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. 2002 Mar;11(3):467–478. doi: 10.1110/ps.33002

Table 1.

Data collection and MIR analysis

Data set Maximum resolution Measured reflections Unique reflections Rmergea,b (%) Completeness (%) Number of sites Rderivc (%) Rcullisd (%) Phasing powere Used resolution
PCMBSf 2.80 36749 14245 4.5 (6.8) 72 (48) 2 22.4 0.83 1.09 25–3.0
EMPh 2.80 75904 18955 6.0 (8.1) 96 (91) 2 24.3 0.79 1.22 25–3.0
UO3Ac2 • 2H2O 3.00 55982 14633 6.3 (9.5) 91 (86) 2 22.9 0.72 1.77 25–3.0
PIPg 2.80 51718 15007 6.6 (13.6) 76 (54) 2 23.8 0.71 1.75 25–3.0
K2PtCl4 2.80 19944 12951 5.1 (9.0) 64 (40) 2 17.7 0.88 0.85 25–3.0
K[Au(II)(CN)2] 2.80 31518 15553 4.5 (6.4) 79 (60) 2 25.8 0.92 0.68 25–3.0
PdCl2 2.80 27849 16425 3.8 (5.5) 83 (62) 2 16.4 0.94 0.56 25–3.0
DFP-derivative 1.80 235197 69158 2.4 (10.8) 94 (97) 15–1.8
Native 1.80 188976 49177 5.3 (13.8) 68 (27) 20–2.0

a Numbers in parentheses in the columns for Rmerge and Completeness correspond to data from the highest resolution shell.

bRmerge = ∑|IiIm/∑|m where Ii and Im are the observed intensity and mean intensity of related reflections respectively.

cRderiv = ∑|FPHFP|/∑|FP|, where FPH is the structure–factor amplitude of the derivative crystal and FP is that of the native crystal.

dRcullis = ∑||FPH ± FP| − |FH(calc)||/∑|FPHFP|, where FPH and FP are defined as above and FH(calc) is the calculated heavy atom structure–factor amplitude.

e Phasing power = FH/E, the root mean square (rms) heavy-atom structure–factor amplitude divided by the lack of closure.

f PCMBS = p-chlormercuriphenylsulfonic acid monosodium salt.

g PIP = Di-μ-iodobis(ethylenediamine)-di-platinum (II) nitrate.

h EMP = ethylene mercury phsophate.