Z. Bryknar et al., ESR AND OPTICAL SPECTROSCOPY OF COPPER-DOPED PLZT ELECTROOPTIC CERAMICS, Applied physics A: Materials science & processing, 66(5), 1998, pp. 555-559
Nominally pure and Cu-doped (0.01, 0.1, and 1 wt% of copper oxide) PLZ
T 8/65/35 ceramics were investigated with regard to their ESR and opti
cal spectra (absorption and luminescence). ESR investigations were per
formed at 4.2 K less than or equal to T less than or equal to 300 K in
the X and K bands both before and after annealing the samples in oxyg
en and hydrogen atmospheres. The observed spectra were shown to be a s
uperposition of Cu2+ spectra in axial and cubic crystal fields. Cu2+ s
ubstitutes for Ti4+ and the excess charge can be compensated by La3+ o
n a nearest-neighbor site, thus creating axial symmetry. The centers o
f cubic symmetry are those where the charge is compensated in distant
spheres. In contrast to pure PLZT, PLZT:Cu exhibits a new luminescence
band peaking at 1.18 eV. This emission is ascribed to the T-2(2)(D) -
-> E-2(D) transition of Cu2+(3d(9)) which can be excited either in the
resonant 1.87 eV band or via charge-transfer excitation bands at 2.40
, 2.57, and 3.03 eV. The absorption band at 1.45 eV is assumed to be t
hat of Cu+ ions. Annealing in hydrogen and in oxygen atmospheres cause
d decrease and restoration, respectively, of the ESR and luminescence
intensities as a consequence of Cu2+ conversion into Cu1+ and vice ver
sa.