Abstract

Background: Large argon-based neutrino detectors, such as those planned for the Deep Underground Neutrino Experiment, have the potential to provide unique sensitivity to low-energy (few to tens of MeV) electron neutrinos produced by core-collapse supernovae. Despite their importance for neutrino energy reconstruction, nuclear de-excitations following charged-current $\nu_e$ absorption on $^{40}$Ar have never been studied in detail at supernova energies. Purpose: I develop a model of nuclear de-excitations that occur following the $^{40}\mathrm{Ar}(\nu_e,e^{-})^{40}\mathrm{K}^*$ reaction. This model is applied to the calculation of exclusive cross sections. Methods: A simple expression for the inclusive differential cross section is derived under the allowed approximation. Nuclear de-excitations are described using a combination of measured $\gamma$-ray decay schemes and the Hauser-Feshbach statistical model. All calculations are carried out using a novel Monte Carlo event generator called MARLEY (Model of Argon Reaction Low Energy Yields). Results: Various total and differential cross sections are presented. Two de-excitation modes, one involving only $\gamma$-rays and the other including single neutron emission, are found to be dominant at few tens-of-MeV energies. Conclusions: Nuclear de-excitations have a strong impact on the achievable energy resolution for supernova $\nu_e$ detection in liquid argon. Tagging events involving neutron emission, though difficult, could substantially improve energy reconstruction. Given a suitable calculation of the inclusive cross section, the MARLEY nuclear de-excitation model may readily be applied to other scattering processes.

Highlights

  • Core-collapse supernovae are exceptionally intense sources of tens-of-MeV neutrinos and antineutrinos of all flavors

  • While much remains to be done to fully exploit the lowenergy capabilities of liquid argon time projection chambers (LArTPCs), a first demonstration by the ArgoNeuT [27] experiment of reconstruction of MeVscale activity due to accelerator-neutrino-induced neutrons and de-excitation γ rays achieved a detection threshold of around 200–300 keV [28]. These encouraging initial results have prompted further experimental work by MicroBooNE [29] and multiple simulation-based studies considering the implications for reconstruction of both high- and low-energy physics events [30,31]

  • Final-state interactions (FSIs) of the outgoing charged lepton with the Coulomb field of the nucleus have a significant effect on the cross section at low energies

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Summary

Background

Large argon-based neutrino detectors, such as those planned for the Deep Underground Neutrino Experiment, have the potential to provide unique sensitivity to low-energy (few to tens of MeV) electron neutrinos produced by core-collapse supernovae. Despite their importance for neutrino energy reconstruction, nuclear de-excitations following charged-current νe absorption on 40Ar have never been studied in detail at supernova energies. Purpose: I develop a model of nuclear de-excitations that occur following the 40Ar(νe, e−) 40K∗ reaction This model is applied to the calculation of exclusive cross sections. Given a suitable calculation of the inclusive cross section, the MARLEY nuclear de-excitation model may readily be applied to other scattering processes

INTRODUCTION
INCLUSIVE CROSS-SECTION MODEL
Allowed approximation
Coulomb corrections
ALLOWED NUCLEAR MATRIX ELEMENTS
Re-evaluation of existing measurements
Extension to higher excitation energies
Adopted matrix elements
NUCLEAR DE-EXCITATION MODEL
Bound states
Unbound states
Differential decay widths
Fragment transmission coefficients
Transitions to discrete nuclear levels
Nuclear level density
RESULTS
Inclusive cross section
Electron angle and energy distributions
Neutrino energy reconstruction
SUMMARY AND CONCLUSIONS
Ea E f
Total level density
Spin dependence
Nucleon projectiles
Complex projectiles
Methods
Full Text
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