SYNTHESIS, CRYSTAL-STRUCTURE, AND MAGNETIC-PROPERTIES OF A FERROMAGNETICALLY COUPLED DIFLUORO-BRIDGED DINUCLEAR CHROMIUM(III) COMPLEX WITH A SUBSTITUTED TETRAHYDROSALEN DERIVATIVE AS LIGAND
R. Sanzenbacher et al., SYNTHESIS, CRYSTAL-STRUCTURE, AND MAGNETIC-PROPERTIES OF A FERROMAGNETICALLY COUPLED DIFLUORO-BRIDGED DINUCLEAR CHROMIUM(III) COMPLEX WITH A SUBSTITUTED TETRAHYDROSALEN DERIVATIVE AS LIGAND, Inorganic chemistry, 35(26), 1996, pp. 7493-7499
A novel difluoro-bridged dinuclear chromium(III) complex has been synt
hesized by the reaction of trans-[Cr-(py)(4)F-2]ClO4 in 2-methoxyethan
ol with a substituted tetrahydrosalen derivative L(8) (L(8) means the
negatively charged ligand obtained by dissociation of two protons from
H(2)L(8) = droxy-3,5-di-tert-butylbenzyl)-1,2-ethanediamine), The cry
stal structure of [CrL(8)F](2) . 2C(3)H(8)O(2) has been determined. Th
e crystal system is triclinic, and the lattice constants are a 9.604(2
) Angstrom, b = 13.346(2) Angstrom, c 15.751(2) Angstrom, alpha = 74.0
0(1)degrees, beta = 87.94(1)degrees, and gamma = 70.55(1)degrees. Z =
1 and the volume of the unit cell is 1826.40(49) Angstrom(3). The spac
e group is <(P)over bar 1> (No. 2). The refinement of 456 variables in
cludes 6279 of the 7631 independent reflections, The final residual is
4.08%. The centrosymmetric dinuclear molecule consists of two slightl
y distorted octahedrally cis coordinated chromium centers bound togeth
er by two fluoride bridges. The Cr-F-Cr angle is 100.90(4)degrees, and
the Cr-F(bridge) distances are 2.0172(8) and 1.9754(9) Angstrom, and
the Cr-Cr distance is 3.0787(4) Angstrom. The configuration of the din
uclear molecule is cis, cis-O, O'-Delta, Lambda, where cis refers to t
he position of the two oxygen donors and Delta and Lambda refer to the
configuration of the two N, O chelates of the tetradentate ligand L(8
) at each of the two chromium(III) centers. The two chromium-(III) cen
ters in the complex are ferromagnetically coupled. On basis of measure
ments of the field-dependent magnetization and the magnetic susceptibi
lity, respectively, it has been shown unambiguously that the ground st
ate is a septet state. It has not been possible to determine the monoa
tomic zero field splitting parameter D from the magnetic susceptibilit
y measurements, but the parameter has been determined from the EPR spe
ctra measured at 4 and 21 K. From simulation of the EPR spectra the fo
llowing parameters have been obtained: J = -1.4 cm(-1), D-e = 0.008 cm
(-1), E(e) = -0.015 cm(-1), D-a = D-b = -0.658 cm(-1), E(a) = E(b) = 0
.133 cm(-1), g(xa) = g(xb) = g(ya) = g(yb) = 1.98 and g(za) = g(zb) =
2.00.