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Developments in Ceramic Materials Research

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Optical Fluoride and Oxysulfide <strong>Ceramic</strong>s: Preparation and Characterization 81<br />

27) under pulsed copper vapor laser excitation at 511 nm (tp = 10 ns; f = 10 kHz) and a timecorrelated<br />

s<strong>in</strong>gle-photon count<strong>in</strong>g detection technique. The time- resolved fluorescence<br />

spectrum at the 4 G7/2→ 4 I13/2 transition is measured at room temperature for the La2O2S:Nd 3+<br />

(1 wt%) optical ceramics with gate width tgate=79 ns and gate delay td=59 ns (curve 1 at<br />

Figure 28) and for the Gd2O2S:Nd 3+ (0.5 wt%) optical ceramics these values are set to tgate =<br />

40 ns and td= 39 ns (curve 2 at Figure 28) us<strong>in</strong>g the same technique and a special program of<br />

our own for multichannel amplitude analyzer (MCA, EGandG Ortec) operation. The gate<br />

delays are set to m<strong>in</strong>imize the <strong>in</strong>fluence of a small fraction of the powerful pump radiation<br />

pass<strong>in</strong>g through the monochromator and KS-11 glass filter. The decay times are measured at<br />

the long time scale of fluorescence k<strong>in</strong>etics decay. The measured decay times (Table 2) are<br />

determ<strong>in</strong>ed by MR of the 4 G7/2→ 4 G5/2; 2 G7/2 transition, because a contribution of radiative<br />

decay is negligible [52]. The MR rate of the 4 I11/2→ 4 I9/2 transition is of the order of magnitude<br />

of the measured rate of the 4 G7/2→ 4 G5/2; 2 G7/2 transition. So, the depletion of the low laser<br />

level is not slower than several hundred nanoseconds.<br />

Photon counts<br />

10 1<br />

10 0<br />

10 -1<br />

10 -2<br />

10 -3<br />

10 -4<br />

4<br />

G7/2 level<br />

T=77 K<br />

3<br />

1 La2O2S:Nd 3+ τ=75 ns<br />

2Gd2O2S:Nd 3+ τ=27 ns<br />

3 set-up response function τ=12 ns<br />

0 100 200 300 400 500 600<br />

2<br />

time, ns<br />

Figure 27. Fluorescence k<strong>in</strong>etics of the 4 G 7/2 manifold <strong>in</strong> La 2O 2S:Nd 3+ (1 wt%)—1, Gd 2O 2S:Nd 3+<br />

(0.5 wt%)−2 at 77 K under 511 nm excitation detected at the 4 G 7/2 → 4 I 13/2 transition and the set- up<br />

response function—3.<br />

Table 2. The measured and multiphonon relaxation decay times for the 4 G7/2 level of<br />

Nd 3+ <strong>in</strong> optical ceramics with low-phonon spectra at 77 K and room temperature and<br />

parameters hav<strong>in</strong>g <strong>in</strong>fluence on multiphonon transition rate<br />

Optical<br />

samples<br />

ΔEm<strong>in</strong> (cm −1 ) ωmax pm<strong>in</strong> τmeas = τMR at 77 K (ns)<br />

La2O2S:Nd 3+ 1517 400 4 75 38<br />

Gd2O2S:Nd 3+ 1500 440 4 27 19<br />

1<br />

τmeas = τ MR at 300 K<br />

(ns)

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