Crystal structure and spectroscopy of a hydrogen-bridged one-dimensional Cu(II) complex containing both octahedral and square pyramidal geometries inthe same unit cell
C. Karunakaran et al., Crystal structure and spectroscopy of a hydrogen-bridged one-dimensional Cu(II) complex containing both octahedral and square pyramidal geometries inthe same unit cell, J CHEM CRYS, 30(5), 2000, pp. 351-357
Single crystals of the helical hydrogen-bridged one-dimensional Cu(II) comp
lex, [Cu(stpy)(2) (CH3COO)(2)(H2O)(2)] (1) [CU(Stpy)(2)(CH3COO)(2)(H2O)] (2
), are prepared and characterized by elemental and thermal analyses, IR, el
ectronic and X-ray crystal structure determination. The crystals are monocl
inic, of space group C2/c, with unit cell parameters a = 31.842(7) Angstrom
, b = 5.9829(10) Angstrom, c = 30.970(14) Angstrom, beta = 111.78(3)degrees
, Z = 4. The asymmetric unit contains two different types of Cu(II) polyhed
ra, namely, octahedron and square pyramid within the same unit cell. 1 has
elongated octahedral geometry with two nitrogen atoms from stpy and two oxy
gen atoms from synmonodentate acetate ligands, transcoordinated to Cu(II) i
n the basal plane. The oxygen atoms of the two water molecules occupy the a
xial positions. 2 has Cu(II) coordination polyhedra similar to 1, except th
at only one of the apical positions is occupied by a water molecule. The st
ructure consists of two independent linear chains, one involving octahedral
(1) and the other involving square-pyramidal (2) polyhedra, held by hydrog
en bridges. The Cu-Cu intra- and interchain separations in both 1 and 2 are
5.983 and 8.214 Angstrom. The unit cell packing shows weak pi -stacking be
tween adjacent coordinated stpy ligands in the chain, resulting in ladder-t
ype structure. Further, the extended packing reveals helical arrangement of
Cu(II) polyhedra in the lattice.