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Developments in Ceramic Materials Research

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Optical Fluoride and Oxysulfide <strong>Ceramic</strong>s: Preparation and Characterization 85<br />

At higher concentration of Nd 3+ (0.5 wt%) the fluorescence k<strong>in</strong>etics shows<br />

nonexponential decay <strong>in</strong>dependent on the temperature. This can be a result of concentration<br />

quench<strong>in</strong>g or presence of different types of optical centers (Figure 29a). To check these ideas<br />

time-resolved fluorescence spectra are measured us<strong>in</strong>g standard gated Boxcar averager (PAR<br />

162/164) with variable time gate tgate and gate delay td. Time-resolved fluorescent spectra<br />

measured at 77 K under 893.5 nm pulsed laser excitation at different time gates and gate<br />

delays do not show any significant changes for this sample (Figure 30). This <strong>in</strong>dicates the<br />

absence of different types of optical centers <strong>in</strong> the Gd2O2S:Nd 3+ optical ceramics for the<br />

concentrations of Nd 3+ up to 0.5 wt% and confirms that nonexponential fluorescence decay<br />

deals with concentration quench<strong>in</strong>g. The energy transfer k<strong>in</strong>etics for the Gd2O2S:Nd 3+ (0.5<br />

wt%) (Figure 29b) was obta<strong>in</strong>ed by subtract<strong>in</strong>g the <strong>in</strong>tracenter decay us<strong>in</strong>g the lifetime<br />

measured for the Gd2O2S: Nd 3+ (0.1 wt%) ceramic sample with m<strong>in</strong>imal concentration of<br />

Nd 3+ (τmeas=107.0 μs) (curve 1 <strong>in</strong> Figure 29a). The energy transfer k<strong>in</strong>etics <strong>in</strong> the<br />

Gd2O2S:Nd 3+ (0.5 wt%) ceramic sample can be analyzed <strong>in</strong> terms of the model of Eqs. (4),<br />

(5).<br />

By plott<strong>in</strong>g the energy transfer k<strong>in</strong>etics −lg(−ln I(t)) as a function of lg(t) for<br />

Gd2O2S:Nd 3+ (0.5 wt%) (Figure 31a), we can determ<strong>in</strong>e from the slope of this graph the<br />

exponent of the time parameter tg =3/s [see Eq. (4)], and to determ<strong>in</strong>e the s parameter. We<br />

found that tg eventually tends to , which corresponds to s=6 and the dipole–dipole<br />

quench<strong>in</strong>g <strong>in</strong>teraction between the excited and unexcited Nd 3+ ions.<br />

Fluorescence, a.u.<br />

3<br />

2<br />

1<br />

2<br />

1<br />

λ, nm<br />

Gd<br />

2O2S:Nd 3+ (0.5 %)<br />

T=77 K<br />

t gate = 200 μs τd = 350 μs<br />

t gate = 1 μs τd = 20 μs<br />

0<br />

1060 1070 1080 1090 1100 1110 1120<br />

Figure 30. Time- resolved fluorescence spectra measured at the 4 F 3/2→ 4 I 11/2 transition of Nd 3+ <strong>in</strong> the<br />

Gd 2O 2S:Nd 3+ (0.5 wt%) optical ceramics at 77 K under 893.5 nm pulsed laser excitation with 300 μm<br />

slits width, gate width tgate=1 μs, and gate delay t d=20 μs—1; and t gate=200 μs and t d=350 μs—2.

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