Two-dimensional molecular-based ferrimagnets incorporating decamethylmetallocenium cations

1996 
Four new molecular-based magnets have been synthesized, and their magnetic properties have been investigated in detail. Their formulae are [M′(C5Me5)2]2M2[Cu(opba)]3·(DMSO)x(H2O)y with M′= Fe, M = Mn, x = 5, y = 4 (1), M′= Fe, M = Co, x = 6, y = 4 (2), M′= Co, M = Mn, x = 5.5, y = 4 (3) and M′= Co, M = Co, x = 5.5, y = 4 (4)[opba =ortho-phenylenebis(oxamato)]. The decamethylmetallocenium cations [Fe(C5Me5)2]+ and [Co(C5Me5)2]+ are most probably located between the anionic honeycomb-like networks Mn2[Cu(opba)]3 and Co2[Cu(opba)]3. Compounds 1–4 are two-dimensional ferrimagnets exhibiting a spontaneous magnetization below a critical temperature, Tc, of 14 K for 1, 27 K for 2, 13 K for 3 and 27.5 K for 4. Compounds 1 and 3, with MnII ions in the layered framework structure, do not exhibit magnetic hysteresis, while 2 and 4, with CoII in the layered framework structure, exhibit a wide magnetic hysteresis loop. The coercive fields at 2 K are found to be equal to 3.5 × 103 Oe for 2 and 5.3 × 103 Oe for 4. The latter is one of the largest values reported so far for a molecular-based magnet. The Mossbaer spectra for 1 and 2 have been recorded at various temperatures. These spectra suggest that the [Fe(C5Me5)2]+ units occupy two sites between the layers with a 50/50 distribution, and that they are not directly involved in the long-range magnetic ordering.
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