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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Pairing properties in <strong>nuclei</strong> <strong>and</strong> in neutron stars<br />
<strong>IPN</strong>O Participation: J. Margueron, E. Khan<br />
Collaboration : University of Aizu-Wakamatsu, Tohoku University, Institut d'Astronomie et d'Astrophysique<br />
de Bruxelles, N<strong>IPN</strong>E Bucharest.<br />
Les propriétés d’appariement des <strong>noyaux</strong> ainsi que des étoiles à neutrons sont étudiés dans des modèles<br />
de champ moyen Hartree-Fock-Bogoliubov. Pour cela, nous proposons une interaction d’appariement de<br />
portée nulle et dépendante de la densité, non-empirique (non-ajusté sur des <strong>noyaux</strong>), qui reproduit la longueur<br />
de diffusion dans le canal 1 S 0 ainsi que les calculs ab-initio de gap dans la matière uniforme. Pour<br />
reproduire à la fois la matière symétrique et la matière de neutrons, nous avons du introduire une dépendance<br />
en isospin dans la force d’appariement. Nous discutons aussi les effets de polarisation du milieu audelà<br />
du premier ordre BCS. D’une étude systématique sur des <strong>noyaux</strong> semi-magiques (chaines isotopiques<br />
et isotoniques) nous avons montré que l’interaction d’appariement au premier ordre BCS reproduit très bien<br />
les données expérimentales. Nous avons montré l’impact des différent modèles d’appariement sur le refroidissement<br />
des étoiles à neutrons.<br />
The pairing gap is an important quantity to underst<strong>and</strong><br />
the cooling of neutron stars, as it modifies<br />
the specific heat as well as neutrino emission processes<br />
(1). It is also important to underst<strong>and</strong> the<br />
Glitches of neutron stars. A precise <strong>and</strong> well constrained<br />
theory for pairing in neutron stars is thus<br />
necessary.<br />
Among these constrains are those given by <strong>nuclei</strong>.<br />
In a marked contrast with electronic systems, the<br />
nuclear interaction is already attractive in the first<br />
order approximation (BCS). Nevertheless, it has<br />
been shown that higher order contributions, such<br />
that medium polarization, may lead to important<br />
corrections to the nuclear interaction in the particle<br />
-particle channel <strong>and</strong> therefore to the pairing gap in<br />
uniform matter as well as in finite <strong>nuclei</strong>.<br />
We have proposed an effective density-dependent<br />
pairing interaction that reproduces both the neutron-neutron<br />
scattering length in the 1 S 0 channel<br />
<strong>and</strong> the neutron pairing gap in uniform matter (2).<br />
In order to simultaneously describe the density<br />
dependence of the neutron pairing gap for both<br />
symmetric <strong>and</strong> neutron matter, it was necessary to<br />
include an isospin dependence in the effective<br />
pairing interaction. Depending on whether the medium<br />
polarization effects on the pairing gap calculated<br />
in Ref.(3) are taken into account or not, we<br />
have proposed two different density dependences<br />
in the pairing interaction (hereafter named Bare<br />
<strong>and</strong> Induced). The comparison of the predictions of<br />
these interactions with the odd-even mass staggering<br />
(OEMS) in semi-magic <strong>nuclei</strong> is shown in Fig.1<br />
(for isotopic chain) <strong>and</strong> Fig.2 (for isotonic chain).<br />
The HFB calculations based on the IS+IV Bare<br />
pairing force well account for the experimental<br />
OEMS (similar comparison for the binding energy<br />
<strong>and</strong> the two neutrons separation energy are shown<br />
in Ref.(4)). This result suggests that a global nonempirical<br />
pairing interaction depending on both the<br />
IS <strong>and</strong> IV densities can be adjusted to be used for<br />
a wide range of the nuclear chart. In contrast, the<br />
IS Bare force, which is adjusted only in symmetric<br />
matter, fails to correctly reproduce isotopic <strong>and</strong><br />
isotonic systematic, <strong>and</strong> the IS+IV induced pairing<br />
force, which includes medium polarization, under<br />
estimate the OESM.<br />
In Ref.(4) it has also been shown, with the local<br />
density approximation (LDA), that the pairing field<br />
deduced from the pairing gaps in infinite matter<br />
reproduces qualitatively well the pairing field for<br />
finite <strong>nuclei</strong> obtained with the HFB method.<br />
Despite the differences between finite <strong>nuclei</strong> <strong>and</strong><br />
neutron stars matter, self-consistent mean field<br />
models could be extrapolated to infinite matter under<br />
the extreme conditions realized in stars (1,5).<br />
The crust of neutron stars is made of nuclear clusters<br />
where the HFB model is applicable within the<br />
Wigner-Seitz approximation. In Ref.(5), a comparison<br />
between b<strong>and</strong> theory <strong>and</strong> mean field approximation<br />
has sheld light on the domain of application<br />
of mean field models. A systematic calculation of<br />
the neutron specific heat in the crust of neutron<br />
stars has therefore been performed <strong>and</strong> has been<br />
used in a model for the cooling of neutron stars (1).<br />
The effects of the clusters are moderated, but nonnegligeable.<br />
Larger effects induced by the pairing<br />
force have been observed. These results motivate<br />
the comparison of the different pairing interactions<br />
in finite <strong>nuclei</strong>, such as in Ref.(4), with an improved<br />
description of medium polarization.<br />
References:<br />
(1) M. Fortin, F. Grill, J. Margueron,<strong>and</strong> N. S<strong>and</strong>ulescu,<br />
submitted to Phys. Rev. C,<br />
ArXiv/0910.5488(nucl-th).<br />
(2) J. Margueron, H. Sagawa, <strong>and</strong> K. Hagino,<br />
Phys. Rev. C 76, 064316 (2007).<br />
(3) L. G. Cao, U. Lombardo, <strong>and</strong> P. Schuck, Phys.<br />
Rev. C 74, 064301 (2006).<br />
(4) J. Margueron, H. Sagawa, <strong>and</strong> K. Hagino,<br />
Phys. Rev. C 77, 054309 (2008).<br />
(5) N. Chamel, J. Margueron, E. Khan, Phys. Rev.<br />
C 79, 012801 (2009).<br />
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