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Volumen II - SAM

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Congreso <strong>SAM</strong>/CONAMET 2009 Buenos Aires, 19 al 23 de Octubre de 2009<br />

M2 [GPa]<br />

1.0<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0.0<br />

300 400 500 600 700 800 900 1000 1100<br />

T [K]<br />

Figure 3. Experimental loss modulus data and adjusted background.<br />

The line in Figure 4 is the HN function adjusted to the isolated loss peak. The activation energy H is 2.02 eV,<br />

while the parameters α is close to 0.5 and β is about 0.7; the peak temperature is 834 K.<br />

M 2 [GPa]<br />

1.0<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0.0<br />

300 400 500 600 700 800 900 1000 1100<br />

T [K]<br />

Figure 4. Isolated peak and adjusted function after background subtraction.<br />

The results for the resolved peak are in agreement with previous works on non-irradiated and neutronirradiated<br />

samples [14]. The damping peak in the sample has a value of Q -1 (M2/M1) about 16x10 3 which is<br />

twice larger than unirradiated and neutron irradiated samples (dose less than 1x10 -5 dpa, with 5 ppm<br />

irradiation produced defects). This is in agreement with a larger quantity of defects produced by the<br />

irradiation in the present work. In addition, the activation energy obtained for the loss peak is also in<br />

agreement with previous reported works [15].<br />

4. CONCLUSIONS<br />

This work presents a systematic procedure for the estimation and subtraction of the background in loss<br />

relaxation spectra. The only assumptions on the background function are quite reasonable from a physical<br />

standpoint, namely, that the general shape of the background corresponds to the low temperature side of a<br />

1141

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