English
 
Help Privacy Policy Disclaimer
  Advanced SearchBrowse

Item

ITEM ACTIONSEXPORT

Released

Journal Article

ESR and optical spectroscopy of copper-doped PLZT electro-optic ceramics

MPS-Authors
/persons/resource/persons22089

Schulz,  Hans-Joachim
Inorganic Chemistry, Fritz Haber Institute, Max Planck Society;

External Resource
No external resources are shared
Fulltext (restricted access)
There are currently no full texts shared for your IP range.
Fulltext (public)
There are no public fulltexts stored in PuRe
Supplementary Material (public)
There is no public supplementary material available
Citation

Bryknar, Z., Bykov, I., Glinchuk, M., Laguta, V., Maximenko, Y., Potuček, Z., et al. (1998). ESR and optical spectroscopy of copper-doped PLZT electro-optic ceramics. Applied Physics A, 66, 555-559. doi:10.1007/s003390050712.


Cite as: https://hdl.handle.net/21.11116/0000-0008-2ED8-2
Abstract
Nominally pure and Cu-doped (0.01, 0.1, and 1 wt% of copper oxide) PLZT 8/65/35 ceramics were investigated with regard to their ESR and optical spectra (absorption and luminescence). ESR investigations were performed at 4.2K ≤ T ≤ 300 K in the X and K bands both before and after annealing the samples in oxygen and hydrogen atmospheres. The observed spectra were shown to be a superposition of Cu2+ spectra in axial and cubic crystal fields. Cu2+ substitutes for Ti4+ and the excess charge can be compensated by La3+ on a nearest-neighbor site, thus creating axialsymmetry. The centers of 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 2T2(D)→ 2E(D) transition of Cu2+(3d9) 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 that of Cu+ ions. Annealing in hydrogen and in oxygen atmospheres caused decrease and restoration, respectively, of the ESR and luminescence intensities as a consequence of Cu2+ conversion into Cu1+ and vice versa.