F. Basuli et al. / Journal of Organometallic Chemistry 696 (2011) 235e243
243
structure was solved using SHELXS-97 and refined with SHELXL-97.
Acknowledgements
A direct-method solution was calculated which provided most non-
hydrogen atoms from the E-map. Full-matrix least squares/differ-
ence Fourier cycles were performed which located the remaining
non-hydrogen atoms. The structure was found as proposed with
two independent molecules per asymmetric unit. All non-hydrogen
atoms were refined with anisotropic displacement parameters. All
hydrogen atoms were placed in ideal positions and refined as riding
atoms with relative isotropic displacement parameters.
GOF ¼ 0.756 and the final refinement converged at R(F) ¼ 0.0447
(observed data) and wR(F2) ¼ 0.0848 (refinement data).
We thank Dr. Aneetha Halikhedkar for insightful discussions and
Indiana University-Bloomington, and the Chemical Sciences, Geo-
sciences and Biosciences Division, Office of Basic Energy Science, Office
of Science, U.S. Department of Energy (No. DE-FG02-07ER15893) for
financial support of this research.
Appendix A. Supplementary material
CCDC 786995e787001 contain the supplementary crystallo-
graphic data for this paper. These data can be obtained free of
charge from The Cambridge Crystallographic Data Center via www.
Single crystals of 6 were grown from a fluorobenzene/hexane-
layered solution at room temperature under an N2 atmosphere. Crystal
data for C50H46BF20N3Ti, 6: M ¼ 1127.61, Monoclinic, space group P2
(1)/n, a ¼ 17.654(2) Å, b ¼ 13.7175(17) Å, c ¼ 21.887(3) Å,
a
¼
g
¼ 90ꢀ,
b
¼ 109.354(3)ꢀ, U ¼ 5000.9(11) Å, Z ¼ 4, Dc ¼ 1.498 g cmꢁ3
, l
References
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a
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reflections 6443 (Rint ¼ 0.0682). The structure was solved using
SHELXS-97 and refined with SHELXL-97. A direct-method solutionwas
calculated which provided most non-hydrogen atoms from the E-map.
Full-matrix least squares/difference Fourier cycles were performed
which located the remaining non-hydrogen atoms. All non-hydrogen
atoms were refined with anisotropic displacement parameters. All
hydrogen atoms were placed in ideal positions and refined as riding
atoms with relative isotropic displacement parameters. GOF ¼ 0.825
and the final refinement converged at R(F) ¼ 0.0351 (observed data)
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(F) ¼ 0.0653 (observed data) and wR(F2) ¼ 0.2124 (refinement data).
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refined with anisotropic displacement parameters. All hydrogen
atoms were placed in ideal positions and refined as riding atoms
with relative isotropic displacement parameters. GOF ¼ 0.966 and
the final refinement converged at R(F) ¼ 0.0447 (observed data)
and wR(F2) ¼ 0.1286 (refinement data).
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