[CR(BIPY)(C2O4)(2)](-) - A VERSATILE BUILDING-BLOCK FOR THE DESIGN OFHETEROPOLYMETALLIC SYSTEMS .2. SYNTHESES AND CRYSTAL-STRUCTURES OF PY)(2)(MU-C2O4)(2)(C2O4)(2)(H2O)(2)CENTER-DOT-1(1) 2H2O AND (AGCR(BIPY)(MU-C2O4)(2)(H2O)(2))(2) AND MAGNETIC-PROPERTIES OF THE COPPER(II) DERIVATIVE/
M. Andruh et al., [CR(BIPY)(C2O4)(2)](-) - A VERSATILE BUILDING-BLOCK FOR THE DESIGN OFHETEROPOLYMETALLIC SYSTEMS .2. SYNTHESES AND CRYSTAL-STRUCTURES OF PY)(2)(MU-C2O4)(2)(C2O4)(2)(H2O)(2)CENTER-DOT-1(1) 2H2O AND (AGCR(BIPY)(MU-C2O4)(2)(H2O)(2))(2) AND MAGNETIC-PROPERTIES OF THE COPPER(II) DERIVATIVE/, Inorganica Chimica Acta, 251(1-2), 1996, pp. 309-317
The compounds CuCr2(bipy)(2)(mu-C2O4)(2)(C2O4)(2)(H2O)(2) . 11/2H(2)O
(1) and (AgCr(bipy)(mu-C2O4)(2)(H2O)(2))(2) (2) have been obtained by
self-assembling [Cr(bipy)(C2O4)(2)](-) building blocks with Cu(II) and
Ag(I) ions, respectively. The molecular and crystal structures of the
two compounds were determined. Crystal 1 is monoclinic, C2/c, a = 20.
379(14), b = 11.037(4), c = 17.480(7) Angstrom, beta = 124.83(3)degree
s, Z = 4 and R = 0.0369. Its structure consists of discrete linear {Cr
CuCr} trinuclear species with the copper atom lying on an inversion ce
nter. The copper atom exhibits [4 + 2] axially elongated octahedral ge
ometry, the apical positions being occupied by two oxalato oxygen atom
s. The Cu-O bond distances are 1.953(4) (H2O), 1.998(3) and 2.357(3) A
ngstrom, the Cr-O bonds vary from 1.945(3) to 1.982(3) Angstrom, and t
he Cr-N bonds are 2.031(4) and 2.054(3) Angstrom. The Cr ... Cu distan
ces are 5.288 Angstrom. Crystal 2 is monoclinic, P2(1)/c, a = 14.639(1
6), b = 15.553(10), c = 16.899(12) Angstrom, beta = 114.70(4)degrees,
Z = 4 and R = 0.0629, and contains discrete tetranuclear cycles formed
by two chromium and two sliver atoms bridged by the oxalato groups. T
he silver atoms are penta-coordinated, exhibiting distorted trigonal b
ipyramidal geometries. The Ag-O bond distances vary from 2.350(8) to 2
.548(7) Angstrom, while the Cr-O bonds are in the range 1.942(7) to 1.
982(6) Angstrom. The magnetic susceptibility data of 1 reveal an irreg
ular spin state structure with S = 5/2 ground state and an antiferroma
gnetic interaction between the central copper(II) and the chromium(III
) atoms (J = - 18.8 cm(-1)).