Syntheses, crystal structures, magnetic properties, and EPR spectra of tetranuclear copper(II) complexes featuring pairs of "Roof-Shaped" Cu2X2 dimers with hydroxide, methoxide and azide bridges
B. Graham et al., Syntheses, crystal structures, magnetic properties, and EPR spectra of tetranuclear copper(II) complexes featuring pairs of "Roof-Shaped" Cu2X2 dimers with hydroxide, methoxide and azide bridges, INORG CHEM, 40(7), 2001, pp. 1536-1543
Hydroxo- and methoxo-bridged tetranuclear copper(II) complexes of the tetra
macrocyclic ligand 1,2,4,5-tetrakis (1,4,7-triazacyclonon-1-ylmethyl)benzen
e (L-dur): have been prepared from [Cu4Ldur(H2O)(8)](ClO4)(8). 9H(2)O (1) A
ddition of base to an aqueous solution of I gave [Cu4Ldur(mu (2)-OH)(4)](Cl
O4)(4) (2). Diffusion of MeOH into a DMF solution of 2 produces [Cu4Ldur(mu
(2)-OMe)(4)](ClO4)(4). HClO4.2/3MeOH (3), a complex which hydrolyzes on ex
posure to moisture regenerating 2. The structurally related azido-bridged c
omplex, [Cu4Ldur(mu (2)-N-3)(4)](PF6)(4). 5H(2)O . 6CH(3)CN (4), was produc
ed by reaction of L-dur With 4 molar equiv of Cu(OAc)(2).H2O and NaN3 in th
e presence of excess KPF6. Compounds 2-4 crystallize in the triclinic space
group P (1) over bar (No. 2) with a = 10.248(1) Angstrom, b = 12.130(2) An
gstrom, c = 14.353(2) Angstrom, alpha = 82.23(1)degrees, beta = 60.79(1)deg
rees, gamma = 65.71(1)degrees, and Z = 1 for 2, a = 10.2985(3) Angstrom, b
= 12.1182(4) X, c = 13.9705(3) Angstrom, alpha = 89.978(2)degrees, beta = 8
2.038(2)degrees, gamma = 65.095(2)degrees, and Z = 1 for 3, and a = 12.059(
2) Angstrom, b = 12.554(2) Angstrom, c = 14.051(2) Angstrom, alpha = 91.85(
1)degrees, beta = 98.22(1)degrees, gamma = 105.62(1)degrees, and Z = 1 for
4. The complexes feature pairs of isolated dibridged copper(II) dimers with
"roof-shaped" Cu2(mu (2)-X)? cores (X = OH-. OMe-, N-3(-)), as indicated b
y the dihedral angle between the two CuX2 planes (159 degrees for 2, 161 de
grees for 3, and 153 degrees for 4). This leads to Cu Cu distances of 2.962
(4) Angstrom for 3, 2.962(1) Angstrom for 3, and 3.006(5) Angstrom for 4. V
ariable-temperature magnetic susceptibility measurements indicate weak anti
ferromagnetic coupling (J = -27 cm(-1)) for the hydroxo-bridged copper(II)
centers in 2 and very strong antiferromagnetic coupling (J = -269 cm cm(-1)
) for the methoxo-bridged copper(II) centers in 3. Pairs of copper(II) cent
ers in 4 display the strongest ferromagnetic interaction (J = 94 cm(-1)) re
ported thus far for bis(mu (2)-1,1-azido)-bridged dicopper units. Spectral
measurements on a neat powdered sample of 4 at 33.9 GHz or 90 Ghz confirm t
he spin-triplet ground state for the azido-bridged copper(II) pairs.