Determining the Neutrino Mass Hierarchy from the Next Galactic Supernova ✛ ✦

Original: "Neutrino mass ordering from the next Galactic supernova at DUNE, HK, and JUNO"
arXiv:2606.06580v1 · 2026-06-04 · CC BY 4.0 · 5 min
The neutrino signal from a future massive star explosion in the Milky Way will allow us to establish whether neutrino masses are normally or inversely ordered.

Context

Supernova explosions are grand cosmic events in which a massive star, having exhausted its nuclear fuel, collapses, giving birth to a neutron star or a black hole. In a matter of seconds, energy comparable to the total radiation of an entire galaxy is released, and 99% of it is carried away by neutrinos—particles predicted by Wolfgang Pauli back in 1930. Supernova explosions also serve as the main factories of heavy elements and cosmic dust, spreading them throughout the Galaxy. Studying the neutrino signal from the next supernova, which is expected in the Milky Way at any moment, will not only unravel the explosion mechanism but also answer a fundamental question: how are the masses of the three types of neutrinos ordered—normally or inversely? This knowledge is critically important for understanding dark matter and the expansion of the Universe, since neutrinos, though nearly elusive, contribute to the cosmological balance.

Methods

The analysis used results from hydrodynamic simulations of supernova core collapse from the Garching Group with progenitor masses from 12 to 27 solar masses. It is important to note that the fate of the collapsing core depends on the mass limit established by Subrahmanyan Chandrasekhar. The initial neutrino fluxes underwent flavor conversion according to three scenarios: standard MSW oscillations for normal (NO) and inverted (IO) hierarchy, as well as a full exchange (FE) scenario, which could arise from fast collective effects in the dense medium where entropy and density reach extreme values. Using the SNOwGLoBES package, expected events were calculated in detectors: DUNE (liquid argon, 40 kt), Hyper-Kamiokande (water, 187 kt), and JUNO (liquid scintillator, 20 kt), located at a distance of 10 kpc from the supernova. The statistical analysis included the chi-squared method for both time-dependent spectra and integral characteristics—cumulative events and their ratio at 20 and 100 ms—thus circumventing model uncertainties.

Results

The neutronization burst, a sharp peak of electron neutrinos lasting about 20–30 milliseconds, turned out to be an almost model-independent indicator: for the inverted hierarchy it is clearly visible, while for the normal hierarchy it is practically absent. In the DUNE detector, the sensitivity to hierarchy discrimination exceeds 6σ for all considered models, and in Hyper-Kamiokande—at least 4σ. This means that even a single event will give a reliable answer. For the accretion phase, the analysis of the rise in the electron antineutrino flux, caused by the faster increase in the luminosity of heavy-lepton neutrinos, showed that using the ratio of cumulative events at 20 and 100 ms, the significance in HK reaches ∼5σ, and in JUNO—∼3σ. Thus, combining data from several detectors and different explosion phases will provide multiple cross-checks of the result. Interestingly, the FE scenario, predicted in some models of collective oscillations, somewhat reduces the contrast but does not destroy it completely, leaving an opportunity to test the theory of collective effects itself.

Implications

The results confirm that the next galactic supernova will most likely finally clarify the neutrino mass hierarchy—a task that accelerator and reactor experiments have not yet been able to solve. Back in the mid-20th century, the pioneer of neutrino astrophysics John Wheeler discussed the possibility of obtaining information about processes in stellar interiors precisely through neutrinos. This measurement has far-reaching consequences: it will constrain the spectrum of allowed theoretical models in particle physics, influence our understanding of the Big Bang and the subsequent evolution of the Universe. Just as the cosmic microwave background serves as an echo of the hot Universe, the neutrino background carries information about the first moments of creation. Success in determining the hierarchy will also shed light on the nature of collective neutrino oscillations, which represent new, not yet fully understood physics.

Future development

Further improvement of three-dimensional hydrodynamic simulations including magnetic fields and rotation will allow refinement of neutrino luminosities and reduction of systematic errors. Planned upgrades of detectors, including Hyper-Kamiokande and DUNE, as well as the commissioning of new neutrino telescopes such as IceCube-Gen2, will increase statistical significance. Of particular interest is the theoretical investigation of fast collective oscillations—a phenomenon that could radically change the picture of neutrino flavors in the supernova interior. Joint analysis of neutrino data with gravitational-wave and electromagnetic observations within the framework of multimessenger astronomy will become standard upon detection of the next galactic supernova.

Impact

Determining the neutrino mass hierarchy will impact elementary particle physics, nuclear physics, astrophysics, and cosmology. In astrophysics, it will improve understanding of supernova explosion mechanisms and the formation of compact objects—neutron stars and black holes. In cosmology, it will refine models of large-scale structure formation and the contribution of neutrinos to dark matter.

