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. 2010 Feb 10;152(4):1842–1850. doi: 10.1104/pp.109.150680

Table I. Data collection and phasing statistics.

All the datasets were collected at 120 K on Rigaku RU-H3R rotating anode generator using MAR345dtb detector. Phases were determined using MIR. Data in parentheses are for highest resolution bin.

Dataset Native HgCN Pb(CH3COO)2 CdCl2
Space group P212121 P212121 P212121 P212121
Unit cell dimensions (Å; a, b, c) 83.2, 88.1, 154.5 83.4, 89.0, 154.1 83.4, 85.9, 154.1 82.8, 87.4, 154.0
Resolution (Å) 50–2.2 (2.32–2.2) 50-2.8 (2.882.8) 50–2.5 (2.59–2.5) 50–2.5 (2.61–2.5)
Observed reflections 185,883 (26,826) 101,610 (9,155) 124,744 (11,542) 182,495 (17,141)
Unique reflections 54,633 (8,105) 28,804 (2,543) 38,827 (3,607) 37,629 (3,586)
Rmerge (%)a 12.9 (49.1) 13.4 (32.22) 13.7 (40.6) 8.7 (25.9)
Completion (%) 93.9 (96.5) 97.3 (88.0) 99.0 (93.8) 97.1 (94.6)
Multiplicity 3.4 (3.3) 3.5 (3.6) 3.2 (3.2) 4.79 (4.78)
I/σ 5.2 (1.9) 3.0 (1.5) 2.8 (1.2) 3.7 (1.8)
MIR statistics
    Riso (%)b 20.6 17.1 11.9
    Phasing powerc; centric (acentric) 0.87 (1.11) 0.51 (0.61) 0.24 (0.25)
    Rcullis (%)d 0.66 0.71 0.83
    No. of sites 5 4 1
    Figure of merit/Z score 0.40/22.2
a

Rmerge = Σ[I − (I)]/Σ(I), where I is the integrated intensity of a given reflection.

b

Riso = Σ|FPHFP|/ΣFP, where FPH and FP are derivative and native structure factor amplitudes, respectively.

c

Phasing power = <r.m.s. heavy atom structure factor>/<r.m.s. lack of closure>.

d

Rcullis = Σ‖FPH ± FP| − FH|/Σ|FPHFP| for centric reflections.