Rl. Oushoorn et al., LANTHANIDE(III)-COPPER(II) MOLECULAR-COMPOUNDS WITH A LADDER-LIKE MOTIF - STRUCTURE AND MAGNETIC-PROPERTIES, Bulletin de la Societe chimique de France, 133(7-8), 1996, pp. 777-782
The reaction of Ln(III) ions with the precursor [Cu(opba)](2-) in DMF
has afforded a series of structurally isomorphous compounds of formula
Ln(2)[Cu(opba)](3) . xDMF . yH(2)O (x approximate to 10, y approximat
e to 4); Ln stands for a lanthanide atom, from Tb to Lu, or for Y, opb
a stands for ortho-phenylenebis(oxamato), and DMF stands for dimethylf
ormamide. The crystal structure has been solved for Ln = Tm. The space
group is P2(1)2(1)2(1), with a = 9.864(2) Angstrom, b = 20.855(2) Ang
strom, c = 39.101(9) Angstrom, Z = 4 The structure consists of ladder-
type motifs, parallel to each other, with infinite Tm[Cu(opba)] sidepi
eces and [Cu(opba)] rungs joining two Tm atoms. The temperature depend
ences of the magnetic susceptibility for all compounds have been inves
tigated, and have revealed a striking difference between the compounds
with Ln = Tb and Dy and those with Ln = Ho, Er, Tm, and Yb. For the f
ormer compounds, significant Ln(III)-Cu(II) magnetic interactions have
been detected, which leads to the divergence of the product chi(M)T o
f the molar magnetic susceptibility with temperature. At this stage, i
t has not been possible to specify whether the compounds are one-dimen
sional ferri- or ferromagnets. In contrast, for the Ln = Ho, Er, Tm an
d Yb compounds, the Ln(III)-Cu(II) interactions, if any, are hidden by
the crystal field effects.