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exotic nuclei structure and reaction noyaux exotiques ... - IPN - IN2P3

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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

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