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

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Relic astrophysical <strong>and</strong> cosmological neutrinos<br />

<strong>and</strong> their discovery<br />

<strong>IPN</strong>O Participation: C. Volpe, J. Kneller, S. Galais<br />

Collaboration : R. Lazauskas (IPHC Strasbourg), C. Lunardini (University of Arizona), P. Vogel<br />

(CALTECH)<br />

Deux fonds de neutrinos n’ont jamais été observé: les neutrinos reliques de supernovae (à effondrement<br />

gravitationnel) et les neutrino cosmologiques, provenant de l’Univers primordiale. Les premiers pourront<br />

etre observés dans les prochains détécteurs de gr<strong>and</strong>e taille, selon les calculs actuels. Une étude de faisabilité<br />

(LAGUNA, FP7, 2008-10) se déroule à l’heure actuelle. Nous réalisons des calculs très poussés de<br />

propagation des neutrinos dans les étoiles massives et nous faisons des prédictions pour ces observatoires<br />

de prochaine génération. Nous explorons aussi des voies alternatives. Par exemple nous avons étudié la<br />

possibilité d’observer les neutrinos reliques provenant des explosions galactiques par la mesure du Technetium-97<br />

dans la roche. En ce qui concerne les neutrinos cosmologiques, nous n’avons à présent que des<br />

effets indirects, dans BBN et sur les gr<strong>and</strong>es <strong>structure</strong>s. Une stratégie interessante a été proposée récemment:<br />

la capture sur <strong>noyaux</strong> radioactifs.<br />

Two diffuse neutrino backgrounds have never<br />

been observed : the one formed by past corecollapse<br />

supernova explosions <strong>and</strong> the cosmological<br />

background produced by the Early Universe.<br />

The energy range of these two backgrounds are<br />

very different, the first being in the several tens of<br />

MeV energy range while the second has typical<br />

energies of meV.<br />

The diffuse supernova neutrino background<br />

The observation of the relic supernova neutrino<br />

background would bring key information on the<br />

star formation rate, on the supernova dynamics<br />

<strong>and</strong> on unknown neutrino properties. The current<br />

best limits come from the Super-Kamiok<strong>and</strong>e <strong>and</strong><br />

SNO observations. Present predictions show that<br />

the use of large scale observatories, such as<br />

MEMPHYS, GLACIER or LENA (LAGUNA DS,<br />

FP7, 2008-2010), or of advanced technologies<br />

(like adding Gadolinium to water) should bring to<br />

the diffuse supernova neutrino background discovery.<br />

We have performed the very first calculations<br />

including the neutrino-neutrino interaction <strong>and</strong><br />

shock waves <strong>and</strong> shown the latter impact the predictions<br />

at the level of 10-20%. Such variations are<br />

important since they are of the same order as the<br />

variations induced by the still unknown neutrino<br />

parameters (third neutrino mixing angle <strong>and</strong> hierarchy).<br />

Our calculations show that shock wave effects<br />

should be included in future predictions. With<br />

this aim we have proposed a schematic model.<br />

Besides we have shown that the shock wave suppresses<br />

the sensitivity on the neutrino-neutrino<br />

interaction [1].<br />

In [2] we have investigated the possibility to observe<br />

relic galactic supernova neutrinos by the<br />

measurement of Technetium-97 abundance in Molybdenum-98<br />

ore, following a previous idea of Hax<br />

ton <strong>and</strong> Jonhson [3]. Indeed electron neutrinos interact<br />

with Mo-98 <strong>and</strong> depending on their energy<br />

can eject one neutron leaving Tc-97. This specific<br />

process is particularly interesting since the threshold<br />

suppresses the huge solar neutrino background.<br />

We have perfomed the most updated calculations<br />

including the progress in neutrino physics <strong>and</strong> including<br />

our underst<strong>and</strong>ing of neutrino propagation<br />

in dense media. Our results show that the contribution<br />

coming from relic supernova is at the level of<br />

10% of the total contribution (solar plus supernovae).<br />

We conclude that to make this strategy<br />

clearly attractive one needs very precise solar neutrino<br />

measurements <strong>and</strong> systematic measurements<br />

of neutrino-nucleus cross sections. Note that the<br />

experimental sensitivity reaches the level required<br />

for this measurement.<br />

[1] S. Galais, J. Kneller, C. Volpe, J. Gava, Phys.<br />

Rev. D 81, 053002 (2010, arXiv: 0906.5294 .<br />

[2] R. Lazauskas, C. Lunardini, C. Volpe, JCAP<br />

0904, 029 (2009), arXiv: 0901.0581 .<br />

[3] Haxton <strong>and</strong> Johson, Nature 333, 325 (1988).<br />

The cosmological neutrino background<br />

The interest the capture on radioactive <strong>nuclei</strong> for<br />

cosmological neutrios was first pointed out by<br />

Weinberg. In a recent paper Cocco, Mangano <strong>and</strong><br />

Messina have used it to show the interest for the<br />

cosmological neutrino backgroiund observation [4].<br />

In [5] we have analyzed the possibility <strong>and</strong> calculated<br />

the number of events associated to the capture<br />

on tritium. Since this process does not have<br />

any threshold, the associated cross sections are<br />

very large.<br />

[4] Cocco, Mangano <strong>and</strong> Messina JCAP 0706, 015<br />

(2007), arXiv: 0703075.<br />

[5] R. Lazauskas, P. Vogel, C. Volpe, Jour. Phys. G<br />

35, 025001 (2008), arXiv: 0710.5312.<br />

80

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