P. Comba et al., INTERPRETATION OF ELECTRONIC AND EPR-SPECTRA OF COPPER(II) AMINE COMPLEXES - A TEST OF THE MM-AOM METHOD, Inorganic chemistry, 34(15), 1995, pp. 3903-3911
The strain energy minimized structures (MM) of a series of copper(II)
tetraamines ([Cu((R)-ahaz)((S)-ahaz)](2+), (R)-ahaz (1)= (R)- 3-aminoh
exahydroazepine, (S)-ahaz (2)= (S)-3 -aminohexahydroazepine; [Cu((S)-a
haz)(2)(OH2)](2+); [CU(mn[13]aneN(4))(OH2)(2)](2+), mn[l3]aneN(4) (3)
= 2-methyl-12-nitro-l,4,7,10-tetraazacyclotridecane; [Cu(mn[l3]aneN(4)
)(OH2)](2+); [Cu(mn[14]aneN(4))(OH2)](2+), mn[l4]aneN(4) (4)= -methyl-
6-nitro-1,4,8,11-tetraazacyclotetradecane; [Cu(mn[15]aneN(4))(OH2)](2), mn[ 15]aneN(4) (5)= methyl-10-nitro-1,4,8,12-tetraazacyclopentadeca
ne; [Cu(mn[15]aneN(4))(OH2)(2)](2+); [Cu(mn[16]aneN(4))(OH2)](+), mn[1
6]ane N-4 (6) = 3-methyl-3-nitro-1,5,9,13-tetraazacyclohexadecane; [Cu
(en)(2)(OH2)(2)](2+), en (7) = ethane-1,2-diamine), with square planar
, square pyramidal, and distorted octahedral chromophores exhibiting v
arious degrees of tetrahedral distortion of the central coordination p
lane, are in good agreement with published X-ray structures (where ava
ilable) and the two crystal structures reported ip this paper. [Cu(2)(
2)(ClO)(4)](ClO4) crystallizes in the orthorhombic space group P2(1)2(
1)2(1), with a 18.194(4) Angstrom, Z = 4, and R, = 0.061. [Cu(5)(C1)21
2and0 crystallizes in the 6.884(2) W, b = 9.090(3) Angstrom, c = 9.21
4(2) Angstrom, cc = 105.13(2)0, P = 107.40(2)'', y = 107.85(2)0, Z = 1
, and R, = 0.022. The spin Hamiltonian parameters and electronic trans
itions, estimated with the angular overlap model (AOM) based on the st
rain energy minimized structures of the chromophores, where generally
water is used as axial ligand (MM-AOM), are in reasonable agreement wi
th the calculated spectroscopic parameters based on experimental struc
tures (AOM) and with the experimental spectroscopic data (UV-vis-near-
IR and EPR spectra ofsingle crystals, powders, glasses, and solutions)
. The calculated spectroscopic data are based on a constant set of ele
ctronic parameters which depend on the degree of substitution of the a
mine, on the Cu-N bond length, and on the degree of misdirected valenc
es.