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
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
Latest Results from GRAAL<br />
<strong>IPN</strong>O Participation: J.-P. Didelez, M. Guidal, E. Hourany, R. Kunne<br />
Collaboration : GRAAL<br />
Depuis l’arrêt de l’expérience GRAAL à l’ESRF de Grenoble en 2008, plusieurs publications sont apparues.<br />
Elles résultent de l’analyse des états finals complexes menée à bien par les différentes équipes de la Collaboration<br />
GRAAL. Il s’agit de la photo-production simultanée de π° et de η, la mesure des observables de<br />
polarisation correspondant au canal KΛ, la photo-production de π° et de η sur le neutron et enfin,<br />
l’observation des effets du milieu nucléaire affectant la photo-production de mésons sur les <strong>noyaux</strong>.<br />
Simultaneous photoproduction of π° <strong>and</strong><br />
ηmesons on the proton<br />
The two baryonic resonances S11(1535) <strong>and</strong> Δ<br />
(1700) are expected to be dynamically generated<br />
in this channel, as quasi-bound states of a meson<br />
<strong>and</strong> a baryon. It is remarkable that there is almost<br />
no excitation of the S11(1535), but exclusive<br />
excitation of the Δ(1700), decaying to η Δ(1232)<br />
<strong>and</strong> then to η π° p. This decay mode for the Δ<br />
(1700) was not known before. Therefore, the Δ<br />
(1700) could be considered as a Δ(1232) + η in the<br />
same way as the S11(1535) can be described as a<br />
N + η system (Ref. 1).<br />
Polarization observables for the γp → KΛ<br />
<strong>reaction</strong><br />
The KΛ channel has been presented since the<br />
beginning of the GRAAL venture, as the most<br />
promising one, because it allows to measure<br />
double polarization observables, the Λ polarization<br />
in the final state being accessible through its decay<br />
products. The double polarization (beam-recoil)<br />
observables Ox <strong>and</strong> Oz have been measured<br />
from threshold to 1500 MeV. Values for the target<br />
asymmetry T could also be extracted, despite the<br />
use of an unpolarized target. Those new data<br />
confirm the complexity of this channel, by requiring<br />
inclusion of poorly known resonances in theoretical<br />
models (Ref. 2).<br />
Photoproductionon of π° or η meson on the<br />
neutron<br />
The beam asymmetry Σ for π° has been measured<br />
from quasi-free nucleons in a deuterium target.<br />
Results are very similar to those obtained with a<br />
free proton target below 0.82 GeV <strong>and</strong> significantly<br />
different at higher energies (Ref. 3). The values<br />
are fairly well reproduced by recent partial wave<br />
analysis.<br />
Σ beam asymmetries <strong>and</strong> cross sections for η have<br />
been deduced from the photoproduction on quasifree<br />
nucleons in a deuterium target. The analysis<br />
has been completed by our late colleague E. Hourany<br />
using an original method similar to the one<br />
used for the double π° photoproduction on the<br />
neutron (Ref 4). The GRAAL detector allows com<br />
Figure 1 : In part (a), various data on the total<br />
cross section for η photoproduction on the proton.<br />
In (b), the ratio of the cross section on the neutron<br />
to the one on the proton is shown: by solid squares<br />
(this work), thick line from the MAID code <strong>and</strong> thin<br />
line from Zhao model. In (c), the total cross section<br />
on the free proton deduced from (a): empty circles<br />
<strong>and</strong> the one scaled for the free neutron: dots.<br />
Predictions from MAID <strong>and</strong> Zhao: thick <strong>and</strong> thin<br />
lines respectively (continuous for the neutron <strong>and</strong><br />
dotted for the proton).<br />
plete kinematical reconstruction of the final state<br />
<strong>and</strong> therefore, determination of the momentum of<br />
the so called « spectator nucleon ». This in turn<br />
permits the selection of quasi-free events <strong>and</strong> corrections<br />
for any underlying background.<br />
The analysis compares quasi-free nucleon data<br />
(neutron <strong>and</strong> proton) to previous free proton data<br />
to access « free » neutron observables.<br />
As shown on Fig. 1, the total cross section on the<br />
neutron is found to be higher than the proton one<br />
50