ChemComm
Communication
2 Spin-Crossover Materials: Properties and Applications, ed. M. A. Halcrow,
John Wiley & Sons, Ltd, 1st edn, 2013.
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Fig. 4 57Fe Mossbauer spectra of [Fe(Lpz)2(NCS)2] measured at variable
¨
temperatures with an applied field of 47 mT parallel to the g-rays. The
sample was initially quench cooled in liquid nitrogen before being cooled to
5.3 K in the spectrometer. Slow warming (B1 K minÀ1) to 100 K then 150 K
and 250 K produced the spectra shown. The sample was then slowly cooled
back to 150 K, confirming the presence of a hysteresis. The spectra are
deconvoluted into high spin (red solid line) and low spin (blue dashed line).
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Letard and M. A. Halcrow, Eur. J. Inorg. Chem., 2013, 819–831.
for E = S and Se; Fig. 4 and Fig. S9, ESI†) differ depending on whether
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they were measured upon cooling or warming, confirming the
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hysteretic nature of the SCO event. The low Lamb–Mossbauer factor
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26 M. G. Cowan, J. Olguın, S. Narayanaswamy, J. L. Tallon and
of the NCBH3 complex at high temperatures precluded measurement
at higher temperatures but the data (Fig. S10, ESI†) do confirm that,
in contrast to the other two complexes, this E = BH3 sample is fully LS
at 5.6 K. All results are in good agreement with the magnetic data.
In summary, we report a family of iron(II) complexes of the new
pyrazine-containing ligand Lpz. Unusually, SCO events are observed
for all three complexes, with hysteresis observed in two of these cases,
and the crossover temperatures can be predictably tuned by varying
the coordinated anion. Further work investigating the intricacies of
this and related systems is currently underway.
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27 N. Wannarit, O. Roubeau, S. Youngme, S. J. Teat and P. Gamez,
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28 The unsubstituted (i.e. R = H) pyridine–triazole–pyrazine ligand
3-(pyrazin-2-yl)-5-(pyridin-2-yl)-1,2,4-triazole and its ruthenium,
osmium and copper complexes have been reported: W. R. Browne,
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32 The crystal was cooled at a rate of 2 K minÀ1 to prevent ‘‘flash
freezing’’ trapping it in the HS state.
We thank the University of Otago and the Marsden Fund
(RSNZ) for supporting this research, the MacDiarmid Institute
¨
for the Mossbauer spectrometer and magnetometers, Dr S.
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33 J. Olguın and S. Brooker, in Spin-Crossover Materials: Properties and
Chong (Callaghan Innovation) for his help, and Dr J. L. Tallon
(Callaghan Innovation) for advice.
Applications, ed. M. A. Halcrow, John Wiley & Sons, Ltd, 1st edn, 2013,
pp. 77–120.
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34 R. Kulmaczewski, J. Olguın, J. A. Kitchen, H. L. C. Feltham, G. N. L.
Jameson, J. L. Tallon and S. Brooker, J. Am. Chem. Soc., 2013, submitted.
35 R. G. Miller, S. Narayanaswamy, J. L. Tallon and S. Brooker, New
J. Chem., submitted.
36 Interestingly, this crossover occurs at a significantly lower tempera-
ture than that observed in [Fe(ptdpt)2(NCS)2] (T1/2 = 231 K), ref. 20.
Notes and references
1 Spin Crossover in Transition Metal Compounds, Volumes I–III of Topics in
Current Chemistry, ed. P. Gu¨tlich and H. A. Goodwin, 2004; P. Gu¨tlich,
A. B. Gaspar and Y. Garcia, Beilstein J. Org. Chem., 2013, 9, 342–391.
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