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
Figure 2. Invariant mass distribution of e + e - pairs compared with the HSD vacuum and in-medium scenarios [4]. The HSD in-medium prediction took into account collisional broadening and simultaneous dropping masses of ρ 0 and ω in nuclear environment. Experimental data points are the same as in Figure 1. medium. The HSD calculation suggests that the most sensitive part of our spectrum to possible in-medium modifications should be the region of 0.5-0.8 GeV/c 2 (see Figure 2) . Non of the predicted results by transport code gives a fully convincing explanation of the data in the vector meson mass region. One of the reasons might be the parameterization of the elementary cross sections which overestimates the ρ 0 meson cross section measured in pp collisions [6]. Further progress will be made by extending our measurements to heavy reaction systems like Au+Au and Ag+Ag. References [1]. G. Agakichiev et al., HADES collaboration, Phys. Rev. Lett. 98 (2007) 052302 and Phys. Lett. B 43 (2008) 663 [2]. G. Agakichiev et al., HADES collaboration, arXiv:910.5875 [3]. K. Schmidt et al., Phys. Rev. C (2009) 064908 [4]. E.I. Bratkovskaya and W. Cassing, Nucl. Phys. A 807 (2008) 214-250 [5]. G. E. Brown and M. Rho, Phys. Rev. Lett. 66 (1991) 2720 [6]. F. Balestra et al., Phys. Rev. Lett. 89 (2002) 092001 31
Status of the HADES experiments (II): dilepton channels in elementary reactions IPNO Participation: J.L. Boyard, T. Hennino, T. Liu, E. Morinière, B. Ramstein, M. Sudol. Collaboration : CAS-Rez, FZR-Dresden, GSI-Darmstadt, INR-Moscow, INFN/LNSCatania, INFN/University-Milano, ITEP-Moscow, SIP/Jag. Univ-Cracow, JW Goethe Univ.-Frankfurt, JINR- Dubna, J Liebig Univ.-Giessen, LIP-Coimbra, TUM-München, Univ., Santiago de Compostela, Univ. of Cyprus-Nicosia, NPI-Rez, Univ. Valencia La production de dielectrons en réactions pp et dp à 1.25 GeV/nucléon a été étudiée avec HADES (High Acceptance DiElectron Spectrometer) à GSI. Les résultats obtenus en canaux inclusifs et exclusifs sont présentés et comparés à des modèles. Pour la première fois, le processus de décroissance Dalitz du ( Ne + e - ) a pu être identifié. Le taux d’événements mesurés est en accord avec le rapport de branchement calculé en QED (4.2 10 -5 ). Motivation The first results from the HADES collaboration obtained in C+C and Ar+KCl systems [1] have pointed to the important role played by the nucleon -nucleon bremsstrahlung and Daliz decay processes in the dilepton production at intermediate invariant masses ( 0.15 < M ee < 0.5 GeV/c 2 ), The contribution of these dilepton sources has therefore to be clarified, as a prerequisite to the study of and in-medium properties. In particular, the new results from the HSD transport model [2] use the recent bremsstrahlung calculation from [3], which is a factor 2-4 higher than other predictions [4]. Meanwhile, other transport models reproduce quite well the data with different relative contributions of bremstrahlung and Dalitz decay processes. Inclusive dilepton spectra: Following these motivations, inclusive e + e - spectra (Fig.1) were measured in the p+p and quasi-free n+p reactions studied with HADES in experiments with the GSI proton and deuterium beams at 1.25 GeV [5], i.e. below the production threshold. Two different approaches for the analysis of these spectra were followed in our event generator PLUTO [6]. The first one is based on the dominance of the resonance. In analogy with the transport model calculations, it provides a description of the following channels: N N e e - ( 0 Dalitz decay) Ne e - ( Dalitz decay) The details of the treatment of the production and pionic decay could be checked quite precisely, using the new measurements by HADES in the hadronic channels [7]. Two options for the N- transition form factors are used: either a constant magnetic form factor (G M =3, G E =0, G C =0) in agreement with the photon-point measurements, or the two-component quark-model [8], which is mainly based on the Vector Meson Dominance model in our energy range. As shown on fig.1, there is a good agreement, for both reactions, between the dilepton yield measured at low invariant masses and the simulation of the 0 Dalitz decay. In the case of the pp reaction, the region of invariant masses larger than 140 MeV/c 2 is well described by the simulation of the Dalitz decay. The agreement is even better when the two-component Fig. 1: Invariant mass distribution of electron pairs measured in p+p (top) and quasi-free n+p (bottom) reactions at a beam energy of 1.25 GeV. The dashed and long-dashed lines show the contributions of 0 and Dalitz decays, respectively, in simulations using the resonance model. The enhancement due to the N- transition form factor [8] is shown as the grey area. The dashed and full lines are the results of OBE models [3] and [4], respectively. The contribution has been added in the case of the n+p reaction. 32
