Dalton Transactions
Communication
methods. Nevertheless, clearly the post synthetic approach
leads to a specific molecular arrangement and physical pro-
perties and opens up the way towards the preparation of
new SCO complexes. The methodology used in this work is
currently under investigation to determine the synergetic
effect between SCO and different physical or chemical pro-
perties that cannot be accessed through the direct synthetic
methodology.
Fig. 3 13C CP-MAS (left) and 13C MAS (right) NMR spectra of samples 1,
3, 5 and 6.
Conflicts of interest
In order to probe the composition of the samples in depth, There are no conflicts to declare.
we used Mössbauer spectroscopy and NMR spectroscopy, the
latter being rarely used to characterize paramagnetic SCO
materials. 13C CP-MAS and 13C MAS NMR are two different
techniques used to obtain the NMR spectra in the solid state;
Acknowledgements
while the first is adapted for diamagnetic systems, the latter A. E.-C. thanks the CONACyT (Mexico) for the postdoctoral
permits us to study also the paramagnetic entities that are grant. We thank Yannick Coppel for NMR measurements and
associated with faster nuclei relaxation.19,20 Indeed, in the discussions.
13C CP-MAS spectra at room temperature (Fig. 3), we only
observe a peak at 155 ppm corresponding to the triazole core
for samples 1–4. Although the intensities of the peaks seem to
be similar due to an increase in the number of scans (to
Notes and references
observe the peaks, see the ESI†), they decrease from sample 1
to sample 4 in accordance with the increase of susceptibility.
Indeed, from the magnetic behaviour observed in Fig. 2, it is
clear that at room temperature (heating mode) 1 is diamag-
netic, and this characteristic is lost with the degree of trans-
formation (Fig. S13†), explaining the decrease in the intensity
of the 13C CP-MAS peak. Moreover, the difficulty in obtaining a
signal for sample 5 is in agreement with the majority of HS
fractions. In this case, we cannot detect 13C spins in the direct
vicinity of the paramagnetic species, which are certainly
severely broadened to be indistinguishable from the base-
line.21 As expected sample 6 is also silent as it is fully paramag-
netic. Mössbauer data were collected for sample 5 at 80 and
325 K and confirmed the residual LS fraction at high tempera-
ture suspected by magnetic measurements (see the ESI†).
The 13C MAS NMR (Fig. 3) spectrum at room temperature
confirms the diamagnetic entities for 1, while the introduction
of the imine ligand leads to the appearance of new peaks at
59 ppm (OCH3), 115 and 137 ppm (aromatic carbons of p-ani-
saldehyde), 169 ppm (triazole core) and 200 ppm (CHvN)
attributed to the paramagnetic species that increase in inten-
sity in agreement with the degree of transformation. Clearly,
in contrast to the 13C CP-MAS experiment, 13C MAS NMR
allows for the study of the whole system in all cases.
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Dalton Trans., 2019, 48, 16853–16856 | 16855