Neutrinos from core-collapse supernovae

arXiv:2509.16306 · astro-ph.HE, hep-ph · Submitted 2025-09-19 · Read on arXiv

astro-ph.HE, hep-ph

Submitted: 2025-09-19

Updated: 2026-03-28

Comments: To be published in the Encyclopedia of Particle Physics (in a different format), final version with a few additional references

Journal ref: Encycl. Part. Phys. 3 (2026) 307-349

DOI: 10.1016/B978-0-443-26598-3.00065-1

Code: https://github.com/sebhoof/snax

Project page: https://snews2.org

License: http://creativecommons.org/licenses/by/4.0/

The gist: The core of a massive star (M > 8 Msun) eventually collapses.

Terminology

Abstract

The core of a massive star (M > 8 Msun) eventually collapses. This implosion usually triggers a supernova (SN) explosion that ejects most of the stellar envelope and leaves behind a neutron star (NS) with a mass of up to about 2 Msun. Sometimes the explosion fails and a black hole forms instead. The NS radiates its immense binding energy (some 10% of its rest mass or 2-4 times10 53 erg) almost entirely as neutrinos and antineutrinos of all flavors with typical energies of some 10 MeV. This makes core-collapse SNe the most powerful neutrino factories in the Universe. Such a signal was observed once - with limited statistics - from SN 1987A in the Large Magellanic Cloud. Today, however, many large neutrino detectors act as SN observatories and would register a high-statistics signal. A future Galactic SN, though rare (1-3 per century), would produce a wealth of astrophysical and particle-physics information, including possible signatures for new particles. Neutrinos are key to SN dynamics in the framework of the Bethe-Wilson delayed explosion paradigm. After collapse, they are trapped in the core for a few seconds, forming a dense neutrino plasma that can exhibit collective flavor evolution caused by the weak interaction, a subject of intense theoretical research.

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