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Status of the HADES experiments (II):<br />
dilepton channels in elementary <strong>reaction</strong>s<br />
<strong>IPN</strong>O Participation: J.L. Boyard, T. Hennino, T. Liu, E. Morinière, B. Ramstein, M. Sudol.<br />
Collaboration : CAS-Rez, FZR-Dresden, GSI-Darmstadt, INR-Moscow, INFN/LNSCatania,<br />
INFN/University-Milano, ITEP-Moscow, SIP/Jag. Univ-Cracow, JW Goethe Univ.-Frankfurt, JINR-<br />
Dubna, J Liebig Univ.-Giessen, LIP-Coimbra, TUM-München, Univ., Santiago de Compostela, Univ.<br />
of Cyprus-Nicosia, NPI-Rez, Univ. Valencia<br />
La production de dielectrons en réactions pp et dp à 1.25 GeV/nucléon a été étudiée avec HADES (High<br />
Acceptance DiElectron Spectrometer) à GSI. Les résultats obtenus en canaux inclusifs et exclusifs sont<br />
présentés et comparés à des modèles. Pour la première fois, le processus de décroissance Dalitz du (<br />
Ne + e - ) a pu être identifié. Le taux d’événements mesurés est en accord avec le rapport de branchement<br />
calculé en QED (4.2 10 -5 ).<br />
Motivation<br />
The first results from the HADES collaboration obtained<br />
in C+C <strong>and</strong> Ar+KCl systems [1] have<br />
pointed to the important role played by the nucleon<br />
-nucleon bremsstrahlung <strong>and</strong> Daliz decay processes<br />
in the dilepton production at intermediate<br />
invariant masses ( 0.15 < M ee < 0.5 GeV/c 2 ), The<br />
contribution of these dilepton sources has therefore<br />
to be clarified, as a prerequisite to the study of<br />
<strong>and</strong> in-medium properties.<br />
In particular, the new results from the HSD transport<br />
model [2] use the recent bremsstrahlung calculation<br />
from [3], which is a factor 2-4 higher than<br />
other predictions [4]. Meanwhile, other transport<br />
models reproduce quite well the data with different<br />
relative contributions of bremstrahlung <strong>and</strong> Dalitz<br />
decay processes.<br />
Inclusive dilepton spectra:<br />
Following these motivations, inclusive e + e - spectra<br />
(Fig.1) were measured in the p+p <strong>and</strong> quasi-free<br />
n+p <strong>reaction</strong>s studied with HADES in experiments<br />
with the GSI proton <strong>and</strong> deuterium beams at 1.25<br />
GeV [5], i.e. below the production threshold.<br />
Two different approaches for the analysis of these<br />
spectra were followed in our event generator<br />
PLUTO [6]. The first one is based on the dominance<br />
of the resonance. In analogy with the<br />
transport model calculations, it provides a description<br />
of the following channels:<br />
N N e e - ( 0 Dalitz decay)<br />
Ne e - ( Dalitz decay)<br />
The details of the treatment of the production<br />
<strong>and</strong> pionic decay could be checked quite precisely,<br />
using the new measurements by HADES in the<br />
hadronic channels [7]. Two options for the N-<br />
transition form factors are used: either a constant<br />
magnetic form factor (G M =3, G E =0, G C =0) in agreement<br />
with the photon-point measurements, or the<br />
two-component quark-model [8], which is mainly<br />
based on the Vector Meson Dominance model in<br />
our energy range. As shown on fig.1, there is a<br />
good agreement, for both <strong>reaction</strong>s, between the<br />
dilepton yield measured at low invariant masses<br />
<strong>and</strong> the simulation of the<br />
0 Dalitz decay. In the<br />
case of the pp <strong>reaction</strong>, the region of invariant<br />
masses larger than 140 MeV/c 2 is well described<br />
by the simulation of the Dalitz decay. The agreement<br />
is even better when the two-component<br />
Fig. 1: Invariant mass distribution of electron pairs<br />
measured in p+p (top) <strong>and</strong> quasi-free n+p (bottom)<br />
<strong>reaction</strong>s at a beam energy of 1.25 GeV. The dashed<br />
<strong>and</strong> long-dashed lines show the contributions<br />
of<br />
0 <strong>and</strong> Dalitz decays, respectively, in simulations<br />
using the resonance model. The enhancement<br />
due to the N- transition form factor [8] is<br />
shown as the grey area. The dashed <strong>and</strong> full lines<br />
are the results of OBE models [3] <strong>and</strong> [4], respectively.<br />
The contribution has been added in the case<br />
of the n+p <strong>reaction</strong>.<br />
32