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

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

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a convenient and useful "language". with which, the elastic<br />

scattering may be <strong>de</strong>scribed and analyzed.<br />

Nuclei clearly exhibit other features besi<strong>de</strong>s the<br />

gross ones mentioned above. These other properties are more<br />

closely related to specific nuclear structure aspects, e.g.,<br />

<strong>de</strong>formation. Therefore one would expect several important<br />

<strong>de</strong>viations from the optical behavior. Here, we shall discuss<br />

in <strong>de</strong>tail two such <strong>de</strong>viations.<br />

The paper is divi<strong>de</strong>d into two sections. The first,<br />

section II <strong>de</strong>als-with the anomalous large-angle scattering of<br />

na-nuclei. We shall concentrate on direct reaction interpretation<br />

of the anomalous behaviour and leave out completely intermediate<br />

structure resonance explanation. In section III we turn to the<br />

effect of nuclear <strong>de</strong>formation on -- at not too large energies.<br />

R<br />

A convenient vehicle through which one may discuss the effect<br />

of the coupling to low-lying collective states is long-range<br />

absorption, which we shall discuss in <strong>de</strong>tail.<br />

II. ANOMALOUS BACK-ANGLE SCATTERING<br />

A well-known case usually cited as exhibiting<br />

<strong>de</strong>viations from pure optical behaviour is that referring to<br />

systems behaving anomalously at back angles (a-scattering,<br />

160+28 Si , etc.). What one usually discovers in these systems<br />

is a large increase in --2-- (0) at back angles accompanied<br />

° Ruth<br />

by a rather regular angular structure. Further, the excitation<br />

function —2-- In,E) at 0=n exhibits quite a conspicuous<br />

o Ruth<br />

intermediate structure with an average width of about 1 MeV.<br />

To put the situation into perspective we show in Fig. 1 a plot<br />

d _ e,<br />

of the experimental excitation function --- (E,n)<br />

dr E<br />

for<br />

16 28<br />

0 + Si and 16 0+ 30 Si. One sees clearly that the data sit<br />

log

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