Abstract

Non-standard neutrino self interactions (NSSI) could be stronger than Fermi interactions. We investigate the ability to constrain these four-neutrino interactions by their effect on the flux of neutrinos originating from a galactic supernova. In the dense medium of a core collapse supernova, these new self interactions can have a significant impact on neutrino oscillations, leading to changes at the flavor evolution and spectra level. We use simulations of the neutrino flux from a 13 solar mass, core collapse supernova at 10 kpc away, and numerically propagate these neutrinos through the stellar medium taking into account vacuum/MSW oscillations, SM ν − ν scattering as well as ν − ν interactions that arise from NSSI. We pass the resulting neutrino flux to a simulation of the future Hyper-Kamiokande detector to see what constraints on NSSI parameters are possible when the next galactic supernova becomes visible. We find that these constraints depend strongly on the neutrino mass hierarchy and if the NSSI is flavor-violating or preserving. Sensitivity to NSSI in the normal hierarchy (NH) at Hyper-K is limited by the experiment’s ability to efficiently detect νe, but deviations from no NSSI could be seen if the NSSI is particularly strong. In the inverted hierarchy (IH) scenario, Hyper-K can significantly improve constraints on flavor-violating NSSI down to mathcal{O} (10−1)GF.

Highlights

  • SN1987A with the time period over which the neutrinos were detected [7]

  • We develop simple physical observables to examine in the event of future galactic supernova and estimate the sensitivity of Hyper-K to NSSI after applying these more realistic simulations of neutrino flux and detector response

  • We show the number of inverse beta decay (IBD) and elastic scattering (ES) events vs. time for both the normal hierarchy (NH) and inverted hierarchy (IH), for no NSSI, {g1, g3} = {0, 0.2} (FP-NSSI), and {g1, g3} = {0.2, 0} (FV-NSSI)

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Summary

Neutrino production in core collapse supernova

We begin with a brief description of the current picture of neutrino production in a core collapse supernova. The core stops collapsing and rebounds, sending a shockwave outwards, dissipating energy by photodissociation of nuclei leaving behind a plethora of free nucleons These nucleons capture electrons, producing a large number of νe which pile up behind the shock wave, until they reach a zone of low enough density and are released in a few milliseconds. This is known as the neutronization burst. The left plot of figure 1 covers the whole time profile from infall to 20 seconds where the initial spike of νe from the neutronization burst is prominent, followed by an increase in flux of νx (x is any other (anti)lepton flavor) over the accretion phase. The right plot shows the cooling phase from ∼ 1 second on, showing the near degeneracy of the flux between all flavors

NSSI and neutrino transport in supernova simulations
Computational approach and simulation results
Standard oscillation — no NSSI
NSSI added
Hyper-K sensitivity to NSSI
Findings
Conclusion
Full Text
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