518
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cm23, Z 6, crystal size 0.3 £ 0.3 £ 0.01 mm, colour
colourless, habit plate, temperature 150(2) K, l(Mo Ka)
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0.71073 A, m(Mo Ka) 0.495 mm21, T(SADABS)min,max
˚
0.710509, 1.000000, 2umax 56.50, hkl range 225 25, 224
24, 241 48, N 110,846, Nind 19,480(Rmerge 0.0704), Nobs
12,009(I . 2s(I)), Nvar 736, residuals* R1(F) 0.0821,
wR2(F 2) 0.2431, GoF(all) 0.982, Drmin,max 21.166, 1.606
23
˚
A
e2
.
*R1 ¼ SkFoj–jFck/SjFoj for Fo . 2s(Fo); wR2 ¼
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(Sw(F2o –F2c)2/S(wFc2)2)1/2 all reflections w ¼ 1/[s 2(Fo2) þ
(0.1628P)2 þ 0.0000P] where P ¼ (Fo2 þ 2F2c)/3.
Specific refinement details
The S(3) arm of the ligand is disordered over two positions
with occupancies of 0.7 and 0.3, which were modelled with
equal anisotropic displacement parameters and a number of
bond length and angle restraints. Both the S(1) containing
arm and the triflate anion display a significant amount of
thermal motion and/or unresolved disorder. Accordingly,
both bond length and angle restraints along with thermal
parameter restraints were required. In addition to these
problems, there is a significant amount of unresolved
electron density present in the lattice. Despite numerous
attempts at modelling this disorder including the use of
rigid bodies, no satisfactory model could be found, and
accordingly, the SQUEEZE (27) function of PLATON (28)
was employed to remove the contributions of this
unresolved electron density from the model.
Acknowledgements
We thank the Australian Research Council for funding
(DP0555883) and Dr Nicholas Proschogo (The University of
Sydney) for assistance with mass spectral data.
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