exotic nuclei structure and reaction noyaux exotiques ... - IPN - IN2P3
exotic nuclei structure and reaction noyaux exotiques ... - IPN - IN2P3
exotic nuclei structure and reaction noyaux exotiques ... - IPN - IN2P3
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Isospin effects on fragment <strong>and</strong> particle multiplicities<br />
in multifragmentation<br />
<strong>IPN</strong>O Participation: F. Gagnon-Moisan, B. Borderie, E. Galichet, M. F. Rivet<br />
Collaboration : INDRA<br />
LPC Caen, ENSICAEN, Université de Caen, CNRS/<strong>IN2P3</strong>, Caen, France<br />
GANIL, CEA et CNRS/<strong>IN2P3</strong>, Caen, France<br />
<strong>IPN</strong> Lyon, Université Claude Bernard Lyon1, CNRS/<strong>IN2P3</strong>, Villeurbanne, France<br />
IRFU/SPhN, CEA/Saclay Gif-sur-Yvette, France<br />
Laboratoire de Physique Nucléaire, Université Laval, Québec, Canada<br />
Dpt de Scienze Fisiche e Sez. INFN, Università di Napoli « Federico II », Napoli, Italy<br />
N<strong>IPN</strong>E, Bucharest Magurele, Romania<br />
Les effets d’isospin sont étudiés dans les collisions centrales conduisant à la multifragmentation de sources<br />
de quasi-fusion de projectiles de xénon ( 124,136 Xe) accélérés à 32 et 45 MeV/nucléon et de <strong>noyaux</strong> cibles<br />
d’étain ( 112,124 Sn). Les mesures montrent que les multiplicités de produits chargés dépendent du rapport<br />
N/Z du système total (projectile+cible), mais pas de la configuration particulière de la voie d’entrée<br />
(pour un même N/Z). A une énergie incidente donnée on observe que, lorsque N/Z augmente, la multiplicité<br />
de particules légères (H, He) décroît alors que la multiplicité de fragments croît. Cet effet peut être attribué<br />
à l’effet stabilisateur d’un plus gr<strong>and</strong> nombre de neutrons disponibles pour former des fragments. Des simulations<br />
de collisions à l’aide d’un code de transport reproduisent la tendance observée expérimentalement.<br />
60°, in order to eliminate those resulting from collisions<br />
keeping a strong binary character.<br />
System<br />
N/Z sys<br />
124 Xe+ 112 Sn 1.269<br />
124 Xe+ 124 Sn 1.385<br />
129 Xe+ nat Sn 1.385<br />
136 Xe+ 112 Sn 1.385<br />
136 Xe+ 124 Sn 1.5<br />
With the advent of rare ions accelerators expected<br />
in a near future, nuclear physicists hope to get<br />
information on the symmetry energy term of the<br />
Equation of State of <strong>nuclei</strong>, particularly on its density<br />
dependence. In the mean time stable isotopes<br />
which cover a large enough domain in isospin (N/<br />
Z) can provide precious information. In this aim the<br />
INDRA collaboration studied collisions between<br />
124,136 Xe projectiles, accelerated to 32 <strong>and</strong> 45 MeV/<br />
nucleon by the GANIL facility, <strong>and</strong> 112,124 Sn targets.<br />
The effects of a variation of the N/Z of the composite<br />
system, N/Z sys , <strong>and</strong> those of different entrance<br />
channels leading to the same composite system<br />
were explored. Previous results were added to enrich<br />
this study.<br />
Experimental data<br />
The charged <strong>reaction</strong> products were collected<br />
with the INDRA array. Quasi-fusion <strong>reaction</strong>s were<br />
selected by requiring a high quality of detection in<br />
charge <strong>and</strong> linear momentum: the sum of the<br />
charges of the detected products should be at<br />
least equal to 80 (the total system charge is 104),<br />
<strong>and</strong> that of their pseudo-impulsion (ZxV) should be<br />
greater than 75% of the projectile one. Moreover<br />
we selected events with a flow angle larger than<br />
Figure 1: Total charged product multiplicities<br />
(triangles <strong>and</strong> full lines) for the different Xe+Sn<br />
systems at 32 (open symbols) <strong>and</strong> 45 (close<br />
symbols) MeV/nucleon vs the system N/Z.<br />
Each color characterizes a given projectile.<br />
See table for the systems. All statistical errors<br />
amount to 0.04.<br />
The evolution of different multiplicities of charged<br />
products is followed as a function of the incident<br />
energy <strong>and</strong> of the N/Z of the composite system.<br />
Figure 1 <strong>and</strong> 2 show the results for the total multiplicity,<br />
M tot , <strong>and</strong> the light charged particle multiplicity,<br />
M lcp . Both increase with the incident energy,<br />
they are in all cases about 30% higher at 45 MeV/<br />
nucleon. Conversely, M tot <strong>and</strong> M lcp decrease when<br />
the composite system gets more neutron-rich. M lcp<br />
is 15% smaller for the neutron-richer system than<br />
for the poorer while M tot is only smaller by 9%. This<br />
104