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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<br />

due to the virtual GQR excitation together with other<br />

Ruth<br />

small effects, has been observed recently by Lynch et al. 16) .<br />

Although we have presented our expresJ<br />

a<br />

ion for .--<br />

° R<br />

Eq. (23), that correspond to the case of one real stationary<br />

phase point, a<strong>de</strong>quate at sub-barrier energies, the generalization<br />

to above barrier energies is quite simple. This comes about<br />

as a result of the rather slow it-<strong>de</strong>pen<strong>de</strong>nce of Vpol(r), which<br />

even in cases involving two stationary phase points, i.e.<br />

Coulomb rainbow scattering or Fresnel diffraction, can be<br />

factored out as a common factor to both contributions. This is<br />

particularly valid near the rainbow angle (or critical Fresnel<br />

angle). Therefore we may write in general<br />

ck-f tz (.12—(e))/<br />

do-<br />

cf*<br />

f.da,<br />

where I corresponds to the average value of the two stationary<br />

phase angular momenta. To show the a<strong>de</strong>quacy of the above<br />

<strong>de</strong>scription we show in figure (9) the calculation of 0 °<br />

Ruth<br />

for<br />

16 0+ 184 W at EL =90 MeV done both though optical mo<strong>de</strong>l<br />

calculation that inclu<strong>de</strong>d V<br />

pol<br />

and the result obtained from<br />

Eq. (26) with 1 0<br />

)<br />

calculated with an optical potential<br />

Ruth o<br />

that does not contain V<br />

pol . The agreement is very, good.<br />

128<br />

(26)

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