6533b86cfe1ef96bd12c82f9
RESEARCH PRODUCT
Shell-model computed cross sections for charged-current scattering of astrophysical neutrinos off 40Ar
Joel KostensaloKai ZuberJouni Suhonensubject
solar radiationSHELL model01 natural sciencesdark matternucleus-neutrino interactionsNuclear physicspimeä aineCross section (physics)0103 physical sciences010306 general physicsauringonsäteilydark energyCharged currentPhysicsta114010308 nuclear & particles physicsScatteringNuclear shell modelneutriinotshell modelneutrinosDistribution (mathematics)solar neutrinosHigh Energy Physics::ExperimentNeutrinopimeä energiaParametrizationdescription
Charged-current (anti)neutrino-$^{40}\mathrm{Ar}$ cross sections for astrophysical neutrinos have been calculated. The initial and final nuclear states were calculated using the nuclear shell model. The folded solar-neutrino scattering cross section was found to be $1.78(23)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}42}\phantom{\rule{4pt}{0ex}}{\mathrm{cm}}^{2}$, which is higher than what the previous papers have reported. The contributions from the ${1}^{\ensuremath{-}}$ and ${2}^{\ensuremath{-}}$ multipoles were found to be significant at supernova-neutrino energies, confirming the random-phase approximation (RPA) result of a previous study. The effects of neutrino flavor conversions in dense stellar matter (matter oscillations) were found to enhance the neutrino-scattering cross sections significantly for both the normal and inverted mass hierarchies. For the antineutrino scattering, only a small difference between the nonoscillating and inverted-hierarchy cross sections was found, while the normal-hierarchy cross section was 2--3 times larger than that of the nonoscillating cross section, depending on the adopted parametrization of the Fermi-Dirac distribution. This property of the supernova-antineutrino signal could probably be used to distinguish between the two hierarchies in megaton LAr detectors.
year | journal | country | edition | language |
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2018-03-06 | Physical Review C |