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Developments in Ceramic Materials Research

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Fluorescence, a.u.<br />

Optical Fluoride and Oxysulfide <strong>Ceramic</strong>s: Preparation and Characterization 79<br />

1800<br />

1600<br />

1400<br />

1200<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

1071.1<br />

1074.5<br />

1076.2<br />

1080.2<br />

1082.4<br />

1092.8<br />

1090.1<br />

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

4 F3/2 --> 4 I 11/2<br />

T=300 K<br />

T=77 K<br />

0<br />

1060 1070 1080 1090 1100 1110<br />

b<br />

Figure 24. Fluorescence spectra of the 4 F 3/2→ 4 I 11/2 transition <strong>in</strong> Gd 2O 2S:Nd 3+ (0.1 wt%)—a and<br />

La2O 2S:Nd 3+ (1 wt%)—b under 812 nm laser excitation at 77 and 300 K.<br />

The fluorescence spectrum at the 4 F3/2→ 4 I11/2 transition is measured with high spectral<br />

resolution <strong>in</strong> Gd2O2S:Nd 3+ (0.1 wt%) (Figure 24a) and La2O2S:Nd 3+ (1 wt%) (Figure 24b) at<br />

77 and 300 K us<strong>in</strong>g CW diode laser excitation. The positions of the three lowest CF levels of<br />

the 4 I11/2 manifold are found <strong>in</strong> the Gd2O2S:Nd 3+ ceramics (Figure 22). The fluorescence<br />

spectral l<strong>in</strong>es measured at the 4 F3/2→ 4 I11/2 CF level transitions <strong>in</strong> the Gd2O2S:Nd 3+ (0.1 wt%)<br />

optical ceramics at 77 and 300 K are much more narrow (Figure 24a) compar<strong>in</strong>g to those <strong>in</strong><br />

the La2O2S:Nd 3+ (1 wt%) optical ceramics (Figure 24b), because of the same reasons as <strong>in</strong> the<br />

case of absorption spectra.<br />

MULTIPHONON RELAXATION IN OXYSULFIDE CERAMICS [49]<br />

The 4 I11/2 state can be potentially a bottleneck dur<strong>in</strong>g 1-μm las<strong>in</strong>g and gives rise to<br />

transient absorption at laser wavelength. So, the faster the rate of multiphonon relaxation<br />

(MR), faster the depletion of the 4 I11/2 level and the smaller the losses [50].<br />

It is a well-known fact that the energy gaps of the 4 G7/2→ 4 G5/2; 2 G7/2 and the 4 I11/2→ 4 I9/2<br />

transitions of Nd 3+ are nearly the same <strong>in</strong> oxide (ħωmax = 800 cm -1 ) and fluoride (ħωmax = 400<br />

cm -1 ) crystals and their relaxation rates are mostly determ<strong>in</strong>ed by MR. The cut-off frequencies<br />

about 440 and 400 cm −1 , respectively, are found from Raman spectra of the Gd2O2S and<br />

La2O2S optical ceramics doped by Nd 3+ (Figure 25). Highly sensitive Raman spectrometer<br />

with photon count<strong>in</strong>g is used for measurements. The value ωmax for the La2O2S optical<br />

ceramics is <strong>in</strong> a good agreement with that measured <strong>in</strong> the La2O2S crystal [51]. Therefore, one<br />

can estimate the rate of the 4 I11/2→ 4 I9/2 transition from the rate of the 4 G7/2→ 4 G5/2; 2 G7/2<br />

b)

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