X-ray crystal structure analysis
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10 We are aware that the application of 3 times the esd values, taking
the deviation as positive for one atom and as negative for the other,
makes these differences in distance, strictly speaking, non-significant.
In terms of probability, what the esd values indicate is that we do not
have the certainty that the distances are unequal. However, in favor of
considering them probably different it can be argued that, from another
point of view, these esd values also indicate a high probability (perhaps
more than 70%) that these distances are really different and in the
short/long order indicated by the experimental values. For this reason,
in the text we refer to these distances as “apparently” different and
the effects observed are only suggested to be influenced in part by this
difference in distance, assuming that it is real.
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Single crystals of 3, 5·CH2Cl2, 7 and 8 suitable for X-ray
diffraction studies were obtained from slow diffusion of Et2O into
a dichloromethane solution of the products at -20 ◦C. Crystals
were mounted in glass fibers, and diffraction measurements were
made using a Bruker SMART CCD and Varian Supernova area-
16
˚
detector diffractometers with Mo-Ka radiation (l = 0.71073 A).
Intensities were integ◦rated from several series of exposures, each
exposure covering 0.3 in w, the total data set being a hemisphere.17
Absorption corrections were applied, based on multiple and
symmetry-equivalent measurements.18 The structures were solved
by direct methods and refined by least squares on weighted F2
values for all reflections (see Table 3).19 All non-hydrogen atoms
were assigned anisotropic displacement parameters and refined
without positional constraints. All the hydrogen atoms, including
those involved in hydrogen bonding, were calculated with a riding
model. Complex neutral-atom scattering factors were used.20 In
the structure of compound 5 the methyl groups of the PMe3
ligand were affected by incipient disorder, which despite repeated
attempts could not be successfully modeled. Crystallographic data
(excluding structure factors) for the structures reported in this
paper have CCDC reference numbers 818347 for 3, 818344 for 5,
818347 for 7, and 818350 for 8.
Acknowledgements
We thank the Spanish Comisio´n Interministerial de Ciencia y Tec-
nolog´ıa (CTQ2008-03954/BQU, INTECAT Consolider Ingenio
2010 (CSD2006-0003), and the Junta de Castilla y Leo´n (Project
VA248A11-2) for financial support.
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