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scaled with SCALEPACK. Several scans in w and v directions
were made to increase the number of redundant reflections,
which were averaged in the refinement cycles. This procedure
replaces in a good approximation an empirical absorption
correction. The structures were solved with direct methods
(SHELXS86) and refined against F2 (SHELX97). All non-
hydrogen atoms were refined with anisotropic displacement
parameters, except three carbon atoms of (4PzNN)2Ni(hfac)2.
Hydrogen atoms attached to carbon atoms were calculated
and refined with isotropic displacement parameters 1.2 or 1.5
times higher than the value of their carbon atoms. Hydrogen
atoms attached to nitrogen were found and refined isotropi-
cally, except for (4PzNN)2Ni(hfac)2, where all hydrogen atoms
were calculated. The solvent CHCl3 of (4PzNN)2Ni(hfac)2
lies near a symmetry centre and is disordered with partial
overlying positions. The fluorine atoms of two CF3 groups in
4PzNN?Co(hfac)2 have a 2 : 1 positional disorder.
The quality of the data set of (4PzNN)2Ni(hfac)2 is reduced
by the small crystal size with low diffraction and visible
intensities on the frames below 2H 34u.
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Acknowledgements
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We warmly thank Carlos Go´mez (Universitat de Vale`ncia) for
the magnetic susceptibility data and Daniel Ruiz-Molina
(ICMAB-CSIC) for help with its interpretation. This work
was supported by grants from the Programa Nacional de
Materiales of the DGI (Spain, MAT2003-04699), the EU
Marie Curie RTN QuEMolNa (MRTN-CT-2003-504880),
and the NoE MAGMANet (515767-2). We also thank referees
for constructive and helpful comments.
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2744 | J. Mater. Chem., 2006, 16, 2736–2745
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