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The European Physical Journal BISSN: 1434-6028 (printed version) Abstract Volume 4 Issue 3 (1998) pp 269-277 Optical and paramagnetic properties of titanium centres in ZnS
J. Dziesiaty (1), M.U. Lehr (2), P. Peka (2), A. Klimakow (1), S. Müller (1), H.-J. Schulz (2) (a)
(1) Humboldt-Universität zu Berlin, Institut für Physik, Invalidenstrasse 110, 10099 Berlin, Germany Received: 3 October 1997 / Revised: 17 December 1998 / Accepted: 18 May 1998 Abstract: ZnS:Ti crystals grown by different methods are investigated at low temperatures (2 K $\leq T \leq 80$ K) by electron paramagnetic resonance (EPR) and optical spectroscopies, mainly with regard to their photoluminescence properties, including excitation and sensitisation spectra. The more familiar lattice-neutral Ti2+(d2) ion on a cubic site (AN) presents an isotropic EPR signal with g=1.928 observable up to 80 K. Signals of axial PN and AS sites are detected in the same temperature range. This Ti2+ ion exhibits the $^3T_2(F) \rightarrow{}^3A_2(F)$ transition in emission, structured by no-phonon lines (NPL) of centres in various environments, with the AN site represented at 3613 cm-1, and the 3T1(F) and 3T1(P) bands in excitation spectra. Substitutional Ti3+(d1) is identified by an anisotropic EPR spectrum at T = 3.5 K, indicating a quasistatic Jahn-Teller effect at the doubly degenerate 2E(D) ground state, while in the first excited vibronic state a quasidynamic JT effect in the strain-split vibronic 2E/2A2 manifold is found. A new luminescence band centred at 4500 cm-1 with NPL structures near 5000 cm-1 represents AN, PN and AS sites in the $^2T_2(D) \rightarrow{}^2E(D)$ transition. Charge-transfer processes are described in a one-particle model, depicting the Ti3+/Ti2+ donor level at 12 900 cm-1 below the conduction-band edge.
PACS. 71.70.-d Level splitting and interactions- 76.30.Fc Iron group (3d) ions and impurities (Ti-Cu)- 78.55.Et II-VI semiconductors
(a) email: schulz@fhi-berlin.mpg.de Article in PDF-Format (350 KB) Online publication: August 17, 1998 |