dc.contributor.author |
XENOULIS, AC |
en |
dc.contributor.author |
PAPADOPOULOS, CT |
en |
dc.contributor.author |
VLASTOU, R |
en |
dc.contributor.author |
ADAMIDES, E |
en |
dc.date.accessioned |
2014-03-01T01:42:53Z |
|
dc.date.available |
2014-03-01T01:42:53Z |
|
dc.date.issued |
1994 |
en |
dc.identifier.issn |
0375-9474 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/23965 |
|
dc.subject |
F-19 |
en |
dc.subject |
SI-30 |
en |
dc.subject |
V-51 |
en |
dc.subject |
(LI,X(LI-7)) |
en |
dc.subject |
E = 10-18 MEV |
en |
dc.subject |
MEASURED RELATIVE SIGMA(E) FOR (P2N) |
en |
dc.subject |
(DN) |
en |
dc.subject |
T-EMISSION |
en |
dc.subject |
F-19(L,X(L-7)) |
en |
dc.subject |
E = 10-18 MEV |
en |
dc.subject |
MEASURED ABSOLUTE SIGMA(E) FOR (P2N) |
en |
dc.subject |
(DN) |
en |
dc.subject |
T-EMISSION |
en |
dc.subject |
CALCULATED RELATIVE |
en |
dc.subject |
ABSOLUTE SIGMA(E) FOR P2N |
en |
dc.subject |
DN AND T-EVAPORATION |
en |
dc.subject |
STATISTICAL MODEL |
en |
dc.subject.classification |
Physics, Nuclear |
en |
dc.subject.other |
BREAKUP |
en |
dc.subject.other |
LI-7 |
en |
dc.subject.other |
COMPETITION |
en |
dc.subject.other |
FUSION |
en |
dc.subject.other |
C-12 |
en |
dc.title |
MECHANISMS INVOLVED IN THE PRODUCTION OF THE A-3 RESIDUAL NUCLEUS BY P2N, DN AND T-EMISSION IN LI-7-INDUCED NUCLEAR-REACTIONS |
en |
heal.type |
journalArticle |
en |
heal.language |
English |
en |
heal.publicationDate |
1994 |
en |
heal.abstract |
The competition between p2n, dn and t emission for three Li-7-induced reactions on F-19, Si-30 and V-51 targets as well as the absolute p2n, dn and t emission cross sections in the reaction F-19 + Li-7 have been measured, each at several bombarding energies, and compared with relevant statistical-model calculations. This comparison, indicating that at least one of the dn and p2n exit channels is induced with significant strength by a non-statistical mechanism, suggests that, in addition to the traditionally expected direct alpha transfer and evaporation, a third non-statistical reaction mechanism is involved even at very low bombarding energies. The characteristics of this third mechanism are presented and discussed. |
en |
heal.publisher |
ELSEVIER SCIENCE BV |
en |
heal.journalName |
NUCLEAR PHYSICS A |
en |
dc.identifier.isi |
ISI:A1994PL94100012 |
en |
dc.identifier.volume |
579 |
en |
dc.identifier.issue |
1-2 |
en |
dc.identifier.spage |
197 |
en |
dc.identifier.epage |
206 |
en |