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Developments in Ceramic Materials Research

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88<br />

Fluorescence, a.u.<br />

I transfer , a.u.<br />

0.1<br />

0.01<br />

0.001<br />

T. T. Basiev, V. A. Demidenko, K. V. Dykel’skii et al.<br />

1<br />

0.1<br />

1<br />

time, μs<br />

La 2 O 2 S:Nd 3+ (1 w. %)<br />

0 200 400 600<br />

time, μs<br />

a)<br />

La 2 O 2 S:Nd 3+ (1 w. %)<br />

0 20 40 60 80 100<br />

Figure 32. Fluorescence k<strong>in</strong>etics decay of the 4 F 3/2 manifold of the Nd 3+ ion <strong>in</strong> the La 2O 2S:Nd 3+ (1 wt%)<br />

ceramic sample measured under 904 nm laser excitation at 1.08 μm fluorescence detection at 300 K—a<br />

and the Forster stage of energy transfer k<strong>in</strong>etics—b.<br />

An average rate of energy migration can be calculated from experimental data with the<br />

follow<strong>in</strong>g equation:<br />

Us<strong>in</strong>g the follow<strong>in</strong>g equation for hopp<strong>in</strong>g model of energy migration:<br />

b)<br />

(7)<br />

(8)

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