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April 3, 20261 citationsOpen Access

Neutrino quantum kinetics in three flavors

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SSShashank ShalgarITIrene Tamborra

Key Points

  • This research aims to understand the role of neutrino flavor conversion in supernova mechanisms through quantum kinetic equations.
  • Analyzed neutrino quantum kinetic equations in three flavors without attenuation terms.
  • Considered advection and non-forward collisions in a spherically symmetric shell around neutrino decoupling.
  • Utilized two post-bounce times (0.25 s and 1 s) to examine flavor dynamics and heating rates.
  • Flavor equipartition achieved at tpb = 1 s; (anti)neutrino emissions among flavors become similar.
  • No equipartition at early tpb = 0.25 s; flavor conversion dynamics differ significantly.
  • Neutrino heating rate increases by up to 30% when flavor conversion is included.

Abstract

The impact of neutrino flavor conversion on the supernova mechanism is yet to be fully understood. We present multi-energy and multi-angle solutions of the neutrino quantum kinetic equations in three flavors, without employing any attenuation term for the neutrino self-interaction strength and taking into account neutrino advection and non-forward collisions with the background medium. Flavor evolution is explored within a spherically symmetric shell surrounding the region of neutrino decoupling in the interior of a core-collapse supernova, relying on the output of a spherically symmetric core-collapse supernova model with a progenitor mass of 18.6 M circle dot. We select two representative post-bounce times: tpb = 0.25 s (no angular crossings are present and flavor conversion is triggered by slow collective effects) and tpb = 1 s (angular crossings trigger fast flavor instabilities). We find that flavor equipartition is achieved for the late post-bounce time (tpb = 1 s), where the (anti)neutrino emission properties among different flavors tend to approach each other. In this case, nue tends to nux = (numu + nutau)/2 and a similar trend holds for neutrinos. However, flavor equipartition does not occur for our early post-bounce time (tpb = 0.25 s). Accounting for weak-magnetism corrections, crossings in the mu and tau lepton number angular distributions arise; however, such crossings have a magnitude smaller than the one occurring in the electron sector and negligibly affect flavor evolution. Because of flavor conversion, the neutrino heating rate increases up to 30% with respect to the case where flavor conversion is neglected.

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Cite This Study

Shalgar et al. (2025) studied this question.

synapsesocial.com/papers/69cf5db15a333a821460ba2ehttps://doi.org/10.1088/1475-7516/2025/12/026
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