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arxiv: 1106.1167 · v2 · pith:5N63FLQJnew · submitted 2011-06-06 · 🌌 astro-ph.SR · hep-ph· nucl-th

The Role of Collective Neutrino Flavor Oscillations in Core-Collapse Supernova Shock Revival

classification 🌌 astro-ph.SR hep-phnucl-th
keywords neutrinocore-collapseflavoroscillationscollectiveshocksupernovaeffects
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We explore the effects of collective neutrino flavor oscillations due to neutrino-neutrino interactions on the neutrino heating behind a stalled core-collapse supernova shock. We carry out axisymmetric (2D) radiation-hydrodynamic core-collapse supernova simulations, tracking the first 400 ms of the post-core-bounce evolution in 11.2 solar mass and 15 solar mass progenitor stars. Using inputs from these 2D simulations, we perform neutrino flavor oscillation calculations in multi-energy single-angle and multi-angle single-energy approximations. Our results show that flavor conversions do not set in until close to or outside the stalled shock, enhancing heating by not more than a few percent in the most optimistic case. Consequently, we conclude that the postbounce pre-explosion dynamics of standard core-collapse supernovae remains unaffected by neutrino oscillations. Multi-angle effects in regions of high electron density can further inhibit collective oscillations, strengthening our conclusion.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Flavor Conversion Enhances or Suppresses Supernova Explodability Independent of the Progenitor Mass

    astro-ph.HE 2026-05 unverdicted novelty 5.0

    Neutrino flavor conversion in supernova cores can enhance or suppress explodability depending on the conversion location, independent of progenitor mass.

  2. Neutrino Flavor Conversion Shapes the Rate of Failed Core-collapse Supernovae

    astro-ph.HE 2026-05 unverdicted novelty 5.0

    Simulations of 195 stellar progenitors indicate that neutrino flavor conversion alters explodability and remnant mass distributions, particularly for stars of 16-30 solar masses.