74
J Chem Crystallogr (2008) 38:71–75
˚
environment, with the Cu(2) atom displaced 0.205(1) A
symmetry center in the middle of the Cu–Cu bond and,
consequently, both copper atoms are identical and the
asymmetric unit contains only two ligands. Our polymorph
is much more irregular, crystallized in the monoclinic
P21/c space group, and the asymmetric unit contains one
whole dimeric molecule. The Cu–Nthiazole bond lengths are
from the best plane defined by the Cu(2)N4 chromophore.
The torsion angles Namido–Cu–Cu–Nthiazole of 17.78(9)° are
higher than those previously published, as one would
expect for a more distorted structure.
˚
in the range 1.912(2)–1.964(2) A, and the Cu–Nsulfonamido
˚
bond lengths are in the range 1.932(2)–2.003(2) A, and a
Spectroscopic Properties
clear trend depending on the kinds of atoms involved in the
bond is not observed—in contrast to the previously pub-
lished compound. For the copper atom labeled as Cu(1) the
The IR spectrum of the complex does not contain the band
observed in the ligand at 3,136 cm-1, which is attributed to
m(N–H) stretching. This difference in the spectra indicates
that the ligand is in the anionic amidate form in the com-
plex. The spectrum also shows weak bands in the aromatic
˚
Cu–Nthiazole bond lengths are about 0.08 A shorter than the
Cu–Nsulfonamido bond lengths, but for the copper atom
labeled as Cu(2) the opposite trend is found. The cis bond
angles in both CuN4 chromophores are almost regular. The
trans bond angles range from 162.11(9)° to 173.69(9)°, i.e.
different to that found previously, with one trans angle
virtually linear (178°) and the other clearly bent (155.7°)
due the small bite of the bridging ligand. The distance
region and these are due to m(C=N) (1,608–1,587 cm-1
)
and m(C=C) (1,580–1,555 cm-1). These bands are shifted
to lower frequencies with respect to those in the free ligand
as a result of coordination through the sulfonamide nitro-
gen atom. The band at 1,322 cm-1, which is attributed to
mas(S=O), and band at 1,140 cm-1, attributed to the
˚
between the two Cu centers, Cu(1)–Cu(2), is 2.7859(5) A
and this is slightly longer than that found previously.
The two CuN4 planes are almost parallel, with a dihedral
angle between the two CuN4 mean planes of 0.4(1)°. The
planes are slightly distorted, with the Nsulfonamido atoms
˚
0.089(1) A above the theoretical best plane and the Nthiazole
˚
atoms 0.089(1) A below it. The Cu(1) atom is displaced
msym(S=O) vibration, are also present in the spectrum along
with a band at 2,921 cm-1, corresponding to m(CH3).
The next step in our work was to study the spectroscopic
properties of the complex by applying the Electron Para-
magnetic Resonance (EPR) technique at the X- and Q-
bands. The complex has a total electronic spin S = 1, and
the zero-field splitting parameters, D and E, are close to
2,127 and 14 Gauss, respectively. Analysis of the EPR
measurements of a crystalline sample are currently under-
way through the investigation of the spectral lines obtained
on changing the relative angle of crystal orientation with
the direction of the magnetic field.
˚
0.209(1) A below, in the opposite direction to the other
Cu(2)N4 plane, in such a way than the distorted prism
formed by the donor atoms is capped by the copper atoms
(see Fig. 2). Similar values are found for the Cu(2)
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Fig. 2 View of the cage formed by the two CuN4 chromophores
123