Layered molecule-based magnets formed by decamethylmetallocenium cations and two-dimensional bimetallic complexes [M(II)Ru(III)(ox)(3)](-)(M(II) = Mn, Fe, Co, Cu and Zn; ox = oxalate)
E. Coronado et al., Layered molecule-based magnets formed by decamethylmetallocenium cations and two-dimensional bimetallic complexes [M(II)Ru(III)(ox)(3)](-)(M(II) = Mn, Fe, Co, Cu and Zn; ox = oxalate), J SOL ST CH, 159(2), 2001, pp. 391-402
A new series of hybrid organometallic-inorganic layered magnets with formul
a [Z(III)Cp(2)(*)] [(MRuIII)-Ru-II(ox)(3)] (Z(III) = Co and Fe; M-II = Mn,
Fe, Co, Cu, and Zn; ox = oxalate: Cp* = pentamethylcyclopentadienyl) has be
en prepared. All of these compounds are isostructural to the previously rep
orted [Z(III)Cp(2)*] [(MMIII)-M-II(ox)(3)] (M-III = Cr, Fe) series and crys
tallize in the monoclinic space group C2/m, as found by powder X-ray diffra
ction analysis. They are novel examples of magnetic materials formed by bim
etallic oxalate-based extended layers separated by layers of organometallic
cations, The magnetic properties of all these compounds have been investig
ated (ac and de magnetic susceptibilities and field dependence of the isoth
ermal magnetization at 2 K), In particular, it has been found that Fe-II an
d Co-II derivatives behave as magnets with ordering temperatures of 12.8 an
d 2.8 K, respectively, while no long-range magnetic ordering has been detec
ted down to 2 K in the Mn-II and Cu-II derivatives. The magnetic ordering i
n the Fe-II derivatives has been confirmed through Mossbauer spectroscopy.
This technique has also made it possible to observe the spin polarization o
f the paramagnetic [FeCp2*](+) units caused by the internal magnetic field
created by the bimetallic layers in the ordered state. (C) 2001 Academic Pr
ess.