Determination of the structure of EuTETA and the luminescence properties of EuTETA and EuDOTA (TETA=1,4,8,11-tetraazacyclotetradecane-1,4,8,11-tetraacetate and DOTA=1,4,7,10-tetraazacyclododecane-1,4,7,10-tetraacetate)
Jg. Kang et al., Determination of the structure of EuTETA and the luminescence properties of EuTETA and EuDOTA (TETA=1,4,8,11-tetraazacyclotetradecane-1,4,8,11-tetraacetate and DOTA=1,4,7,10-tetraazacyclododecane-1,4,7,10-tetraacetate), INORG CHIM, 310(1), 2000, pp. 56-64
The crystal structure and the luminescence of the complex Na[Eu(TETA)]. 2H(
2)O . 4NaCl (TETA = 1,4,8,11-tetraazacyclotetradecane-1,4,8,11-tetraacetate
) have been determined. The space group is P (1) over bar, and the lattice
parameters are a = 9.283(2) Angstrom, b = 17.794(3) Angstrom, c = 19.8087(1
7) Angstrom, alpha = 70.733(11)degrees, beta = 83.474(12)degrees, gamma = 8
8.478(18)degrees, V = 3068.6(9) Angstrom (3), rho = 1.890 g cm(-3), and Z =
2. The luminescence of Na[EuDOTA .H2O]. 3H(2)O (DOTA = 1,4,7,10-tetraazacy
clododecane-1,4,7,10-tetraacetate) has also been reported. In the TETA macr
ocycle, the Eu(III) is completely encapsulated via coordination to the four
nitrogen atoms and the four carboxylate oxygen atoms of the ligand. The ge
ometry of the eight-coordinate polyhedron is a strongly distorted dodecahed
ron. The characteristic feature in the geometry is the conformation of the
pendant carboxylate arms. The asymmetric unit consists of two independent m
olecules, differentiated from the helicities of the pendant arms. When the
EuTETA and EuDOTA crystals are excited by UV light, they produce very chara
cteristic luminescences responsible for the D-5(0)-->F-7(J) (J = 0, 1, 2, 3
, 4) transitions. Unlike the EuDOTA complex, the luminescence structure of
the EuTETA complex is significantly affected by the crystalline state. This
might be due to the rigidity of the complex. The energy-level schemes of t
he F-7(J) states and detailed assignments for the observed luminescence lin
es of the EuTETA and EuDOTA complexes have been proposed by phenomenologica
l simulation in the framework of the crystal-field Hamiltonian. (C) 2000 El
sevier Science B.V. All rights reserved.