(l = 0.71073 A). Raw frame data were integrated with SAINT
program.34a Semi-empirical absorption correction with
SADABS34b was applied. The structure was solved by direct
methods employing SHELXS-97 program34c and expanded
using Fourier techniques. All non-H atoms were refined
anisotropically. All of the C-bound H atoms were observable
from a difference Fourier map but were all placed at
geometrical positions with C–H = 0.93, 0.96, 0.97 A for
phenyl, methyl and methylene H-atoms. The positions of H
atoms were calculated based on riding mode with Uiso(H) =
1.2Ueq(Carrier). Details of the restraints used in the refinement
can be found in the ESI.w CCDC reference numbers 814059
(for 6) and 814060 (for 3).
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Acknowledgements
V. W.-W. Y. acknowledges the support from The University
of Hong Kong under the Distinguished Research Achievement
Award Scheme and the URC Strategic Research Theme on
Molecular Materials. This work has been supported by the
University Grants Committee Areas of Excellence Scheme
(AoE/P-03/08). G. D. acknowledges the receipt of a post-
graduate studentship, administrated by The University of
Hong Kong. We are grateful to Dr L. Szeto for her assistance
in X-ray crystal structure data collection and determination.
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