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VI Reunião de Trabalho Física Nuclear.pdf - Sociedade Brasileira ...

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Fig.6- The <strong>de</strong>-<br />

averagingfunc- tion D(a,E) 0<br />

calculated with<br />

In 4<br />

.<br />

11= 7.36 Em<br />

LiJ<br />

3<br />

(full line) and 0<br />

ft. 5.8 Em<br />

(dashed line).<br />

2<br />

F.<br />

011IIII I<br />

20 30 40 59 60 70 80 90 100'<br />

ECM (MeV)<br />

regular, with the second:peaking at E cm = 45 MeV attaining<br />

a value very close to the first major peaking at E cm o 23 MeV.<br />

This is in contrast to the finding of Ref. SO) where there was<br />

a great disparity in favor of the second peaking.<br />

It would be quite interesting to test the sensitivity<br />

of the <strong>de</strong>-averaging function to the anomalous radius experimentally<br />

by measuring averaged data for two different values of the<br />

averaging angle interval.<br />

II. STATIC AND DYNAMIC DEFORMATION EFFECTS: ILX MICE ABSCIRETICV<br />

Another important case showin a clear <strong>de</strong>viation from<br />

the optical behaviour involves the scattering of <strong>de</strong>formed<br />

targets and/or projectiles at energies close to the Coulomb<br />

barrier. As a result of the strong Coulomb excitation of<br />

collective states, one expects a gradual <strong>de</strong>population of the<br />

elastic channel, even at sub-barrier energies. A nice example<br />

showing this effect is presented in Fig. 7 involving the system<br />

120

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