    KAu(CN)2 1.4880 3.5 12.7 (3.5) 0.076 (0.335) 4.0 99.9 (100.0) 0.5 0.2
    NATI 0.9330 2.9 14.0 (3.0) 0.075 (0.336) 3.1 95.9 (95.9)
P. aeruginosa SulA:P. aeruginosa FtsZ, space group C2, a = 78.0 Å, b = 54.0 Å, c = 250.7 Å, β = 101.1°
    PEAK 0.9793 3.9 18.2 (6.6) 0.064 (0.194) 10.8 (5.4) 96.4 (96.0)
    INFL 0.9797 3.9 17.2 (5.9) 0.065 (0.216) 10.4 (5.2) 96.5 (96.5)
    HREM 0.9393 3.9 18.7 (9.0) 0.068 (0.131) 10.6 (5.3) 96.4 (96.4)
P. aeruginosa SulAΔ35:P. aeruginosa FtsZ, space group P212121, a = 55.6 Å, b = 75.4 Å, c = 241.0 Å
    NATI 0.9393 2.1 11.4 (3.7) 0.096 (0.334) 3.8 99.7 (99.7)
*

Signal-to-noise ratio of merged intensities, in brackets for the highest-resolution shell

Rm: ΣhΣi|I(h, i) - I(h)|/ΣhΣiI (h, i), where I(h, i) are symmetry-related intensities, and I(h) is the mean intensity of the reflection with unique index h, in parentheses for the highest-resolution bin

Multiplicity for unique reflections, anomalous multiplicity in brackets

§

Completeness for unique reflections; anomalous completeness is identical, because inverse beam geometry was used, in parentheses for the highest-resolution bin. Correlation coefficients of anomalous differences at different wavelengths for the MAD experiment: PEAK vs. INFL, 0.47; PEAK vs. HREM, 0.57; INFL vs. HREM, 0.31

PhP, phasing power; acentric reflections for isomorphous and anomalous phasing, respectively. Figure of merit for all acentric reflections is 0.39