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