Next steps

A key step will be the development and testing of rapid alert protocols for all operating neutrino observatories, so that upon detecting a burst, immediate pointing of optical, X-ray, and gravitational-wave instruments is ensured. It is also necessary to continue theoretical studies of collective neutrino oscillations under realistic conditions of a collapsing core.

Key open problems

The neutrino mass hierarchy problem is closely linked to other fundamental questions: why fermion masses differ so greatly, whether a sterile neutrino exists, and what the nature of dark matter is. The neutrino signal from a supernova can also provide unique information about the equation of state of nuclear matter at supranuclear densities, which is important for understanding the structure of neutron stars and gravitational-wave signals from their mergers.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

The study employs hydrodynamic models of core collapse, neutrino flavor transformation, and calculations of expected events in the DUNE, Hyper-Kamiokande, and JUNO detectors. The analysis shows that the neutronization burst is an almost model-free indicator of the mass hierarchy: it is clearly visible for the inverted hierarchy and practically absent for the normal one, with a sensitivity exceeding 6σ in DUNE. For the accretion phase, the ratio of cumulative events at 20 and 100 ms yields a significance of up to 5σ in Hyper-Kamiokande.

Where its strength is

The key strength is the use of the neutronization burst as an almost model-free indicator, which reduces dependence on supernova model uncertainties. This allows achieving high statistical significance even from a single event, making the result robust.

Where it could go next

Worth trying

  • Test how including pre-supernova neutrinos could improve the time window for determining the hierarchy.
  • Use data from SN 2021foa to calibrate detector responses to the neutronization burst.
  • Assess the impact of fast collective oscillations on the visibility of the neutronization burst in different models.

Why this may matter

Determining the neutrino mass hierarchy from the next supernova could answer a fundamental question in particle physics that is difficult to address in terrestrial experiments, while also improving our understanding of supernova explosion mechanisms.

Original abstract

as written by the authors arXiv:2606.06580v1

The next Galactic core-collapse supernova (CCSN) will offer a unique opportunity to determine the neutrino mass ordering. We focus on two observables: the electron neutrino ($$ u_e$$) neutronization burst and the rise-time of the electron antineutrino ($$\bar{ u}_e$$) flux during the accretion phase. The neutronization burst, a sharp $$ u_e$$ peak within $$\sim 20$$-$$30$$ ms, provides a clean and robust signature of mass ordering through its appearance or disappearance. During the accretion phase, the faster rise of heavy lepton flavor neutrinos ($$ u_x$$) leads to a distinct faster rise-time behavior of the oscillated $$\bar{ u}_e$$ signal, resulting in mass ordering discrimination. Using realistic CCSN simulations for multiple progenitor masses, we compute event rates and perform a statistical analysis for a Galactic ($$10$$~kpc) CCSN event at DUNE, Hyper-Kamiokande (HK), and JUNO detectors. The neutronization burst remains largely independent of SN hydrodynamic simulation models, with DUNE and HK achieving $$\gtrsim 6\sigma$$ and $$\gtrsim 4\sigma$$ sensitivity for normal (NO) to inverted ordering (IO) discrimination, respectively. However, the rise-time observable is prone to progenitor degeneracies. To mitigate this cumulative and ratio-based observables constructed at characteristic timescales ($$20$$ ms & $$100$$ ms) are used. The resulting confidence levels from the rise-time analysis to discriminate IO/NO in HK and JUNO are $$\sim 5\sigma$$ and $$\sim 3\sigma$$, respectively. Our results highlight the complementarity of detectors and observables, and demonstrate that combining neutronization burst and accretion phase information will be crucial for a definitive determination of the neutrino mass ordering in the next Galactic supernova.

In the first 20 milliseconds of the neutronization burst, so many neutrinos are emitted that on Earth, despite tens of thousands of light-years distance, the DUNE detector will register about 100 events. For comparison, a year of observing solar neutrinos in a similar detector yields roughly the same number.

F_{\bar{\nu}_e}^{\text{NO}} = \cos^2\theta_{12} F^0_{\bar{\nu}_e} + \sin^2\theta_{12} F^0_{\nu_x}
The oscillated flux is a mixture of the original antineutrino flux and the heavy-lepton neutrino flux, weighted by the squares of the sine and cosine of the mixing angle θ12.

Key numbers

  • total number of emitted neutrinos: ~1058
  • duration of the neutronization burst: 20–30 ms
  • significance level of hierarchy separation in DUNE: ≳6σ
  • distance to the galactic supernova: 10 kpc
  • mass of the Hyper-Kamiokande detector: 187 kt
Scientists
Paul DiracBernhard RiemannJoseph WeberKarl SchwarzschildKip ThorneRainer Weiss
Concepts
juno neutron star mass limit neutron star structure supernova nucleosynthesis nicer neutrino detection scintillator accretion rate supernova core collapse electron neutrino superdense matter hyper kamiokande stellar explosion dune nuclear stability nuclear reaction mass gap crust nucleon progenitor nustar